(particularly high speed units such as QB, QD,
QDX, and QV) when pumping liquids indicates
presence of gas bubbles in the pumping chamber
which are reducing pumping capacity and may be
damaging cylinder walls. Such bubbles may be
traced to 1) a poor seal at the suction fitting, 2) fluid
vaporization (cavitation) or, 3) degassing of the
fluid.
a) To correct suction fitting leaks in stainless steel
pump heads, remove fitting and wrap two layers of
Teflon tape (standard Lab plumbing variety, 1 to 2
mil thick x 1/2" wide) tightly into the threads of the
fitting. Replace fitting in cylinder port, drawing
threads tightly on the Teflon tape. (see para 16).
b) To eliminate vaporization and degassing noise,
reduce suction load. This may be accomplished
by: 1) Using the 3/8" dia. TUBE ADAPTER R4122 supplied with each pump on the suction line of
the pump head to increase inside diameter of the
suction line (use 1/2" dia. TUBE ADAPTER R4126K on -3 PHM’s.); 2) reduction of suction lift height;
3) pressurization of suction supply container; 4) locating pump below supply source to permit gravity
flow aid; 5) reduce viscosity of fluid by heating or
thinning; 6) reduce flow rate by adjusting pump to
lower setting on flow scale; 7) install FMI PD-HF
PULSE SUPPRESSORS in suction and discharge
lines.
Improvements in noise abatement and pump life
can be gained by putting pulse suppression hardware in the plumbing circuits adjacent to the pump
suction and discharge ports - particularly with high
speed pumps that are plumbed with rigid tubing.
Theory holds that if part of a generated pulse is resiliently stored, the part not stored is smaller and
thus easier to get into motion; the stored part of the
pulse dissipating behind the part that is in motion
sustains motion, causing an undulating flow to be
transmitted rather than a series of pulses. Result:
less noise, less energy used and less agitation of
the pumped fluid. So for pulse noise and vibration
problems, put a little resilience in your circuit.
There are a number of rather easy ways to do it:
c) The simplest method is to use resilient tubing
between the pump and the fluid circuit. Experiment
a bit with standard elastomers - viton, hypalon,
gum rubber, soft vinyl or other. Use only unreinforced tubing (reinforcement takes away the resilience). Always shield this type of arrangement
so that a possible tube rupture will not endanger
people or equipment.
d) Another popular pulse suppression arrangement involves a gas bubble trap as described in
the final sentences of para. 12. A bubble in such a
vertical trap will suppress pulse shock and noise
temporarily. However, since gas and a liquid in
contact under agitated conditions seldom stabilize,
the trapped gas may absorb into the passing liquid
and disappear leaving no pulse suppression or the
fluid may contribute to the gas quantity, overload
the trap and cause random pumping errors as occasional bubbles enter the flow stream. This can
be overcome by fitting a soft slug of closed-cellplastic foam or a soft pillow of thin-wall plastic tubing (ends sealed) into the vertical dead end
extension of the fluid line. The gas trapped in the
foam or pillow will provide the required resilience
but will not be absorbed by the flow stream.
e)Since each fluid and circuit exhibits differing
characteristics, a bit of experimentation may be
necessary. The results are usually worth the effort.
11. FOR BEST LOW FLOW PUMPING RESULTS:
Use a pump having a maximum flow rating as near
to the desired flow rate as possible and keep suction and discharge pressures essentially constant
(see para 13). FMI pumps using R479 Low Flow
Kits or designated LF are specifically designed for
low flow/low dead volume, 1/4-28 flat bottom fittings.
12. LOW FLOW BUBBLE PROBLEMS.
A common cause of trouble in metering pump applications requiring low flow rates - a few milliliters
per minute or less - is the seemingly inevitable gas
bubble trapped in the pumping head of the metering pump. It expands on the suction stroke and
contracts on the discharge stroke, allowing little, if
any, liquid to pass through the pump. Such bubbles, though often attributed to leaks in pump
seals, can usually be traced to gases released by
the pumped fluid in response to pumping agitation
or pressure/temperature changes. When so identified, this potential source of metering pump error
can be effectively controlled in most fluid circuits.
