An approximation for the boundary-layer shape in Figs. 1.5b and P1.51 is the formula TY - U sin 28 и(у) 0 < y< 8

Elements Of Electromagnetics
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Fluid mechanics problem

**Boundary-Layer Shape Approximation**

An approximation for the boundary-layer shape in Figs. 1.5b and P1.51 is represented by the following formula:

\[ u(y) \approx U \sin\left(\frac{\pi y}{2 \delta}\right), \quad 0 \le y \le \delta \]

where:
- \( U \) is the stream velocity far from the wall.
- \( \delta \) is the boundary layer thickness.
- \( y \) is the distance from the wall.

If the fluid is helium at 20°C and 1 atm, and given that \( U = 10.8 \, \text{m/s} \) and \( \delta = 3 \, \text{cm} \), use the formula to:
1. Estimate the wall shear stress \( \tau_w \) in Pa.
2. Find the position in the boundary layer where \( \tau \) is one-half of \( \tau_w \).

**Diagram Explanation:**

The diagram below illustrates the boundary layer where the velocity \( u(y) \) varies from zero at the wall to the free stream velocity \( U \) at \( y = \delta \).

- The x-axis represents the distance from the wall along the boundary layer.
- The y-axis represents the distance perpendicular to the wall.
  
  \[
  \begin{array}{c|c}
  &y \\ \hline
  0 & \\
  & \\
  & \\
  & y = \delta \\ 
  \end{array}
  \]

- The horizontal arrows denote the velocity profile \( u(y) \) which increases from zero at the wall (lower part of the graph) to \( U \) at \( y = \delta \) (upper part of the graph).

**Steps for Calculations:**

1. **Wall Shear Stress \( \tau_w \):**
   To estimate the wall shear stress:
   \[
   \tau_w = \mu \left. \frac{\partial u}{\partial y} \right|_{y=0}
   \]
   where \( \mu \) is the dynamic viscosity of helium at 20°C.

2. **Position in Boundary Layer:**
   To find the position \( y \) where the shear stress is half of \( \tau_w \):
   \[
   \tau = \
Transcribed Image Text:**Boundary-Layer Shape Approximation** An approximation for the boundary-layer shape in Figs. 1.5b and P1.51 is represented by the following formula: \[ u(y) \approx U \sin\left(\frac{\pi y}{2 \delta}\right), \quad 0 \le y \le \delta \] where: - \( U \) is the stream velocity far from the wall. - \( \delta \) is the boundary layer thickness. - \( y \) is the distance from the wall. If the fluid is helium at 20°C and 1 atm, and given that \( U = 10.8 \, \text{m/s} \) and \( \delta = 3 \, \text{cm} \), use the formula to: 1. Estimate the wall shear stress \( \tau_w \) in Pa. 2. Find the position in the boundary layer where \( \tau \) is one-half of \( \tau_w \). **Diagram Explanation:** The diagram below illustrates the boundary layer where the velocity \( u(y) \) varies from zero at the wall to the free stream velocity \( U \) at \( y = \delta \). - The x-axis represents the distance from the wall along the boundary layer. - The y-axis represents the distance perpendicular to the wall. \[ \begin{array}{c|c} &y \\ \hline 0 & \\ & \\ & \\ & y = \delta \\ \end{array} \] - The horizontal arrows denote the velocity profile \( u(y) \) which increases from zero at the wall (lower part of the graph) to \( U \) at \( y = \delta \) (upper part of the graph). **Steps for Calculations:** 1. **Wall Shear Stress \( \tau_w \):** To estimate the wall shear stress: \[ \tau_w = \mu \left. \frac{\partial u}{\partial y} \right|_{y=0} \] where \( \mu \) is the dynamic viscosity of helium at 20°C. 2. **Position in Boundary Layer:** To find the position \( y \) where the shear stress is half of \( \tau_w \): \[ \tau = \
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