The emf (\( \varepsilon \)) induced in an inductor is related to the rate of change of current and self-inductance (\( L \)) by the formula:
\[ |\varepsilon| = L \frac{dI}{dt}. \]
Step 1: Determine the rate of change of current
The given current is:
\[ I = 3t + 8. \]
Differentiate \( I \) with respect to \( t \):
\[ \frac{dI}{dt} = 3 \, \text{A/s}. \]
Step 2: Substitute the given values
The magnitude of induced emf is \( |\varepsilon| = 12 \, \text{mV} = 12 \times 10^{-3} \, \text{V} \). Substituting into the formula:
\[ 12 \times 10^{-3} = L \cdot 3. \]
Step 3: Solve for \( L \)
Rearrange to find \( L \):
\[ L = \frac{12 \times 10^{-3}}{3} = 4 \times 10^{-3} \, \text{H}. \]
Convert to millihenries:
\[ L = 4 \, \text{mH}. \]
Thus, the self-inductance of the inductor is \( L = 4 \, \text{mH} \).
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 : \(A_2 \rightleftharpoons 2A\)