To determine the coefficient of viscosity of glycerin using the rotating cylinder method.
- Rotating cylinder viscometer setup
- Glycerin sample
- Two concentric cylinders (inner and outer)
- Motor with variable speed control
- Tachometer/rpm counter
- Adjustable pulley system
- Stop watch
- Thermometer
- Weighing balance
- Vernier caliper
- Micrometer screw gauge
- Thread and weights/spring balance
The rotating cylinder method for determining viscosity is based on the measurement of torque required to rotate a cylinder at a constant angular velocity when it is immersed in the fluid whose viscosity is to be determined.
When an inner cylinder rotates inside a stationary outer cylinder with the space between filled with glycerin, the viscous drag of the fluid creates a torque. The magnitude of this torque is directly proportional to the coefficient of viscosity of the fluid.
For two concentric cylinders with the inner one rotating and the outer one stationary, the torque ($\tau$) experienced by the rotating cylinder due to viscous drag is given by:
Where:
- $\eta$ (eta) = coefficient of viscosity
- $L$ = height of the rotating cylinder in contact with the fluid
- $\omega$ (omega) = angular velocity of the rotating cylinder
- $R_1$ = radius of the inner cylinder
- $R_2$ = radius of the outer cylinder
This relationship is derived from the fundamental principles of fluid mechanics. The viscous fluid between the cylinders is subjected to shear stress which is proportional to the rate of shear strain and the coefficient of viscosity. The torque required to maintain rotation is directly proportional to the viscosity of the fluid.
From the measured torque and angular velocity, we can determine the coefficient of viscosity using:
In practical terms, the torque can be measured by:
- Using the applied force ($F$) and the effective radius of the pulley ($r$): $\tau = F \times r$
- Or by measuring the tension in the thread connected to a weight: $\tau = (M - m)g \times r$
Where:
- $M$ = mass applied to produce rotation
- $m$ = mass required to overcome the friction of bearings (determined separately)
- $g$ = acceleration due to gravity
- $r$ = radius of the pulley
Finally, the coefficient of viscosity is:
Where $\omega = 2\pi N/60$ and $N$ is the speed in rpm.
Setup Preparation:
- Measure the dimensions of the inner and outer cylinders (radii $R_1$ and $R_2$) using the vernier caliper.
- Measure the effective height ($L$) of the inner cylinder that will be immersed in glycerin.
- Set up the rotating cylinder apparatus, ensuring the cylinders are concentric.
- Clean the cylinders thoroughly and dry them.
System Calibration:
- Determine the frictional torque of the system by running the inner cylinder without glycerin.
- Record the minimum weight ($m$) required to overcome friction and initiate rotation.
Experiment Execution:
- Fill the space between the cylinders with glycerin up to the marked height.
- Record the temperature of glycerin using the thermometer.
- Attach a known weight ($M$) to the thread wound around the pulley.
- Release the weight and measure the steady rotational speed ($N$) using the tachometer.
- Repeat steps for at least 5 different weights to obtain multiple data points.
- For each weight, take 3 readings and use the average value for calculations.
Additional Measurements:
- Measure the radius of the pulley ($r$) using the micrometer.
- Record the room temperature.
Table 1: Dimensions of the Apparatus
Parameter | Symbol | Measured Value | Unit |
---|---|---|---|
Radius of inner cylinder | $R_1$ | ... | m |
Radius of outer cylinder | $R_2$ | ... | m |
Effective height of cylinder | $L$ | ... | m |
Radius of pulley | $r$ | ... | m |
Frictional mass | $m$ | ... | kg |
Table 2: Experimental Observations
S.No. | Applied Mass ($M$) | Angular Speed ($N$) | Temperature of Glycerin |
---|---|---|---|
(kg) | (rpm) | (°C) | |
1 | |||
2 | |||
3 | |||
4 | |||
5 |
For each observation:
- Calculate the effective torque: $\tau = (M - m)g \times r$
- Convert rotational speed to angular velocity: $\omega = 2\pi N/60$
- Calculate viscosity using the formula:
$$\eta = \frac{(M - m)g \times r(R_2^2 - R_1^2)}{4\pi L \omega R_1^2 R_2^2}$$
- Calculate the mean value of $\eta$ from all observations.
- Calculate the standard deviation to determine the precision of the measurements.
Sample Calculation (for the first observation):
- Torque ($\tau$) = $(M_1 - m)g \times r = $ ... N·m
- Angular velocity ($\omega$) = $2\pi \times N_1/60 = $ ... rad/s
- Coefficient of viscosity ($\eta$) = ... Pa·s
The coefficient of viscosity of glycerin at temperature T = ... °C is found to be $\eta = $ ... $\pm$ ... Pa·s (or Poise).
- Ensure the inner and outer cylinders are perfectly concentric to avoid uneven fluid distribution.
- The inner cylinder should not touch the outer cylinder during rotation.
- Take measurements only after the system has reached a steady rotational speed.
- Keep the temperature constant throughout the experiment as viscosity is strongly temperature-dependent.
- Clean all surfaces thoroughly before filling with glycerin to avoid contamination.
- Avoid air bubbles in the glycerin sample.
- Ensure that the thread does not slip on the pulley.
- Maintain a slow and controlled release of weights to achieve steady rotation.
- Take multiple readings and use the average for better accuracy.
- Allow sufficient time for the glycerin to reach equilibrium temperature.
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