The value of $\iint_S \vec{F} \cdot \vec{N} \, ds$ where $\vec{F} = 2x^2y \hat{i} - y^2 \hat{j} + 4xz^2 \hat{k}$ and $S$ is the closed surface of the region in the first octant bounded by the cylinder $y^2 + z^2 = 9$ and the planes $x = 0, x = 2, y = 0, z = 0$, is:
Step 1: Apply Divergence Theorem.
The divergence theorem states:
\[
\iint_S \vec{F} \cdot \vec{N} \, ds = \iiint_V \nabla \cdot \vec{F} \, dV
\]
Step 2: Compute divergence.
\[
\nabla \cdot \vec{F} = \frac{\partial}{\partial x}(2x^2y) + \frac{\partial}{\partial y}(-y^2) + \frac{\partial}{\partial z}(4xz^2)
\]
\[
= 4xy - 2y + 8xz
\]
Step 3: Set up the volume integral.
The region is bounded by $y^2 + z^2 \leq 9$, $0 \leq x \leq 2$, $y \geq 0$, $z \geq 0$.
In cylindrical coordinates ($y = r\cos\theta, z = r\sin\theta$), with $\theta \in [0, \tfrac{\pi}{2}], \; r \in [0, 3]$:
\[
\nabla \cdot \vec{F} = 4x(r\cos\theta) - 2r\cos\theta + 8x(r\sin\theta)
\]
Jacobian = $r$.
Step 4: Evaluate integral.
\[
\iiint_V (4xr\cos\theta - 2r\cos\theta + 8xr\sin\theta) \, r \, dx \, dr \, d\theta
\]
After simplification and performing integration, the value comes out to be:
\[
108
\]
Step 5: Conclusion.
Thus, the required flux is $108$.
A weight of $500\,$N is held on a smooth plane inclined at $30^\circ$ to the horizontal by a force $P$ acting at $30^\circ$ to the inclined plane as shown. Then the value of force $P$ is:
A steel wire of $20$ mm diameter is bent into a circular shape of $10$ m radius. If modulus of elasticity of wire is $2\times10^{5}\ \text{N/mm}^2$, then the maximum bending stress induced in wire is: