In this case, we can use the formula for the current division between the galvanometer and the shunt resistance.
The total current \( I = 1 \, A \) is split between the galvanometer and the shunt.
We use the concept of parallel resistance to calculate the current through the shunt.
Let \( I_g \) be the current through the galvanometer, and \( I_s \) be the current through the shunt.
The total current \( I \) is the sum of the currents through the galvanometer and the shunt: \[ I = I_g + I_s \]
Using the parallel resistance rule for current division: \[ \frac{I_g}{I_s} = \frac{R_s}{R_g} \] where:
- \( R_s = 2 \, \Omega \) is the resistance of the shunt,
- \( R_g = 8 \, \Omega \) is the resistance of the galvanometer. Thus: \[ \frac{I_g}{I_s} = \frac{2}{8} = \frac{1}{4} \] From this ratio, we know that: \[ I_g = \frac{1}{4} \cdot I_s \] Since the total current \( I = 1 \, A \), we have: \[ I_s + I_g = 1 \] \[ I_s + \frac{1}{4} \cdot I_s = 1 \] \[ \frac{5}{4} \cdot I_s = 1 \] \[ I_s = \frac{4}{5} = 0.8 \, \text{A} \]
Thus, the current passing through the shunt is \( 0.8 \, \text{A} \).
Therefore, the correct answer is: \[ \text{(2) } 0.8 \, \text{A} \]
The graph between variation of resistance of a wire as a function of its diameter keeping other parameters like length and temperature constant is
A wire of resistance $ R $ is bent into a triangular pyramid as shown in the figure, with each segment having the same length. The resistance between points $ A $ and $ B $ is $ \frac{R}{n} $. The value of $ n $ is:
Two point charges M and N having charges +q and -q respectively are placed at a distance apart. Force acting between them is F. If 30% of charge of N is transferred to M, then the force between the charges becomes:
If the ratio of lengths, radii and Young's Moduli of steel and brass wires in the figure are $ a $, $ b $, and $ c $ respectively, then the corresponding ratio of increase in their lengths would be: