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do not include tables in your answer, detailed explanation ,A 10-in-diameter circular plate is placed over a fixed bottom plate with a
0.1-in. gap between the two plates filled with glycerin as shown in the figure
below. Determine the torque required to rotate the circular plate slowly at 4
rpm. Assume that the velocity distribution in the gap is linear and that the
shear stress on the edge of the rotating plate is negligible. (Assume the
viscosity of glycerin is 3.13 x 102 Ib - s/ft2)
Rotating plate
Torque
/ 0.1in. gap
[: | ft'lb
Question:
Act like a helpful tutor and exlain me :
Give step-by-step solution with explanation and final answer:
do not include tables in your answer, detailed explanation ,A 10-in-diameter circular plate is placed over a fixed bottom plate with a
0.1-in. gap between the two plates filled with glycerin as shown in the figure
below. Determine the torque required to rotate the circular plate slowly at 4
rpm. Assume that the velocity distribution in the gap is linear and that the
shear stress on the edge of the rotating plate is negligible. (Assume the
viscosity of glycerin is 3.13 x 102 Ib - s/ft2)
Rotating plate
Torque
/ 0.1in. gap
[: | ft'lb
This is AI generated Response.
Asked by: manish kumar
Created at: 2025-10-26 20:17:27
Final Answer:
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Certainly! Here's a step-by explanation to determine torque required to the circular plate:
---
### Given:
- Diameter the plate, \( = 10 \text in} \)
- Radius of the plate, \( = \frac{D}{2} =5 \text in} \)
- Gap between plates, \( h = .1text{ in} \)
- Viscosity of glycerin, \( \eta = 3.13 \times 10^{-2} \text{ lb·s/ft}^2 \)
- Rotation speed, \( \omega = 4 \text{ rpm} \)
- Shear stress at the edge is negligible
- The velocity distribution is linear
---
### Step 1: Convert rotation speed to rad/sec
\[ \omega = 4 \text{ rpm} \]
\[ \omega_{rad/sec} = \frac{4 \times 2\pi}{60} = \frac{8\pi}{60} = \frac{2\pi}{15} \text{ rad/sec} \]
---
### Step 2: Calculate the velocity at the outer edge
\[ v = R \times \omega_{rad/sec} \]
Convert \( R \) from inches to feet:
\[ R = 5 \text{ in} = \frac{5}{12} \text{ ft} \]
\[ v = \frac{5}{12} \times \frac{2\pi}{15} = \frac{5 \times 2\pi}{12 \times 15} = \frac{10\pi}{180} = \frac{\pi}{18} \text{ ft/sec} \]
---
### Step 3: Find the shear stress
Since the velocity distribution is linear across the gap:
\[ \tau = \eta \times \frac{v}{h} \]
Convert \( h \) from inches to feet:
\[ h = \frac{.1}{12} \text{ ft} \]
\[ \tau = 3.13 \times 10^{-2} \times \frac{\pi/18}{.1/12} \]
Simplify denominator:
\[ \frac{\pi/18}{.1/12} = \frac{\pi/18}{.00833} \]
\[ \Rightarrow \tau = 3.13 \times 10^{-2} \times \frac{\pi/18}{.00833} \]
Calculate:
\[ \frac{\pi/18}{.00833} = \frac{\pi}{18 \times .00833} \]
\[ = \frac{\pi}{.14994} \approx \frac{3.1416}{.14994} \approx 20.96 \]
So:
\[ \tau \approx 3.13 \times 10^{-2} \times 20.96 \approx .657 \text{ lb/ft}^2 \]
---
### Step 4: Calculate the torque
The torque \( T \) is given by integrating shear stress over the surface area:
\[ T = \int_{}^{R} \tau \times 2\pi r^2 dr \]
Since \( \tau \) varies linearly with \( r \), and shear stress at the edge is primarily responsible:
\[ T \approx \tau \times \text{Area} \times R \]
\[ T = \tau \times \pi R^2 \times R \]
\[ T = \tau \times \pi R^3 \]
Convert \( R \) to feet:
\[ R = 5/12 \text{ ft} \]
Calculate:
\[ T = .657 \times \pi \times \left(\frac{5}{12}\right)^3 \]
\[ T = .657 \times 3.1416 \times \frac{125}{1728} \]
\[ T \approx .657 \times 3.1416 \times .0724 \]
\[ T \approx .657 \times .227 \approx .149 \text{ ft·lb} \]
---
### **Final Answer:**
\[
\boxed{
\text{Torque} \approx .149 \text{ ft·lb}
}
\]
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