1. Experiment is contained in the WACKER's Experimental Kit.

No

 2. Experimental procedure has been modified

/

 3. A separate experimental procedure has been devised

Yes

 4. Video clip available

No

 5. Flash animation available

No

 6. Other materials: Worksheet 9

Viscosity of Silicone Fluids/Variant A

TopDown 1 Materials, Chemicals, Time Needed
  • Laboratory stand
  • Retort
  • Magnetic hot plate and stirrer bar
  • Glass beaker, 1 l
  • Glass tube (length = approx. 50 cm, Ø = 6 mm)
  • 2 metal balls ( Ø = 3.5 mm and 5.5 mm)
  • Thermometer (100 °C)
  • Stop-watch
  • Magnet
  • Small plastic funnel
  • Fine permanent felt-tip marker
  • Triangle
  • Rubber stopper

A single measurement at a given temperature takes about 5 minutes. The total time needed for the measurement series, which involves different temperatures, depends essentially on the heating and cooling rate of the waterbath and is hard to predict. In general, given a methodical approach, 1.5 hours should suffice for the series of measurements (see 4 Tips and comments).
Series of measurements on other oils take more time because the tube has to be rinsed, dried and then equilibrated again each time.

TopDown 2 Procedure and Observations

Set up the apparatus as shown in the diagram.
Clamp the glass tube at a slight angle of around 10°. The precise angle is not critical for the calculation later because it is allowed for in the apparatus constant. However, to ensure that the readings are comparable, all measurements must be carried out at the exact same angle. This is achieved by keeping the retaining clamp in one position. Do not change its position throughout the experiment.

Before the glass tube is clamped in position, make two marks on it, one about 3 cm beneath the water surface and the other 1.5 cm above the rubber stopper.

Then fill the tube with the respective oil, ensuring there are no bubbles, add the steel ball and clamp the tube in position.
The glass tube must be equilibrated at this temperature for at least 5 minutes before the measurements are started.

For the measurement itself, use the magnet, which has also been equilibrated, to draw the steel ball up to about 1 cm below the water surface and then measure the time for the ball to fall between the two markings. Take five readings at each temperature.
  If the “fall time” for the larger ball is too long, use the smaller one. Doing this does not affect the temperature dependence.
For each oil (see list of chemicals), determine the fall time at five temperatures roughly 10 °C apart (approx. 10 °C, room temperature, 35 °C, 45 °C, 55 °C).
It will be seen that the fall time decreases in all oils as the temperature rises.
The fall time in silicone fluids is much longer than in the other oils.
TopDown The following fall times were measured in a reference experiment:
    Fall time in s
OIL Temperature in °C No. 1 No. 2 No. 3 No. 4 No. 5 Æ


Olive oil

Æ (ball)
= 5.5 mm

9 24.80 24.00 24.20 24.00 24.00 24.20
25 11.10 11.20 12.00 12.00 12.00 11.66
38 7.00 7.00 7.00 7.00 7.00 7.00
50 5.00 5.00 5.00 5.00 5.00 5.00
58 4.00 4.00 4.00 4.00 4.00 4.00

Sewing machine oil

Æ (ball)
= 5.5 mm

9 13.00 13.50 13.50 13.00 13.00 13.20
24 6.00 6.00 6.00 6.00 6.00 6.00
38 3.80 4.00 4.00 3.80 3.80 3.88
45 3.00 2.00 2.00 3.00 2.50 2.50
55 2.00 2.00 2.00 2.00 2.00 2.00
SILFOAM®
AK 5000


Æ (ball)
= 3.5 mm
13 112.00 109.00 108.00 109.00 109.00 109.40
25 86.00 80.00 85.00 83.00 83.00 83.40
38 60.00 64.00 64.00 60.00 62.00 62.00
47 53.00 54.00 53.00 53.00 53.00 53.20
100 24.00 24.00 22.00 24.00 23.00 23.40
SILFOAM®
 AK 1000


Æ (ball)
= 3.5 mm
17 19.70 19.20 20.00 20.10 20.00 19.80
25 18.00 17.00 18.00 17.00 17.00 17.40
33 14.90 14.00 15.00 15.00 14.90 14.76
43 12.00 12.00 11.80 12.00 12.00 11.96
56 9.00 9.80 9.90 9.00 9.00 9.34
As may be seen, there is very good reproducibility among the readings.

TopDown 3 Discussion of Results

The natural logarithm of the fall time decreases linearly with rise in temperature. This is illustrated in the diagram with the readings from the reference experiment.
Additionally, it may be seen from the slope of the curves that the viscosity (which is proportional to the fall time measured here) is not so dependent on the temperature in the case of the silicone fluids as it is with the other oils.
This property of silicone fluids is a key factor in their use in hydraulic equipment that must function reliably at temperatures that vary considerably. One such case is airplanes, where mineral oils would be unsuitable because their viscosity is too dependent on the temperature.

TopDown 4 Tips and Comments

  • For school use, it is advisable to dispense with calculating the viscosity from the fall time readings and simply to convey that viscosity and fall time are related to each other in the form of “the higher, the longer.”
  • It is best to leave the fall times in silicone fluid until last as silicone fluid is hard to remove from the glass tube.
    To shorten the experiment time, it is advisable to keep two very large glass beakers containing very hot and cold water handy so that the temperatures for making the readings can be adjusted quickly.
  • Metal balls of different sizes can be obtained in bicycle shops, for example.
  • The experiment illustrates clearly that the viscosity (fall time) of silicone fluids is less dependent on the temperature than it is for other oils. This may be explained in terms of their linear structure and the comparative lack of interactions between silicone molecules.
  • The experiment is suitable for introducing advanced chemistry students to the concept of viscosity. Normally, this is only done with organic oils. Silicone fluid makes a good oil for comparison because of its special properties and its importance in industry.
  • The experiment is ideal for classrooms because it is easy to conduct and the chemicals employed are relatively safe. To save time, groups of pupils could study a different oil.
  • To enhance the pupils’ computer skills, a computer should be used for the evaluation. The evaluation could also be set as homework.

TopDown  5 Supplementary Information

Viscosity (internal friction) is the property of a liquid to resist mutual displacement of two adjacent layers. Nowadays, the so-called dynamic viscosity η = t/D is defined as the ratio of the shear stress to the velocity gradient parallel to the direction of flow.
In Newtonian fluids, the viscosity at a given temperature is a property of the material. That is not true of non-Newtonian fluids. With non-Newtonian fluids, the flow rate governs whether the viscosity decreases or increases. These phenomena are observed, for example, when liquid pastes (e.g. tooth paste, artists’ colors) are squeezed from tubes and spread quickly.
TopBottom  6 References
A. Tomanek: Silicones & Industry, A compendium for practical use, instruction and reference, Hanser, Münich, Vienna (1990)
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