MHT CET · Physics · Electromagnetic Induction
A long, rectangular conducting loop of width \(l\) mass \(m\) and resistance \(R\) is placed partly in a perpendicular magnetic field \(B\). It is pushed downwards with velocity \(v\) so that it may continue to fall freely. The velocity \(v\) is \((g=\) acceleration due to gravity)

- A \(\frac{m g R^2}{B l}\)
- B \(\frac{m g R}{B^2 l^2}\)
- C \(\frac{m g l}{B^2 R^2}\)
- D \(\frac{B^2 l^2 R}{m g}\)
Answer & Solution
Correct Answer
(B) \(\frac{m g R}{B^2 l^2}\)
Step-by-step Solution
Detailed explanation
The motional emf is given by: \(V=B v l\)
Current in the loop,
\(i=\frac{V}{R}=\frac{B v l}{R}\)
During free fall the electromagnetic force felt by the loop balances its weight, and since the loop is long so we assume its falling with a terminal velocity.
\(\begin{aligned}
& \therefore i l B=m g \\
& \Rightarrow B\left(\frac{B v l}{R}\right) l=m g \\
& \Rightarrow v=\frac{m g R}{B^2 l^2}
\end{aligned}\)
Current in the loop,
\(i=\frac{V}{R}=\frac{B v l}{R}\)
During free fall the electromagnetic force felt by the loop balances its weight, and since the loop is long so we assume its falling with a terminal velocity.
\(\begin{aligned}
& \therefore i l B=m g \\
& \Rightarrow B\left(\frac{B v l}{R}\right) l=m g \\
& \Rightarrow v=\frac{m g R}{B^2 l^2}
\end{aligned}\)
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