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Question: Plane rectangular loop is placed in a magnetic field. The loop was pulled out of the magnetic field ...

Plane rectangular loop is placed in a magnetic field. The loop was pulled out of the magnetic field at a velocity which is not constant. Assume the magnetic induction in the region is B\overrightarrow{B} and it is uniform and constant. The EMF induced in the loop due to this field is εi\varepsilon_i whose maximum value is εm\varepsilon_m. Now εi\varepsilon_i is plotted against time t as shown in the graph. Which of the following are/is correct statement(s):

A

εm\varepsilon_m is independent of rate of removal of coil from the field.

B

The total charge that passes through any point of the loop in the process of complete removal of the loop does not depend on velocity of removal.

C

The total area under the curve (εi\varepsilon_i vs t) is independent of rate of removal of coil from the field.

D

The area under the curve is dependent on the rate of removal of the coil.

Answer

Options (B) and (C) are correct.

Explanation

Solution

The problem involves a rectangular loop being pulled out of a uniform and constant magnetic field. We need to analyze the induced EMF (εi\varepsilon_i), its maximum value (εm\varepsilon_m), the total charge (QQ), and the area under the εi\varepsilon_i vs. time graph.

Let the width of the loop (the side perpendicular to the velocity and magnetic field) be ll, and the length of the loop (the side parallel to the velocity) be ww. The magnetic field strength is BB. The resistance of the loop is RR.

  1. Induced EMF: According to Faraday's Law of Electromagnetic Induction, the induced EMF is given by: εi=dΦBdt\varepsilon_i = -\frac{d\Phi_B}{dt} where ΦB\Phi_B is the magnetic flux through the loop. When the loop is pulled out of the field, the area inside the field changes. If the velocity of the loop is vv, the rate of change of area is lvl v. So, the magnitude of the induced EMF is εi=Blv\varepsilon_i = Blv.

  2. Analysis of Options:

    (A) εm\varepsilon_m is independent of rate of removal of coil from the field. The maximum EMF, εm\varepsilon_m, occurs when the velocity is maximum, vmaxv_{max}. So, εm=Blvmax\varepsilon_m = Blv_{max}. The "rate of removal" refers to the velocity of the coil. If the coil is removed at a higher rate, vmaxv_{max} will be higher, and consequently, εm\varepsilon_m will be higher. Therefore, εm\varepsilon_m is dependent on the rate of removal. Statement (A) is incorrect.

    (B) The total charge that passes through any point of the loop in the process of complete removal of the loop does not depend on velocity of removal. The induced current is I=εiRI = \frac{\varepsilon_i}{R}. The total charge QQ is the integral of current over time: Q=Idt=εiRdtQ = \int I dt = \int \frac{\varepsilon_i}{R} dt Substituting εi=dΦBdt\varepsilon_i = -\frac{d\Phi_B}{dt}: Q=1R(dΦBdt)dt=1RdΦB=1R[ΦB]initialfinalQ = \int \frac{1}{R} \left(-\frac{d\Phi_B}{dt}\right) dt = -\frac{1}{R} \int d\Phi_B = -\frac{1}{R} [\Phi_B]_{initial}^{final} Initially, the loop is completely inside the magnetic field, so the flux is Φinitial=B(Area of loop)=Blw\Phi_{initial} = B \cdot (\text{Area of loop}) = Blw. Finally, the loop is completely out of the magnetic field, so the flux is Φfinal=0\Phi_{final} = 0. The change in flux is ΔΦB=ΦfinalΦinitial=0Blw=Blw\Delta\Phi_B = \Phi_{final} - \Phi_{initial} = 0 - Blw = -Blw. Therefore, the magnitude of the total charge is Q=BlwR=BlwR|Q| = \frac{|-Blw|}{R} = \frac{Blw}{R}. This expression for QQ depends only on BB, ll, ww, and RR, which are constants for the given setup. It does not depend on the velocity profile (how fast or slow the loop is removed). Statement (B) is correct.

    (C) The total area under the curve (εi\varepsilon_i vs t) is independent of rate of removal of coil from the field. The area under the εi\varepsilon_i vs t curve is given by εidt\int \varepsilon_i dt. From Faraday's Law, εidt=(dΦBdt)dt=dΦB=[ΦB]initialfinal\int \varepsilon_i dt = \int \left(-\frac{d\Phi_B}{dt}\right) dt = -\int d\Phi_B = -[\Phi_B]_{initial}^{final}. As calculated in option (B), the change in flux is ΔΦB=Blw\Delta\Phi_B = -Blw. So, the area under the curve is (Blw)=Blw-(-Blw) = Blw. This area BlwBlw depends only on the magnetic field strength and the dimensions of the loop. It does not depend on the velocity profile (rate of removal). Statement (C) is correct.

    (D) The area under the curve is dependent on the rate of removal of the coil. This statement contradicts statement (C). Since (C) is correct, (D) must be incorrect.

Based on the analysis, statements (B) and (C) are correct.