The problem involves calculating the velocity of water at the center of a pipe assuming laminar flow. For laminar flow in a circular pipe, the velocity profile is parabolic, and the maximum velocity, \( V_{\text{max}} \), occurs at the center.
The formula for the maximum velocity is:
\( V_{\text{max}} = \frac{{\Delta P \cdot R^2}}{{4 \cdot \mu \cdot L}} \)where:
- \(\Delta P = 0.2 \, \text{Pa}\) is the pressure drop.
- \(R = 0.05 \, \text{m}\) is the radius of the pipe (half of the diameter).
- \(\mu = \nu \cdot \rho = 1 \times 10^{-6} \, \text{m}^2/\text{s} \times 1000 \, \text{kg/m}^3 = 0.001 \, \text{Pa}\cdot\text{s}\) is the dynamic viscosity of water.
- \(L = 10 \, \text{m}\) is the length of the pipe.
Substituting these values:
\( V_{\text{max}} = \frac{{0.2 \times (0.05)^2}}{{4 \times 0.001 \times 10}} = \frac{{0.2 \times 0.0025}}{{0.04}} = \frac{{0.0005}}{{0.04}} = 0.0125 \, \text{m/s} \)Converting this velocity to mm/s:
\( V_{\text{max}} = 0.0125 \, \text{m/s} \times 1000 = 12.5 \, \text{mm/s} \)Given the expected range is 12.3 to 12.3 mm/s, the computed velocity of 12.5 mm/s falls slightly outside the provided range, indicating either a subtle error in problem setup or expected precision. For educational purposes, calculated result is valid within expected physics accuracy.