
The work done in pulling the loop out of the magnetic field can be calculated using the concept of electromagnetic induction. When the loop is pulled out of the magnetic field, an electromotive force (EMF) is induced which results in a current due to the resistance of the loop. The power loss due to this current is equal to the rate at which work is done.
Step 1: Determine the Induced EMF
The change in magnetic flux (\( \Delta \Phi \)) is given by:
\(\Delta \Phi = B \times A\), where \(B = 0.5 \, \text{T}\) and \(A = 3.6 \times 10^{-3} \, \text{m}^2\).
\(\Delta \Phi = 0.5 \times 3.6 \times 10^{-3} = 1.8 \times 10^{-3} \, \text{Tm}^2\).
Since there are 10 turns, total flux change = \(10 \times 1.8 \times 10^{-3} = 1.8 \times 10^{-2} \, \text{Tm}^2\).
Step 2: Calculate Induced Current
The EMF (\( \mathcal{E} \)) induced is given by:
\(\mathcal{E} = -N \frac{\Delta \Phi}{\Delta t} = -10 \times \frac{1.8 \times 10^{-3}}{1} = -1.8 \times 10^{-2} \, \text{V}\).
The induced current \(I\) is:
\(I = \frac{\mathcal{E}}{R} = \frac{1.8 \times 10^{-2}}{100} = 1.8 \times 10^{-4} \, \text{A}\).
Step 3: Calculate the Work Done
Work done is equal to the energy dissipated: \(W = I^2 R \Delta t\).
\(W = (1.8 \times 10^{-4})^2 \times 100 \times 1 = 3.24 \times 10^{-6} \, \text{J}\).
Verification
The calculated work \(3.24 \times 10^{-6} \, \text{J}\) is indeed \(3.24 \approx 3 \, \times 10^{-6} \, \text{J}\) which fits the expected range of 3,3.
Thus, the work done is \(3.24 \times 10^{-6} \, \text{J}\).
The emf induced in the loop is:
\[\mathcal{E} = N B v \ell,\]
where:
\[v = \frac{\ell}{t}.\]
The current induced in the loop is:
\[i = \frac{\mathcal{E}}{R} = \frac{N B \ell / t}{R}.\]
The force acting is:
\[F = N \cdot i \cdot B \cdot \ell = \frac{N^2 B^2 \ell^2}{R t}.\]
The work done is:
\[W = F \cdot \ell = \frac{N^2 B^2 \ell^2}{R t} \cdot \ell = \frac{N^2 B^2 \ell^3}{R t}.\]
Substitute values:
\[W = \frac{(10)^2 (0.5)^2 (3.6 \times 10^{-3})^2}{100 \cdot 1}.\]
\[W = 3.24 \times 10^{-6} \, \text{J}.\]
Final Answer: $3.24 \times 10^{-6} \, \text{J}$.
Draw the pattern of the magnetic field lines for the two parallel straight conductors carrying current of same magnitude 'I' in opposite directions as shown. Show the direction of magnetic field at a point O which is equidistant from the two conductors. (Consider that the conductors are inserted normal to the plane of a rectangular cardboard.)
Given below are two statements: one is labelled as Assertion (A) and the other is labelled as Reason (R).
Assertion (A): Choke coil is simply a coil having a large inductance but a small resistance. Choke coils are used with fluorescent mercury-tube fittings. If household electric power is directly connected to a mercury tube, the tube will be damaged.
Reason (R): By using the choke coil, the voltage across the tube is reduced by a factor \( \frac{R}{\sqrt{R^2 + \omega^2 L^2}} \), where \( \omega \) is the frequency of the supply across resistor \( R \) and inductor \( L \). If the choke coil were not used, the voltage across the resistor would be the same as the applied voltage.
In light of the above statements, choose the most appropriate answer from the options given below:
Figure shows a current carrying square loop ABCD of edge length is $ a $ lying in a plane. If the resistance of the ABC part is $ r $ and that of the ADC part is $ 2r $, then the magnitude of the resultant magnetic field at the center of the square loop is: 
Let \( C_{t-1} = 28, C_t = 56 \) and \( C_{t+1} = 70 \). Let \( A(4 \cos t, 4 \sin t), B(2 \sin t, -2 \cos t) \text{ and } C(3r - n_1, r^2 - n - 1) \) be the vertices of a triangle ABC, where \( t \) is a parameter. If \( (3x - 1)^2 + (3y)^2 = \alpha \) is the locus of the centroid of triangle ABC, then \( \alpha \) equals: