A photon of energy \(E\) ejects a photoelectron from a metal surface whose work function is \(W_0\). If this electron enters into a uniform magnetic field of induction \(B\) in a direction perpendicular to the field and describes a circular path of radius \(r\), then the radius \(r\) is given by (in the usual notation)
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Use \(r=\frac{mv}{eB}\) and \(v=\sqrt{\frac{2K}{m}}\). Here \(K=E-W_0\).
Step 1: Photoelectron kinetic energy.
\[
K = E - W_0
\] Step 2: Relate kinetic energy with velocity.
\[
K = \frac{1}{2}mv^2
\Rightarrow v = \sqrt{\frac{2(E-W_0)}{m}}
\] Step 3: Radius of circular motion in magnetic field.
For particle moving perpendicular to magnetic field:
\[
r = \frac{mv}{eB}
\] Step 4: Substitute \(v\).
\[
r = \frac{m}{eB}\sqrt{\frac{2(E-W_0)}{m}}
= \frac{\sqrt{2m(E-W_0)}}{eB}
\] Final Answer:
\[
\boxed{\dfrac{\sqrt{2m(E-W_0)}}{eB}}
\]