Concept:
For a uniformly charged semicircular ring, the horizontal components of electric field cancel due to symmetry, while the vertical components add.
The electric field at the centre of a uniformly charged semicircular ring is
\[
E = \frac{2k\lambda}{R}
\]
where
- \(k = \dfrac{1}{4\pi\varepsilon_0}\)
- \(\lambda\) = linear charge density
- \(R\) = radius of the semicircle
The linear charge density is
\[
\lambda = \frac{Q}{\pi R}
\]
Substituting this into the electric field formula gives
\[
E = \frac{2kQ}{\pi R^2}
\]
Step 1: Substitute the known values.}
Given
\[
E = 100 \, \text{V/m}, \quad R = 10\,\text{cm} = 0.1\,\text{m}
\]
Using
\[
E = \frac{2kQ}{\pi R^2}
\]
\[
100 = \frac{2}{\pi (0.1)^2}\left(\frac{1}{4\pi\varepsilon_0}\right)Q
\]
Step 2: Solve for total charge \(Q\).}
Rearranging,
\[
Q = \frac{100 \times \pi \times (0.1)^2}{2k}
\]
Substitute \(k = \dfrac{1}{4\pi\varepsilon_0}\)
\[
Q = \frac{100 \times \pi \times 0.01}{2} \times 4\pi\varepsilon_0
\]
\[
Q = 2\pi^2 \varepsilon_0
\]
Since \(\pi^2 \approx 10\),
\[
Q \approx 20\varepsilon_0
\]
Thus,
\[
\boxed{Q = 20\varepsilon_0}
\]