To find the induced current in the circuit at \( t = 2 \, \text{s} \), we first need to determine the electromotive force (emf) induced in the circuit using Faraday's Law of electromagnetic induction. The emf (\( \varepsilon \)) is given by the negative rate of change of magnetic flux (\( \phi \)) with respect to time, \( \varepsilon = -\frac{d\phi}{dt} \). Given \( \phi = 5t^2 - 36t + 1 \), we differentiate: \(\frac{d\phi}{dt} = \frac{d}{dt}(5t^2 - 36t + 1) = 10t - 36\).
Substitute \( t = 2 \) into the derivative:
\(\left.\frac{d\phi}{dt}\right|_{t=2} = 10(2) - 36 = 20 - 36 = -16 \, \text{Wb/s}.\)
The induced emf is \(\varepsilon = -\left(-16\right) = 16 \, \text{V}.\)
Using Ohm's Law, \( I = \frac{\varepsilon}{R} \), with resistance \( R = 8 \, \Omega \):
\( I = \frac{16}{8} = 2 \, \text{A}.\)
The computed current, \( 2 \, \text{A} \), fits the expected range of 2 to 2 A. Therefore, the induced current at \( t = 2 \, \text{s} \) is \( 2 \, \text{A}. \)
The emf \( \varepsilon \) induced in the circuit is given by Faraday’s law:
\[ \varepsilon = -\frac{d\Phi}{dt}. \]Calculate \( \frac{d\Phi}{dt} \):
\[ \frac{d\Phi}{dt} = 10t - 36. \]At \( t = 2 \, \text{s} \):
\[ \varepsilon = -(10 \cdot 2 - 36) = -(-16) = 16 \, \text{V}. \]The induced current \( i \) in the circuit is:
\[ i = \frac{\varepsilon}{R} = \frac{16}{8} = 2 \, \text{A}. \]Thus, the induced current at \( t = 2 \, \text{s} \) is:
\[ 2 \, \text{A}. \]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,

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 : \(A_2 \rightleftharpoons 2A\)