Step 1: Use Faraday's law.
Induced emf = $B l v$ for a rod of length $l$ moving with velocity $v$ perpendicular to a magnetic field.
Here the side of length $w$ cuts the magnetic flux, so magnitude = $B w v$.
Step 2: Analyse entry into field.
When the front of the loop enters the field region, only one vertical segment is cutting flux ⇒ emf = $+Bwv$.
Step 3: When the loop is fully inside.
Two opposite vertical sides cut equal flux in opposite directions ⇒ net emf = $0$.
Step 4: When the loop leaves the field.
Only the back segment cuts the flux ⇒ emf = $-Bwv$.
Step 5: Conclusion.
The emf–position graph must show:
• +Bwv at entry
• 0 while fully inside
• –Bwv at exit
This matches option (B).

At a particular temperature T, Planck's energy density of black body radiation in terms of frequency is \(\rho_T(\nu) = 8 \times 10^{-18} \text{ J/m}^3 \text{ Hz}^{-1}\) at \(\nu = 3 \times 10^{14}\) Hz. Then Planck's energy density \(\rho_T(\lambda)\) at the corresponding wavelength (\(\lambda\)) has the value \rule{1cm}{0.15mm} \(\times 10^2 \text{ J/m}^4\). (in integer)
[Speed of light \(c = 3 \times 10^8\) m/s]
(Note: The unit for \(\rho_T(\nu)\) in the original problem was given as J/m³, which is dimensionally incorrect for a spectral density. The correct unit J/(m³·Hz) or J·s/m³ is used here for the solution.)
A current \( I = 10A \) flows in an infinitely long wire along the axis of a hemisphere. The value of \( \int (\mathbf{v} \times \mathbf{B}) \cdot d\mathbf{s} \) over the hemispherical surface as shown in the figure is: 
A rectangular loop of dimension \( L \) and width \( w \) moves with a constant velocity \( v \) away from an infinitely long straight wire carrying a current \( I \) in the plane of the loop as shown in the figure below. Let \( R \) be the resistance of the loop. What is the current in the loop at the instant the near-side is at a distance \( r \) from the wire? 
