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Water at 20^(@) is flowing in a pipe of ...

Water at `20^(@)` is flowing in a pipe of radius `20.0 cm` . The viscosity of water at `20^(@)C` is `1.005` centipise. If the water's speed in the centre of the pipe is `3.00m//s`, what is water's speed:
(a) `10.0cm` from the centre of the pipe(half way between the centre and the walls)
(b) at the wall of the pipe?

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To solve the problem, we will use the concept of laminar flow in a pipe and apply the Hagen-Poiseuille equation. The velocity profile of a fluid flowing through a circular pipe is parabolic, and we can use the following relationship to find the velocity at different points in the pipe. ### Given Data: - Radius of the pipe, \( R = 20.0 \, \text{cm} = 0.20 \, \text{m} \) - Viscosity of water, \( \eta = 1.005 \, \text{cP} = 1.005 \times 10^{-3} \, \text{Pa.s} \) (since \( 1 \, \text{cP} = 1 \times 10^{-3} \, \text{Pa.s} \)) - Speed of water at the center of the pipe, \( V_1 = 3.00 \, \text{m/s} \) - Distance from the center for part (a), \( r_1 = 10.0 \, \text{cm} = 0.10 \, \text{m} \) - Distance from the center for part (b), \( r_2 = R = 20.0 \, \text{cm} = 0.20 \, \text{m} \) ### Step-by-Step Solution: #### Part (a): Speed at 10.0 cm from the center of the pipe 1. **Use the velocity ratio equation:** The velocity at a distance \( r \) from the center of the pipe can be related to the velocity at the center using the formula: \[ \frac{V_1}{V_2} = \frac{R^2 - 0^2}{R^2 - r^2} \] where \( V_2 \) is the velocity at distance \( r \) from the center. 2. **Substitute the known values:** For \( r_1 = 10.0 \, \text{cm} = 0.10 \, \text{m} \): \[ \frac{3.00}{V_2} = \frac{(0.20)^2 - 0^2}{(0.20)^2 - (0.10)^2} \] 3. **Calculate the squares:** \[ (0.20)^2 = 0.04 \, \text{m}^2 \] \[ (0.10)^2 = 0.01 \, \text{m}^2 \] 4. **Plug in the values:** \[ \frac{3.00}{V_2} = \frac{0.04}{0.04 - 0.01} = \frac{0.04}{0.03} \] 5. **Simplify the equation:** \[ \frac{3.00}{V_2} = \frac{4}{3} \] 6. **Cross-multiply to solve for \( V_2 \):** \[ 3.00 \times 3 = 4 \times V_2 \implies 9.00 = 4V_2 \implies V_2 = \frac{9.00}{4} = 2.25 \, \text{m/s} \] #### Part (b): Speed at the wall of the pipe 1. **Use the same velocity ratio equation:** For \( r_2 = R = 20.0 \, \text{cm} = 0.20 \, \text{m} \): \[ \frac{V_1}{V_2} = \frac{R^2 - 0^2}{R^2 - R^2} \] 2. **Notice the denominator:** The denominator becomes zero: \[ \frac{V_1}{V_2} = \frac{0.04}{0} \implies \text{undefined} \] 3. **Interpret the result:** This indicates that the velocity at the wall of the pipe is zero: \[ V_2 = 0 \, \text{m/s} \] ### Final Answers: - (a) The speed of water at 10.0 cm from the center of the pipe is \( 2.25 \, \text{m/s} \). - (b) The speed of water at the wall of the pipe is \( 0 \, \text{m/s} \).

To solve the problem, we will use the concept of laminar flow in a pipe and apply the Hagen-Poiseuille equation. The velocity profile of a fluid flowing through a circular pipe is parabolic, and we can use the following relationship to find the velocity at different points in the pipe. ### Given Data: - Radius of the pipe, \( R = 20.0 \, \text{cm} = 0.20 \, \text{m} \) - Viscosity of water, \( \eta = 1.005 \, \text{cP} = 1.005 \times 10^{-3} \, \text{Pa.s} \) (since \( 1 \, \text{cP} = 1 \times 10^{-3} \, \text{Pa.s} \)) - Speed of water at the center of the pipe, \( V_1 = 3.00 \, \text{m/s} \) - Distance from the center for part (a), \( r_1 = 10.0 \, \text{cm} = 0.10 \, \text{m} \) - Distance from the center for part (b), \( r_2 = R = 20.0 \, \text{cm} = 0.20 \, \text{m} \) ...
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