The voltage ratio in a transformer is equal to the turns ratio:
\( \frac{V_s}{V_p} = \frac{N_s}{N_p} \)
where \( V_s \) and \( V_p \) are the secondary and primary voltages, and \( N_s \) and \( N_p \) are the number of turns in the secondary and primary coils, respectively. Given \( V_p = 12 \, \text{kV} = 12000 \, \text{V} \) and \( V_s = 120 \, \text{V} \), we have:
\( \frac{120}{12000} = \frac{N_s}{N_p} \quad \Rightarrow \quad \frac{N_s}{N_p} = \frac{1}{100} \)
For an ideal transformer, the input power is equal to the output power:
\( P_{in} = P_{out} \)
Power is given by \( P = IV \), so:
\( I_p V_p = I_s V_s = 60 \, \text{kW} = 60000 \, \text{W} \)
We can calculate the primary current (\( I_p \)):
\( I_p = \frac{60000}{V_p} = \frac{60000}{12000} = 5 \, \text{A} \)
Similarly, we can calculate the secondary current (\( I_s \)):
\( I_s = \frac{60000}{V_s} = \frac{60000}{120} = 500 \, \text{A} \)
The secondary resistance (\( R_s \)) can be calculated using Ohm’s law:
\( R_s = \frac{V_s}{I_s} = \frac{120}{500} = 0.24 \, \Omega = 240 \, \text{m}\Omega \)
The value of the resistive load in the secondary circuit is \( 240 \, \text{m}\Omega \).
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 : \(A_2 \rightleftharpoons 2A\)