Step 1: Recall boundary layer theory (Blasius).
For a laminar flat–plate boundary layer, the thickness scales as
\[
\delta \sim \sqrt{\frac{\nu x}{U_\infty}}
\;\;\Rightarrow\;\; \delta \propto x^{1/2}.
\]
Step 2: Momentum thickness.
The momentum thickness is defined as
\[
\theta(x) = \int_0^\infty \frac{u}{U_\infty}\left(1-\frac{u}{U_\infty}\right)dy.
\]
From the Blasius similarity solution, one obtains
\[
\theta(x) = \frac{0.664}{\sqrt{Re_x}}\, x
\]
where \(Re_x = \frac{U_\infty x}{\nu}\).
Step 3: Simplify scaling.
\[
\theta(x) \sim \frac{x}{\sqrt{x}} \sim x^{1/2}.
\]
Final Answer:
\[
\boxed{\theta \propto x^{1/2}}
\]
A flexible chain of mass $m$ is hanging as shown. Find tension at the lowest point. 
