The electric field \( \mathbf{E} \) is related to the electric potential \( V \) by:
\[
\mathbf{E} = - \nabla V
\]
Taking the partial derivatives of \( V \) with respect to \( x \), \( y \), and \( z \), we get:
\[
E_x = - \frac{\partial V}{\partial x} = 5 \, \text{Vm}^{-1}, \quad E_y = - \frac{\partial V}{\partial y} = -3 \, \text{Vm}^{-1}, \quad E_z = - \frac{\partial V}{\partial z} = -\frac{\sqrt{15}}{2\sqrt{z}} \, \text{Vm}^{-1}
\]
The magnitude of the electric field is:
\[
E = \sqrt{E_x^2 + E_y^2 + E_z^2}
\]
Substituting the values, we find that the magnitude of the electric field is 7 \( \text{Vm}^{-1} \).