Step 1: Define Variables: - Let x represent the current per division. - Initially, the full-scale deflection current Ig for 25 divisions is:
Ig = 25x
Step 2: After Applying the Shunt: - With the shunt applied, the deflection drops to 5 divisions, so the new current through the galvanometer becomes:
Ig = 5x
- The remaining current bypasses through the shunt, giving the total current I:
I = 25x
- The total current I is divided between the galvanometer and the shunt. So, the current through the shunt is:
I - Ig = 25x - 5x = 20x
Step 3: Using the Shunt Resistance: - The shunt resistance S = 24Ω. - Since the potential difference across the galvanometer and the shunt must be equal, we have:
Ig ⋅ G = (I - Ig) ⋅ S
- Substituting Ig = 5x, I - Ig = 20x, and S = 24Ω:
5x ⋅ G = 20x ⋅ 24
Step 4: Solving for G: - Cancel x from both sides:
5G = 20 × 24
- Simplify:
G = \( \frac{20 \times 24}{5} \) = 4 × 24 = 96Ω
So, the correct answer is: 96Ω
Galvanometer:
A galvanometer is an instrument used to show the direction and strength of the current passing through it. In a galvanometer, a coil placed in a magnetic field experiences a torque and hence gets deflected when a current passes through it.
The name "galvanometer" is derived from the surname of Italian scientist Luigi Galvani, who in 1791 discovered that electric current makes a dead frog’s leg jerk.
A spring attached to the coil provides a counter torque. In equilibrium, the deflecting torque is balanced by the restoring torque of the spring, and we have the relation:
\[ NBAI = k\phi \]
Where:
As the current \( I_g \) that produces full-scale deflection in the galvanometer is very small, the galvanometer alone cannot be used to measure current in electric circuits.
To convert a galvanometer into an ammeter (to measure larger currents), a small resistance called a shunt is connected in parallel to the galvanometer.
To convert it into a voltmeter (to measure potential difference), a high resistance is connected in series with the galvanometer.