
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: $3.24 \times 10^{-6} \, \text{J}$.
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

| List I | List II |
|---|---|
| A. \( \oint \vec{B} \cdot d\vec{l} = \mu_0 i_c + \mu_0 \epsilon_0 \frac{d\phi_E}{dt} \) | I. Gauss' law for electricity |
| B. \( \oint \vec{E} \cdot d\vec{l} = -\frac{d\phi_B}{dt} \) | II. Gauss' law for magnetism |
| C. \( \oint \vec{E} \cdot d\vec{A} = \frac{Q}{\epsilon_0} \) | III. Faraday law |
| D. \( \oint \vec{B} \cdot d\vec{A} = 0 \) | IV. Ampere – Maxwell law |
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)