Given:
- Resistance of galvanometer: \( R_g = 100 \, \Omega \)
- Series resistance: \( R_s = 400 \, \Omega \)
- Voltage measured: \( V = 10 \, \text{V} \)
Step 1: Calculating the Current through the Galvanometer
The current through the galvanometer, \( i_g \), is given by:
\[ i_g = \frac{V}{R_g + R_s} = \frac{10}{400 + 100} = \frac{10}{500} = 20 \times 10^{-3} \, \text{A}. \]
Step 2: Converting the Galvanometer to an Ammeter
To convert the galvanometer into an ammeter that can read up to 10 A, we need to connect a shunt resistance \( S \) in parallel with the galvanometer. The shunt resistance is given by:
\[ i_g R_g = (I - i_g) S, \]
where \( I = 10 \, \text{A} \) is the total current.
Rearranging for \( S \):
\[ S = \frac{i_g R_g}{I - i_g} = \frac{20 \times 10^{-3} \times 100}{10 - 20 \times 10^{-3}}. \]
Simplifying:
\[ S = \frac{2}{9.98} \approx 0.2 \, \Omega. \]
Step 3: Expressing \( S \) in the Required Form
Given that \( S = x \times 10^{-2} \, \Omega \), we have:
\[ x = 20. \]
Therefore, the value of \( x \) is 20.
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 : \(A_2 \rightleftharpoons 2A\)