To find the position \(x_0\) where the second charge (\(40 \, \mu \text{C}\)) should be located so that the net electric field is zero at \(x = 2 \, \text{cm}\):
Step 1: Balance the Electric Fields
The net electric field at \(x = 2 \, \text{cm}\) is zero when the contributions from both charges cancel out:
\[
E_{\text{net}} = 0 \implies K \cdot \frac{10 \times 10^{-6}}{(2)^2} = K \cdot \frac{40 \times 10^{-6}}{(x_0 - 2)^2}.
\]
Step 2: Simplify the Equation
Divide out \(K\) and simplify the terms:
\[
\frac{10}{4} = \frac{40}{(x_0 - 2)^2}.
\]
\[
\frac{1}{2} = \frac{2}{(x_0 - 2)^2}.
\]
Step 3: Solve for \(x_0\)
Rearrange the equation:
\[
(x_0 - 2)^2 = 4.
\]
Take the square root of both sides:
\[
x_0 - 2 = \pm 2.
\]
Thus:
\[
x_0 = 4 \, \text{cm} \quad \text{or} \quad x_0 = 6 \, \text{cm}.
\]
Step 4: Choose the Correct Value of \(x_0\)
Since the second charge is positioned to the right of \(x = 2 \, \text{cm}\), the correct location is:
\[
x_0 = 6 \, \text{cm}.
\]
Final Answer:
\[
\boxed{x_0 = 6 \, \text{cm}}
\]