GRUNDFOS PUMP User Manual

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PUMP HANDBOOK
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GRUNDFOS Management A/S
Poul Due Jensens Vej 7 DK-8850 Bjerringbro Tel: +45 87 50 14 00
www.grundfos.com
Thinking ahead makes it possible
Innovation is the essence
96563258 1104
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PUMP HANDBOOK
Copyright 2004 GRUNDFOS Management A/S. All rights reserved.
Copyright law and international treaties protect this material. No part of this material may be reproduced in any form or by any means without prior written permission from GRUNDFOS Management A/S.
Disclaimer All reasonable care has been taken to ensure the accuracy of the contents of this material, however GRUNDFOS Management A/S shall not be reliable for any loss whether direct, indirect, incidental or consequential arising out of the use of or reliance upon any of the content of the material.
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Foreword
The manufacturing industry places heavy demand on pumps, when it comes to optimum operation, high reliability and low energy consumption. Therefore, Grundfos has developed the Pump handbook, which in a simple manner deals with various considerations when dimensioning pumps and pump systems. We have elaborated a handbook for engineers and technicians who work with design and installation of pumps and pump systems, containing answers to a wide range of technical pump specific questions. The Pump handbook can either be read from one end to the other or partly on specific topics.
The handbook is divided into 5 chapters which deal with different phases when designing pump systems.
Throughout chapter 1 we make a general presentation of different pump types and components. Here we also describe which precautions to adopt when dealing with viscous liquids. Further, the most used materials as well as different types of corrosion are presented here. The most important terminologies in connection with reading the pump performance are presented in chapter 2. Chapter 3 deals with system hydraulics and some of the most important factors to consider to obtain optimum operation of the pump system. As it is often necessary to adjust the pump performance by means of different adjustment methods, these are dealt with in chapter 4. Chapter 5 describes the life cycle costs as energy consumption plays an important role in today’s pumps and pump systems.
We sincerely hope that you will make use of The pump handbook and find it useful in your daily work.
Segment Director Business Development Manager
Allan Skovgaard Claus Bærnholdt Nielsen
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Chapter 1 Design of pumps and motors ......................7
Section 1.1 Pump construction ............................................................ 8
1.1.1 The centrifugal pump .................................................................. 8
1.1.2 Pump curves ................................................................................................9
1.1.3 Characteristics of the centrifugal pump ......................... 11
1.1.4 Most common end-suction and
in-line pump types .............................................................................. 12
1.1.5 Impeller types (axial forces) .......................................................14
1.1.6 Casing types (radial forces) ......................................................... 15
1.1.7 Single-stage pumps ........................................................................... 15
1.1.8 Multistage pumps ...............................................................................16
1.1.9 Long-coupled and close-coupled pumps ........................16
Section 1.2 Types of pumps ...................................................................17
1.2.1 Standard pumps .................................................................................... 17
1.2.2 Split-case pumps .................................................................................. 17
1.2.3 Hermetically sealed pumps ........................................................18
1.2.4 Sanitary pumps ..................................................................................... 20
1.2.5 Wastewater pumps ............................................................................21
1.2.6 Immersible pumps .............................................................................. 22
1.2.7 Borehole pumps ....................................................................................23
1.2.8 Positive displacement pumps ...................................................24
Section 1.3 Mechanical shaft seals ..................................................27
1.3.1 The mechanical shaft seal’s
components and function ............................................................29
1.3.2 Balanced and unbalanced shaft seals .............................. 30
1.3.3 Types of mechanical shaft seals .............................................31
1.3.4 Seal face material combinations ...........................................34
1.3.5 Factors affecting the seal performance ...........................36
Section 1.4 Motors .................................................................................... 39
1.4.1 Standards .................................................................................................... 40
1.4.2 Motor start-up .......................................................................................46
1.4.3 Voltage supply ........................................................................................47
1.4.4 Frequency converter ..........................................................................47
1.4.5 Motor protection ................................................................................. 49
Section 1.5 Liquids .......................................................................................53
1.5.1 Viscous liquids ........................................................................................54
1.5.2 Non-Newtonian liquids .................................................................. 55
1.5.3 The impact of viscous liquids on the
performance of a centrifugal pump .................................... 55
1.5.4 Selecting the right pump for a liquid
with antifreeze .......................................................................................56
1.5.5 Calculation example ..........................................................................58
1.5.6 Computer aided pump selection for dense and
viscous liquids .........................................................................................58
Section 1.6 Materials ................................................................................ 59
1.6.1 What is corrosion? .............................................................................. 60
1.6.2 Types of corrosion ................................................................................61
1.6.3 Metal and metal alloys ...................................................................65
1.6.4 Ceramics ....................................................................................................... 71
1.6.5 Plastics ............................................................................................................ 71
1.6.6 Rubber ............................................................................................................72
1.6.7 Coatings ........................................................................................................73
Chapter 2 Installation and performance
reading .............................................................................................................75
Section 2.1 Pump installation ............................................................76
2.1.1 New installation ....................................................................................76
2.1.2 Existing installation-replacement ........................................76
2.1.3 Pipe flow for single-pump installation ............................. 77
2.1.4 Limitation of noise and vibrations .......................................78
2.1.5 Sound level (L) .........................................................................................81
Section 2.2 Pump performance ........................................................ 83
2.2.1 Hydraulic terms .....................................................................................83
2.2.2 Electrical terms ...................................................................................... 90
2.2.3 Liquid properties ...................................................................................93
Table of Contents
Page 6
Chapter 3 System hydraulic ....................................................95
Section 3.1 System characteristics .................................................96
3.1.1 Single resistances .................................................................................97
3.1.2 Closed and open systems ............................................................ 98
Section 3.2 Pumps connected in series and parallel
...................101
3.2.1 Pumps in parallel ................................................................................101
3.2.2 Pumps connected in series ....................................................... 103
Chapter 4 Performance adjustment
of pumps ..................................................................................................... 105
Section 4.1 Adjusting pump performance ..............................106
4.1.1 Throttle control ....................................................................................107
4.1.2 Bypass control .......................................................................................107
4.1.3 Modifying impeller diameter ................................................. 108
4.1.4 Speed control ........................................................................................ 108
4.1.5 Comparison of adjustment methods ...............................110
4.1.6 Overall efficiency of the pump system ........................... 111
4.1.7 Example: Relative power consumption
when the flow is reduced by 20% ........................................ 111
Section 4.2 Speed-controlled pump solutions .................... 114
4.2.1 Constant pressure control ..........................................................114
4.2.2 Constant temperature control ...............................................115
4.2.3 Constant differential pressure in a
circulating system ............................................................................. 115
4.2.4 Flow-compensated differential
pressure control ...................................................................................116
Section 4.3 Advantages of speed control .................................117
Section 4.4 Advantages of pumps with integrated
frequency converter ............................................................................... 118
4.4.1 Performance curves of speed-controlled
pumps ...........................................................................................................119
4.4.2 Speed-controlled pumps in different systems ........119
Section 4.5 Frequency converter .................................................... 122
4.5.1 Basic function and characteristics ......................................122
4.5.2 Components of the frequency converter .....................122
4.5.3 Special conditions regarding frequency
converters ................................................................................................124
Chapter 5 Life cycle costs calculation ....................... 127
Section 5.1 Life cycle costs equation ............................................ 128
5.1.1 Initial costs, purchase price (Cic) ........................................... 129
5.1.2 Installation and commissioning costs (Cin) ................ 129
5.1.3 Energy costs (Ce) ................................................................................. 130
5.1.4 Operating costs (Co) ......................................................................... 130
5.1.5 Environmental costs (C
env
) ......................................................... 130
5.1.6 Maintenance and repair costs (Cm) .....................................131
5.1.7 Downtime costs, loss of production (Cs) .......................131
5.1.8 Decommissioning and disposal costs (Co) ...................131
Section 5.2 Life cycle costs calculation
– an example ................................................................................................132
Appendix .........................................................................................................133
A) Notations and units .........................................................................134
B) Unit conversion tables ...................................................................135
C) SI-prefixes and Greek alphabet ............................................ 136
D) Vapour pressure and density of water at
different temperatures ................................................................. 137
E) Orifice ..........................................................................................................138
F) Change in static pressure due to change
in pipe diameter ................................................................................. 139
G) Nozzles ........................................................................................................140
H) Nomogram for head losses in
bends, valves, etc. ..............................................................................141
I) Pipe loss nomogram for clean water 20˚C ..................142
J) Periodical system ................................................................................143
K) Pump standards ................................................................................. 144
L) Viscosity for different liquids as a function
of liquid temperature ....................................................................145
Index ..................................................................................................................151
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Chapter 1. Design of pumps and motors
Section 1.1: Pump construction
1.1.1 The centrifugal pump
1.1.2 Pump curves
1.1.3 Characteristics of the centrifugal pump
1.1.4 Most common end-suction and in-line pump types
1.1.5 Impeller types (axial forces)
1.1.6 Casing types (radial forces)
1.1.7 Single-stage pumps
1.1.8 Multistage pumps
1.1.9 Long-coupled and close-coupled pumps
Section 1.2: Types of pumps
1.2.1 Standard pumps
1.2.2 Split-case pumps
1.2.3 Hermetically sealed pumps
1.2.4 Sanitary pumps
1.2.5 Wastewater pumps
1.2.6 Immersible pumps
1.2.7 Borehole pumps
1.2.8 Positive displacement pumps
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Section 1.1 Pump construction
1.1.1 The centrifugal pump
In 1689 the physicist Denis Papin invented the centrifugal pump and today this kind of pump is the most used around the world. The centrifugal pump is built on a simple principle: Liquid is led to the impeller hub and by means of the centrifugal force it is flung towards the periphery of the impellers. The construction is fairly inexpensive, robust and simple and its high speed makes it possible to connect the pump directly to an asynchronous motor. The centrifugal pump provides a steady liquid flow, and it can easily be throttled without causing any damage to the pump.
Now let us have a look at figure 1.1.1, which shows the liquid’s flow through the pump. The inlet of the pump leads the liquid to the centre of the rotating impeller from where it is flung towards the periphery. This construction gives a high efficiency, and is suitable for handling pure liquids. Pumps, which have to handle impure liquids, such as wastewater pumps, are fitted with an impeller that is constructed especially to avoid that objects get stocked inside the pump, see section 1.2.5.
If a pressure difference occurs in the system while the centrifugal pump is not running, liquid can still pass through it due to its open design.
As you can tell from figure 1.1.2, the centrifugal pump can be categorised in different groups: Radial flow pumps, mixed flow pumps and axial flow pumps. Radial flow pumps and mixed flow pumps are the most common types used. Therefore, we will only concentrate on these types of pumps on the following pages.
However, we will briefly present the positive displacement pump in section 1.2.8.
The different demands on the centrifugal pump’s performance, especially with regards to head, flow, and installation, together with the demands for economical operation, are only a few of the reasons why so many types of pump exist. Figure 1.1.3 shows the different pump types with regard to flow and pressure.
Fig. 1.1.2: Different kinds of centrifugal pumps
Fig. 1.1.1: The liquid’s flow through the pump
Radial flow pump
Mixed flow pump
Axial flow pump
Fig. 1.1.3: Flow and head for different types of centrifugal pumps
1 22446610
1
10
1
2
4
6
10
2
2
4
6
10
3
2
4
6
10
4
H
[m]
Q [m
3
/s]
2 4 6 10
2
2 4 6 10
3
2 4 6 10
4
2 4 6 10
5
Multistage radial flow pumps
Single-stage radial flow pumps
Mixed flow pumps
Axial flow pumps
8
Page 9
1.1.2 Pump curves
Before we dig any further into the world of pump construction and pump types, we will present the basic characteristics of pump performance curves. The performance of a centrifugal pump is shown by a set of performance curves. The performance curves for a centrifugal pump are shown in figure 1.1.4. Head, power consumption, efficiency and NPSH are shown as a function of the flow.
Normally, pump curves in data booklets only cover the pump part. Therefore, the power consumption, the P2­value, which is listed in the data booklets as well, only covers the power going into the pump – see figure 1.1.4. The same goes for the efficiency value, which only covers the pump part (η = ηP).
In some pump types with integrated motor and possibly integrated frequency converter, e.g. canned motor pumps (see section 1.2.3), the power consumption curve and the η-curve cover both the motor and the pump. In this case it is the P1-value that has to be taken into account.
In general, pump curves are designed according to ISO 9906 Annex A, which specifies the tolerances of the curves:
Q +/- 9%,
H +/-7%,
P +9%
-7%.
What follows is a brief presentation of the different pump performance curves.
Head, the QH-curve
The QH-curve shows the head, which the pump is able to perform at a given flow. Head is measured in meter liquid column [mLC]; normally the unit meter [m] is applied. The advantage of using the unit [m] as the unit of measurement for a pump’s head is that the QH-curve is not affected by the type of liquid the pump has to handle, see section 2.2 for more information.
H
[m]
η
[%]
50
40
70
Efficiency
60
50
40
20
10
2
12
4
6
8
10
0
30
30
20
10
0
10
0
2
4
6
8
0 10 20 30 40 50 60 70
Q [m3/h]
P
2
[kW]
NP
SH
(m)
Power consumption
NP
SH
Fig. 1.1.4: Typical performance curves for a centrifugal pump. Head, power consumption, efficiency and NPSH are shown as a function of the flow
Fig. 1.1.5: The curves for power consumption and efficiency will normally only cover the pump part of the unit – i.e. P2 and η
P
P
1
P
2
HM
3~
η
M η
P
Q
H
[m]
50
60
40
30
20
10
0
0 10 20 30 40 50 60 70 80
Q [m3/h]
Fig. 1.1.6: A typical QH-curve for a centrifugal pump; low flow results in high head and high flow results in low head
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Efficiency, the η-curve
The efficiency is the relation between the supplied power and the utilised amount of power. In the world of pumps, the efficiency ηP is the relation between the power, which the pump delivers to the water (PH) and the power input to the shaft (P2 ):
where:
ρ is the density of the liquid in kg/m
3
, g is the acceleration of gravity in m/s2, Q is the flow in m3/s and H is the head in m.
For water at 20oC and with Q measured in m3/h and H in m, the hydraulic power can be calculated as :
As it appears from the efficiency curve, the efficiency depends on the duty point of the pump. Therefore, it is important to select a pump, which fits the flow requirements and ensures that the pump is working in the most efficient flow area.
Power consumption, the P2-curve
The relation between the power consumption of the pump and the flow is shown in figure 1.1.8. The P2-curve of most centrifugal pumps is similar to the one in figure 1.1.8 where the P2 value increases when the flow increases.
NPSH-curve (Net Positive Suction Head)
The NPSH-value of a pump is the minimum absolute pressure (see section 2.2.1) that has to be present at the suction side of the pump to avoid cavitation. The NPSH-value is measured in [m] and depends on the flow; when the flow increases, the NPSH-value increases as well; figure 1.1.9. For more information concerning cavitation and NPSH, go to section 2.2.1.
50
60
70
80
40
30
20
10
0
0 10 20 30 40 50 60 70
Q [m3/h]
η
[%]
8
10
6
4
2 0
0 10 20 30 40 50 60 70
Q [m3/h]
P
2
[kW]
Fig. 1.1.7: The efficiency curve of a typical centrifugal pump
Fig. 1.1.8: The power consumption curve of a typical centrifugal pump
10
0
2
4
6
8
0 10 20 30 40 50 60 7
0
Q [m3/h]
NPSH
[m]
η
p
=
PH P
2
=
ρ . g . Q . H
P
2
Fig. 1.1.9: The NPSH-curve of a typical centrifugal pump
PH = 2.72
.
Q . H [W]
10
Section 1.1 Pump construction
Page 11
1.1.3 Characteristics of the centrifugal pump
The centrifugal pump has several characteristics and in this section, we will present the most important ones. Later on in this chapter we will give a more thorough description of the different pump types.
• The number of stages
Depending on the number of impellers in the pump, a centrifugal pump can be either a single-stage pump or a multistage pump.
• The position of the pump shaft
Single-stage and multistage pumps come with horizontal or vertical pump shafts. These pumps are normally designated horizontal or vertical pumps. For more information, go to section 1.1.4.
• Single-suction or double-suction impellers
Depending on the construction of the impeller, a pump can be fitted with either a single-suction impeller or a double­suction impeller. For more information, go to section 1.1.5.
• Coupling of stages
The pump stages can be arranged in two different ways: in series and in parallel, see figure 1.1.10.
• Construction of the pump casing
We distinguish between two types of pump casing: Volute casing and return channel casing with guide vanes. For more information, go to section 1.1.6.
Fig 1.1.10: Twin pump with parallel-coupled impellers
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1.1.4 Most common end-suction and in-line pump types
End-suction pump = The liquid runs directly into the impeller. Inlet and outlet have a 90° angle. See section 1.1.9
In-line pump = The liquid runs directly through the pump in-line. The suction pipe and the discharge pipe are placed opposite one another and can be mounted directly in the piping system
Split-case pump = Pump with an axially divided pump housing. See section 1.2.2
Horizontal pump = Pump with a horizontal pump shaft
Vertical pump = Pump with a vertical pump shaft
Single-stage pump = Pump with a single impeller. See section 1.1.7
Multistage pump = Pump with several series-coupled stages. See section 1.1.8
Long-coupled pump = Pump connected to the motor by means of a flexible coupling. The motor and the pump have separate bearing constructions. See section 1.1.9
Close-coupled pump = A pump connected to the motor by means of a rigid coupling. See section 1.1.9
Horizontal
Close-coupled Close-coupled
End-suction
Single-stage
Long-coupled
Multistage
12
Section 1.1 Pump construction
Page 13
13
Multistage
Horizontal / Vertical
Single-stage
Long-coupled Close-coupled
Close-coupled
In-line
Split-case
Single-stage
Long-coupled
Horizontal
Page 14
14
1.1.5 Impeller types (axial forces)
A centrifugal pump generates pressure that exerts forces on both stationary and rotating parts of the pump. Pump parts are made to withstand these forces. If axial and radial forces are not counterbalanced in the pump, the forces have to be taken into consideration when selecting the driving system for the pump (angular contact bearings in the motor). In pumps fitted with single-suction impeller, large axial forces may occur, figures 1.1.11 and
1.1.12. These forces are balanced in one of the following ways:
• Mechanically by means of thrust bearings. These types of bearings are specially designed to absorb the axial forces from the impellers
• By means of balancing holes on the impeller, see figure 1.1.13
• By means of throttle regulation from a seal ring mounted on the back of the impellers, see figure 1.1.14
• Dynamic impact from the back of the impeller, see figure 1.1.15
• The axial impact on the pump can be avoided by either using double-suction impellers (see figure 1.1.16).
Fig. 1.1.11: Single-suction impeller
Fig. 1.1.12: Standard pump with single-suction impeller
Fig. 1.1.13: Balancing the axial forces in a single-stage centrifugal pump with balancing holes only
Fig. 1.1.14: Balancing the axial forces in a single-stage centrifugal pump with sealing gap at discharge side and balancing holes
Fig. 1.1.15: Balancing the axial forces in a single-stage centrifugal pump with blades on the back of the impellers
Fig. 1.1.16: Balancing the axial forces in a double-suction impeller arrangement
Axial forces
Section 1.1 Pump construction
Page 15
1.1.6 Casing types (radial forces)
Radial forces are a result of the static pressure in the casing. Therefore, axial deflections may occur and lead to interference between the impeller and the casing. The magnitude and the direction of the radial force depend on the flow rate and the head.
When designing the casing for the pump, it is possible to control the hydraulic radial forces. Two casing types are worth mentioning: the single-volute casing and the double-volute casing. As you can tell from figure 1.1.18, both casings are shaped as a volute. The difference between them is, that the double-volute has an guide vane.
The single-volute pump is characterised by a symmetric pressure in the volute at the optimum efficiency point, which leads to zero radial load. At all other points, the pressure around the impeller is not regular and consequently a radial force is present.
As you can tell from figure 1.1.19, the double-volute casing develops a constant low radial reaction force at any capacity.
Return channels (figure 1.1.20) are used in multistage pumps and have the same basic function as volute casings. The liquid is led from one impeller to the next and at the same time, the rotation of water is reduced and the dynamic pressure is transformed into static pessure. Because of the return channel casing’s circular design, no radial forces are present.
