To determine the resistance of a moving coil galvanometer, the concept of shunt resistance is employed. A shunt is implemented to reduce the galvanometer's deflection. The deflection of a galvanometer is directly proportional to the current flowing through it, and inversely proportional to the applied shunt resistance.
Given:
The relationship between deflections and resistances is expressed by the formula:
\(\frac{D_1}{D_2} = 1 + \frac{G}{S}\)
where \( G \) represents the resistance of the galvanometer coil.
Substituting the provided values:
\(\frac{25}{5} = 1 + \frac{G}{24}\)
Simplifying the left side of the equation yields:
\(\frac{25}{5} = 5\)
Therefore:
\(5 = 1 + \frac{G}{24}\)
Rearranging to solve for the term with \( G \):
\(5 - 1 = \frac{G}{24}\) \(4 = \frac{G}{24}\)
Finally, calculating \( G \):
\(G = 4 \times 24 = 96 \, \Omega\)
The resistance of the galvanometer coil, \( G \), is \( 96 \, \Omega \).
The determined resistance of the galvanometer is \( 96 \, \Omega \).
Assertion (A): The deflection in a galvanometer is directly proportional to the current passing through it.
Reason (R): The coil of a galvanometer is suspended in a uniform radial magnetic field.