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Question: A conducting loop (as shown) has total resistance R. A uniform magnetic field $B = \gamma t$ is appl...

A conducting loop (as shown) has total resistance R. A uniform magnetic field B=γtB = \gamma t is applied perpendicular outwards to plane of the loop where γ\gamma is a constant and tt is time as shown. The induced current flowing through loop is

Answer

γ(a2+b2)R\frac{\gamma (a^2 + b^2)}{R}

Explanation

Solution

The problem asks for the induced current in a conducting loop due to a time-varying magnetic field.

  1. Calculate the total area of the loop:
    The loop consists of two square sections.
    Area of the first square (top) = b×b=b2b \times b = b^2.
    Area of the second square (bottom) = a×a=a2a \times a = a^2.
    The total area (AtotalA_{total}) through which the magnetic field passes is the sum of these areas:
    Atotal=a2+b2A_{total} = a^2 + b^2

  2. Calculate the magnetic flux (ΦB\Phi_B):
    The magnetic field B=γtB = \gamma t is uniform and applied perpendicular outwards to the plane of the loop.
    The magnetic flux is given by ΦB=BAtotal\Phi_B = B \cdot A_{total}.
    Substituting the given values:
    ΦB=(γt)(a2+b2)\Phi_B = (\gamma t)(a^2 + b^2)

  3. Calculate the induced electromotive force (EMF) using Faraday's Law:
    Faraday's Law states that the induced EMF (E\mathcal{E}) is the negative rate of change of magnetic flux:
    E=dΦBdt\mathcal{E} = - \frac{d\Phi_B}{dt}
    E=ddt[γt(a2+b2)]\mathcal{E} = - \frac{d}{dt} [\gamma t (a^2 + b^2)]
    Since γ\gamma, aa, and bb are constants:
    E=γ(a2+b2)dtdt\mathcal{E} = - \gamma (a^2 + b^2) \frac{dt}{dt}
    E=γ(a2+b2)\mathcal{E} = - \gamma (a^2 + b^2)
    The magnitude of the induced EMF is:
    E=γ(a2+b2)|\mathcal{E}| = \gamma (a^2 + b^2)

  4. Calculate the induced current (I) using Ohm's Law:
    The total resistance of the loop is given as RR.
    According to Ohm's Law, the induced current is:
    I=ERI = \frac{|\mathcal{E}|}{R}
    Substituting the magnitude of EMF:
    I=γ(a2+b2)RI = \frac{\gamma (a^2 + b^2)}{R}

The direction of the current can be found using Lenz's Law. Since the outward magnetic field is increasing, the induced current will flow in a clockwise direction to produce an inward magnetic field, opposing the change. The question only asks for the magnitude of the current.

The final answer is γ(a2+b2)R\frac{\gamma (a^2 + b^2)}{R}

Explanation of the solution:
The total area of the loop is A=a2+b2A = a^2 + b^2. The magnetic flux through the loop is ΦB=BA=γt(a2+b2)\Phi_B = B \cdot A = \gamma t (a^2 + b^2). By Faraday's Law, the induced EMF is E=dΦBdt=γ(a2+b2)\mathcal{E} = -\frac{d\Phi_B}{dt} = -\gamma (a^2 + b^2). The magnitude of the induced EMF is E=γ(a2+b2)|\mathcal{E}| = \gamma (a^2 + b^2). Using Ohm's Law, the induced current is I=ER=γ(a2+b2)RI = \frac{|\mathcal{E}|}{R} = \frac{\gamma (a^2 + b^2)}{R}.

Answer:
The induced current flowing through the loop is γ(a2+b2)R\frac{\gamma (a^2 + b^2)}{R}.