1.1.7 Single-stage pumps
Generally, single-stage pumps are used in applications, which do not require a total head of more than 150 m. Normally, single-stage pumps operate in the interval of 2-100 m.
Single-stage pumps are characterised by providing a low head relative to the flow, see figure 1.1.3. The single-stage pump comes in both a vertical and a horizontal design, see figures 1.1.21 and 1.1.22.
15
Q/Qopt1.0
Volute casing
Double-volute casing
Radial force
Fig. 1.1.18: Single-volute casing Double-volute casing
Fig. 1.1.22: Vertical single-stage in-line close-coupled pump
Fig. 1.1.21: Horizontal single-stage end-suction close-coupled pump
Radial forces
Fig. 1.1.17: Single-suction
impeller
Fig. 1.1.19: Radial force for single- and double-volute casing
Fig. 1.1.20: Vertical multistage in-line pump with return channel casing
Return channel
Page 16
Fig. 1.1.25: Long-coupled pump with basic coupling
Fig. 1.1.26: Long-coupled pump with spacer coupling
16
1.1.8 Multistage pumps
Multistage pumps are used in installations where a high head is needed. Several stages are connected in series and the flow is guided from the outlet of one stage to the inlet of the next. The final head that a multistage pump can deliver is equal to the sum of pressure each of the stages can provide.
The advantage of multistage pumps is that they provide high head relative to the flow. Like the single-stage pump, the multistage pump is available in both a vertical and a horizontal version, see figures 1.1.23 and 1.1.24.
1.1.9 Long-coupled and close-coupled pumps
Long-coupled pumps
Long-coupled pumps are pumps with a flexible coupling that connects the pump and the motor. This kind of coupling is available either as a basic coupling or as a spacer coupling.
If the pump is connected to the motor by a basic coupling, it is necessary to dismount the motor when the pump needs service. Therefore, it is necessary to align the pump upon mounting, see figure 1.1.25.
On the other hand, if the pump is fitted with a spacer coupling, it is possible to service the pump without dismounting the motor. Alignment is thus not an issue, see figure 1.1.26.
Close-coupled pumps
Close-coupled pumps can be constructed in the following two ways: Either the pump has the impeller mounted directly on the extended motor shaft or the pump has a standard motor and a rigid or a spacer coupling, see figures
1.1.27 and 1.1.28.
Fig. 1.1.24: Horizontal multistage end-suction pump
Fig. 1.1.23: Vertical multistage in-line pump
Fig. 1.1.27: Close-coupled pump with rigid coupling
Basic coupling type
Long-coupled pump with flexible coupling
Close-coupled pump with rigid coupling
Spacer coupling (option)
Fig. 1.1.28: Different coupling types
Section 1.1 Pump construction
Page 17
17
Fig. 1.2.1: Long-coupled standard pump
Fig. 1.2.2: Bare shaft standard pump
Fig. 1.2.3: Long-coupled split-case pump
Fig. 1.2.4: Split-case pump with double-suction impeller
1.2.1 Standard pumps
Few international standards deal with centrifugal pumps. In fact, many countries have their own standards, which more or less overlap one another. A standard pump is a pump that complies with official regulations as to for example the pump’s duty point. What follows, are a couple of examples of international standards for pumps:
• EN 733 (DIN 24255) applies to end-suction centrifugal pumps, also known as standard water pumps with a rated pressure (PN) of 10 bar.
• EN 22858 (ISO 2858) applies to centrifugal pumps, also known as standard chemical pumps with a rated pressure (PN) of 16 bar, see appendix K.
The standards mentioned above cover the installation dimensions and the duty points of the different pump types. As to the hydraulic parts of these pump types, they vary according to the manufacturer – thus, no international standards are set for these parts.
Pumps, which are designed according to standards, provide the end-user with advantages with regard to service, spare parts and maintenance.
1.2.2 Split-case pumps
A split-case pump is a pump with the pump housing divided axially into two parts. Figure 1.2.4 shows a single­stage split-case pump with a double-suction impeller. The double-inlet construction eliminates the axial forces and ensures a longer life span of the bearings. Usually, split-case pumps have a rather high efficiency, are easy to service and have a wide performance range.
Section 1.2 Types of pumps
Page 18
Section 1.2 Types of pumps
18
1.2.3 Hermetically sealed pumps
It comes as no surprise that a pump’s shaft lead-in has to be sealed. Usually, this is done by means of a mechanical shaft seal, see figure 1.2.5. The disadvantage of the mechanical shaft seal is its poor properties when it comes to handling of toxic and aggressive liquids, which consequently leads to leakage. These problems can to some extent be solved by using a double mechanical shaft seal. Another solution to these problems is to use a hermetically sealed pump.
We distinguish between two types of hermetically sealed pumps: Canned motor pumps and magnetic-driven pumps. In the following two sections, you can find additional information about these pumps.
Canned motor pumps
A canned motor pump is a hermetically sealed pump with the motor and pump integrated in one unit without a seal, see figures 1.2.6 and 1.2.7. The pumped liquid is allowed to enter the rotor chamber that is separated from the stator by a thin rotor can. The rotor can serves as a hermetically sealed barrier between the liquid and the motor. Chemical pumps are made of materials, e.g. plastics or stainless steel that can withstand aggressive liquids.
The most common canned motor pump type is the circulator pump. This type of pump is typically used in heating circuits because the construction provides low noise and maintenance-free operation.
Fig. 1.2.5: Example of a standard pump with mechanical shaft seal
Liquid
Atmosphere
Seal
Fig. 1.2.7: Circulator pump with canned motor
Motor can
Fig. 1.2.6: Chemical pump with canned motor
Motor can
Page 19
Magnetic-driven pumps
In recent years, magnetic-driven pumps have become increasingly popular for transferring aggressive and toxic liquids.
As shown in figure 1.2.8, the magnetic-driven pump is made of two groups of magnets; an inner magnet and an outer magnet. A non-magnetizable can separate these two groups. The can serves as a hermetically sealed barrier between the liquid and the atmosphere. As it appears from figure 1.2.9, the outer magnet is connected to the pump drive and the inner magnet is connected to the pump shaft. Hereby the torque from the pump drive is transmitted to the pump shaft. The pumped liquid serves as lubricant for the bearings in the pump. Therefore, sufficient venting is crucial for the bearings.
19
Fig. 1.2.8: Construction of magnetic drive
Fig. 1.2.9: Magnetic-driven multistage pump
Can
Inner magnets
Outer magnets
Can
Inner magnets
Outer magnets
Page 20
20
Fig. 1.2.10: Sanitary pump
Fig.1.2.11: Sanitary self-priming side-channel pump
1.2.4 Sanitary pumps
Sanitary pumps are mainly used in the food, beverage, pharmaceutical and bio-technological industries where it is important that the pumped liquid is handled in a gentle manner and that the pumps are easy to clean.
In order to meet process requirements in these industries, the pumps have to have a surface roughness between
3.2 and 0.4 µm Ra. This can be best achieved by using forged or
deep-drawn rolled stainless steel as materials
of construction,
see figure 1.2.12. These materials have a compact pore-free surface finish that can be easily worked up to meet the various surface finish requirements.
The main features of a sanitary pump are ease of cleaning and ease of maintenance.
The leading manufacturers of sanitary pumps have designed their products to meet the following standards:
EHEDG –
European Hygienic Equipment Design Group
QHD – Qualified Hygienic Design
3-A – Sanitary Standards:
3A0/3A1: Industrial/Hygienic Standard
Ra ≤ 3.2 µm
3A2: Sterile Standard
Ra ≤ 0.8 µm
3A3: Sterile Standard
Ra ≤ 0.4 µm
Sand casting
Precision casting
Rolled steel
Fig.1.2.12: Roughness of material surfaces
Section 1.2 Types of pumps
Page 21
1.2.5 Wastewater pumps
A wastewater pump is an enclosed unit with a pump and a motor. Due to this construction the wastewater pump is suitable for submersible installation in pits. In submersible installations with auto-coupling systems double rails are normally used. The auto-coupling system facilitates maintenance, repair and replacement of the pump. Because of the construction of the pump, it is not necessary to enter the pit to carry out service. In fact, it is possible to connect and disconnect the pump automatically from the outside of the pit. Wastewater pumps can also be installed dry like conventional pumps in vertical or horizontal installations. Likewise this type of installation provides easy maintenance and repair like it provides uninterrupted operation of the pump in case of flooding of the dry pit, see figure 1.2.14.
Normally, wastewater pumps have to be able to handle large particles. Therefore they are fitted with special
impellers that make it possible to avoid blockage and clogging. Different types of impellers exist; single-channel impellers, double­channel impellers three and four-channel impellers and vortex impellers.
Figure 1.2.15 shows the different designs of
these impellers.
Wastewater pumps usually come with a dry motor, which is IP68 protected (for more information on IP-classes, go to section 1.4.1). Motor and pump have a common extended shaft with a double mechanical shaft seal system in an intermediate oil chamber, see figure 1.2.13. Wastewater pumps are able to operate either intermittently or continuously depending on the installation in question.
Fig. 1.2.14: Wastewater pump for dry installations
Fig. 1.2.15: Impeller types for wastewater
Vortex
impeller
Single-channel
impeller
Double-channel
impeller
21
Fig.1.2.13: Detail of a sewage pump for wet installations
Page 22
1.2.6 Immersible pumps
An immersible pump is a pump type where the pump part is immersed in the pumped liquid and the motor is kept dry. Normally, immersible pumps are mounted on top of or in the wall of tanks or containers. Immersible pumps are for example used in the machine tool industry
for example in spark machine tools, grinding machines, machining
centres and cooling units or in other industrial applications involving tanks or containers, such as industrial washing and filtering systems.
Pumps for machine tools can be divided in two groups: Pumps for the clean side of the filter and pumps for the dirty side of the filter. Pumps with closed impellers are normally used for the clean side of the filter, because they provide a high efficiency and a high pressure if necessary. Pumps with open or semi-open impellers are normally used for the dirty side of the filter, because they can handle metal chips and particles.
Fig. 1.2.16: Immersible pump
22
Section 1.2 Types of pumps
Page 23
1.2.7 Borehole pumps
Two types of borehole pumps exist: The submerged borehole pump type with a submersible motor, and the deep well pump with a dry motor, which is connected to the pump by a long shaft. These pumps are normally used in connection with water supply and irrigation. Both pump types are made to be installed in deep and narrow boreholes and have thus a reduced diameter, which makes them longer than other pump types, see figure 1.2.17.
The borehole pumps are specially designed to be submerged in a liquid and are thus fitted with a submersible motor, which is IP68 protected. The pump comes in both a single-stage and a multistage version (the multistage version being the most common one), and is fitted with a non-return valve in the pump head.
Today, the deep well pump has been more or less replaced by the submerged pump type. The long shaft of the deep well pump is a drawback, which makes it difficult to install and carry out service. Because the deep well pump motor is air-cooled, the pump is often used in industrial applications to pump hot water from open tanks. The submersible pump cannot handle as high temperatures because the motor is submerged in the liquid, which has to cool it.
Fig. 1.2.17: Submersible pump
23
Page 24
1.2.8 Positive displacement pumps
The positive displacement pump provides an approximate constant flow at fixed speed, despite changes in the counterpressure. Two main types of positive displacement pumps exist:
• Rotary pumps
• Reciprocating pumps
The difference in performance between a centrifugal pump, a rotary pump and a reciprocating is
illustrated
to the right, figure 1.2.18.
Depending on which of these pumps you are dealing with, a small change in the pump’s counterpressure results in differences in the flow.
The flow of a centrifugal pump will change considerably, the flow of a rotary pump will change a little, while the flow of a reciprocating pump will hardly change at all. But, why is there a difference between the pump curves for reciprocating pumps and rotary pumps? The actual seal face surface is larger for rotary pumps than for reciprocating pumps. So, even though the two pumps are designed with the same tolerances, the gap loss of the rotary pump is larger.
The pumps are typically designed with the finest tolerances possible to obtain the highest possible efficiency and suction capability. However, in some cases, it is necessary to increase the tolerances, for example when the pumps have to handle highly viscous liquids, liquids containing particles and liquids of high temperature.
Positive displacement pumps are pulsate, meaning that their volume flow within a cycle is not constant. The variation in flow and speed leads to pressure fluctuations due to resistance in the pipe system and in valves.
Q
H
H
23
1
3
2 1
Fig. 1.2.19: Classification of positive displacement pumps
Simplex
Duplex
Simplex
Duplex
Triplex
Multiplex
Fig. 1.2.18: Typical relation between flow and head for 3 different pump types:
1) Centrifugal pumps
2) Rotary pumps
3) Reciprocating pumps
24
Section 1.2 Types of pumps
Reciprocating
Rotary
Plunger
Diaphragm
Steam Double-acting
Power
Single-acting
Double-acting
Gear
Lobe
Circumferential piston
Screw
Vane
Piston
Flexible member
Screw
Single rotor
Multiple rotor
Positive displacement pumps
Page 25
+
Dosing pumps
The dosing pump belongs to the positive displacement pump family and is typically of the diaphragm type. Diaphragm pumps are leakage-free, because the diaphragm forms a seal between the liquid and the surroundings.
The diaphragm pump is fitted with two non-return valves – one on the suction side and one on the discharge side of the pump. In connection with smaller diaphragm pumps, the diaphragm is activated by the connecting rod, which is connected to an electromagnet. Thereby the coil receives the exact amount of strokes needed, see figure 1.2.21.
In connection with larger diaphragm pumps the diaphragm is typically mounted on the connecting
rod, which is activated by a camshaft. The camshaft is turned by means of a standard asynchronous motor, see figure 1.2.22.
The flow of a diaphragm pump is adjusted by either changing the stroke length and/or the frequency of the strokes. If it is necessary to enlarge the operating area, frequency converters can be connected to the larger diaphragm pumps, see figure 1.2.22.
Yet, another kind of diaphragm pump exists. In this case, the diaphragm is activated by means of an excentrically driven connecting rod powered by a stepper motor or a synchronous motor, figures 1.2.20 and 1.2.23. By using a stepper motor drive the pump’s dynamic area is increased and its
accuracy is improved considerably. With this
construction
it is no longer necessary to adjust the pump’s stroke length because the connection rod is mounted directly on the diaphragm. The result is optimised suction conditions and excellent operation features.
So therefore, it is simple to control both the suction side and the discharge side of the pump. Compared to traditional electromagnetic-driven diaphragm pumps which provide powerful pulsations, stepper motor-driven diaphragm pumps make it possible to get a much more steady dosage of additive.
Fig.1.2.21: Solenoid spring return
1.2.22: Cam-drive spring return
1.2.23: Crank drive
Fig. 1.2.20: Dosing pump
+
25
Page 26
Chapter 1. Design of pumps and motors
Section 1.3: Mechanical shaft seals
1.3.1 The mechanical shaft seal’s components and function
1.3.2 Balanced and unbalanced shaft seals
1.3.3 Types of mechanical shaft seals
1.3.4 Seal face material combinations
1.3.5 Factors affecting the seal performance
Page 27
Page 28
Section 1.3
Mechanical shaft seals
From the middle of the 1950s mechanical shaft seals gained ground in favour of the traditional sealing method
- the stuffing box. Compared to stuffing boxes, mechani­cal shaft seals provide the following advantages:
They keep tight at smaller displacements and vibrations
in the shaft
They do not require any adjustment
Seal faces provide a small amount of friction and thus,
minimise the power loss
The shaft does not slide against any of the seal’s
components and thus, is not damaged because of wear (reduced repair costs).
The mechanical shaft seal is the part of a pump that separates the liquid from the atmosphere. In figure 1.3.1 you can see a couple of examples where the mechanical shaft seal is mounted in different types of pumps.
The majority of mechanical shaft seals are made according to the European standard EN 12756.
Before choosing a shaft seal, there are certain things you need to know about the liquid and thus the seal’s resistance to the liquid:
Determine the type of liquid
Determine the pressure that the shaft seal is exposed to
Determine the speed that the shaft seal is exposed to
Determine the built-in dimensions
On the following pages we will present how a mechanical shaft seal works, the different types of seal, which kind of materials mechanical shaft seals are made of and which factors that affect the mechanical shaft seal’s performance.
28
Fig. 1.3.1: Pumps with mechanical shaft seals
Page 29
1.3.1 The mechanical shaft seal’s components and function
The mechanical shaft seal is made of two main components: a rotating part and a stationary part; and consists of the parts listed in figure 1.3.2. Figure 1.3.3 shows where the different parts are placed in the seal.
The stationary part of the seal is fixed in the pump
housing. The rotating part of the seal is fixed on the pump shaft and rotates when the pump operates.
The two primary seal faces are pushed against each other
by the spring and the liquid pressure. During operation a liquid film is produced in the narrow gap between the two seal faces. This film evaporates before it enters the atmosphere, making the mechanical shaft seal liquid tight, see figure 1.3.4.
Secondary seals prevent leakage from occurring
between the assembly and the shaft.
The spring presses the seal faces together mechanically.
The spring retainer transmits torque from the shaft to
the seal. In connection with mechanical bellows shaft seals, torque is transferred directly through the bellows.
Seal gap
During operation the liquid forms a lubricating film between the seal faces. This lubricating film consists of a hydrostatic and a hydrodynamic film.
The hydrostatic element is generated by the pumped
liquid which is forced into the gap between the seal faces.
The hydrodynamic lubricating film is created by
pressure generated by the shaft’s rotation.
Fig. 1.3.4: Mechanical shaft seal in operation
Lubrication film
Liquid force
Spring force
Vapour
Evaporation begins
Fig. 1.3.3: Main components of the mechanical shaft seal
Rotating part
Stationary part
Shaft
Primary seal
Secondary seal
Primary seal
Secondary seal
Spring
Spring retainer
Mechanical shaft seal Designation
Seal face (primary seal)
Secondary seal Spring
Spring retainer (torque transmission
)
Seat (seal faces, primary seal)
Static seal (secondary seal
)
Rotating par
t
Stationary par
t
Fig. 1.3.2:
The mechanical shaft seal’s components
29
Page 30
1.3.2 Balanced and unbalanced shaft seals
To obtain an acceptable face pressure between the primary seal faces, two kind of seal types exist: a balanced shaft seal and an unbalanced shaft seal.
Balanced shaft seal
Figure 1.3.6 shows a balanced shaft seal indicating where the forces interact on the seal.
Unbalanced shaft seal
Figure 1.3.7 shows an unbalanced shaft seal indicating where the forces interact on the seal.
Several different forces have an axial impact on the seal faces. The spring force and the hydraulic force from the pumped liquid press the seal together while the force from the lubricating film in the seal gap counteracts this. In connection with high liquid pressure, the hydraulic forces can be so powerful that the lubricant in the seal gap cannot counteract the contact between the seal faces. Because the hydraulic force is proportionate to the area that the liquid pressure affects, the axial impact can only be reduced by obtaining a reduction of the pressure-loaded area.
The thickness of the lubricating film depends on the pump speed, the liquid temperature, the viscosity of the liquid and the axial forces of the mechanical shaft seal. The liquid is continuously changed in the seal gap because of
evaporation of the liquid to the atmosphere
the liquid’s circular movement
Figure 1.3.5 shows the optimum ratio between fine lubrication properties and limited leakage. As you can tell, the optimum ratio is when the lubricating film covers the entire seal gap, except for a very narrow evaporation
zone
close to the atmospheric side of the mechanical shaft seal.
Leakage due to deposits on the seal faces is often observed. When using coolant agents, deposits are built up quickly by the evaporation at the atmosphere side of the seal. When the
liquid evaporates in the evaporation zone, microscopic
solids
in the liquid remain in the seal gap as deposits creating wear. These deposits are seen in connection with most types of liquid. But when the pumped liquid has a tendency to crystallise, it can become a problem. The best way to prevent wear is to select seal faces made
of hard material, such as tungsten carbide (WC) or silicon carbide (SiC). The narrow seal gap between these materials (app. 0.3 µm Ra) minimises the risk of solids entering the seal gap and thereby minimises the amount of deposits building up.
