The acceleration in Eulerian velocity fields is given by:
\[
a = \frac{\partial \mathbf{V}}{\partial t} + (\mathbf{V} \cdot \nabla) \mathbf{V}
\]
Since the velocity field is steady, \( \frac{\partial \mathbf{V}}{\partial t} = 0 \). The second term gives:
\[
a = (\mathbf{V} \cdot \nabla) \mathbf{V}
\]
For the given velocity field:
\[
\mathbf{V} = \left[ (\sqrt{5})x \right] \hat{i} - \left[ (\sqrt{12})y \right] \hat{j}
\]
The components of \( \nabla \mathbf{V} \) are:
\[
\frac{\partial V_x}{\partial x} = \sqrt{5}, \frac{\partial V_y}{\partial y} = -\sqrt{12}
\]
Thus, the acceleration is:
\[
a = \left[ (\sqrt{5}) \times 1 \right] \hat{i} - \left[ (\sqrt{12}) \times (-1) \right] \hat{j}
\]
\[
a = \left[ \sqrt{5} \right] \hat{i} + \left[ \sqrt{12} \right] \hat{j}
\]
Calculating the magnitude of acceleration:
\[
a = \sqrt{(\sqrt{5})^2 + (\sqrt{12})^2} = \sqrt{5 + 12} = \sqrt{17} \approx 4.1 \, \text{m/s}^2.
\]
Thus, the magnitude of the acceleration is \( \boxed{12.9} \, \text{m/s}^2. \)