Step 1: Relate potential difference to kinetic energy and velocity
When an electron (charge $e$, mass $m_e$) is accelerated from rest through a potential difference $V$, its potential energy is converted into kinetic energy.
\[
e V = \frac{1}{2} m_e v^2
\]
From this, we can express the velocity $v$ as:
\[
v = \sqrt{\frac{2eV}{m_e}} \quad \cdots (1)
\]
Step 2: Relate velocity to the maximum magnetic force
When a charged particle moves in a uniform magnetic field $B$, the magnetic force $F$ on it is given by:
\[
F = qvB \sin\theta
\]
For an electron ($q=e$), the force is $F = evB \sin\theta$.
The maximum force occurs when $\sin\theta = 1$ (i.e., the velocity is perpendicular to the magnetic field), so:
\[
F_{\text{max}} = evB \quad \cdots (2)
\]
Step 3: Combine the relationships for the first case
Substitute equation (1) into equation (2):
\[
F = eB \sqrt{\frac{2eV_1}{m_e}} \quad \cdots (3)
\]
Here, $F$ is the maximum force when the potential difference is $V_1$.
Step 4: Combine the relationships for the second case
When the potential difference is changed to $V_2$, the maximum force becomes $4F$.
Let the new force be $F' = 4F$.
\[
4F = eB \sqrt{\frac{2eV_2}{m_e}} \quad \cdots (4)
\]
Step 5: Find the ratio \( \frac{V_1}{V_2} \)
Divide equation (3) by equation (4):
\[
\frac{F}{4F} = \frac{eB \sqrt{\frac{2eV_1}{m_e}}}{eB \sqrt{\frac{2eV_2}{m_e}}}
\]
\[
\frac{1}{4} = \sqrt{\frac{V_1}{V_2}}
\]
To remove the square root, square both sides:
\[
\left(\frac{1}{4}\right)^2 = \frac{V_1}{V_2}
\]
\[
\frac{1}{16} = \frac{V_1}{V_2}
\]
So, the ratio $\frac{V_1}{V_2}$ is $1:16$.
Step 6: Analyze Options
\begin{itemize}
\item Option (1): 1 : 4. Incorrect.
\item Option (2): 4 : 1. Incorrect.
\item Option (3): 2 : 1. Incorrect.
\item Option (4): 1 : 16. Correct, as it matches our calculated ratio.
\end{itemize}