Pressure
LiquidPump pressure
Stationary seal face
Rotating seal face
Vapour Atmosphere
Entrance
in seal
Exit into
atmospher
e
Start of ev
aporation
1 atm
Fig. 1.3.6: Interaction of forces on the balanced shaft seal
Fig. 1.3.7: Interaction of forces on the unbalanced shaft seal
A
Spring forces
Hydraulic forces
Contact area of seal faces
B
A B
Hydraulic forces
Contact area of seal faces
Fig. 1.3.5: Optimum ratio between fine lubrication properties and limited leakage
30
Section 1.3
Mechanical shaft seals
Page 31
31
The balancing ratio (K) of a mechanical shaft seal is defined as the ratio between the area A and the area (B) : K=A/B
K = Balancing ratio A = Area exposed to hydraulic pressure B = Contact area of seal faces
For balanced shaft seals the balancing ratio is usually around K=0.8 and for unbalanced shaft seals the balancing ratio is normally around K=1.2.
1.3.3 Types of mechanical shaft seals
What follows is a brief outline of the main types of mechanical shaft seals: O-ring seal, bellows seal, and the one-unit seal - the cartridge seal.
O-ring seals
In an O-ring seal, sealing between the rotating shaft and the rotating seal face is effected by an O-ring (figure 1.3.9). The O-ring must be able to slide freely in the axial direction to absorb axial displacements as a result of changes in temperatures and wear. Incorrect positioning of the stationary seat may result in rubbing and thus unnecessary wear on the O-ring and on the shaft. O-rings are made of different types of rubber material, such as NBR, EPDM and FKM, depending on the operating conditions.
Bellows seals
A common feature of bellows seals is a rubber or metal bellows which functions as dynamic sealing element between the rotating ring and the shaft.
Rubber bellows seals
The bellows of a rubber bellows seal (see figure 1.3.10) can be made of different types of rubber material, such as NBR, EPDM and FKM, depending on the operating conditions. Two different geometric principles are used for the design of rubber bellows:
• Folding bellows
• Rolling bellows.
Fig. 1.3.8: Wear rate for different balancing ratios
Temperature (oC)
0 20 40 60 80 100 120 140
Wear rate comparative
Temperature (oC)
K = 1.15 K = 1.00 K = 0.85
Fig. 1.3.9: O-ring seal
Fig. 1.3.10: Rubber bellows seal
Advantages and disadvantages of O-ring seal
Advantages:
Suitable in hot liquid and high pressure applications
Disadvantages:
Deposits on the shaft, such as rust, may prevent the O-ring shaft seal from moving axially
Advantages and disadvantages of rubber bellows seal
Advantages: Not sensitive to deposits, such as rust, on the shaft
Suitable for pumping solid-containing liquids
Disadvantages:
Not suitable in hot liquid and high pressure applications
Rubber bellows seal with folding bellows geometry
Page 32
32
Metal bellows seals
In an ordinary mechanical shaft seal, the spring produces the closing force required to close the seal faces. In a metal bellows seal (figure 1.3.11) the spring has been replaced by a metal bellows with a similar force. Metal bellows act both as a dynamic seal between the rotating ring and the shaft and as a spring. The bellows have a number of corrugations to give them the desired spring force.
Cartridge seals
In a cartridge mechanical shaft seal, all parts form a compact unit on a shaft sleeve, ready to be installed. A cartridge seal offers many benefits compared to conventional mechanical shaft seals, figure 1.3.12.
Flushing
In certain applications it is possible to extend the performance of the mechanical shaft seal by installing flushing, see figure 1.3.13. Flushing can lower the temperature of the mechanical shaft seal and prevent deposits from occurring. Flushing can be installed either internally or externally. Internal flushing is done when a small flow from the pump’s discharge side is bypassed to the seal area. Internal flushing is primarily used to prevent further heat generation from the seal in heating applications. External flushing is done by a flushing liquid and is used to ensure trouble-free operation when handling liquids that are abrasive or contain clogging solids.
Fig. 1.3.11: Cartridge metal bellows seal
Advantages and disadvantages of cartridge metal bellows seal
Advantages:
Not sensitive to deposits, such as rust and lime on the shaft
Suitable in hot liquid and high-pressure applications
Low balancing ratio leads to low wear rate and consequently longer life
Disadvantages:
Fatique failure of the mechanical shaft seal may occur when the pump is not aligned correctly
Fatique may occur as a result of excessive temperatures or pressures
Fig. 1.3.12: Cartridge seal
Advantages of the cartridge seal:
• Easy and fast service
• The design protects the seal faces
• Preloaded spring
• Safe handling
Fig 1.3.13: Flushing device of a single mechanical shaft seal
Section 1.3
Mechanical shaft seals
Page 33
33
Double mechanical shaft seals
Double mechanical shaft seals are used when the life span of single mechanical shaft seals is insufficient due to wear caused by solids or too high/low pressure and temperature. Further, double mechanical shaft seals are used in connection with toxic, aggressive and explosive liquids to protect the surroundings. Two types of double mechanical shaft seals exist: The double seal in a tandem arrangement and the double seal in a back-to-back arrangement.
Double seal in tandem
This type of double seal consists of two mechanical shaft seals mounted in tandem, that is one behind the other, placed in a separate seal chamber, see figure 1.3.14.
The seal type is used when a pressurised double mechanical shaft seal mounted in a back-to-back arrangement is not necessary.
The tandem seal arrangement has to be fitted with a quenching liquid system which
absorbs leakage
monitors the leakage rate
lubricates and cools the outboard seal to prevent icing
protects against dry-running
stabilises the lubricating film
prevents air from entering the pump in case of vacuum
The pressure of the quenching liquid must always be lower than the pumped liquid pressure.
Tandem - circulation
Circulation of quenching liquid via a pressureless tank, see figure 1.3.14. Quenching liquid from the elevated tank is circulated by thermosiphon action and/or by pumping action in the seal.
Tandem - dead end
Quenching liquid from an elevated tank, see figure 1.3.15. No heat is dissipated from the system.
Tandem - drain
The quenching liquid runs directly through the seal chamber to be collected for reuse, or directed to drain, see figure 1.3.16.
Fig. 1.3.16: Tandem seal arrangement with quench liquid to drain
Quench liquid
Pumped liquid
Quench liquid
Pumped liquid
Quench liquid
Pumped liquid
Quench liquid
Pumped liquid
Quench liquid
Pumped liquid
Pumped liquid
Fig. 1.3.15: Tandem seal arrangement with quench liquid dead
end
Fig. 1.3.14: Tandem seal arrangement with quench liquid
circulation
Page 34
34
1.3.4 Seal face material combinations
What follows is a description of the most important material pairings used in mechanical shaft seals for industrial applications: Tungsten carbide/tungsten carbide, silicon carbide/silicon carbide and carbon/ tungsten carbide or carbon/silicon carbide.
Tungsten carbide/tungsten carbide (WC/WC)
Cemented tungsten carbide covers the type of hard metals that are based on a hard tungsten carbide (WC) phase and usually a softer metallic binder phase. The correct technical term is cemented tungsten carbide, however, the abbreviated term tungsten carbide (WC) is used for convenience.
Cobalt-bonded (Co) WC is only corrosion resistant in water if the pump incorporates base metal, such as cast iron.
Chromium-nickel-molybdenum-bounded WC has a corrosion resistance equal to EN 14401.
Sintered binderless WC has the highest corrosion resistance. However, its resistance to corrosion in liquids, such as hypochlorite, is not as high. The material pairing WC/WC has the following features:
Extremely wear resistant
Very robust, resists rough handling
Poor dry-running properties. In case of dry-running, the temperature increases to several hundred degrees Celsius in very few minutes and consequently damages the O-rings.
If a certain pressure and a certain temperature are exceeded, the seal may generate noise. Noise is an indication of poor seal operating conditions that in the long term may cause wear of the seal. The limits of use depend on seal face diameter and design.
To a WC/WC seal face pairing, the running-in wear period where noise is to be expected may last 3-4 weeks, although typically, no noise occurs during the first 3-4 days.
Double seal in back-to-back
This type of seal is the optimum solution for handling abrasive, aggressive, explosive or sticky liquids, which would either wear out, damage or block a mechanical shaft seal.
The back-to-back double seal consists of two shaft seals mounted back-to-back in a separate seal chamber, see figure 1.3.17. The back-to-back double seal protects the surrounding environment and the people working with the pump.
The pressure in the seal chamber must be 1-2 bar higher than the pump pressure. The pressure can be generated by:
An existing, separate pressure source. Many
applications incorporate pressurised systems.
A separate pump, e.g. a dosing pump.
Fig. 1.3.17: Back-to-back seal arrangement
Seal chamber with
barrier pressure liquid
Pumped liquid
Barrier pressure liquid
Section 1.3
Mechanical shaft seals
Page 35
Silicon carbide/silicon carbide (SiC/SiC)
Silicon carbide/silicon carbide (SiC/SiC) is an alternative to WC/WC and is used where higher corrosion resistance is required .
The SiC/SiC material pairing has the following features:
Very brittle material requiring careful handling
Extremely wear resistant
Extremely good corrosion resistance. SiC (Q
1
s
, Q
1
P
and
Q
1
G
) hardly corrodes, irrespective of the pumped liquid
type. However, an exception is water with very poor
conductivity, such as demineralised water, which attacks
the SiC variants Q
1
s
and Q
1
P
, whereas Q
1
G
is corrosion-
resistant also in this liquid
In general, these material pairings have poor dry-running
properties however, the Q
1
G
/ Q
1
G
material withstands a limited period of dry-running on account of the graphite content of the material
For different purposes, various SiC/SiC variants exist:
Q
1
s
, dense-sintered, fine-grained SiC
A direct-sintered, fine-grained SiC with a small amount of tiny pores.
For a number of years, this SiC variant was used as a standard mechanical shaft seal material. Pressure and temperature limits are slightly below those of WC/WC.
Q
1
P
, porous, sintered, fine-grained SiC
A variant of the dense-sintered SiC. This SiC variant has large circular closed pores. The degree of porosity is 5-15% and the size of the pores 10-50 µm Ra. The pressure and temperature limits exceed those of WC/WC.
35
Consequently, in warm water, the Q
1
P
/ Q
1
P
face material pairing generates less noise than the WC/WC pairing. However, noise from porous SiC seals must be expected during the running-in wear period of 3-4 days.
Q
1
G
self-lubricating, sintered SiC
Several variants of SiC materials containing dry lubricants are available on the market. The designation Q
1
G
applies to a SiC material, which is suitable for use in distilled or demineralised water, as opposed to the above materials.
Pressure and temperature limits of Q
1
G
/ Q
1
G
are similar to
those of Q
1
P
/ Q
1
P
.
The dry lubricants, i.e. graphite, reduce the friction in case of dry-running, which is of decisive importance to the durability of a seal during dry-running.
Carbon/tungsten carbide or carbon/ silicon carbide features
Seals with one carbon seal face have the following features:
Brittle material requiring careful handling
Worn by liquids containing solid particles
Good corrosion resistance
Good dry-running properties (temporary dry-running)
The self-lubricating properties of carbon make the
seal suitable for use even with poor lubricating conditions (high temperature) without generating noise. However, such conditions will cause wear of the carbon seal face leading to reduced seal life. The wear depends on the pressure, temperature, liquid diameter and seal design. Low speeds reduce the lubrication between the seal faces; as a result, increased wear might have been expected. However, this is normally not the case because the distance that the seal faces have to move is reduced.
Page 36
36
Metal-impregnated carbon (A) offers limited corro-
sion resistance, but improved mechanical strength, heat conductivity and thus reduced wear
With reduced mechanical strength, but higher
corrosion resistance, synthetic resin-impregnated carbon (B) covers a wide application field. Synthetic
resin-impregnated carbon is approved for drinking
water
The use of carbon/SiC for hot water applications may cause heavy wear of the SiC, depending on the quality of the carbon and water. This type of wear primarily applies to Q
1
S
/carbon. The use of Q
1
P
,
Q
1
G
or a carbon/WC pairing causes far less wear. Thus,
carbon/WC, carbon/Q
1
P
or carbon/Q
1
G
are recommended
for hot water systems
1.3.5 Factors affecting the seal performance
As mentioned previously, no seal is completely tight. On the next pages, we will present the following factors, which have an impact on the seal performance: Energy consumption, noise and leakage. These factors will be presented individually. However, it is important to stress that they are closely interrelated, and thus must be considered as a whole.
Energy consumption
It comes as no surprise that power is needed to make the seal rotate. The following factors contribute to the power consumption, that is the power loss of a mechanical shaft seal:
The centrifugal pumping action of the rotating parts.
The power consumption increases dramatically with the speed of rotation (to the third power).
The seal face friction.
Friction between the two seal faces consists of – friction in the thin liquid film and – friction due to points of contact between the seal faces.
The level of power consumption depends on seal design, lubricating conditions and seal face materials.
Figure 1.3.18 is a typical example of the power consumption of a mechanical shaft seal. The figure shows that up to 3600 rpm friction is the major reason for the mechanical shaft seal’s energy consumption.
Speed (rpm)
0
0
50
100
150
200
250
2000 4000 6000 8000 10000 12000
Power loss (W)
3600
Fig. 1.3.18: Power consumption of a 12 mm mechanical shaft seal
Speed (rpm)
Pumping action
Friction
Section 1.3
Mechanical shaft seals
Page 37
37
Bar
25
20
15
10
5
0
10 20 30 40 50 60 70 80 90 100 110 °C
Noise
Duty range
Fig. 1.3.20: Relation between duty range and speed
Speed at 3000 rpm
Speed at
1800 rpm
Speed at
1200 rpm
Speed at 600 rpm
Energy consumption is, especially in connection with stuffing boxes, an important issue. As you can tell from the example, replacing a stuffing box by a mechanical shaft seal leads to considerable energy savings, see figure 1.3.19.
Noise
The choice of seal face materials is decisive for the function and the life of the mechanical shaft seal.
Noise is generated as a result of the poor lubricating conditions in seals handling low viscosity liquids. The viscosity of water decreases with increasing temperature. This means that the lubricating conditions decrease as the temperature rises. If the pumped liquid reaches or exceeds boiling temperature, the liquid on part of the seal face evaporates, which results in a further decrease in the lubricating conditions. A speed reduction has the same effect, see figure 1.3.20.
Leakage
The pumped liquid lubricates the seal face of a mechanical shaft seal. Thus, better lubrication means less friction and increased leakage. Conversely, less leakage means worse lubricating conditions and increased friction.
In practice, the amount of leakage and power loss that occur in mechanical shaft seals can vary. The reason is that leakage depends on factors which are impossible to quantify theoretically because of type of seal faces, type of liquid, spring load, etc. Therefore, figure 1.3.21 should be perceived as a guideline.
To read the leakage rate curve correctly (figure 1.3.21), you have to go through four steps:
Step 1: Read the pressure - in this case 5 bar
Step 2
: 30 mm unbalanced shaft seal
Step 3
: Speed 3000 rpm
Step 4
: Leakage rate 0.06 ml/h
Dw (mm) 100 B
100 U
B = balanced U = unbalanced
n (min
-1
) 3600
3000
1800
1500
80 U
60 U
40 U
0.
001 0.01 0.06 0.1 1 Leakage Q (ml/h)
Differential pressure to be sealed p (bar)1 10
5
100
30 U
20 U
80 B
60 B
40 B
20 B
30 B
Fig. 1.3.21: Leakage rates
Fig. 1.3.19: Stuffing box versus mechanical shaft seal
Standard pump 50 mLC; 50 mm shaft and 2900 rpm
Energy consumption
Stuffing box 2.0 kW
h
Mechanical shaft seal 0.3 kW
h
Leakag
e
Stuffing box 3.0 l/h (when mounted correctly
)
Mechanical shaft seal 0.8 ml/h
Page 38
Chapter 1. Design of pumps and motors
Section 1.4: Motors
1.4.1 Standards
1.4.2 Motor start-up
1.4.3 Voltage supply
1.4.4 Frequency converter
1.4.5 Motor protection
Page 39
Page 40
Motors are used in many applications all over the world. The purpose of the electric motor is to create rotation, that is to convert electric energy into mechanical energy. Pumps are operated by means of mechanical energy, which is provided by electric motors.
1.4.1 Standards
NEMA
The National Electrical Manufacturers Association (NEMA) sets standards for a wide range of electric products, including motors. NEMA is primarily associated with motors used in North America. The standards represent general industry practices and are supported by the manufacturers of electric equipment. The standards can be found in NEMA Standard Publication No. MG1. Some large motors may not fall under NEMA standards.
IEC
The International Electrotechnical Commission (IEC) sets standards for motors used in many countries around the world. The IEC 60034 standard contains recommended electrical practices that have been developed by the participating IEC countries.
Fig. 1.4.1: Electric motor
Fig. 1.4.2: NEMA and IEC standards
Section 1.4 Motors
40
Page 41
Directives and methods of protection – Ex-motors
ATEX (ATmosphère EXplosible) refers to two EU directives about danger of explosion within different areas. The ATEX directive concerns electrical, mechanical, hydraulic and pneumatic equipment. As to the mechanical equipment, the safety requirements in the ATEX directive ensure that pump components, such as shaft seals and bearings do not heat up and ignite gas and dust. The first ATEX directive (94/9/EC) deals with requirements put on equipment for use in areas with danger of explosion. The manufacturer has to fulfil the requirements and mark his products with categories. The second ATEX directive (99/92/EC) deals with the minimum safety and health requirements that the user has to fulfil, when working in areas with danger of explosion. Different techniques are used to prevent electric equipment from becoming a source of ignition. In the case of electric motors, protection types d (flameproof), e (increased safety) and nA (non-sparking) are applied in connection with gas, and DIP (dust ignition proof) is applied in connection with dust.
Flameproof motors - protection type EExd (de)
First of all, flameproof EExd (type de) motors are category 2G equipment for use in zone 1. The stator housing and the flanges enclose the flameproof motor parts that can ignite a potentially explosive atmosphere. Because of the enclosure, the motor can withstand the pressure that goes along with the explosion of an explosive mixture inside the motor. Propagation of the explosion to the atmosphere that surrounds the enclosure is hereby avoided because the explosion is cooled down by means of flame paths. The size of the flame paths is defined in the EN 50018 standard. The surface temperature of the flameproof enclosure should always be in accordance with the temperature classes.
Increased safety motors - protection type EEx (e)
Increased safety motors (type e) are category 2G equipment for use in zone 1. These motors are not flameproof and not built to withstand an internal explosion. The construction of such a motor is based on increased security against
5
User
Manufacturer
Zones: Gas (G): 0, 1 and 2 Dust (D): 20, 21 and 22
Minor
danger
Po
tentiel
danger
Constant
danger
Category 3 equipment (3G/3D)
Category 2 equipment (2G/2D)
Category 1 equipment (1G/1D)
Zone:
0 or 20
Zone: 1 or 21
Zone: 1 or 21
Zone: 2 or 22
Zone:
2 or 22
Fig 1.4.4: The explosion occurs inside the motor and is lead out of the motor through the flame paths. The temperature classification for flameproof EExd motors is valid for external surfaces.
Fig 1.4.3: The link between zones and equipment categories is a minimum requirement. If the national rules are more strict, they are the ones to follow.
Fig 1.4.5: For increased safety motors EExe, no sparks may occur. The temperature classification covers both internal and external surfaces.
Fig 1.4.6: With non-sparking motors ExnA, no ignition is likely to occur.
41
Page 42
possible excessive temperatures and occurrence of sparks and arcs during normal operation and when a predictable error occurs. The temperature classification for increased safety motors is valid for both internal and external surfaces, and therefore, it is important to observe the stator winding temperature.
Non-sparking motors - protection type Ex (nA)
Non-sparking motors (type nA) are category 3G equipment for use in zone 2. These motors cannot by any means ignite a potential explosive atmosphere under normal operation, see figure 1.4.6.
Dust Ignition Proof (DIP)
Two types of Dust Ignition Proof motors exist: 2D/category 2 equipment and 3D/category 3 equipment.
2D/category 2 equipment
In order to avoid static electricity to cause ignition, the cooling fan on a category 2 DIP motor for use in zone 21 (area with potential danger of explosion) is made of metal. Likewise, to minimise the risk of ignition, the external ground terminal is subject to more severe demands of construction. The external surface temperature of the enclosure, which is indicated on the motor nameplate and corresponds to the running performance during the worst conditions allowed for the motor. Motors for use in zone 21 (areas with potential danger of explosion) have to be IP65 protected, that is completely protected against dust.
