Step 1: Expression for magnetic force.
The magnetic force on a charged particle moving perpendicular to a magnetic field is
\[
F = qvB
\]
Step 2: Relation between velocity and accelerating potential.
For an electron accelerated through potential \(V\):
\[
\frac{1}{2}mv^2 = eV \Rightarrow v \propto \sqrt{V}
\]
Step 3: Effect of doubling the potential.
When potential becomes \(2V\):
\[
v' = \sqrt{2}\,v
\]
Hence,
\[
F' = qv'B = \sqrt{2}\,F
\]