The familiar bubbles that form on the inside walls
of a tumbler of tap water after it stands for a period
of time at room temperature demonstrate the typical liquid degassing that results from pressure reduction (water line pressure to atmospheric) and/or
temperature elevation (from ground ambient to air
ambient). In this case, the bubbles contain air, hydrogen, carbon dioxide or other gaseous materials
carried in the water; only small quantities of vaporized water are present. Some liquids respond to
agitation and/or pressure/temperature changes by
chemically separating into liquid and gas fractions;
others simply vaporize, physically changing from
liquid to gaseous form. Examples of liquids releasing gas or changing from liquid to gaseous form in
response to agitation and temperature/pressure
changes are numerous in the modern technical environment and many techniques have been devised to compensate for or correct their presence.
The most common practices for bubble control employ:
a) pressure on the suction side of the pump circuit
to encourage gas retention in the liquid or,
b) employ natural buoyancy of the bubbles to carry
them away from or through the pump head.
To apply pressure on the suction side of the pump,
locate the pump physically below the supply vessel. Each two feet of elevation difference represents pressure of approximately one pound per
square inch (psi). Bubbles that do occur will return
to the supply vessel by buoyant lift. This is called
a positive suction or flooded suction arrangement.
If it is necessary to draw liquid up from the supply
vessel to the pump head, negative suction pressure must be contemplated - again, approximately
1 psi per two feet of lift. Most liquids will release
some gas when held at negative pressure and
since the volume of gas released is generally proportionate to the volume of liquid subjected to the
negative pressure, suction line diameter should be
kept small for small flows (except heavy, viscous or
tacky liquids which require large flow area for mobility). A vertical dead-end extension of the suction
line can be provided above the pump suction port
to trap line-generated bubbles before they enter
the pump. This extension should be liquid filled at
the start of a pumping period. Stand the pump vertically by loosening the screws and repositioning
the Multi-Position Tilt Stand Q650 so that pump is
in standing position, or hang the pump vertically by
its base key slots. The discharge port should now
be above the suction port allowing bubbles that
enter the pump head to pass directly through with
buoyant assist. Discharge lines should be inclined
upward from pump head and bubble traps should
be purged as often as necessary to assure liquid
flow continuity.
13. SYSTEM ACCURACY FACTORS.
Several interrelated factors are involved in the exceptional operating accuracy possible in systems
using FMI PUMPS. Of primary concern are the following:
a) FMI PUMP DISPLACEMENT precision is based
on a simplified positive stroke mechanism which
has no secondary linkages to produce stroke to
stroke mechanical errors and has no gravity actuated or spring loaded valves to introduce random
valve seating errors. The single mechanical linkage component between the PUMP piston and its
drive elements is a precision spherical bearing
which transforms circular drive motion into elliptical
thrust motion (reciprocation). The total mechanical
clearance of this linkage is less than 0.1% of the
maximum pump stroke length or, approximately
0.0003". Thus it may be said that PUMP displacement precision (stroke to stroke) is in the order of
the mechanical linkage clearance; that is to say,
stroke to stroke displacement is reproducible to
less than 0.5% within the rated capacity of a given
pump model.
b) FMI PUMP VALVING is performed by a flat in
the piston which is mechanically aligned with one
cylinder port during the suction portion of each
stroke and with the other cylinder port during the
discharge portion of each stroke. The flat alignment is controlled by the single drive bearing discussed in the preceding sentences. The valve
action is therefore mechanically precise, and free
of random closure variations.
c) FLUID SLIP, a term commonly used to describe
the migration of fluid around the internal moving
parts of gear, lobe and vane pumps, is the volumetric difference between physical component displacement and fluid through-put of a pump system.
In the FMI PUMP, slip loss refers to the fluid which
passes through the clearance space (approx.
.0002") between the piston and the cylinder wall.
Since this clearance represents a restrictive passage of essentially constant dimension, it will be
readily seen that the slip rate is determined by viscosity, pressure and time: e.g. assuming constant
fluid viscosity and pressure, slip will be a smaller
factor in a high repetition rate pump (short time per
stroke) than in a low repetition rate pump. As viscosity increases and pressure decreases, time (or
repetition rate) becomes less a significant contributor to slip loss.
d) STROKE REPETITION RATE is directly related
to drive motor speed which in turn is influenced by
work load and electrical supply voltage, i.e., motor
speed decreases when work load increases and
when electrical supply voltage (115 Volts AC) decreases. This motor speed variation may amount
to as much as 15% for work load variations between zero discharge pressure and maximum
rated discharge pressure. A 10% voltage drop may
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