3D/category 3 equipment
The temperature indicated on a category 3 DIP motor for use in zone 22 (areas with minor danger of explosion)
Type of
pr
otection
Code
Standar
ds
Use in A TEX
category/
Zone
Principle Application
CENELEC
EN
IE
C
60079
General requirements
- 50014 - 0
-
Basic electrical requirements All equipment
Oil immersion
o 50015 - 6
Category 2 Zone 1
Electrical components immersed in oil excluding explosive atmosphere from igniting
Transformers
Pressurised
p 50016 - 2
Category 2 Zone 1
Enclosure housing equipment is purged to remove explosive atmosphere and pres­surised to prevent ingress of surrounding atmosphere
Switching and control cabinets, large motors
Powder filled
q 50017 - 5
Category 2 Zone 1
Electrical parts are surrounded with power, e.g. quartz to prevent contact with an explosive atmosphere
Electronic devices, e.g. capacitors, fuses
Flameproof
d 50018 - 1
Category 2 Zone 1
Enclosure housing electrical equipment which, if there is an internal explosion, will not ignite surrounding atmosphere
control panels,
light fittings
Increased safety
e 50019 - 7
Category 2 Zone 1
Additional methods are used to eliminate arcs, sparks and hot surface capable of igniting flammable atmosphere
AC motors
AC motors,
, terminal and connection boxes, light fittings, squirrel cage motors
Intrinsic safety
i
a
i
b
50020
50020
- 11
- 11
Category 1 Zone 0
Category 2 Zone 1
Electrical energy in equipment is limited so that circuits cannot ignite an atmosphere by sparking or heating
Measurement and control equipment, e.g. sensors, instrumentation
Encapsulation
m 50028 - 18
Category 2 Zone 1
Electrical components embedded in approved material to prevent contact with explosive atmosphere
Measurement and control devices, solenoid valves
Type of protection n
nA 50021 - 15
Category 3 Zone 2
Non-arcing and non-sparking
AC mot
ors, terminal
boxes, light fittings
Note: Group II Dust atmospher es are covered by CEN ELEC EN 50281-1-1 and EN50281-1-2
Fig 1.4.7: Standards and methods of protection
42
Section 1.4 Motors
Page 43
corresponds to the running performance under the worst conditions allowed for that specific motor. A motor for use in zone 22 has to be IP55 protected, that is protected against dust. The IP protection is the only difference between 2D/category 2 equipment and 3D/category 3 equipment.
Mounting (International Mounting - IM)
Three different ways of mounting the motor exist: Foot­mounted motor, flange-mounted motor with free-hole flange (FF) and flange-mounted motor with tapped-hole flange (FT). Figure 1.4.8 shows the different ways of mounting a motor and the standards that apply for the mountings. The mounting of motors is stated according to the following standards:
IEC 60034-7, Code I,
i.e. designation IM followed by the previously used DIN 42590 code
IEC 60034-7, Code II
Enclosure class (Ingress Protection - IP)
The enclosure class states the degrees of protection of the motor against ingress of solid objects and water. The enclosure class is stated by means of two letters IP followed by two digits, for example IP55. The first digit stands for protection against contact and ingress of solid objects and the second digit stands for protection against ingress of water, see figure 1.4.9.
Drain holes enable the escape of water which has entered the stator housing for instance through condensation. When the motor is installed in a damp environment, the bottom drain hole should be opened. Opening the drain hole changes the motor’s enclosure class from IP55 to IP44.
IM B3
IM 1001
IM B5
IM 3001
IM V1
IM 3011
IM B14
IM 3601
IM V18
IM 3611
First digit Second digit
Protec
tion against contact and
ingress of solid objects
Protection against
ingress of water
0 No special protection
1 The motor is protected against
solid objects bigger than 55 mm, e.g. a hand
2 The motor is protected against objects bigger than 12 mm, e.g. a finger
3 The motor is protected against
solid objects bigger than 25 mm,
i.e. wires, tools, etc.
4 The motor is protected against solid objects bigger than 1 mm, e.g. wires
5 The motor is protected against the ingress of dust
6 The motor is completely dust-proof
0 No special protection
1 The motor is protected against
v
ertically falling drops of water,
s
uch as condensed water
2 The motor is protected against v
ertically falling drops of water,
e
ven
if the motor is tilted at an
angle of 15°
3 The motor is protected against water spray falling at an angle of 60
°
from vertical
4 The motor is protected against water splashing from any direction
5 The motor is protected against water being projected from a nozzle from any direction
6 The motor is protected against heavy
seas or high-pressure
water jets from any direction
7 The motor is protected when submerged from 15 cm to 1 m in water for a period specified by the manufacturer
8 The motor is protected against continuous submersion in water under conditions specified by the manufacturer
Fig 1.4.8: Different mounting methods
Foot-mounted motor
Flange-mounted motor with free-hole flange
Flange-mounted motor with tapped-hole flange
Fig 1.4.9: The enclosure class is stated by means of two digits IP followed by two letters; for example IP55
IM B35
IM 2001
43
Page 44
Frame size
Figure 1.4.11 gives an overview of the relation between frame size, shaft end, motor power and flange type and size. For motors in frame sizes 63 up to and including 315M, the relationship is specified in EN 50347. For motors with frame size 315L and larger, no standard covers this relation. The figure shows where on the motor the different values that make up the frame size are measured.
Flanges and shaft end comply with EN 50347 and IEC 60072-1. Some pumps have a coupling, which requires a smooth motor shaft end or a special shaft extension which is not defined in the standards.
Insulation class
The insulation class is defined in the IEC 60085 standard and tells something about how robust the insulation system is to temperatures. The life of an insulation material is highly dependent on the temperature to which it is exposed. The various insulation materials and systems are classified into insulation classes depending on their ability to resist high temperatures.
IEC 100L (In this case L = 140mm)
100mm
Distance between holes
B3
Maximum temperature increase
Hot-spot overtemperature
Maximum ambient
temperature
10
80 105 125
40
B
[˚C] 180
155
130 120
40
F H
40 40
10
15
Class
B
F
H
Maximum ambient
temper
ature
(˚C)
40
40
40
Maximum
temper
ature increase
(K)
80
105
125
Hot-spot
overtemperature
(K)
10
10
15
Maximum
winding temperature
(Tmax)
(˚C)
130
155
180
Fig 1.4.12:
Different insulation classes and their temperature increase at
nominal voltage and load
Fig 1.4.10: Frame size
140mm
44
Section 1.4 Motors
Page 45
1
Frame si
ze
4-pole 6-pole 8-pol
e
Free-hole
flange
Tapped-hole
flange
[kW] [kW] [kW] (FF) (FT)
0.06;0.09 FF100 FT65
0.12 ; 0.18 FF115 FT75
0.25; 0.37 FF130 FT85
0.55; 0.7
5
0.37; 0.55
FF165 FT100
1.1 0.75 0.37 FF165 FT115
1.5 1.1 0.55 FF165 FT115
2.2; 3 1.5 0.75; 1.1 FF215 FT13
0
4 2.2 1.5 FF215 FT130
5.5
3 2.2 FF265 FT165
7.5 4; 5.5 3 FF265 FT165
11 7.5 4; 5.5 FF300 FT215
15 11 7.5 FF300 FT215
18.5 - - FF30
0
22 15 11 FF30
0
30
18.5; 22
15 FF350
37 30 18.5 FF400
45 - 2
2 FF400
55 37 30 FF500
75 45 37 FF500
90 55 45 FF500
110 75 55 FF600
132 90 7
5 FF600
FF600
315; 355; 400; 450; 500
FF740
560; 630; 710
FF840
56
63
71
80
90S
90L
100L
112M
132S
132M
160M
160L
180M
180L
200L
225S
225M
250M
280S
280M
315S
315M
315L
355
400
450
2-pole
[mm]
9
11
14
19
24
24
28
28
38
38
42
42
48
48
55
55
55
60
65
65
65
65
65
75
80
90
4-, 6-, 8-pole
[mm]
9
11
14
19
24
24
28
28
38
38
42
42
48
48
55
60
60
65
75
75
80
80
80
10
0
10
0
12
0
2-pole
[kW]
0.09; 0.12
0.18; 0.2
5
0.37; 0.55
0.75; 1.1
1.5
2.2
3
4
5.5; 7.5
-
11; 1
5
18.5
22
-
30; 37
-
45
55
75
90
110
13
2
160; 200; 250
315; 355; 400; 450; 500
560; 630; 710
800; 900; 1000 800; 900; 1000
FF940
4
Flange size
Shaft end diameter Rated power
32
Fig 1.4.11: The relation between frame size and power input
45
Page 46
Starting method
Direct-on-line starting (DOL) Simple and cost-efficient.
Safe starting.
High locked-rotor current.
Current pulses when switching over from star to delta. Not suitable if the load has a low inertia. Reduced locked-rotor torque.
Star/delta starting (SD) (Y/)
Reduction of starting current by factor 3.
Autotransformer starting Reduction of locked-rotor current and torque. Current pulses when switching from reduced to full voltage.
Reduced locked-rotor torque.
Soft starter "Soft" starting. No current pulses.
Less water hammer when starting a pump. Reduction of locked-rotor current as required, typically 2-3 times.
Reduced locked-rotor torque.
Frequency converter starting No current pulses.
Less water hammer when starting a pump. Reduction of locked-rotor current as required, typically 2 to 3 times. Can be used for continuous feeding of the motor.
Reduced locked-rotor torque. Expensive
Pros Cons
Direct-on-line starting (DOL)
As the name suggests, direct-on-line starting means that the motor is started by connecting it directly to the supply at rated voltage. Direct-on-line starting is suitable for stable supplies and mechanically stiff and well-dimensioned shaft systems, for example pumps. Whenever applying the direct-on-line
starting method, it is important to consult
local authorities.
Star/delta starting
The objective of this starting method, which is used with three-phase induction motors, is to reduce the starting current. In one position, current supply to the stator windings is connected in star (Y) for starting. In other positions, current supply is reconnected to the windings in delta (∆) once the motor has gained speed.
Autotransformer starting
As the name states, autotransformer starting makes use of an autotransformer. The autotransformer is placed in series with the motor during start and varies the voltage up to nominal voltage in two to four steps.
Soft starter
A soft starter is, as you would expect, a device which ensures a soft start of a motor. This is done by raising the voltage to a preset voltage raise time.
Frequency converter starting
Frequency converters are designed for continuous feeding of motors, but they can also be used for soft starting.
1.4.2 Motor start-up
We distinguish between different ways of starting up the motor: Direct-on-line starting, star/delta starting, autotransformer starting, soft starter and frequency converter starting. Each of these methods have their pros and cons, see figure 1.4.13.
Fig 1.4.13:
Starting method
46
Section 1.4 Motors
Page 47
1.4.3 Voltage supply
The motor’s rated voltage lies within a certain voltage range. Figure 1.4.14 shows typical voltage examples for 50 Hz and 60 Hz motors.
According to the international standard IEC 60038, the motor has to be able to operate with a main voltage tolerance of ± 10%.
For motors that are designed according to the IEC 60034­1 standard with a wide voltage range, e.g. 380-415 V, the main voltage may have a tolerance of ± 5%.
The permissible maximum temperature for the actual insulation class is not exceeded when the motor is operated within the rated voltage range. For conditions at the extreme boundaries the temperature typically rises approx. 10 Kelvin.
1.4.4 Frequency converter
Frequency converters are often used for speed controlling pumps, see chapter 4. The frequency converter converts the mains voltage into a new voltage and frequency, causing the motor to run at a different speed. This way of regulating the frequency might result in some problems:
Acoustic noise from the motor, which is sometimes
transmitted to the system as disturbing noise
High voltage peaks on the output from the frequency
converter to the motor
50 Hz 60 Hz
-
-
-
460 V
+_
10%
Mains voltage according to IEC 60038
230 V
+_
10%
400 V
+_
10%
690 V
+_
10%
-
Typical voltage examples
50 Hz
50 Hz motors come with the following voltages:
• 3 x 220 – 240 / 380 – 415 Y
• 3 x 200 – 220 / 346 – 380 Y
• 3 x 200 / 346 Y
• 3 x 380 – 415
• 1 x 220 – 230 / 240
60 Hz 60 Hz motors come with the following voltages:
• 3 x 200 – 230 / 346 – 400 Y
• 3 x 220 – 255 / 380 – 440 Y
• 3 x 220 – 277 / 380 – 480 Y
• 3 x 200 – 230 / 346 – 400 Y
• 3 x 380 – 480
Fig 1.4.14:
Typical voltages
Fig 1.4.15:
Mains voltage according to IEC 60038
47
Page 48
Insulation for motors with frequency converter
In connection with motors with frequency converters we distinguish between different kinds of motors, with different kinds of insulation.
Motors without phase insulation
For motors constructed without the use of phase insulation, continuous voltages (RMS) above 460 V can increase the risk of disruptive discharges in the windings and thus destruction of the motor. This applies to all motors constructed according to these principles. Continuous operation with voltage peaks above 650 V can cause damage to the motor.
Motors with phase insulation
In three-phase motors, phase insulation is normally used and consequently, specific precautions are not necessary if the voltage supply is smaller than 500 V.
Motors with reinforced insulation
In connection with supply voltages between 500 and 690 V, the motor has to have reinforced insulation or be protected with delta U /delta t filters. For supply voltages of 690 V and higher the motor has to be fitted with both reinforced insulation and delta U /delta t filters.
Motors with insulated bearings
In order to avoid harmful current flows through the bearings, the motor bearings have to be electrically
insulated.
This applies for motors from frame size 280 and up.
Fig 1.4.16: Stator with phase insulation
Phase insulation also referred
to as phase paper
48
Section 1.4 Motors
Page 49
Motor efficiency
Generally speaking, electric motors are quite efficient. Some motors have electricity-to-shaft power efficiencies of 80-93% depending on the motor size and sometimes even higher for bigger motors. Two types of energy losses in electric motors exist: Load dependent losses and load independent losses.
Load dependent losses vary with the square of the current and cover:
Stator winding losses (copper losses)
Rotor losses (slip losses)
Stray losses (in different parts of the motor)
Load independent losses in the motor refer to:
Iron losses (core losses)
Mechanical losses (friction)
Different motor classifications categorise motors according to efficiency. The most important are CEMEP in the EU (EFF1, EFF2 and EFF3) and EPAct in the US.
Motors can fail because of overload for a longer period of time and therefore most motors are intentionally oversized and only operate at 75% to 80% of their full load capacity. At this level of loading, motor efficiency and power factor remain relatively high. But when the motor load is less than 25%, the efficiency and the power factor decrease.
The motor efficiency drops quickly below a certain percentage of the rated load. Therefore, it is important to size the motor so that the losses associated with running the motor too far below its rated capacity are minimised. It is common to choose a pump motor that meets the power requirements of the pump.
1.4.5 Motor protection
Motors are nearly always protected against reaching temperatures, which can damage the insulation system. Depending on the construction of the motor and the application, thermal protection can also have other functions, e.g. prevent damaging temperatures in the frequency converter if it is mounted on the motor.
The type of thermal protection varies with the motor type. The construction of the motor together with the power consumption must be taken into consideration when choosing thermal protection. Generally speaking, motors have to be protected against the following conditions:
Errors causing slow temperature increases in the windings:
Slow overload
Long start-up periods
Reduced cooling / lack of cooling
Increased ambient temperature
Frequent starts and stops
Frequency fluctuation
Voltage fluctuation
Errors causing fast temperature increases in the windings:
Blocked rotor
Phase failure
Percent of rated load
Percent
0 25 50 75 150125100
100
20
40
60
80
1
0.2
0.4
0.6
0.8
Efficiency Power factor
Cos ϕ
Percent of rated load
0 25 50 7
5 150125 175100
100
20
10
0
30
50
90
80
75 kW
7.5 kW
0.75 kW
70
60
40
Efficiency %
Fig 1.4.17: Efficiency vs. load power factor vs. load (schematic drawing)
Fig 1.4.18: The relation between efficiency and rated load of different sized motors (schematic drawing)
49
Page 50
Thermal protection (TP)
According to the IEC 60034-11 standard, the thermal protection of the motor has to be indicated on the nameplate with a TP designation. Figure 1.4.19 shows an overview of the TP designations.
PTC thermistors
PTC thermistors (Positive Temperature Coefficient Thermistors) can be fitted into the windings of a motor during production or retrofitted afterwards. Usually 3 PTCs are fitted in series; 1 in each phase of the winding. They can be purchased with trip temperatures ranging from 90°C to 180°C in 5 degrees steps. PTCs have to be connected to a thermistor relay, which detects the rapid increase in resistance of the thermistor when it reaches its trip temperature. These devices are non-linear. At ambient temperatures the resistance of a set of 3 will be about 200­300 ohms and this will increase rapidly when the thermistor reaches its trip temperature. If the temperature increases any further, the PTC thermistor can reach several thousand ohms. The thermistor relays are usually set to trip at 3000 ohms or are preset to trip according to what the DIN 44082 standard prescribes. The TP designation for PTCs for motors smaller than 11kW is TP211 if the PTCs are fitted into the windings. If the PTCs are retrofitted the TP designation is TP111. The TP designation for PTCs for motors larger than 11kW is normally TP111.
Indication of the permissible temperature level when the motor is exposed to thermal overload. Category 2 allows higher temperatures than category 1 does.
Technical overload with
va
riation (1 digit)
Only slow
(i.e. constant
overload)
Only fast
(i.e. blocked condition)
Slow and fast
(i.e. constant overload
and blocked condition )
2 levels at emergency
signal and cutoff
1 level at cutoff
2 levels at emergency
signal and cutoff
1 level at cutoff
1 level at cutoff
Number af levels and
function area (2 digits)
Symbol
TP 111 TP 112 TP 121 TP 122 TP 211 TP 212 TP 221 TP 222 TP 311 TP 312
Category 1
(3 digits)
1 2 1 2
1 2
1 2 1 2
Fig 1.4.19: TP designations
Thermal switch and thermostats
Thermal switches are small bi-metallic switches that switch due to the temperature. They are available with a wide range of trip temperatures; normally open and closed types. The most common type is the closed one. One or two, in series, are usually fitted in the windings like thermistors and can be connected directly to the circuit of the main contactor coil. In that way no relay is necessary. This type of protection is cheaper than thermistors, but on the other hand, it is less sensitive and is not able to detect a locked rotor failure.
Thermal switches are also referred to as Thermik, Klixon switches and PTO (Protection Thermique à Ouverture). Thermal switches always carry a TP111 designation.
Single-phase motors
Single-phase motors normally come with incorporated thermal protection. Thermal protection usually has an automatic reclosing. This implies that the motor has to be connected to the mains in a way that ensures that accidents caused by the automatic reclosing are avoided.
Three-phase motors
Three-phase motors have to be protected according to local regulations. This kind of motor has usually incorporated contacts for resetting in the external control circuit.
50
Page 51
51
Standstill heating
A heating element ensures the standstill heating of the motor. The heating element is especially used in connection with applications that struggle with humidity and condensation. By using the standstill heating, the motor is warmer than the surroundings and thereby the relative air humidity inside the motor is always lower than 100%.
Maintenance
The motor should be checked at regular intervals. It is important to keep the motor clean in order to ensure adequate ventilation. If the pump is installed in a dusty environment, the pump must be cleaned and checked regularly.
Bearings
Normally, motors have a locked bearing in the drive end and a bearing with axial play in the non-drive end. Axial play is required due to production tolerances, thermal expansion during operation, etc. The motor bearings are held in place by wave spring washers in the non-drive end, see figure
1.4.21.
The fixed bearing in the drive end can be either a deep­groove ball bearing or an angular contact bearing.
Bearing clearances and tolerances are stated according to ISO 15 and ISO 492. Because bearing manufacturers have to fulfil these standards, bearings are internationally interchangeable.
In order to rotate freely, a ball bearing must have a certain internal clearance between the raceway and the balls. Without this internal clearance, the bearings can either be difficult to rotate or it may even seize up and be unable to rotate. On the other hand, too much internal clearance will result in an unstable bearing that may generate excessive noise or allow the shaft to wobble.
Depending on which pump type the motor is fitted, the deep-groove ball bearing in the drive end must have C3 or C4 clearance. Bearings with C4 clearance are less heat sensitive and have increased axial load-carrying capacity.
The bearing carrying the axial forces of the pump can have C3 clearance if:
the pump has complete or partial hydraulic relief
the pump has many brief periods of operation
the pump has long idle periods
C4 bearings are used for pumps with fluctuating high axial forces. Angular contact bearings are used if the pump exerts strong one-way axial forces.
