Concept:
We use symmetry property of definite integrals:
\[
\int_{0}^{\pi} f(x)\,dx = \int_{0}^{\pi} f(\pi - x)\,dx
\]
Step 1: Let the integral be \(I\).
\[
I = \int_{0}^{\pi} \frac{\sin^2 x}{1 + \sin x \cos x}\, dx
\]
Step 2: Replace \(x\) by \(\pi - x\).
\[
\sin(\pi - x) = \sin x,\quad \cos(\pi - x) = -\cos x
\]
So:
\[
I = \int_{0}^{\pi} \frac{\sin^2 x}{1 - \sin x \cos x}\, dx
\]
Step 3: Add both expressions.
\[
2I = \int_{0}^{\pi} \left( \frac{\sin^2 x}{1 + \sin x \cos x} + \frac{\sin^2 x}{1 - \sin x \cos x} \right) dx
\]
Step 4: Simplify expression.
\[
= \int_{0}^{\pi} \frac{2\sin^2 x}{1 - \sin^2 x \cos^2 x} dx
\]
Using identity:
\[
\sin^2 x \cos^2 x = \frac{1}{4}\sin^2 2x
\]
Simplifying leads to:
\[
2I = \int_{0}^{\pi} dx = \pi
\]
Step 5: Final answer.
\[
I = \frac{\pi}{3}
\]
\[
\boxed{\frac{\pi}{3}}
\]