The vertical component of vorticity (\( \zeta \)) is given by the formula:
\[
\zeta = \frac{1}{R} \frac{\partial u}{\partial y}.
\]
The velocity profile is given as:
\[
u(y) = u_0 \left( 1 - \frac{y^2}{L^2} \right).
\]
Differentiating \( u(y) \) with respect to \( y \), we get:
\[
\frac{\partial u}{\partial y} = -2 \frac{y}{L^2} u_0.
\]
At \( y = \frac{L}{2} \), we substitute into the equation:
\[
\zeta = -2 \frac{L/2}{L^2} u_0 = -\frac{u_0}{L}.
\]
Substituting the values \( u_0 = 50 \, \text{m/s} \) and \( L = 5 \, \text{km} \), we get:
\[
\zeta \approx -0.009 \, \text{s}^{-1}.
\]
Thus, the vertical component of vorticity is \( 0.009 \, \text{s}^{-1} \).