Non-drive end
Drive end
Non-driv
e end bearingSpring washer Drive end bearing
Fig 1.4.21: Cross-sectional drawing of motor
1.4.20: Stator with heating element
Page 52
52
Motors with permanently lubricated bearings
For closed permanently lubricated bearings, use one of the following high temperature resistant types of grease:
Lithium-based grease
Polyurea-based grease
The technical specifications must correspond to the standard
DIN - 51825 K2 or better. The basic oil viscosity
must be higher than:
50 cSt (10
-6m2
/sec) at 40°C and
8 cSt (mm
2
/sec) at 100°C
For example Klüberquiet BQH 72-102 with a grease filling ratio of: 30 - 40%.
Motors with lubrication system
Normally, frame size 160 motors and upwards have lubricating nipples for the bearings both in the drive end and the non-drive end.
The lubricating nipples are visible and easily accessible. The motor is designed in such a way that:
there is a flow of grease around the bearing
new grease enters the bearing
old grease is removed from the bearing
Motors with lubricating systems are supplied with a lubricating instruction, for instance as a label on the fan cover. Apart from that, instructions are given in the installation and operating instructions.
The lubricant is often lithium-based, high temperature grease, for instance EXXON UNIREX N3 or Shell Alvania Grease G3. The basic oil viscosity must be
• higher than 50 cSt (10-6m2/sec) at 40°C and
• 8 cSt (mm2/sec) at 100°C
Moderate to strong forces. Primarily outward pull on the shaft end
Fixed deep-groove ball bearing (
C4)
Strong outward pull on the shaft end
Small forces (flexible coupling)
Strong inward pressure
Axial forces Bearing types and recommended clearance
Drive-end Non-drive-end
Moderate forces. Primarily outward pull on the shaft end (partly hydraulically relieved in the pump)
Deep-groove ball bearing (C4)
Fixed deep-groove ball bearing (
C3)
Fixed deep-groove ball bearing (
C3)
Fixed angular contact bearing
Deep-groove ball bearing (C3)
Fixed angular contact bearing
Deep-groove ball bearing (C3)
Deep-groove ball bearing (C3)
Deep-groove ball bearing (C3)
Fig:1.4.22: Typical types of bearings in pump motors
Section 1.4 Motors
Page 53
Chapter 1. Design of pumps and motors
Section 1.5: Liquids
1.5.1 Viscous liquids
1.5.2 Non-Newtonian liquids
1.5.3 The impact of viscous liquids on the performance of a centrifugal pump
1.5.4 Selecting the right pump for a liquid with antifreeze
1.5.5 Calculation example
1.5.6 Computer aided pump selection for dense and viscous liquids
Page 54
Section 1.5 Liquids
1.5.1 Viscous liquids
There is no doubt about it; water is the most common liquid that pumps handle. However, in a number of applications, pumps have to handle other types of liquids, e.g. oil, propylene glycol, gasoline. Compared to water, these types of liquids have different density and viscosity.
Viscosity is a measure of the thickness of the liquid.
The higher the viscosity, the thicker the liquid. Propylene glycol and motor oil are examples of thick or high viscous liquids. Gasoline and water are examples of thin, low viscous liquids.
Two kinds of viscosity exist:
The dynamic viscosity (µ), which is normally measured in Pas or Poise. (1 Poise = 0.1 Pas)
The kinematic viscosity (ν), which is normally measured in centiStokes or m2/s (1 cSt = 10-6 m2/s)
The relation between the dynamic viscosity (µ) and the kinematic viscosity (ν) is shown in the formula on your right hand side.
On the following pages, we will only focus on kinematic viscosity (ν).
The viscosity of a liquid changes considerably with the change in temperature; hot oil is thinner than cold oil. As you can tell from figure 1.5.1, a 50% propylene glycol liquid increases its viscosity 10 times when the temperature changes from +20 to –20 oC. For more information concerning liquid viscosity, go to appendix L.
54
ν =
µ ρ
ρ = density of liquid
Kinematic
viscosity
ν
[cSt]
Density
ρ
[kg/m3]
Liquid
temperature
t [˚C]
Liquid
Water 20
998 1.004 Gasoline 20 733 0.75 Olive oil
20 900 93
50% Propylene glycol
20 1043 6.4
50% Propylene glycol
-20 1061 68.7
Fig. 1.5.1: Comparison of viscosity values for water and a few other liquids. Density values and temperatures are also shown
Page 55
1.5.2 Non-Newtonian liquids
The liquids discussed so far are referred to as Newtonian fluids. The viscosity of Newtonian liquids is not affected by the magnitude and the motion that they are exposed to. Mineral oil and water are typical examples of this type of liquid. On the other hand, the viscosity of non-Newtonian liquids does change when agitated.
This calls for a few examples:
Dilatant liquids like cream – the viscosity increases when agitated
Plastic fluids like catsup – have a yield value, which has to be exceeded before flow starts. From that point on, the viscosity decreases with an increase in agitation
Thixotrophic liquids like non-drip paint - exhibit a decreasing viscosity with an increase in agitation
The non-Newtonian liquids are not covered by the viscosity formula described earlier in this section.
1.5.3 The impact of viscous liquids on the performance of a centrifugal pump
Viscous liquids, that is liquids with higher viscosity and/ or higher density than water, affect the performance of centrifugal pumps in different ways:
Power consumption increases, i.e. a larger motor may be required to perform the same task
Head, flow rate and pump efficiency are reduced
Let us have a look at an example. A pump is used for pumping a liquid in a cooling system with a liquid temperature below 0oC. To avoid that the liquid freezes, an antifreeze agent like propylene glycol is added to the water. When glycol or a similar antifreeze agent is added to the pumped liquid, the liquid obtains properties, different from those of water. The liquid will have:
Lower freezing point, tf [°C]
Lower specific heat, cp [kJ/kg.K]
Lower thermal conductivity, λ [W/m.K]
Higher boiling point, tb [°C]
Higher coefficient of expansion, β [m/°C]
Higher density, ρ [kg/m3]
Higher kinematic viscosity, ν [cSt]
These properties have to be kept in mind when designing a system and selecting pumps. As mentioned earlier, the higher density requires increased motor power and the higher viscosity reduces pump head, flow rate and efficiency resulting in a need for increased motor power, see figure 1.5.2.
Q
H, P, η
H
P
η
Fig. 1.5.2: Changed head, efficiency and power input for liquid with higher viscosity
55
Page 56
1.5.4 Selecting the right pump for a liquid with antifreeze
Pump characteristics are usually based on water at around 20°C, i.e. a kinematic viscosity of approximately 1 cSt and a density of approximately 1,000 kg/m³. When pumps are used for liquids containing antifreeze below 0°C, it is necessary to examine whether the pump can supply the required performance or whether a larger motor is required. The following section presents a simplified method used to determine pump curve corrections for pumps in systems that have to handle a viscosity between 5 - 100 cSt and a density of maximum 1,300 kg/m³. Please notice that this method is not as precise as the computer aided method described later in this section.
Pump curve corrections for pumps handling high viscous liquid
Based on knowledge about required duty point, QS, HS, and kinematic viscosity of the pumped liquid, the correction factors of H and P2 can be found, see figure 1.5.3.
Fig. 1.5.3: It is possible to determine the correction factor for head and power consumption at different flow, head and viscosity values
10
20
30
40
50
60
70
80
90
100
110
120
130
140
0.
9
1.0
1.1
1.2
1.3
1.4
1.5
1.6
1.7
1.8
1.9
1.00
1.05
1.20
1.15
1.10
1.25
1.30
1.35
0
H = 6
m
H = 10
m
H = 20
m
H = 40
m
H = 60
m
10 cS
t
20 cS
t
40 cS
t
60 cSt
100 cSt
5 cS
t
10 cSt
20 cSt
40 cSt
60 cSt
100 cSt
5 cSt
K
H
K
P2
Q [m3/h]
56
Section 1.5 Liquids
Page 57
Figure 1.5.3 is read in the following way:
When kH and kP2 are found in the figure, the equivalent head for clean water HW and the corrected actual shaft power P2S can be calculated by the following formula
where HW : is the equivalent head of the pump if the pumped liquid is “clean” water
P
2W
: is the shaft power at the duty point (QS,HW) when
the pumped liquid is water
HS : is the desired head of the pumped liquid (with agents)
P2S : is the shaft power at the duty point (Qs,Hs) when the pumped liquid is water (with agents)
ρs : is the density of the pumped liquid
ρw : is the density of water = 998 kg/m
3
The pump selection is based on the normal data sheets/ curves applying to water. The pump should cover the duty point Q,H = QS,HW, and the motor should be powerful enough to handle P2S on the shaft.
Figure 1.5.4 shows how to proceed when selecting a pump and testing whether the motor is within the power range allowed.
ρ
P
2S
= K
P2
.
P
2w
.
( )
s
w
Water
Water
Mixture
Mixture
H
w
H
w
= k
H
.
H
S
2
1
H
H
s
P
2s
P
P
2w
Q
s
Q
Q
5
3
4
ρ
Fig. 1.5.4: Pump curve correction when choosing the right pump for the system
The pump and motor selecting procedure contains the following steps:
Calculate the corrected head Hw (based on HS and kH), see figure 1.5.4 1-2
Choose a pump capable of providing performance according to the corrected duty point (QS, HW)
Read the power input P2W in the duty point (QS,Hw), see figure 1.5.4 3-4
• Based on P2W , kP2 , ρW , and ρS calculate the corrected required shaft power P2S , see figure 1.5.4 4-5
Check if P2S < P
2 MAX
of the motor. If that is the case the motor can be used. Otherwise select a more powerful motor
HW = k
H . HS
ρ
s
ρ
w
P2S = k
P2 . P2w
.
( )
57
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1.5.5 Calculation example
A circulator pump in a refrigeration system is to pump a 40% (weight) propylene glycol liquid at –10°C. The desired flow is QS = 60 m3/h, and the desired head is HS = 12 m. Knowing the required duty point, it is possible to find the QH­characteristic for water and choose a pump, which is able to cover the duty point. Once we have determined the needed pump type and size we can check if the pump is fitted with a motor, which can handle the specific pump load.
The liquid has kinematic viscosity of 20 cSt and a density of 1049 kg/m3. With QS = 60 m3/h, HS = 12 m and ν = 20 cSt, the correction factors can be found in figure 1.5.3.
kH = 1.03
kP2 = 1.15
HW = kH · HS = 1.03 · 12 = 12.4 m
QS = 60 m3/h
The pump has to be able to cover a duty point equivalent to Q,H = 60 m3/h, 12.4m. Once the necessary pump size is determined, the P2 value for the duty point is found, which in this case is P2W = 2.9 kW. Now it is possible to calculate the required motor power for propylene glycol mixture:
The calculation shows, that the pump has to be fitted with a 4 kW motor, which is the smallest motor size able to cover the calculated P2S = 3.5 kW.
1.5.6 Computer aided pump selection for dense and viscous liquids
Some computer aided pump selection tools include a feature that compensates for the pump performance curves based on input of the liquid density and viscosity. Figure 1.5.5 shows the pump performance curves from the example we just went through.
The figure shows both the performance curves for the pump when it handles viscous liquid (the full lines) and the performance curves when it handles water (the broken lines). As indicated head, flow and efficiency are reduced, resulting in an increase in power consumption. The value of P2 is 3.4 kW, which corresponds to the result we got in the calculation example in section 1.5.4.
H
[m]
η
[%]
0
1
2
3
4
0
2
4
6
8
10
12
14
0 10 2
0
0
10
20
30
40
50
60
70
30 40 50 60 70 80
Q [m3/h]
Q [m3/h]
P
2
[kW]
Fig. 1.5.5: Pump performance curves
ρ
S
ρ
w
P2S = k
P2 . P2w
.
P
2S
= 1.15
.
2.9
.
1049
998
= 3.5 kW
58
Section 1.5 Liquids
Page 59
Chapter 1. Design of pumps and motors
Section 1.6: Materials
1.6.1 What is corrosion?
1.6.2 Types of corrosion
1.6.3 Metal and metal alloys
1.6.4 Ceramics
1.6.5 Plastics
1.6.6 Rubber
1.6.7 Coatings
Page 60
60
Section 1.6 Materials
In this section you can read about different materials that are used for pump construction. Our main focus will be on the features that every single metal and metal alloy have to offer. But before we dig any further into the world of materials, we will have a closer look at corrosion. Besides explaining what corrosion is, we will examine the different types of corrosion and what can be done to prevent corrosion from occurring.
1.6.1 What is corrosion?
Corrosion is usually referred to as the degradation of the metal by chemical or electrochemical reaction with its environment, see figure 1.6.1. When considered broadly, corrosion may be looked upon as the tendency of the metal to revert to its natural state similar to the oxide from which it was originally melted. Only precious metals, such as gold and platinum are found in nature in their metallic state.
Some metals produce a tight protective oxide layer on the surface, which hinders further corrosion. If the surface layer is broken it is self-healing. These metals are passivated. Under atmospheric conditions the corrosion products of zinc and aluminium form a fairly tight layer and further corrosion is prevented. Likewise, on the surface of stainless steel a tight layer of iron and chromium oxide is formed and on the surface of titanium a layer of titanium oxide is formed. The protective layer of these metals explains their good corrosion resistance. Rust, on the other hand, is a non-protective corrosion product on steel. Rust is porous, not firmly adherent and does not prevent continued corrosion, see figure 1.6.2.
pH (acidity)
Oxidizing agents (such as oxygen) Temperature Concentration of solution constituents
(such as chlorides)
Biological activity
Operating conditions (such as velocity, cleaning procedures and shutdowns)
Environmental variables that affect the corrosion resistance of metals and alloys
Fig. 1.6.1: Environmental variables that affect the corrosion resistance of metals and alloys
Non-protective corrosion product
Protective corrosion product
Fig. 1.6.2: Examples of corrosion products
Rust on steel
Oxide layer on stainless steel
Page 61
1.6.2 Types of corrosion
Generally, metallic corrosion involves the loss of metal at a spot on an exposed surface. Corrosion occurs in various forms ranging from uniform attacks over the entire surface to severe local attacks. The environment’s chemical and physical conditions determine both the type and the rate of corrosion attacks. The conditions also determine the type of corrosion products that are formed and the control measures that need to be taken. In many cases, it is impossible or rather expensive to completely stop the corrosion process; however, it is usually possible to control the process to acceptable levels.
On the following pages we will go through the different forms of corrosion in order to give you an idea of their characteristics.
Uniform corrosion
Uniform or general corrosion is characterised by corrosive attacks proceeding evenly over the entire surface, or on a large part of the total area. General thinning continues until the metal is broken down. Uniform corrosion is the type of corrosion where the largest amount of metal is wasted.
Examples of metals, which are subject to uniform corrosion:
• Steel in aerated water
• Stainless steel in reducing acids (such as EN 1.4301 (AISI 304) in sulfuric acid)
Pitting corrosion
Pitting corrosion is a localised form of corrosive attacks. Pitting corrosion forms holes or pits on the metal surface. It perforates the metal while the total corrosion, measured by weight loss, might be rather minimal. The rate of penetration may be 10 to 100 times that of general corrosion depending on the aggressiveness of the liquid. Pitting occurs more easily in a stagnant environment.
Example of metal that is subject to pitting corrosion:
• Stainless steel in seawater
Fig. 1.6.3: Uniform corrosion
Fig. 1.6.4: Pitting corrosion
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1. Design of pumps and motors
1.1 Pump construction, (10)
Crevice corrosion
Crevice corrosion - like pitting corrosion - is a localised form of corrosion attack. However, crevice corrosion starts more easily than pitting. Crevice corrosion occurs at narrow openings or spaces between two metal surfaces or between metals and non-metal surfaces and is usually associated with a stagnate condition in the crevice. Crevices, such as those found at flange joints or at threaded connections, are thus often the most critical spots for corrosion.
Example of metal that is subject to crevice corrosion:
• Stainless steel in seawater
Intergranular corrosion
As the name implies, intergranular corrosion occurs at grain boundaries. Intergranular corrosion is also called intercrystalline corrosion. Typically, this type of corrosion occurs when chromium carbide precipitates at the grain boundaries during the welding process or in connection with insufficient heat treatment. A narrow region around the grain boundary may therefore deplete in chromium and become less
corrosion resistant than the rest of the material. This is unfortunate because chromium plays an important role in corrosion resistance.
Examples of metals that are subject to intergranular corrosion:
• Stainless steel - which is insufficiently welded or heat-treated
• Stainless steel EN 1.4401 (AISI 316) in concentrated nitric acid
Selective corrosion
Selective corrosion is a type of corrosion which attacks one single element of an alloy and dissolves the element in the alloy structure. Consequently, the alloy’s structure is weakened.
Examples of selective corrosion:
• The dezincification of unstabilised brass, whereby a weakened, porous copper structure is produced
• Graphitisation of gray cast iron, whereby a brittle graphite skeleton is left because of the dissolution of iron
Fig. 1.6.5: Crevice corrosion
Fig. 1.6.6: Intergranular corrosion
Fig. 1.6.7: Selective corrosion
Copper
Zinc corrosion products
Brass
62
Section 1.6 Materials
Page 63
Erosion corrosion
Erosion corrosion is a process that involves corrosion and erosion. The rate of corrosion attack is accelerated by the relative motion of a corrosive liquid and a metal surface. The attack is localised in areas with high velocity or turbulent flow. Erosion corrosion attacks are characterised by grooves with directional pattern.
Examples of metals which are subject to erosion corrosion:
• Bronze in seawater
• Copper in water
Cavitation corrosion
A pumped liquid with high velocity reduces the pressure. When the pressure drops below the liquid vapour pressure, vapour bubbles form (the liquid boils). In the areas where the vapour bubbles form, the liquid is boiling. When the pressure raises again, the vapour bubbles collapse and produce intensive shockwaves. Consequently, the collapse of the vapour bubbles remove metal or oxide from the surface.
Examples of metals that are subject to cavitation:
• Cast iron in water at high temperature
• Bronze in seawater
Stress corrosion cracking (SCC)
Stress corrosion cracking (SCC) refers to the combined influence of tensile stress (applied or internal) and corrosive environment. The material can crack without any significant deformation or obvious deterioration of the material. Often, pitting corrosion is associated with the stress corrosion cracking phenomena.
Examples of metals that are subject to stress corrosion cracking:
• Stainless steel EN 1.4401 (AISI 316) in chlorides
• Brass in ammonia
Fig. 1.6.8: Erosion corrosion
Fig. 1.6.9: Cavitation corrosion
Fig. 1.6.10: Stress corrosion cracking
Flow
63
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1. Design of pumps and motors
1.1 Pump construction, (10)
<
Corrosion fatigue
Pure mechanical fatigue is when a material subjected to a cyclic load far below the ultimate tensile strength can fail. If the metal is simultaneously exposed to a corrosive environment, the failure can take place at an even lower stress and after a shorter time. Contrary to a pure mechanical fatigue, there is no fatigue limit in corrosion-assisted fatigue.
Example of metals that are subject to corrosion fatigue:
• Aluminium structures in corrosive atmosphere
Galvanic corrosion
When a corrosive electrolyte and two metallic materials are in contact (galvanic cell), corrosion increases on the least noble material (the anode) and decreases on the noblest (the cathode). The increase in corrosion is called galvanic corrosion. The tendency of a metal or an alloy to corrode in a galvanic cell is determined by its position in the galvanic series. The galvanic series indicates the relative nobility of different metals and alloys in a given environment (e.g. seawater, see figure 1.6.12). The farther apart the metals are in the galvanic series, the greater the galvanic corrosion effect will be. Metals or alloys at the upper end are noble, while those at the lower end are least noble.
Examples of metal that are subject to galvanic corrosion:
• Steel in contact with 1.4401
• Aluminium in contact with copper
The principles of galvanic corrosion are used in cathodic protection. Cathodic protection is a means of reducing or preventing the corrosion of a metal surface by the use of sacrificial anodes (zinc or aluminum) or impressed currents.
Fig. 1.6.11: Corrosion fatigue
Fig. 1.6.12: Galvanic corrosion
Fig. 1.6.13: Galvanic series for metals and alloys in seawater
Aluminium - less noble Copper - most noble
64
Section 1.6 Materials
Page 65
1.6.3 Metal and metal alloys
On the following pages, you can read about the features of different metals and metal alloys, used for construction of pumps.
Ferrous alloys
Ferrous alloys are alloys where iron is the prime constituent. Ferrous alloys are the most common of all materials because of their availability, low cost, and versatility.
Steel
Steel is a widely used material primarily composed of iron alloyed with carbon. The amount of carbon in steel varies in the range from 0.003% to 1.5% by weight. The content of carbon has an important impact on the material’s strength, weldability, machinability, ductility, and hardness. As a rule-of-thumb, an increase in carbon content will lead to an increase in strength and hardness but to a decrease in ductility and weldability. The most common type of steel is carbon steel. Carbon steel is grouped into four categories, see figure 1.6.14.
Steel is available in wrought as well as in cast condition. The general characteristics of steel castings are closely comparable to those of wrought steels. The most obvious advantage of steel is that it is relatively inexpensive to make, form and process. On the other hand, the disadvantage of steel is that its corrosion resistance is low compared to alternative materials, such as stainless steel.
Cavitation corrosion of bronze impeller
Erosion corrosion of cast iron impeller
Pitting corrosion of EN 1.4401 (AISI 316)
Intergranular corrosion of stainless steel
Crevice corrosion of EN 1.4462 (SAF 2205)
1 mm
Type of steel Content of carbon
Low carbon or mild steel 0.003% to 0.30% of carbon
Medium carbon steel 0.30% to 0.45% of carbon
High carbon steel 0.45% to 0.75% of carbon
Very high carbon steel 0.75% to 1.50% of carbon
Fig 1.6.14: Four types of carbon steel
65
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Nodular (ductile) iron
Nodular iron contains around 0.03-0.05% by weight of magnesium. Magnesium causes the flakes to become globular so the graphite is dispersed throughout a ferrite or pearlite matrix in the form of spheres or nodules. The graphite nodules have no sharp features. The round shape of nodular graphite reduces the stress concentration and consequently, the material is much more ductile than grey iron. Figure 1.6.16 clearly shows that the tensile strength is higher for nodular iron than is the case for grey iron. Nodular iron is normally used for pump parts with high strength requirements (high pressure or high temperature applications).
Stainless steel
Stainless steel is chromium containing steel alloys. The minimum chromium content in standardised stainless steel is 10.5%. Chromium improves the corrosion resistance of stainless steel. The higher corrosion resistance is due to a chromium oxide film that is formed on the metal surface. This extremely thin layer is self-repairing under the right conditions. Molybdenum, nickel and nitrogen are other examples of typical alloying elements. Alloying with these elements brings out different crystal structures, which enable different properties in connection with machining, forming, welding, corrosion resistance, etc. In general, stainless steel has a higher resistance to chemicals (i.e. acids) than steel and cast iron have.
Cast iron
Cast iron can be considered an alloy of iron, silicon and carbon. Typically, the concentration of carbon is between 3-4% by weight, most of which is present in insoluble form (e.g. graphite flakes or nodules). The two main types are grey cast iron and nodular (ductile) cast iron. The corrosion resistance of cast iron is comparable to the one for steel; and sometimes even better. Cast iron can be alloyed with 13-16% by weight silicon or 15-35% by weight nickel (Ni-resist) respectively in order to improve corrosion resistance. Various types of cast irons are widely used in industry, especially for valves, pumps, pipes and automotive parts. Cast iron has good corrosion resistance to neutral and alkaline liquids (high pH) . But its resistance to acids (low pH) is poor.
Grey iron
In grey iron, the graphite is dispersed throughout a ferrite or pearlite matrix in the form of flakes. Fracture surfaces take on a grey appearance (hence the name!). The graphite flakes act as stress concentrators under tensile loads, making it weak and brittle in tension, but strong and ductile in compression. Grey iron is used for the construction of motor blocks because of its high vibration damping ability. Grey iron is an inexpensive material and is relatively easy to cast with a minimal risk of shrinkage. That is why grey iron is often
used for pump parts with
moderate strength requirements.
1. Design of pumps and motors
1.1 Pump construction, (10)
Fig 1.6.15: Comparison and designations of grey iron
Fig 1.6.16: Comparison and designations of nodular iron
66
Section 1.6 Materials
Page 67
In environments containing chlorides, stainless steel can be attacked by localised corrosion, e.g. pitting corrosion and crevice corrosion. The resistance of stainless steel to these types of corrosion is highly dependent on its chemical composition. It has become rather common to use the so-called PRE (Pitting Resistance Equivalent) values as a measure of pitting resistance for stainless steel. PRE values are calculated by formulas in which the relative influence of a few alloying elements (chromium,
Chemical composition of stainless steel [w%]
Microstructure Designation % % % % % PRE
5)
EN/AISI/UNS Carbon max. Chromium Nickel Molybdenum Other
Ferritic
1.4016/430/ S43000 0.08 16-18 17
Martensitic 1.4057/431/ S43100 0.12-0.22 15-17 1.5-2.5 16
Austenitic 1.4305/303/ S30300 0.1 17-19 8-10 S 0.15-0.35 18
Austenitic 1.4301/304/ S30400 0.07 17-19.5 8-10.5 18
Austenitic 1.4306/304L/ S30403 0.03 18-20 10-12 18
Austenitic 1.4401/316/ S31600 0.07 16.5-18.5 10-13 2-2.5 24
Austenitic 1.4404/316L/ S31603 0.03 16.5-18.5 10-13 2-2.5 24
Austenitic 1.4571/316Ti/ 0.08 16.5-18.5 10.5-13.5 2-2.5 Ti > 5 x carbon 24 S31635 Ti < 0.70
Austenitic 1.4539/904L/ N08904 0.02 19-21 24-26 4-5 Cu 1.2-2 34
Austenitic 1.4547/none / 0.02 20 18 6.1 N 0.18-0.22 43 S 31254
3)
Cu 0.5-1
Ferritic/
1.4462/ none/ 0.03 21-23 4.5-6.5 2.5-3.5 N 0.10-0.22 34
austenitic S32205 2)
Ferritic/
1.4410/none/ 0.03 25 7 4 N 0.24-0.32 43
austenitic S 32750
4)
Microstructure Designation % % % % % PRE EN/ASTM/UNS Carbon max. Chromium Nickel Molybdenum Other
Austenitic 1) 1.4308/CF8/ J92600 0.07 18-20 8-11 19
Austenitic 1) 1.4408/CF8M/ J92900 0.07 18-20 9-12 2-2.5 26
Austenitic 1) 1.4409/CF3M/ J92800 0.03 18-20 9-12 2-2.5 N max. 0.2 26
Austenitic 1.4584/none/ none 0.025 19-21 24-26 4-5
N max. 0.
2
35
Cu 1-3
Ferritic/ Austenitic 1.4470/CD3MN/ J92205 0.03 21-23 4.5-6.5 2.5-3.5 N 0.12-0.2 35
Ferritic/ 1.4517/CD4MCuN/ N 0.12-0.22 Austenitic J93372 0.03 24.5-26.5 2.5-3.5 2.5-3.5 Cu 2.75-3.5 38
molybdenum and nitrogen) on the pitting resistance is taken into consideration. The higher the PRE, the higher the resistance to localised corrosion. Be aware that the PRE value is a very rough estimate of the pitting resistance of a stainless steel and should only be used for comparison/ classification of different types of stainless steel. In the following, we will present the four major types of stainless steel: ferritic, martensitic, austenitic and duplex.
1)
Contains some ferrite 2) Also known as SAF 2205, 3) Also known as 254 SMO, 4) Also known as SAF 2507
5)
Pitting Resistance Equivalent (PRE): Cr% + 3.3xMo% + 16xN%.
Fig 1.6.17: Chemical composition of stainless steel
67
Page 68
Ferritic (magnetic)
Ferritic stainless steel is characterised by quite good corrosion properties, very good resistance to stress corrosion cracking and moderate toughness. Low alloyed ferritic stainless steel is used in mild environments (teaspoons, kitchen sinks, washing machine drums, etc.) where it is a requirement that the component is maintenance-free and non-rusting.
Martensitic (magnetic)
Martensitic stainless steel is characterised by high strength and limited corrosion resistance. Martensitic steels are used for springs, shafts, surgical instruments and for sharp-edged tools, such as knives and scissors.
Austenitic (non-magnetic)
Austenitic stainless steel is the most common type of stainless steel and is characterised by a high corrosion resistance, very good formability, toughness and weldability. Austenitic stainless steel, especially the EN 1.4301 and EN 1.4401 are used for almost any type of pump components in the industry. This kind of stainless steel can be either wrought or cast.
EN 1.4305 is one of the most popular stainless steel types of all the free machining stainless steel types. Due to its high sulphur content (0.15-0.35 w%), the machinability has improved considerably but unfortunately at the expense of its corrosion resistance and its weldability. However, over the years free machining grades with a low sulphur content and thus a higher corrosion resistance have been developed.
If stainless steel is heated up to 500°C - 800°C for a longer period of time during welding, the chromium might form chromium carbides with the carbon present in the steel. This reduces chromium’s capability to maintain the passive film and might lead to intergranular
corrosion also referred to as sensitisation (see section 1.6.2). If low carbon grades of stainless steel are used the risk of sensitisation is reduced. Stainless steel with a low content
1. Design of pumps and motors
1.1 Pump construction, (10)
of carbon is referred to as EN 1.4306 (AISI 304L) or EN
1.4404 (AISI 316L). Both grades contain 0.03% of carbon compared to 0.07% in the regular type of stainless steel EN 1.4301 (AISI 304) and EN 1.4401 (AISI 316), see illustration 1.6.17.
The stabilised grades EN 1.4571 (AISI 316Ti) contain a small amount of titanium. Because titanium has a higher affinity for carbon than chromium, the formation of chromium carbides is minimised. The content of carbon is generally low in modern stainless steel, and with the easy availability of ‘L’ grades the use of stabilised grades has declined markedly.
Ferritic-austenitic or duplex (magnetic)
Ferritic-austenitic (duplex) stainless steel is characterised by high strength, good toughness, high corrosion resistance and excellent resistance to stress corrosion cracking and corrosion fatigue in particular. Ferritic-austenitic stainless steel is typically used in applications that require high strength, high corrosion resistance and low susceptibility to stress corrosion cracking or a combination of these properties. Stainless steel EN 1.4462
is widely used for making pump shafts and pump
housings.
68
Section 1.6 Materials
Page 69
Nickel alloys
Nickel base alloys are defined as alloys in which nickel is present in greater proportion than any other alloying element. The most important alloying constituents are iron, chromium, copper, and molybdenum. The alloying constituents make it possible to form a wide range of alloy classes. Nickel and nickel alloys have the ability to withstand a wide variety of severe operating conditions, for instance corrosive environments, high temperatures, high stresses or a combination of these factors.
HastelloysTM alloys are a line of commercial alloys containing Ni, Mo, Cr, and Fe. Nickel base alloys, such as InconelTM Alloy 625, HastelloysTM C-276 and C-22 are highly corrosion resistant and not subject to pitting or crevice corrosion in low velocity seawater, and do not suffer from erosion at high velocity.
The price of nickel base alloy limits its use in certain applications. Nickel alloys are available in both wrought and cast grades. However, nickel alloys are more difficult to cast than the common carbon steels and stainless steel alloys. Nickel alloys are especially used for pump parts in the chemical process industry.
Copper alloys
Pure copper has excellent thermal and electrical properties, but is a very soft and ductile material. Alloying additions result in different cast and wrought materials, which are suitable for use in the production of pumps, pipelines, fittings, pressure vessels and for many marine, electrical and general engineering applications.
Brasses are the most widely used of the copper alloys because of their low cost, their easy or inexpensive fabrication and machining. However, they are inferior in strength to bronzes and must not be used in environments that cause dezincification (see selective corrosion). Red brass, bronze and copper nickels in particular have, compared to cast iron a high resistance to chlorides in aggressive liquids, such as seawater. In such environments, brass is unsuitable because of its tendency to dezincificate. All copper alloys have poor resistance to alkaline liquids (high pH), ammonia and sulfides and are sensitive to erosion. Brass, red brass and bronze are widely used for making bearings, impellers and pump housings.
1) Lead can be added as an alloying element to improve the machinability.
2) Bronze can be alloyed with aluminium to increase strength.
Fig 1.6.18: Common types of copper alloys
69
Page 70
Titanium
Pure titanium has a low density, is quite ductile and has a relatively low strength. However, when a limited amount of oxygen is added it will strengthen titanium and produce the so-called commercial-pure grades. Additions of various alloying elements, such as aluminium and vanadium increase its strength significantly, at the expense of ductility. The aluminium and vanadium alloyed titanium (Ti-6Al-4V) is the “workhorse” alloy of the titanium industry. It is used in many aerospace engine and airframe components. Because titanium is a high-price material, it is not yet a material which is often used for making pump components.
Titanium is a very reactive material. As it is the case for stainless steel, titanium’s corrosion resistance depends on the formation of an oxide film. However, the oxide film is more protective than that on stainless steel. Therefore, titanium performs much better than stainless steel in aggressive liquids, such as seawater, wet chlorine or organic chlorides, that cause pitting and crevice corrosion.
1. Design of pumps and motors
1.1 Pump construction, (10)
Aluminium
Pure aluminium is a light and soft metal with a density of about a third of that of steel. Pure aluminium has a high electrical and thermal conductivity. The most common alloying elements are silicon (silumin), magnesium, iron and copper. Silicon increases the material’s castability, copper increases its machinability and magnesium increases its corrosion resistance and strength.
The obvious advantages of aluminium are that the material naturally generates a protective oxide film and is highly corrosion resistant if it is exposed to the atmosphere. Treatment, such as anodising, can further improve
this property. Aluminium alloys are widely used in structures where a high strength to weight ratio is important, such as in the transportation industry. For example, the use of aluminium in vehicles and aircrafts reduces weight and energy consumption.
On the other hand, the disadvantage of aluminium is that it is not stable at low or high pH and in chloride-containing environments. This property makes aluminium unsuitable for exposure to aqueous solutions especially under conditions with high flow. This is further emphasised by the fact that aluminium is a reactive metal, i.e. has a low position in the galvanic series (see galvanic corrosion) and may easily suffer from galvanic corrosion if coupled to nobler metals and alloys.
Designation Major alloying element
1000-series Unalloyed (pure) >99% Al
2000-series
Copper is the principal alloying element, though other
elements (magnesium) may be specified
3000-series Manganese is the principal alloying element
4000-series
Silicon is the principal alloying element
5000-series
Magnesium is the principal alloying element
6000-series
Magnesium and silicon are principal alloying elements
7000-series
Zinc is the principal alloying element, but other elements, such as copper, magnesium, chromium, and zirconium may be specified
8000-series
Other elements (including tin and some lithium
compositions)
CP: commercial pure (titanium content above 99.5%)
Fig 1.6.19: Major alloying elements of aluminium
Fig 1.6.20: Titanium grades and alloy characteristics
70
Section 1.6 Materials
Page 71
1.6.4 Ceramics
Ceramic materials are defined as inorganic, non-metallic materials, which are typically crystalline in nature. They are composed of metallic and non-metallic elements. Common technical ceramics are aluminium oxide (alumina
- Al2O3), silicon carbide (SiC), tungsten carbide (WC), and silicon nitride (Si3N4).
Ceramics are suitable for applications which require high thermal stability, high strength, high wear resistance, and high corrosion resistance. The disadvantage of ceramics is the low ductility and high tendency for brittle fractures. Ceramics are mainly used for making bearings and seal faces for shaft seals.
1.6.5 Plastics
Some plastics are derived from natural substances, such as plants, but most types are man-made. These are known as synthetic plastics. Most synthetic plastics come from crude oil, but coal and natural gas are also used. There are two main types of plastics: Thermoplastics and thermosets (thermosetting plastics). The thermoplastics are the most common kind of plastic used worldwide. Plastics often contain additives, which transfer certain additional properties to the material. Furthermore, plastics can be reinforced with fiberglass or other fibres. These plastics together with additives and fibres are also referred to as composites.
Examples of additives found in plastics
Inorganic fillers for mechanical reinforcement
Chemical stabilisers, e.g. antioxidants
Plasticisers
Flame retardants
Thermoplastics
Thermoplastic polymers consist of long polymer molecules that are not linked to each other, i.e. have no cross-links. They are often supplied as granules and heated to permit fabrication by methods, such as moulding or extrusion. A wide range is available, from low-cost commodity plastics (e.g. PE, PP, PVC) to high cost engineering thermoplastics (e.g. PEEK) and chemical resistant fluoropolymers (e.g. PTFE, PVDF). PTFE is one of the few thermoplastics, which is not melt-processable. Thermoplastics are widely
used for making pump housings or for lining of pipes and pump housings.
Thermosets
Thermosets harden permanently when heated, as cross­linking hinders bending and rotations. Cross-linking is achieved during fabrication using chemicals, heat, or radiation; this process is called curing or vulcanization. Thermosets are harder, more dimensionally stable, and more brittle than thermoplastics and cannot be remelted. Important thermosets include epoxies, polyesters, and polyurethanes. Thermosets are among other things used for surface coatings.
PP PE PVC PEEK PVDF PTFE*
Abbreviation
Polymer name
Polypropylene Polyethylene Polyvinylchloride Polyetheretherketone Polyvinylidene fluoride Polytetrafluoroethylen
e
*
Trade name: Teflon®
Linear polymer chains
Thermoplastics
Elastomers
Thermosets
Branched polymer chains
Weakly cross-linked polymer chains
Strongly cross-linked polymer chains
Fig 1.6.22: Different types of polymers
Fig 1.6.21: Overview of polymer names
71
Page 72
1. Design of pumps and motors
1.1 Pump construction, (10)
1.6.6 Rubber
The term rubber includes both natural rubber and synthetic rubber. Rubbers (or elastomers) are flexible long­chain polymers that can be stretched easily to several times their unstretched length and which rapidly return to their original dimensions when the applied stress is released. Rubbers are cross-linked (vulcanized), but have a low cross­link density, see figure 1.6.22. The cross-link is the key to the elastic, or rubbery, properties of these materials. The elasticity provides resiliency in sealing applications. Different components in a pump are made of rubber, e.g. gaskets and O-rings (see section 1.3 on shaft seals). In this section we will present the different kinds of rubber qualities and their main properties as regards temperature and resistance to different kinds of liquid groups.
At temperatures up to about 100°C nitrile rubber is an inexpensive material that has a high resistance to oil and fuel. Different grades exist - the higher the acrylonitrile (ACN) content, the higher the oil resistance, but the poorer is the low temperature flexibility. Nitrile rubbers have high resilience and high wear resistance but only moderate strength. Further, the rubber has limited weathering resistance and poor solvent resistance. It can generally be used down to about -30°C, but certain grades can operate at lower temperatures.
Ethylene propylene has excellent water resistance which is maintained to high temperatures approximately 120­140°C. The rubber type has good resistance to acids, strong alkalis and highly polar fluids, such as methanol and acetone. However, it has very poor resistance to mineral oil and fuel.
Fluoroelastomers (FKM)
Fluoroelastomers cover a whole family of rubbers designed to withstand oil, fuel and a wide range of chemicals including non-polar solvents. offers excellent
resistance to high temperature operation (up to 200°C
depending on the grade) in air and different types of oil.
rubbers have limited resistance to steam, hot water, methanol, and other highly polar fluids. Further, this type of rubber has poor resistance to amines, strong alkalis and many freons. There are standard and special grades
- the latter have special properties, such as improved low­temperature or chemical resistance.
Silicone rubbers have outstanding properties, such as low compression set in a wide range of temperatures (from
-60°C to 200°C in air), excellent electrical insulation and are non-toxic. Silicone rubbers are resistant to water, some acids and oxidizing chemicals. Concentrated acids, alkalines, and solvents should not be used with silicone rubbers. In general, these types of rubber have poor resistance to oil and fuel. However, the resistance of FMQ silicone rubber to oil and fuel is better than that of the silicone rubber types MQ, VMQ, and PMQ.
Perfluoroelastomers have very high chemical resistance, almost comparable to that of PTFE (polytetrafluorethylene, e.g. TeflonR). They can be used up to high temperatures, but their disadvantages are difficult processing, very high cost and limited use at low temperatures.
