Step 1: Use Coulomb force as centripetal force.
In Bohr’s model, the electrostatic force provides the centripetal force:
\[
\frac{1}{4\pi \varepsilon_0} \cdot \frac{e^2}{r^2} = \frac{mv^2}{r}
\]
Step 2: Simplify the equation.
\[
\frac{1}{4\pi \varepsilon_0} \cdot \frac{e^2}{r} = mv^2
\]
Step 3: Use Bohr’s quantization condition.
Angular momentum is quantized:
\[
mvr = \frac{nh}{2\pi}
\]
For first orbit, \( n = 1 \):
\[
mvr = \frac{h}{2\pi}
\]
Step 4: Express velocity \( v \).
\[
v = \frac{h}{2\pi mr}
\]
Step 5: Substitute into centripetal equation.
Substitute \( v \) in
Step 2:
\[
\frac{1}{4\pi \varepsilon_0} \cdot \frac{e^2}{r} = m \left( \frac{h}{2\pi mr} \right)^2
\]
Step 6: Simplify to get velocity relation.
After simplification:
\[
v = \frac{e^2}{2\varepsilon_0 h}
\]
Step 7: Find frequency \( \nu \).
Frequency is:
\[
\nu = \frac{v}{2\pi r}
\]
\[
\nu = \frac{e^2}{4\pi \varepsilon_0 h r}
\]
Hence, option (A) is correct.