To determine the value of \( V_B \) in the given circuit where the galvanometer shows no deflection, we need to understand that this condition indicates a balanced Wheatstone bridge. In a balanced Wheatstone bridge, the ratio of the resistances in one arm is equal to the ratio in the other arm.
Given:
In the bridge, since the galvanometer shows no deflection, the potential difference across it is zero. This implies that the potential difference across resistor \( R_1 \) connected with \( V_A \) is equal to the potential difference across resistor \( R \) and \( V_B \).
The formula for balancing a Wheatstone bridge is:
\(\frac{V_A}{R_1} = \frac{V_B}{R}\)
Substituting the given values:
\(\frac{12}{500} = \frac{V_B}{100}\)
Simplifying the equation:
12 \times 100 = V_B \times 500
1200 = 500 \times V_B
V_B = \frac{1200}{500}
V_B = 2.4 \, V
Given the options, the closest value to \( V_B \) is \( 2 \, V \).
Thus, the value of \( V_B \) is 2 V.
The correct answer is 2 V, as no deflection in the galvanometer indicates a balanced bridge condition, which has been satisfied by the derived calculations.