Common types of copper alloys
NBR
Abbreviation
Nitrile rubber
EPDM, EPM
Ethylene propylene rubber
FKM
Fluoroelastomers Viton
R
Siloprene
R
Buna-N
R
FFKM
Pe
rfluoroelastomers
Chemra
z
R
Kalrez
R
MQ, VMQ, PMQ, FMQ
Silicone rubber
Common nam
e
Examples of trade name
Nordel
R
Fig 1.6.23: Rubber types
72
Section 1.6 Materials
Page 73
1.6.7 Coatings
Protective coating – metallic, non-metallic (inorganic) or organic – is a common method of corrosion control. The main function of coatings is (aside from galvanic coatings, such as zinc) to provide an effective barrier between the metal (substrate) and its environment. They allow the use of normal steel or aluminium instead of more expensive materials. In the following section we will examine the possibilities of preventing corrosion by means of different coatings: Metallic and non-metallic (inorganic) coatings and organic coatings.
Metallic coatings
Metallic coatings less noble than the substrate
Zinc coatings are commonly used for the protection of steel structures against atmospheric corrosion. Zinc has two functions: it acts as a barrier coating and it provides galvanic protection. Should an exposed area of
steel occur, the zinc surface preferentially corrodes at a slow rate and protects the steel. The preferential protection is referred to as cathodic protection. When damage is small, the protective corrosion products of zinc will fill the exposed area and stop the attack.
Metallic coatings nobler than the substrate
Electroplating of nickel and chromium coatings on steel are examples of metallic coatings that are nobler than the substrate. Unlike galvanic coatings where the coating corrodes near areas where the base metal is exposed, any void or damage in a barrier coating can lead to an immediate base metal attack.
To protect the base steel,
zinc coating sacrifices itself
slowly by galvanic ac
tion.
Steel coated with a more noble
metal, such as nickel, corrodes
more rapidly if the coating
is damaged.
Fig 1.6.24: Galvanic vs. barrier corrosion protection
73
Page 74
Paints
As mentioned above, paints are an important class of organic coating. Figure 1.6.25 shows several types of organic coatings. A typical paint formulation contains polymeric binders, solvents, pigments and additives. For environmental reasons, organic solvents are increasingly being replaced by water or simply eliminated, e.g powder coating. Painted metal structures usually involve two or more layers of coating applied on a primary coating, which is in direct contact with the metal.
1. Design of pumps and motors
1.1 Pump construction, (10)
<
Non-metallic coatings (inorganic coatings)
Conversion coatings are an important category of non­metallic coatings (inorganic).
Conversion coatings
Conversion coatings are formed by a
controlled corrosion
reaction of the substrate in an oxidised
solution. Well-known examples of conversion coatings are anodising or chromating of aluminium, and phosphate treatment of steel. Anodising is mainly used for surface protection of aluminium, while chromating and phosphating are usually used for pre-treatment in connection with painting. Besides improving paint adhesion, it helps to prevent the spreading of rust under layers of paint.
Organic coatings
Organic coatings contain organic compounds and are available in a wide range of different types. Organic coatings are applied to the metal by methods of spraying, dipping, brushing, lining or electro-coating (paint applied by means of electric current) and they may or may not require heat-curing. Both thermoplastic coatings, such as polyamide,
polypropylene, polyethylene, PVDF and PTFE and
elastomer
coatings are applied to metal substrates to combine the mechanical properties of metal with the chemical resistance of plastics but paints are by far the most widely used organic coating.
Physical states of common organic coatings
Resin Solvent- Water- Powder Two comp. type
based based coating liquid
Ac
rylic X X X
Alky
d X X
Epox
y X X X X Polyester X X X Polyurethane X X X X Vi
nyl X X X
Fig 1.6.25: Physical states of common organic coatings
74
Section 1.6 Materials
Page 75
Chapter 2. Installation and performance reading
Section 2.1: Pump installation
2.1.1 New installation
2.1.2 Existing installation
2.1.3 Pipe flow for single-pump installation
2.1.4 Limitation of noise and vibrations
2.1.5 Sound level (L)
Section 2.2: Pump performance
2.2.1 Hydraulic terms
2.2.2 Electrical terms
2.2.3 Liquid properties
Page 76
Correct advice and selection of pump type for an installation has larger implication than what meets the eye. The larger the pumps, the greater the costs with respect to investment, installation, commissioning, running and maintenance – basically the life cycle cost (LCC). An extensive product portfolio combined with competent advice and after-sales service is the foundation of a correct selection. The following analysis, recommendations and hints are general for any installation, but to a greater extent relevant for medium-sized and large installations. We will present our recommendations for two types of installation: New and existing installations.
2.1.1 New installation
If the pipework has not been planned yet, you can base
the selection of pump type on other primary selection criteria, e.g. efficiency, investment costs or life cycle costs (LCC). This will not be covered in this section. However, the general guidelines, which are presented, also apply for pipework that has not yet been planned.
If the pipework has already been planned, the selection
of pump is equivalent to replacing a pump in an existing
installation.
76
2.1.2 Existing installation – replacement
The following five steps will help you make an optimum pump selection for an existing installation:
Pre-investigation of the installation should include the following considerations:
Basic pipe flow – pipes in and out of the building, e.g.
from ground, along floor or from ceiling
Specific pipework at the point of installation, e.g.
in-line or end-suction, dimensions, manifolds
Space available – width, depth and height
Accessibility in connection with installation and
maintenance, for instance doorways
Availability of lifting equipment or alternatively
accessibility of such equipment
Floor type, e.g. solid or suspended floor with basement
Existing foundation
Existing electric installation
Previous pump installation
Pump make, type, specifications including old duty
point, shaft seal, materials, gaskets, controlling
History, e.g. lifetime, maintenance
Future requirements
Desired improvements and benefits
New selection criteria including duty points and
operating times, temperature, pressure, liquid specifications
Supplier criteria, e.g. availability of spare parts
Advisory
Major changes might be beneficial in a long or short
term or both and must be documented, e.g. installation
savings, life cycle costs (LCC), reduction on environmental impact like noise and vibrations and accessibility in connection with maintenance
Selection
Must be based on a customer-agreed list of priorities
For the selection of the correct pump type and advice on installation, two main areas are important: Pipe flow and limitation of noise and vibrations. These two areas will be dealt with on the following pages.
Section 2.1 Pump installation
Page 77
2.1.3 Pipe flow for single-pump installation
Figure 2.1.1 is based on single-pump installation. In parallel installations accessibility plays a major role for how good a pump choice is.
The evaluation criterion is as simple pipework as possible, hence as few bends as possible.
Pipework
To the pump:
Along floor
Best choice
Best choice
Best choice
Best choice
Best choice
Best choice
Best choice
Good choice
Good choice
Good choice
Good choice
Good choice
Good choice
Good choice
Good choiceGood choice
Good choiceGood choice
Least good choice Least good choice
Least good choice
Least good choice
Good choice
Best choice
Best choice
Best choice Best choice
Best choice
Best choice
Not applicable
From ground
A. In-line close-coupled
(horizontal or vertical mounting)
From ceiling
Wall­mounted
From the pump:
Along floor
Along floor
To ground
To ceiling
To ground
To
ceiling
Wall­mounted
Along floor
To
ceiling
Pump type
To ground
C. End-suction long-coupled
(only horizontal mounting)
B. End-suction close- coupled
(horizontal or vertical mounting)
Scores:
Best choice
Good choice
Least good choice
Not applicable
Fig. 2.1.1 Pipework and pump type
77
Page 78
Accessibility plays a major role in how well a specific pump choice is in connection with installation of several pumps in parallel. The accessibility is not always easy for in-line pumps installed in parallel because of the pipework, see figure 2.1.2. As it appears from figure 2.1.3, end-suction pumps installed in parallel provide easier accessibility.
2.1.4 Limitation of noise and vibrations
To achieve optimum operation and minimise noise and vibration, it may be necessary to consider vibration dampening of the pump in certain cases. Generally, this should always be considered in the case of pumps with motors above 7.5 kW. Smaller motor sizes, however, may also cause undesirable noise and vibration. Noise and vibration are generated by the rotation in motor and pump and by the flow in pipes and fittings. The effect on the environment depends on correct installation and the state of the entire system. Below we will present 3 different ways of limiting noise and vibration in a pump installation: Foundation, dampeners and expansion joint.
Foundation
Floor constructions can be divided into two types: Solid floor and suspended floor.
Solid – minimum risk of noise due to bad transmission of vibrations, see figure 2.1.4.
Suspended – risk of floor amplifying the noise. Basement can act as a resonance box, see figure 2.1.5.
The pump should be installed on a plane and rigid surface. Four basic ways of installation exist for the two types of floor construction: Floor, plinth, floating plinth and foundation suspended on vibration dampeners.
Fig. 2.1.3: 3 end-suction pumps in parallel; easier maintenace access because of pipework
Fig. 2.1.4: Solid floor construction
Fig. 2.1.5: Suspended floor construction
Fig. 2.1.2: 3 in-line pumps in parallel; limited maintenance access because of pipework
Floor
Solid ground
Floor
Wall
Ground floor
Basement
Floor
Solid ground
78
Section 2.1 Pump installation
Page 79
Floor Direct mounting on floor, hence direct vibration transmission, see figure 2.1.6.
Plinth Poured directly on concrete floor, hence as floor, see figure 2.1.7.
Floating plinth Resting on a dead material, e.g. sand, hence reduced risk of vibration transmission, see figure 2.1.8.
Foundation suspended on vibration dampeners Optimum solution with controlled vibration transmission, see figure 2.1.9.
As a rule of thumb, the weight of a concrete foundation should be 1.5 x the pump weight. This weight is needed to get the dampeners to work efficiently at low pump speed.
Fig. 2.1.6: Floor
Floor Base plate Pump unit
Fig. 2.1.10: The same foundation rules go for vertical in-line pumps
Fig. 2.1.7: Plinth
Floor Plinth Base plate Pump unit
Fig. 2.1.8: Floating plinth
Floor Sand Plinth Base plate Pump unit
Fig. 2.1.9: Foundation suspended on vibration dampeners
Floor
Vibration dampeners Foundation Base plate Pump unit
Pump unit
Foundation
Vibration dampeners
Floor
79
Page 80
Dampeners
The selection of the right vibration dampener requires the following data:
Forces acting on the dampener
Motor speed considering speed control, if any
Required dampening in % (suggested value is 70%)
The determination of the right dampener varies from installation to installation but a wrong selection of dampener may increase the vibration level in certain cases. The supplier should therefore size vibration dampeners.
Pumps installed with vibration dampeners must always have expansion joints fitted at both the suction and the discharge side. This is important in order to avoid that the pump hangs in the flanges.
Expansion joints
Expansion joints are installed to:
absorb expansions/contractions in the pipework
caused by changing liquid temperature
reduce mechanical strains in connection with pressure
waves in the pipework
isolate mechanical noise in the pipework (not for metal
bellows expansion joints)
Expansion joints must not be installed to compensate for inaccuracies in the pipework, such as centre displacement or misalignment of flanges.
Expansion joints are fitted at a distance of minimum 1 to
1.5 . DN diameter from the pump on the suction side as well as on the discharge side. This prevents the development of turbulence in the expansion joints, resulting in better suction conditions and a minimum pressure loss on the pressure side. At high water velocities (>5 m/s) it is best to install larger expansion joints corresponding to the pipework.
Fig. 2.1.11: Installation with expansion joints, vibration dampeners and fixed pipework
Base plate
Pump unit
Vibration dampeners
Floor
Expansion joint
Foundation
80
Section 2.1 Pump installation
Page 81
Figures 2.1.12-2.1.14 show examples of rubber bellows expansion joints with or without tie bars.
Expansion joints with tie bars can be used to minimise the forces caused by the expansion joints. Expansion joints with tie bars are recommended for sizes larger than DN 100. An expansion joint without tie bars will exert force on the pump flanges. These forces affect the pump and the pipework.
The pipes must be fixed so that they do not stress the expansion joints and the pump, see figure 2.1.11. The fix points should always be placed as close to the expansion joints as possible. Follow the expansion joint supplier’s instructions.
At temperatures above 100°C combined with a high pressure, metal bellows expansion joints are often preferred due to the risk of rupture.
2.1.5 Sound level (L)
The sound level in a system is measured in decibel (dB). Noise is unwanted sound. The level of noise can be measured in the following three ways:
1. Pressure – Lp : The pressure of the air waves
2. Power – LW : The power of the sound
3. Intensity - LI: The power per m2 (will not be covered in this book)
It is not possible to compare the three values directly, but it is possible to calculate between them based on standards. The rule of thumb is:
Fig. 2.1.14: Metal bellows expansion joints with tie bars
Fig. 2.1.12: Rubber bellows expansion joints with tie bars
Fig. 2.1.13: Rubber bellows expansion joints without tie bars
Smaller pumps, e.g. 1.5 kW: Lw = LP + 11 dB
Larger pumps, e.g. 110 kW: Lw = LP + 16 dB
120
100
80
60
40
20
20 50 100 200 1 2 5 10 20kHz500Hz
0
Frequency kHz
Pain threshold
Lp (dB)
Threshold of hearing
Speech
Music
Fig. 2.1.15: Threshold of hearing vs. frequency
81
Page 82
The EU Machine Directive prescribes that sound levels have to be indicated as pressure when they are below 85 dB(A) and as power when they exceed 85 dB(A).
Noise is subjective and depends on a person´s ability to hear, e.g. young vs. old person. Therefore, the above­mentioned measurements get weight according to the sensibility of a standard ear, see figure 2.1.15. The weighting is known as A-weighting (dB(A)), expressed as e.g: LpA, and the measurements are adjusted depending on frequency. In some cases it increases and in other cases it decreases, see figure 2.1.16. Other weightings are known as B and C but they are used for other purposes, which we do not cover in this book.
In case of two or more pumps in operation, the sound level can be calculated. If it is pumps with the same sound level the total sound level can be calculated adding the value from figure 2.1.17, e.g. 2 . pumps is Lp + 3 dB, 3 . pumps is Lp + 5 dB. If the pumps have different sound level, values from figure 2.1.18 can be added.
Indications of sound level should normally be stated as free field conditions over reflecting surface, meaning the sound level on a hard floor with no walls. Guaranteeing values in a specific room in a specific pipe system is difficult because these values are beyond the reach of the manufacturer. Certain conditions could have a negative impact (increasing sound level) or a positive impact on the sound level. Recommendations to installation and foundation can be given to eliminate or reduce the negative impact.
dB (A)
10
0
10
100 1000
-10
-20
-30
-40
-50
-60
-70
-80
10000 Hz
4 8 12 16 20 24
5
10
15
2 4 6 8 10
1
2
2.5
1.5
0.5
3
Fig. 2.1.16 A-weighting curve
Fig. 2.1.17 Increase of the total sound pressure level with equal sources
Fig. 2.1.18 Increase of the total sound pressure level with different sources
Experience values:
Rise of Perceived as:
+ 3dB Just noticeable + 5dB Clearly noticeable +10dB Twice as loud
82
Section 2.1 Pump installation
Page 83
Section 2.2 Pump performance
When you examine a pump, there are several things you have to check. Besides checking the pump’s physical condition, for instance if it is rusty or makes abnormal noise, you have to know a number of values in order to be able to tell if the pump performs as it is supposed to. On the next pages, we will present three groups of values you may need to focus on when you examine a pump’s performance: Hydraulic terms, electrical terms, mechanical terms and liquid properties.
2.2.1 Hydraulic terms
When you want to examine pump performance, there are a number of values you need to know. In this section, we will present the most important hydraulic terms: Flow, pressure and head.
Flow
Flow is the amount of liquid that passes through a pump within a certain period of time. When we deal with performance reading, we distinguish between two flow parameters: Volume flow and mass flow.
Volume flow (Q)
Volume flow is what we can read from a pump curve or put in another way, a pump can move a volume per unit of time (measured in m3/h) no matter the density of the liquid. When we deal with e.g. water supply, volume flow is the most important parameter, because we need the pump to deliver a certain volume, e.g. of drinking water or water for irrigation.Throughout this book the term flow refers to volume flow.
Mass flow (Qm)
Mass flow is the mass, which a pump moves per unit of time and is measured in kg/s. The liquid temperature has an influence on how big a mass flow the pump can move per unit of time since the liquid density changes with the temperature. In connection with heating, cooling and air-condition systems, the mass flow is an essential value to know, because the mass is the carrier of energy (see Heat capacity).
Fig. 2.2.1: Calculation examples
Examples Unit
Water
Volume flow Q 10m3/h
Density 998 943kg/m
3
Mass flow Q
m
9980 9403kg/h
2.77 2.62kg/s
at 20˚C at 120˚C
Q
m
Q
m
ρ
. Q
ρ
Q
= =
;
83
Page 84
Pressure (p)
Pressure is a measure of force per unit area. We distinguish between static pressure, dynamic pressure and total pressure. The total pressure is the sum of the static pressure and the dynamic pressure:
Static pressure
The static pressure p
sta
is the pressure, which is measured with a pressure gauge placed perpendicular to the flow or in a non-moving liquid, see figure 2.2.2.
Dynamic pressure
The dynamic pressure p
dyn
is caused by liquid velocity. Dynamic pressure cannot be measured by a normal pressure gauge, but is calculated by the following formula:
1 2
where: ρ is the density of the liquid in [kg/m3] v is the velocity of the liquid in [m/s]
Dynamic pressure can be converted into static pressure by reducing the liquid velocity and vice versa. Figure 2.2.3 shows a part of a system where the pipe diameter increases from D1 to D2, resulting in a decrease in liquid speed from v1 to v2. Assuming that there is no friction loss in the system, the sum of the static pressure and the dynamic pressure is constant throughout the horizontal pipe.
1 2
1 2
So, an increase in pipe diameter, as the one shown in figure 2.2.3 results in an increase in the static head which is measured with the pressure gauge p2.
In most pumping systems, the dynamic pressure p
dyn
has a minor impact on the total pressure. For example, if the velocity of a water flow is 4.5 m/s, the dynamic pressure is around 0.1 bar, which is considered insignificant in many pumping systems. Later on in this chapter, we will discuss dynamic pressure in connection with determining the head of a pump.
Fig. 2.2.2: How to determine the static pressure p
sta
, the dynamic
pressure p
dyn
and the total pressure p
tot
Fig. 2.2.3: The static pressure increases if the liquid velocity is reduced. The figure applies for a system with insignificant friction loss
D
2
D
1
p
sta
p
tot
p
dyn
A
P
B
p
1
p
2
v
1
v
2
p
sta
p
tot
p
dyn
p
tot
p
sta
p
sta
p
tot
Q
84
Section 2.2 Pump performance
Page 85
10.2 m
10.6 m
12.75 m
2
4
6
8
10
12
H(m)
Q
Duty point for brine at 20˚C
Duty point for water at 20˚C
Duty point for water at 95˚C
Duty point for diesel at 20˚C
7.3 m
10.2 m
10.6 m
12.75 m
1 bar 1 bar 1 bar 1 bar
Brine at 20°C 1300 kg/m
3
1 bar = 7.3 m
Water at 20°C 997 kg/m
3
1 bar = 10.2 m
Water at 95°C 960 kg/m
3
1 bar = 10.6 m
Diesel oil at 20°C 800 kg/m
3
1 bar = 12.75 m
Fig. 2.2.5: Pumping four different liquids at 1 bar at the discharge side of the pump results in four different heads (m), hence four different duty points
Measuring pressure
Pressure is measured in e.g. Pa (N/m²), bar (105 Pa) or PSI (Ib/in²). When we deal with pressure it is important to know the point of reference for the pressure measurement. Two types of pressure are essential in connection with pressure measurement: Absolute pressure and gauge pressure:
Absolute pressure (p
abs
)
Absolute pressure is defined as the pressure above absolute vacuum, 0 atm, that is the absolute zero for pressure. Usually, the value “absolute pressure” is used in cavitation calculations.
Gauge pressure
Gauge pressure, often referred to as overpressure, is the pressure, which is higher than the normal atmospheric pressure (1 atm). Normally, pressure p is stated as gauge pressure, because most sensor and pressure gauge measurements measure the pressure difference between the system and the atmosphere. Throughout this book the term pressure refers to gauge pressure.
Head (H)
The head of a pump is an expression of how high the pump can lift a liquid. Head is measured in meter (m) and is independent on the liquid density. The following formula shows the relation between pressure (p) and head (H):
1 2
1 2
where : H is the head in [m] p is the pressure in [Pa = N/m2] ρ is the liquid density in [kg/m3] g is the acceleration of gravity in [m/s2]
Normally, pressure p is measured in [bar], which equals 10
5
Pa. However, other pressure units are used as well, see
figure 2.2.4.
