We need to analyze the induced electromotive force (EMF), the induced current, the direction of the current, and the potential differences in the loop.
Step 1: Calculate the Induced EMF
As the loop is pulled through the magnetic field, an EMF is induced in the wires perpendicular to the velocity and magnetic field. The motional EMF induced in a wire of length \(L\) moving with velocity \(v\) perpendicular to a magnetic field \(B\) is given by: \[\mathcal{E} = BLv\]
In this case, the wires \(PQ\) and \(RS\) are the ones experiencing the induced EMF. Both wires have length \(b\), so the total induced EMF is: \[\mathcal{E} = Bvb\]
Step 2: Calculate the Resistance of the Loop
The loop has a total length of \(2(a + b)\). The resistance per unit length is \(\lambda\). Therefore, the total resistance \(R\) of the loop is: \[R = \lambda (2a + 2b) = 2\lambda (a + b)\]
Step 3: Calculate the Induced Current
Using Ohm's Law, the induced current \(I\) in the loop is: \[I = \frac{\mathcal{E}}{R} = \frac{Bvb}{2\lambda(a + b)}\]
Step 4: Determine the Direction of the Current
Using the right-hand rule (or Lenz's Law), as the loop moves to the right, the magnetic flux through the loop decreases (since the area within the field decreases). To oppose this change in flux, the induced current will create a magnetic field pointing downwards (in the same direction as the external field). This requires a clockwise current when viewed from above.
Step 5: Analyze the Potential Differences
Consider the potential difference \(V_P - V_S\) and \(V_Q - V_R\). Since PQ and RS are the source of the emf then \(V_P - V_Q=V_S-V_R=Bvb\) however due to the resistance, some of the potential will be lost hence \(V_P - V_S=V_Q-V_R\) is wrong.
There is definitely induction in part SR, since it is also moving through the magnetic field.
Step 6: Determine the Correct Statements
Conclusion
The correct statements are:
A beam of light of wavelength \(\lambda\) falls on a metal having work function \(\phi\) placed in a magnetic field \(B\). The most energetic electrons, perpendicular to the field, are bent in circular arcs of radius \(R\). If the experiment is performed for different values of \(\lambda\), then the \(B^2 \, \text{vs} \, \frac{1}{\lambda}\) graph will look like (keeping all other quantities constant).