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QJEEM24Ph6e7e: JEE Main 2024 Physics - Class 12 JEEM24Ph6e7e Solution: A coil having 100 turns, area of , carrying current of is…

A coil having 100 turns, area of 5×10−3 m25 \times 10^{-3} \mathrm{~m}^2 , carrying current of 1 mA1 \mathrm{~mA} is placed in uniform magnetic field of 0.20 T0.20 \mathrm{~T} such a way that plane of coil is perpendicular to the magnetic field. The work done in turning the coil through 90∘90^{\circ} is _________ μJ\mu \mathrm{J} .

Step-by-Step Verified Solution

To find the work done in turning the coil through 90∘90^{\circ} , we first need to understand the concept of torque on a current-carrying loop in a magnetic field and how work done relates to the change in potential energy of the system. The potential energy (U) of a magnetic dipole in a magnetic field is given by:

U=−M⃗⋅B⃗U = - \vec{M} \cdot \vec{B}

where:

  • M⃗\vec{M} is the magnetic moment of the coil, and
  • B⃗\vec{B} is the magnetic field.

For a coil with NN turns, carrying current II , and with an area AA , the magnetic moment M⃗\vec{M} is defined as:

M=NI⋅AM = NI \cdot A

Given that the coil has 100100 turns, carries a current of 1 mA=1×10−3 A1 \, \mathrm{mA} = 1 \times 10^{-3} \, \mathrm{A} , and the area of the coil is 5×10−3 m25 \times 10^{-3} \, \mathrm{m}^2 , we can calculate its magnetic moment as follows:

M=100⋅1×10−3⋅5×10−3=0.5×10−3 Am2M = 100 \cdot 1 \times 10^{-3} \cdot 5 \times 10^{-3} = 0.5 \times 10^{-3} \, \mathrm{Am}^2

Since the coil is initially placed such that its plane is perpendicular to the magnetic field (i.e., the angle θ=0∘\theta = 0^{\circ} ), and then it is turned through 90∘90^{\circ} , the initial and final angles ( θi\theta_i and θf\theta_f ) of the coil with respect to the magnetic field are 0∘0^{\circ} and 90∘90^{\circ} respectively. This means the initial potential energy ( UiU_i ) and final potential energy ( UfU_f ) of the system are:

Ui=−MBcos⁡(θi)U_i = - M B \cos(\theta_i)

Uf=−MBcos⁡(θf)U_f = - M B \cos(\theta_f)

Given that B=0.20 TB = 0.20 \, \mathrm{T} , θi=0∘ (cos⁡(0)=1)\theta_i = 0^{\circ} \, (\cos(0) = 1) , and θf=90∘ (cos⁡(90∘)=0)\theta_f = 90^{\circ} \, (\cos(90^{\circ}) = 0) , the potential energies are:

Ui=−0.5×10−3⋅0.20⋅1=−1×10−4 JU_i = - 0.5 \times 10^{-3} \cdot 0.20 \cdot 1 = - 1 \times 10^{-4} \, \mathrm{J}

Uf=−0.5×10−3⋅0.20⋅0=0 JU_f = - 0.5 \times 10^{-3} \cdot 0.20 \cdot 0 = 0 \, \mathrm{J}

The work done ( WW ) is equal to the change in potential energy:

W=Uf−UiW = U_f - U_i

W=0−(−1×10−4)=1×10−4 JW = 0 - (- 1 \times 10^{-4}) = 1 \times 10^{-4} \, \mathrm{J}

Therefore, the work done in turning the coil through 90∘90^{\circ} is 100μJ100 \mu \mathrm{J} .

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