IV.2 Structural Viscosity (Pseudoplasticity and Dilatancy) ............................................................... 16
Appendix A - Maintenance ..................................................................................................17
Appendix B - Calibration of the Ball Constants ................................................................18
Appendix C - Online Help and Additional Resources ......................................................19
Appendix D - Warranty Repair and Service .......................................................................20
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I. INTRODUCTION
Falling Ball Viscometer, Model KF40, complies with the German industry standard DIN 53015.
The measuring principle, according to Höppler, is to determine the falling time of a ball in a
cylindrical glass tube lled with liquid. The working angle of the falling tube in the KF40
are variable at 80°, 70°, 60° and 50° relative to horizontal. The water jacket, surrounding the
falling tube, when connected to a Brookeld circulating temperature bath provides for precise
temperature control of the sample.
The user calculates the dynamic viscosity of the sample by determining the falling time of the
ball between the upper and lower ring marks displayed on the falling tube. Using data on the
ball constants, the density dierence between the liquid sample and the ball, and the working
angle constant, a mathematical equation is used to convert the time measurement to a viscosity
value in centipoise.
Note: The ball constants (forwards and backwards) and ball densities are listed on the test
certicate accompanying the instrument. You must provide the density value for the
liquid that you are testing.
The six (6) balls with dierent diameters and densities enable the KF40 to measure a wide
range of viscosities. The ability to adjust the angle of inclination extends the measuring range
for low viscosity liquids.
For non-Newtonian liquids, by subjecting the same sample to repetitive measurements with the
KF40 at dierent angles, pseudoplastic or dilatant behavior may be determined as explained in
Section IV. Time dependent behavior (thixotropy and rheopexy) may also be noted.
The ease of operation and precise temperature control, using a Brookeld circulating temperature
bath, allows for very reproducible measuring results.
I.1 Components
Component Part No. Quantity
KF40 Falling Ball Viscometer KF40 1
Set of (6) balls with gauge (FB68) in a carrying case (FB26) FB30C 1
Supplied w/certicate stating diameter and mass of each ball
-Ball 1 (glass) FB1 -
-Ball 2 (glass) FB2 -
-Ball 3 (nickel and iron) FB3 -
-Ball 4 (nickel and iron) FB4 -
-Ball 5 (steel) FB5 -
-Ball 6 (steel) FB6 -
Ball Tweezers FB51 1
Wire Cleaning Brush for Sample Tube FB53 1
Brush to clean loose debris from Falling Balls FB52 1
I.3 Details on Viscosity Measurement Range and Accuracy
Per DIN 53015, the Falling Ball method is suitable for measuring dynamic viscosities ranging
from 0.6 mPa•s to 250,000 mPa•s at temperatures from -5ºC to 150ºC. Use is made of six
balls having dierent diameters, each ball covering part of the range. All guideline values and
referenced parameters in the following table are per DIN 53015.
Viscosity
Ball
No.
10.5 to 10Borosilicate glass2.415.81 ± .01 ± 0.0005 0.007
29 to 140Borosilicate glass2.415.6 ± 0.05 ± 0.0005 0.09
These are the accuracy values reported in the DIN53015 standard.
AMETEK Brookeld has determined the accuracy of the viscometer using balls 2 and 3 according
to the method specied in the DIN53015 standard.
To determine the accuracy of the viscometer for balls 1, 4, 5 and 6, please refer to the method
specied in the DIN 53015 standard.
I.4 Description of the Equipment
Refer to Figures 1 and 2. Specic items identied on the Falling Ball Viscometer are identied by
parentheses ( ) in the following steps:
1. The Falling Ball Viscometer must be level. The level is adjusted using the three Leveling
Feet (4) on the base. Adjust so that the bubble level on top of the Falling Ball Viscometer
is centered within the circle. Check level periodically during use.
2. The working angles of the KF40 are 80°, 70°, 60° and 50° relative to horizontal. The DIN
53015 working position of 80° is the preferred position. The dierent working angles are
secured by the adjustment screw (5). To select a working angle, the adjustment screw (5)
should be loosened by turning it counter-clockwise approximately one rotation. After the
working angle is selected, the adjustment screw should then be tightened again.
3. The two running directions of the balls can be chosen by swiveling the viscometer, which
is kept in place by the Stop to hold the viscometer in position (22).
4. The glass tube (6) is surrounded by a waterbath jacket (9) which is xed between the upper
plate (7) and lower plate (8). The upper locking plug (16) with lid (20), the lower locking
plug (17) and accompanying seals (19), and the caps (18) are designed to perform the
following functions within the sample tube:
a. keep the liquid sample tightly sealed.
b. eliminate the formation of air bubbles.
c. avoid a build up of pressure
5. Mounted on the lower and upper plates are inlet/outlet ports (10a and 10b) for connection
to the water bath.
NOTE: Any alteration, modication or replacement of the sample tube, water jacket,
falling tube screw ttings, tension rods or balls renders the ball constants
invalid and requires the re-calibration of the viscometer. See Appendix B.
6. The thermometer screw (11) and thermometer seal (13) with inserted thermometer is screwed
into M10x1 Thermometer attachment thread (12) in the upper plate. The thermometer screw
should be tightened securely to prevent uid leakage.
NOTE: Caution when handling the glass thermometer!
7. The primary function of the ball gauge is to distinguish the two glass balls (Ball No. 1 and
Ball No. 2) from each other. Ball No. 1 will not pass through the ball gauge, whereas Ball
No. 2 will pass through. The ball gauge may also be used to help identify Ball No. 2 through
4.
Page 8
Balls (set of 6)
(p/n FB1-FB6)
Ball Gauge (p/n FB68)
Case (p/n FB26)
Foam Inserts (p/n FB27, FB28 & FB29)
Figure 1
NOTES:
Ball diameters, weights, densities and ball constants (forwards and backwards) are
listed in the test certicate accompanying the viscometer.
The following explains safety symbols which may be found in this operating manual.
Refer to the manual for specic warning or caution information to avoid personal injury
or damage to the instrument.
PrecautionsIf this instrument is used in a manner not specied by the manufacturer, the protection
provided by the instrument may be impaired.
This instrument is not intended for use in a potentially hazardous environment.
The user should ensure that the substances placed under test do not release poisonous,
toxic or ammable gases at the temperatures to which they are subjected to during the
testing.
I.6 Cleaning
Great care should be given to cleaning of the sample tube, the locking plugs and the balls. These
components (material: glass, Ni-iron, steel, perbunane, silicone, stainless steel surfaces) must
not be damaged or subject to chemical action by the cleaning uid.
The cleaning procedure is to be carried out in the following sequence:
• The viscometer is pulled out of the bearing guide (14) in the stand by turning it 90° and
placed in a suitable collecting basin.
• Unscrew the caps and remove the locking plugs in such a way that the ball does not fall into
the collecting basin (possibly damaging the ball). The ball collector (Part No. FB23) is an
optional item that can be purchased on request.
• Clean the sample tube using a suitable cleaning agent for the material being measured with
the cleaning brush (Part No. FB53).
• There must not be any residue remaining in the sample tube or on the balls after they have
been cleaned and are dry. Wipe with a cloth that will not leave bers, if necessary.
• When cleaning, be careful that the cleaning agent does not come into contact with the
The balls are chosen in such a way that the minimum falling time is not less than what is shown
in the table and the maximum falling time is not greater than 300s. The DIN 53015 indicates
that a falling time greater than 300s is allowed, but for practical reasons, a shorter test time
makes more sense.
Ball
No.
Diameter
[mm]
115.81600.510
215.60302.5130
315.603020700
415.20302007800
514.0030100045000
611.0030550070000
The specications for the ball constant and the ball density are taken from the test certicate
which came with the equipment.
The exchange of balls or equipment components between dierent viscometers is not permitted.
Otherwise, the ball constants lose their validity.
When the falling time for the ball is less than the minimum time, turbulence may occur.
II.2 Filling the Sample Tube
Minimum falling
time [s]
Lower measuring range limit
[mPa•s]
Upper
measuring range
limit [mPa•s]
To ll the sample tube:
• The sample tube is locked on the lower plate with the lower locking plug, seal, and cap.
• The liquid is lled up to approximately 25mm beneath the top of the sample tube without
air bubbles. Use a glass lter to remove any impurities when introducing a liquid into the
tube.
• The ball is polished with the leather cloth and bers are removed with the small cleaning
brush, before being inserted into the tube with the ball tweezers. The ball must not be touched
after polishing. The ball will travel to the bottom of the tube. Possible air bubbles in the
sample, or trapped below the ball, are removed with a suitable rod, by rotating the ball.
• Insert the upper locking plug with seal into the sample tube. In so doing, the sample must
enter the inside of the upper locking plug through the opening. The upper locking plug must
not be lled more than half way with the sample in order to minimize pressure build-up due
to the air bubbles. Due to the design of the upper locking plug, air bubbles cannot get into
the sample tube.
• The sample must be free of air bubbles between the two locking plugs. The lid of the upper
locking plug is attached and the temperature control (desired test temperature) must be
achieved. After proper temperature control is achieved, the upper cap is screwed on.
Do not heat the sample with the upper lid attached as pressure may build in the tube.
NOTE: Gas bubbles can be removed by warming up the sample for a short time (approximately
20 degrees above the measuring temperature with the upper locking plug removed)
or by lightly tapping on the lid of the upper locking plug.
II.3 Temperature Control of the Sample
The following are suggested working uids for the circulating temperature bath:
Temperature
Range
-5 to +20°CWater (distilled) - glycol-mixture; mixed
in accordance with the manufacturer’s
instructions for the temperature range
+1°C to +80°CDistilled waterLatex tube
+80°C to +150°CTransparent thermostatic oilInsulated Fluran tube,
Bath Working FluidsTubing
Insulated Latex tubing,
secured with tube band clips
secured with tube band clips
The inlet and outlet ports should be oriented in the following manner. During initial ll of
water jacket, the inlet will be at the bottom of the viscometer and the outlet will be at the top.
The tubing from the circulating bath should be pushed tightly onto the viscometer tubes. By
pulling gently, check whether the tubing is rmly attached. Tubing and circulating baths are
available on request from AMETEK Brookeld or your local authorized dealer. If the water
bath jacket has condensation on the glass, rub with alcohol.
The sample tube is sealed with the upper cap after temperature set point has been achieved.
Allow 30 minutes for thermal equilibrium.
Falling ball viscometers provide precise temperature control for the sample. By measuring
your sample at multiple temperatures, you can determine the temperature viscosity curve.
Before beginning the measurement, the upper cap must be loosened (unscrewed) again to let
o possible pressure.
The time which the balls take to run between the top and bottom ring marks in the sample tube
is determined with a stop watch (resolution 0.01s).
It is recommended that you record the passage of the lower ball point using the ring marks as
follows. Position your eyes at the same height as the ring marks so that these appear as a line.
A dark paper, placed behind the viscometer with its edge at the same height as the ring mark,
shows the ball periphery more distinctly.
With dark liquids, you can better observe the ball in the sample tube by looking from behind
the instrument.
Possible variations in the measuring times may be due to impurities in the sample, air bubbles
or the fact that it has not been brought to the right temperature (insucient temperature control).
Even 0.1°C change in temperature is clearly measurable. The rst forward and return passage
of the ball can be used to achieve a thorough mixing (temperature equalization) of the sample
before running the viscosity test.
BALL BEGINS
DESCENT
START STOPWATCH WHEN
BOTTOM OF
BALL CROSSES OVER THE
RING MARK
BALL
BALL IN
TRANSIT
AT
MIDPOINT
BALL
FINISHES
DESCENT
RING MARK
STOP STOPWATCH WHEN
BOTTOM OF
BALL CROSSES
OVER RING
MARK
With Newtonian liquids absolute values of the dynamic viscosity are calculated, where as,
for non-Newtonian liquids, relative values of the dynamic viscosity (apparent viscosity) are
calculated.
The dynamic viscosity is calculated according to the following equation:
Equation 1:η = t(ρ
where: ηdynamic viscosity [mPa•s]
t traveling time of the ball [s]
ρ1 density of the ball according to the test certicate [g/cm3]
ρ2 density of the sample [g/cm3]
K ball constant according to test certicate [mPa·cm3/g]
F working angle constant
-ρ
1
)K•F
2
Angle of inclination a
(applied to the level)
80° (DIN)1.0
70°0.952
60°0.879
50°0.778
Working angle constant F
The density and ball constant are each stated in the test certicate.
Consideration for buoyancy of the ball in the sample is accounted for by means of (ρ1-ρ2) in
equation (1).
The density of the sample can be determined by:
• referring to the material specications from the manufacturer of the uid
• measuring with a densitometer
Note: Be sure to measure the sample density at the same temperature at which the viscosity
will be measured.
As ρ
sity of the sample to be determined to 0.001g/cm3 (3rd decimal position) for the glass balls and
-ρ
1
becomes small, a higher resolution on density measurement is required. The den-
2
0.01g/cm3 (2nd decimal position) for the metal balls.
Non-Newtonian behavior can be determined when dierent measurement times are recorded
with repeated tests.
IV.1 Thixotrophy/Rheopexy
Thixotropy (rheopexy) is indicated if the traveling times for a ball decreases (increases) when
repeated measurements are made on the same volume of sample.
NOTE: If temperature control is not done correctly, thixotropy or rheopexy can be
inferred by mistake.