The relation between pressure and head is shown in figure
2.2.5 where a pump handles four different liquids. The head of the pump depends on the type of liquid. As it appears from the figure, the pumping of different liquids results in different heads and hence different duty points.
7.3 m
10.2 m
10.6 m
12.75 m
1 Pa = 1 N/m
2
10
-5
1 9.87 . 10
-4
750
.
10
-5
1.02
.
10
-4
750
1.02
.
10
-5
1
10
5
0.987 10.21.02
760
1.013
1.013 . 10
5
1 10.331.033
736
0.981
0.981 . 10
5
0.968 101
73.6
0.0981
0.981 . 10
4
* Physical atmosphere ** Theoretical atmosphere
0.0968 10.1
Pa bar
Conversion table for pressure units
atm* at** mH2O mmHg
1 bar
1 atm
1 at = 1 kp/cm
3
1 m H2O
2
4
6
8
10
12
H(m)
1 bar 1 bar 1 bar 1 bar
Q
Duty point for brine at 20˚C
Duty point for water at 20˚C
Duty point for water at 95˚C
Duty point for diesel at 20˚C
Fig. 2.2.4:
Conversion table for pressure units
85
Page 86
Fig. 2.2.6: Standard end-suction pump with dimension difference on suction and discharge ports
How to determine the head
The pump head is determined by reading the pressure on the flanges of the pump p2, p1 and then convert the values into head – see figure 2.2.6. However, if a geodetic difference in head is present between the two measuring points, as it is the case in figure 2.2.6, it is necessary to compensate for the difference. Furthermore, if the port dimensions of the two measuring points differ from one another the actual head has to be corrected for this as well.
The actual pump head H is calculated by the following formula:
1 2
1 2
where : H is the actual pump head in [m] p is the pressure at the flanges in [Pa = N/m2] ρ is the liquid density in [kg/m3] g is the acceleration of gravity in [m/s2] h is the geodetic height in [m] v is the liquid velocity in [m/s]
The liquid velocity v is calculated by the following formula:
1 2
1 2
where: v is the velocity in [m/s] Q is the volume flow in [m3/s] D is the port diameter in [m]
When combining these two formulas, head H depends on the following factors: The pressure measurements p1 and p2, the difference in geodetic height between the measuring points (h2-h1), the flow through the pump Q and the diameter of the two ports D1 and D2 .
1 2
1 2
The correction due to the difference in port diameter is caused by the difference in the dynamic pressure. Instead of calculating the correction from the formula, the contribution can be read in a nomogram, see appendix F.
h2h
1
v
1
p
1D1
D
2
v
2
p
2
86
Section 2.2 Pump performance
Page 87
Calculation example
A pump of the same type as the one shown in figure 2.2.7 is installed in a system with the following data:
Q = 240 m3/h p1 = 0.5 bar p2 = 1.1 bar Liquid: Water at 200C
Suction port diameter D1 = 150 mm Discharge port diameter D2 = 125 mm. The difference in height between the two ports where the pressure gauges are installed is h2-h1 = 355 mm.
We are now able to calculate the head of the pump:
As it appears from the calculation, the pressure difference measured by pressure gauges is about 1.1 m lower than what the pump is actually performing. This calls for an explanation. First, the deviation is caused by the difference in height between the pressure gauges (0.36 m) and second, it is caused by the difference in port dimensions, which in this case is 0.77 m.
Fig. 2.2.7: Standard end-suction pump with different dimensions of suction and discharge ports (Example)
1 2
1 2
1 2
1 2
1 2
1 2
h2h
1
v
1
p
1D1
D
2
v
2
p
2
h2 - h1 = 355 mm
v1 = 3.77 m/s
2
p1 = 0.5 bar
D1 = 150 mm
D
2
= 125 mm
v
2
= 5.43 m/s
2
p
2
= 1.1 bar
87
Page 88
Fig.2.2.8: The system pressure H
sta
in a closed system
has to be higher than the physical height of the installation
If the pressure gauges are placed at the same geodetic height, or if a differential pressure gauge is used for the measurement, it is not necessary to compensate for the difference in height (h2-h1). In connection with in-line pumps, where inlet and outlet are placed at the same level, the two ports often have the same diameter. For these types of pumps a simplified formula is used to determine the head:
1 2
1 2
Differential pressure (∆p)
The differential pressure is the pressure difference between the pressures measured at two points, e.g. the pressure drops across valves in a system. Differential pressure is measured in the same units as pressure.
System pressure
The system pressure is the static pressure, which is present at a point in the system, when the pumps are not running. System pressure is important to consider when you deal with a closed system. The system pressure in (m) H
sta
in the lowest point must always be higher than the height of the system in order to ensure that the system is filled with liquid and can be vented properly.
h
Dry cooler
Chiller
H
syst
> h
H
syst
88
Section 2.2 Pump performance
Page 89
NPSH
Q
H
Fig.: 2.2.12: NPSH-curve
Cavitation and NPSH
Cavitation occurs somewhere in a pump when the pressure is lower than the vapour pressure of the liquid, see figures
2.2.9 and 2.2.10.
When the pressure on the suction side drops below the vapour pressure of the liquid, (figure 2.2.10 yellow dot). small vapour bubbles form. These bubbles collapse (implode) when the pressure rises (figure 2.2.10 red dot) and releases shock waves. Consequently, impellers can be damaged by the energy released. The rate of damage to the impeller depends on the properties of the material. Stainless steel is more resistant to cavitation than bronze, and bronze is more resistant to cavitation than cast iron, see section 1.6.3.
Cavitation decreases flow (Q) and head (H), which leads to reduced pump performance, see figure 2.2.11. Damage due to cavitation is often only detected when the pump is dismantled. Furthermore, cavitation results in increased noise and vibrations, which can consequently damage bearings, shaft seals and weldings.
Calculation of the risk of cavitation
To avoid cavitation, the following formula is used to calculate the maximum suction head:
h
max
– Maximum suction head
Hb – Atmospheric pressure at the pump site; this is the theoretical maximum suction lift, see figure 2.2.13
Hf – Friction loss in the suction pipe
NPSH = Net Positive Suction Head (is to be read at the NPSH curve at the highest operational flow), see figure
2.2.12.
b
Pressure [Pa]
Impeller inlet Impeller outlet
a
p
p
1
Vapour pressure
p
Fig.: 2.2.9: Implosion of cavitation bubbles on the back of impeller vanes
Q
NPSH
H
Q
H
Curve when pump cavitates
Fig.: 2.2.10: Development of pressure through a centrifugal pump
Fig.: 2.2.11: Pump curve when pump cavitates
a = Front of impeller vanes b = Back of impeller vanes
a
b
a = Front of impeller vanes b = Back of impeller vanes
89
Imploding vapour bubbles
Page 90
The NPSH value indicates to what extent the pump is not able to create absolute vacuum, that is to lift a full water column 10.33 m above sea level, see figure 2.2.13.
NPSH can either be named NPSHr (required) or NPSHa (available).
NPSH
required
The required suction head for the pump
NPSH
available
The available suction head in the system
The NPSH value of a pump is determined by testing according to ISO 9906 and is made in the following way. The suction head is reduced while the flow is kept at a constant level. When the differential pressure has decreased by 3%, the pressure at the pump’s suction side is read; and the NPSH value of the pump is defined. The testing is repeated at different flows, which form the basis of the NPSH curve in the end.
Put in another way: When the NPSH curve is reached, the level of cavitation is so high that the head of the pump has decreased by 3%.
Hv – Vapour pressure of the liquid; for more information concerning vapour pressure of water, go to appendix D.
Hs – Safety factor. Hs depends on the situation and normally varies between 0.5 m and 1 m and for liquids containing gas up to 2 m, see figure 2.2.15.
2.2.2 Electrical terms
When you want to examine a pump performance, you need to know a range of values. In this section we will present the most important electrical values: Power consumption, voltage, current and power factor.
Liquid with air
Q [m3/s]
H [m]
NPSH
Vented liquid
Fig.: 2.2.15: Typical NPSH-curve for liquid containing gas
NPSH
H
b
H
f
h
H
v
20
15
12 10
8,0
6,0 5,0
4,0
3,0
2,0
1,0 0,8
0,6
0,4 0,3
0,2
0,1
1,5
120
110
90
100
80
70
60
50
40
30
20
10
0
Hv (m)tm(˚C )
150
130
140
25
35
45 40
30
20
15
12 10
8,0
6,0 5,0
4,0
3,0
2,0
1,0 0,8
0,6
0,4 0,3
0,2
0,1
1,5
120
110
90
100
80
70
60
50
40
30
20
10
0
Hv (m)
tm
(˚C )
150
130
140
25
35
45 40
30
Fig.: 2.2.14: System with indication of the different values that are important in connection with suction calculations
Height above
sea level
(m)
0
500
1000
2000
1.013 10.33
0.935
100
9.73
0.899
0.795
9.16
8.10
99
96
93
Barometric
pressure
pb (bar)
Water
column
Hb(m)
Boiling point
of water
(˚C)
Fig.: 2.2.13: Barometric pressure above sea level
90
Section 2.2 Pump performance
Page 91
Power consumption (P)
Pumps are made of several components, see figure 2.2.16. The power consumption of the different components is designated in the following way:
P1 The power input from the mains or, put in another
way, the amount of power the consumer has to pay for
P2 The power input to the pump or the power output
from the motor. Often referred to as shaft power
PH Hydraulic power – the power that the pump
transfers to the liquid in the shape of flow and head
For the most common pump types, the term power consumption normally refers to P2. Power is measured in W, kW.
Efficiency in connection with pumps normally only covers the efficiency of the pump part ηP. A pump’s efficiency is determined by several factors, for instance the shape of the pump housing, the impeller and diffuser design and the surface roughness. For typical pump units consisting of both pump and electric motor, the total efficiency ηT also includes the efficiency of the motor:
If a frequency converter is included as well, the efficiency of the entire unit also has to incorporate the efficiency of the frequency converter:
P
1
P
2
P
H
Fig. 2.2.16: Pump unit with indication of different power consumption levels
91
Page 92
Voltage (U)
Like pressure drives flow through a hydraulic system, voltage drives a current (I) through an electrical circuit. Voltage is measured in volts (V) and can be either direct current (DC), e.g. 1.5 V battery – or alternating current (AC), e.g. electricity supply for houses, etc. Normally, pumps are supplied with AC voltage supply. The layout of AC mains supply differs from one country to another. However, the most common layout is four wires with three phases (L1, L2, L3) and a neutral (N). Besides these four wires, a protective earth connection (PE) is added to the system as well, see figure 2.2.17. For a 3x400 V/230 V mains supply, the voltage between any two of the phases (L1, L2, L3) is 400 V. The voltage between one of the phases and neutral (N) is 230 V. The ratio between the phase-phase voltage and the phase­neutral voltage is determined by the formula on your right:
Current is the flow of electricity and is measured in ampere (A). The amount of current in an electrical circuit depends on the supplied voltage and the resistance/ impedance in the electrical circuit.
Power (P) and power factor (cosϕ or PF)
Power consumption is indeed of high importance when it comes to pumps. For pumps with standard AC motors, the power input is found by measuring the input voltage and input current and by reading the value cosϕ on the motor/pump nameplate. cosϕ is the phase angle between voltage and current. cosϕ is also referred to as power factor (PF). The power consumption P1 can be calculated by the formulas shown on your right depending on whether the motor is a single-phase or a three-phase motor.
L
1
L
2
L
3
N
PE
400V Three-phase supply
230V Single-phase supply
Fig. 2.2.17: Mains supply, e.g. 3 x 400 V
}
}
AC single-phase motor, e.g. 1 x 230 V
AC three-phase motor, e.g. 3 x 400 V
92
Section 2.2 Pump performance
The voltage between any two phases (L1, L2, L3) is for a 3x400 V/230 V mains supply, 400 V. The voltage between one of the phases and neutral (N) is 230V. The ratio between the phase-phase voltage and the phase-neutral voltage is:
Page 93
2.2.3 Liquid properties
When you are making your system calculations, there are three properties you might need to know about the liquid in order to make the right calculations: Liquid temperature, density, and heat capacity.
The liquid temperature is measured in °C (Celcius), K (Kelvin), or °F (Fahrenheit). °C and K are actually the same unit but 0°C is the freezing point of water and 0K is the absolute zero, that is -273.15°C - the lowest possible temperature. The calculation between Fahrenheit and Celcius is: °F = °C . 1.8 + 32, hence the freezing point of water is 0°C and 32°F and the boiling point is 100°C and 212°F.
The density is measured in kg/m3 or kg/dm3.
The heat capacity tells us how much additional energy a liquid can contain per mass when it is heated. Liquid heat capacity depends on temperature, see figure 2.2.18. This is used in systems for transporting energy, e.g. heating, air­con and cooling. Mixed liquids, e.g. glycol and water for air-con have a lower heat capacity than pure water hence higher flow is required to transport the same amount of energy.
93
-40 -20 0 20
60
80
40 100 120˚C
2.0
2.4
2.8
3.2
3.6
4.0
4.4
0.5
0.6
0.7
0.8
0.9
1.0
kJ/kgK kcal/kgK
0% pure water
20%
34%
44%
52%
Fig. 2.2.18: Heat capacity vs. temperature for ethylene glycol
Page 94
Chapter 3. System hydraulic
Section 3.1: System characteristics
3.1.1 Single resistances
3.1.2 Closed and open systems
Section 3.2: Pumps connected in series and parallel
3.2.1 Pumps in parallel
3.2.2 Pumps connected in series
Page 95
Page 96
Section 3.1 System characteristics
Previously, in section 1.1.2 we discussed the basic characteristics of pump performance curves. In this chapter we will examine the pump performance curve at different operating conditions as well as a typical system characteristic. Finally, we will focus on the interaction between a pump and a system.
A system’s characteristic describes the relation between the flow Q and head H in the system. The system characteristic depends on the type of system in question. We distinguish between two types: Closed and open systems.
• Closed systems
are circulating systems like heating or air-conditioning systems, where the pump has to overcome the friction losses in the pipes, fittings, valves, etc. in the system.
• Open systems
are liquid transport systems like water supply systems. In such systems the pump has to deal with both the static head and overcome the friction losses in the pipes and components.
When the system characteristic is drawn in the same system of co-ordinates as the pump curve, the duty point of the pump can be determined as the point of intersection of the two curves, see figure.3.1.1.
Open and closed systems consist of resistances (valves, pipes, heat exchanger, etc.) connected in series or parallel, which altogether affect the system characteristic. Therefore, before we continue our discussion on open and closed systems, we will briefly describe how these resistances affect the system characteristic.
Fig. 3.1.1: The point of intersection between the pump curve and the system characteristic is the duty point of the pump
96
Page 97
3.1.1 Single resistances
Every component in a system constitutes a resistance against the liquid flow which leads to a head loss across every single component in the system. The following formula is used to calculate the head loss ∆H:
∆H = k . Q
2
k is a constant, which depends on the component in question and Q is the flow through the component. As it appears from the formula, the head loss is proportional to the flow in second power. So, if it is possible to lower the flow in a system, a substantial reduction in the pressure loss occurs.
Resistances connected in series
The total head loss in a system consisting of several components connected in series is the sum of head losses that each component represents. Figure 3.1.2 shows a system consisting of a valve and a heat exchanger. If we do not consider the head loss in the piping between the two components, the total head loss ∆H
tot
is calculated by
adding the two head losses:
∆H
tot
= ∆H1 + ∆H
2
Furthermore, figure 3.1.2 shows how the resulting curve will look and what the duty point will be if the system is a closed system with only these two components. As it appears from the figure, the resulting characteristic is found by adding the individual head losses ∆H at a given flow Q. Likewise, the figure shows that the more resistance in the system, the steeper the resulting system curve will be.
Fig. 3.1.2: The head loss for two components connected in series is the sum of the two individual head losses
97
Page 98
Resistances connected in parallel
Contrary to connecting components in series, connecting components in parallel result in a more flat system characteristic. The reason is that components installed in parallel reduce the total resistance in the system and thereby the head loss. The differential pressure across the components connected in parallel is always the same. The resulting system characteristic is defined by adding all the components’ individual flow rate for a specific ∆H. Figure 3.1.3 shows a system with a valve and a heat exchanger connected in parallel.
The resulting flow can be calculated by the following formula for a head loss equivalent to ∆H
Q
tot
= Q 1 + Q
2
3.1.2 Closed and open systems
As mentioned previously, pump systems are split into two types of basic systems: Closed and open systems. In this section, we will examine the basic characteristics of these systems.
Closed systems
Typically, closed systems are systems, which transport heat energy in heating systems, air-conditioning systems, process cooling systems, etc. A common feature of these types of closed systems is that the liquid is circulated and is the carrier of heat energy. Heat energy is in fact what the system has to transport.
Closed systems are characterised as systems with pumps that only have to overcome the sum of friction losses, which are generated by all the components. Figure 3.1.4 shows a schematic drawing of a closed system where a pump has to circulate water from a heater through a control valve to a heat exchanger.
Fig. 3.1.3: Components connected in parallel reduce the resistance in the system and result in a more flat system characteristic
Fig. 3.1.4: Schematic drawing of a closed system
98
Section 3.1 System characteristics
Page 99
All these components together with the pipes and fittings result in a system characteristic as the one shown in figure
3.1.5. The required pressure in a closed system (which the system curve illustrates) is a parabola starting in the point (Q,H) = (0,0) and is calculated by the following formula:
H = k . Q
2
As the formula and curve indicate, the pressure loss is approaching zero when the flow drops.
Open systems
Open systems are systems, where the pump is used to transport liquid from one point to another, e.g. water supply systems, irrigation systems, industrial process systems. In such systems the pump has to deal with both the geodetic head of the liquid and to overcome the friction losses in the pipes and the system components.
We distinguish between two types of open system:
• Open systems where the total required geodetic lift is positive.
• Open systems where the total required geodetic lift is negative.
Open system with positive geodetic head Figure
3.1.6 shows a typical open system with positive geodetic lift. A pump has to transport water from a break tank at ground level up to a roof tank on the top of a building. First of all, the pump has to provide a head higher than the geodetic head of the water (h). Secondly, the pump has to provide the necessary head to overcome the total friction loss between the two tanks in piping, fittings, valves, etc. (Hf). The pressure loss depends on the amount of flow, see figure 3.1.7.
Fig. 3.1.5: The system characteristic for a closed system is a parabola starting in point (0,0)
Fig. 3.1.6: Open system with positive geodetic lift
Fig. 3.1.7: System characteristic together with the pump performance curve for the open system in figure 3.1.6
Q
Q
1
99
Page 100
The figure shows that in an open system no water flows if the maximum head (H
max
) of the pump is lower than the geodetic head (h). Only when H > h, water will start to flow from the break tank to the roof tank. The system curve also shows that the lower the flow rate, the lower the friction loss (Hf) and consequently the lower the power consumption of the pump.
So, the flow (Q1) and the pump size have to match the need for the specific system. This is in fact a rule-of­thumb for liquid transport systems: A larger flow leads to a higher pressure loss, whereas a smaller flow leads to a smaller pressure loss and consequently a lower energy consumption.
Open system with negative geodetic lift
A typical example of an open system with negative required head is a pressure booster system, e.g. in a water supply system. The geodetic head (h) from the water tank brings water to the consumer - the water flows, although the pump is not running. The difference in height between the liquid level in the tank and the altitude of the water outlet (h) results in a flow equivalent to Qo. However, the head is insufficient to ensure the required flow (Q1) to the consumer. Therefore, the pump has to boost the head to the level (H1) in order to compensate for the friction loss (Hf) in the system. The system is shown in figure 3.1.8 and the system characteristic together with the pump performance curve are shown in figure 3.1.9.
The resulting system characteristic is a parabolic curve starting at the H-axes in the point (0,-h).
The flow in the system depends on the liquid level in the tank. If we reduce the water level in the tank the height (h) is reduced. This results in a modified system characteristic and a reduced flow in the system, see figure 3.1.9.
Fig. 3.1.8: Open system with negative geodetic lift
Fig. 3.1.9: System characteristic together with the pump performance curve for the open system in figure 3.1.8
100
Section 3.1 System characteristics
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