If E is the electric field due to charge placed inside the metal ball at its center, then the magnitude of electric field due to the charge Q placed at a distance r from it is:
\(E = k\frac{Q}{{{r^2}}}\)
So, the charge inside the metal ball is given as:
\(Q = \frac{{E{r^2}}}{k}\)
Substitute the values in the above expression.
\(\begin{aligned}{c}Q = \frac{{\left( {3.75 \times {{10}^2}\;{\rm{N/C}}} \right) \times {{\left( {3.50 \times 1{{\rm{0}}^{ - 2}}\;{\rm{m}}} \right)}^2}}}{{\left( {9.0 \times {{10}^9}\;{\rm{N}} \cdot {{\rm{m}}^{\rm{2}}}{\rm{/}}{{\rm{C}}^{\rm{2}}}} \right)}}\\ = 5.11 \times {10^{ - 11}}\;{\rm{C}}\end{aligned}\)
Since any charge in a metallic conductor resides on the surface of the conductor, the magnitude of charge that resides on the metal ball is \(5.11 \times {10^{ - 11}}\;{\rm{C}}\). Also, as the electric field points towards the metal ball, the charge on the metal ball must be negative.
Thus, the charge that resides on the surface of the metal ball is \( - 5.11 \times {10^{ - 11}}\;{\rm{C}}\).