Rotational or Capillary Viscometers should be used for better determination of ow behavior.
IV.2 Structural Viscosity (Pseudoplasticity and Dilatancy)
Using the KF40 Falling Ball Viscometer at dierent angles may serve to determine pseudoplastic
or dilatant behavior for non-Newtonian liquids. If the sample is non-Newtonian, the travel time
of the ball multiplied by the sine of the working angle for the KF40 will not remain constant.
This infers non-Newtonian ow behavior. For pseudoplasticity, the calculated value decreases;
for dilatancy, it increases.
NOTE: If temperature control is not done correctly, pseudoplasticity or dilatancy can be
inferred by mistake.
Details about the relative values for pseudoplasticity and dilatancy are related to the diameter
of the ball and the working angle.
More sophisticated equipment, like rotational viscometers/rheometers, should be used for
Brookeld’s certication of the instrument is performed with Ball #2 and Ball #3 as well as
using the Cannon N44 viscosity standard with a nominal value of 92 mPa•s at 20°C.
Re-calibration of the ball constants is required by the operator if:
1. changes in the sample tube or water jacket were made
2. one or more balls were replaced
The calibration requires the use of a Newtonian mineral oil viscosity standard. Choice of the
viscosity standard is according to the ball. Use the appropriate Cannon or Brookeld viscosity
standard that falls within the viscosity measurement range.
BALL NO.123456
Recommended Viscosity
Standards
(cP, mPa•s)
The calibration is made according to the method in DIN 53015 at 20°C ± .05°C. A suitably
calibrated thermometer can be obtained from your local authorized dealer, on request.
CannonCannonCannonCannonCannonN/A
S3N10N100N350N1000N/A
3.9 cP @
20°C
21 cP @
20°C
283 cP @
20°C
830 cP @
20°C
2900 cP @
20°C
N/A
Ball #6 is not recommended for use in performing a calibration check.
The ball constants are determined from (5) running times, in both forward and reverse direction.
The ball constant is calculated according to the following equation:
Equation 3:
K =
η
(ρ1-ρ2)
• t
t Mean value from 5 running times [s]
η Dynamic viscosity of the calibrating uid [mPa•s] at 20°C ± .05 C
ρ1 Density of ball [g/cm3]
ρ2 Density of calibrating uid [g/cm3]
Note: Be sure to measure the sample density at the same temperature at which the viscosity
will be measured.
The expected value of the constant should be similar to the constant stated in the test certicate.
For Ball No. 6, the ball constant changes insignicantly as a function of the falling tube diameter
and diameter of the ball, so that the ball constant is calculated according to the following equation:
Equation 4:
K6 = 1.4057(D-d6)
(0.75042+1.82637 )
d
D
6
D Falling tube diameter (15.94 mm)
d6 Diameter of Ball No. 6 (see calibration certicate)
K6 Ball constant of Ball No. 6
The Brookeld website is a good resource for additional and self-help whenever you need it. Our
website oers a selection of “how-to” videos, application notes, conversion tables, instructional manuals,
material safety data sheets, calibration templates and other technical resources.
www.youtube.com/user/BrookeldEng
Brookeld has its own YouTube channel. Product and Application Videos can be found here.
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request your hard copy of articles by calling our customer service department directly or
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this path: www.brookeldengineering.com/learning-center/articles-and-technical-papers
More Solutions to Sticky Problems
Learn more about viscosity and rheology with our most popular publication. This informative booklet will
provide you with measurement techniques, advice and much more. It’s a must-have for any Brookeld
Viscometer or Rheometer operator. More Solutions is available in print and also as a downloadable
pdf on the Brookeld website by following this path:
http://www.brookeldengineering.com/support/documentation
Training/Courses
Whether it is instrument-specic courses, training to help you better prepare for auditing concerns, or
just a better understanding of your methods, who better to learn from than the worldwide leaders of
viscosity measuring equipment? Visit our Services section on our website to learn more about training.
Brookeld Viscometers are guaranteed for one year from date of purchase against defects in materials and
workmanship. ey are certied against primary viscosity standards traceable to the National Institute
of Standards and Technology (N.I.S.T.). e Viscometer must be returned to AMETEK Brookeld or to
the authorized dealer from whom it was purchased for a warranty evaluation. Transportation is at the
purchaser’s expense. e Viscometer should be shipped in its carrying case together with all spindles
originally provided with the instrument. If returning to Brookeld, please contact us or go on-line for
a return authorization number prior to shipping.
For a copy of the Repair Return Form, go to the Brookeld website: