Determination of Galvanometer Resistance by Half-Deflection Method
1. Aim
To determine the resistance of a given galvanometer by the half-deflection method and to calculate its figure of merit.
2. Apparatus Used
- A moving coil galvanometer
- A low resistance shunt box
- A resistance box (0-10,000 Ω)
- A battery (1.5V or 2V)
- A rheostat
- A one-way key
- Connecting wires
- A meter scale
3. Diagram
Fig.1: Circuit diagram for determining galvanometer resistance by half-deflection method
4. Theory
The half-deflection method is based on the principle that when a galvanometer is connected in parallel with a suitable resistance (shunt), the current through the galvanometer reduces, resulting in a decreased deflection.
When a current flows through a galvanometer, the deflection produced is directly proportional to the current passing through it:
When a galvanometer of resistance G is connected in a circuit with a cell of emf E and a resistance R, the current through the galvanometer is:
When a shunt S is connected across the galvanometer, the current through the galvanometer becomes:
According to the half-deflection method, if S is adjusted such that the deflection becomes half of the original deflection, then:
This means:
Solving this equation:
Further simplification leads to:
Therefore, when the deflection is reduced to half by connecting a shunt across the galvanometer, the value of the shunt resistance equals the resistance of the galvanometer.
5. Formula
1. Resistance of the galvanometer (G):
2. Figure of merit (k):
where:
- I is the current through the galvanometer = $\frac{E}{R+G}$
- n is the deflection in divisions
- E is the emf of the battery
- R is the resistance in the circuit
6. Procedure
- Connect the circuit as shown in the diagram without connecting the shunt resistance.
- Close the key K and adjust the resistance R such that a suitable deflection (preferably near full scale) is obtained on the galvanometer. Record this deflection (n₁).
- Open the key and note the zero error, if any.
- Connect a suitable shunt resistance S across the galvanometer.
- Close the key again and adjust the value of S until the deflection becomes exactly half of the original value (n₂ = n₁/2).
- Record the value of the shunt resistance S when half-deflection is achieved.
- Calculate the resistance of the galvanometer using G = S.
- For determining the figure of merit, calculate the current through the galvanometer: $I = \frac{E}{R+G}$
- Calculate the figure of merit using k = I/n₁.
- Repeat the experiment for different values of R and calculate the average value of G and k.
7. Observation Table
Table 1: Determination of Galvanometer Resistance
S.No. | Circuit resistance (R) Ω | Original deflection (n₁) divisions | Shunt resistance for half-deflection (S) Ω | Galvanometer resistance (G = S) Ω |
---|---|---|---|---|
1. | ||||
2. | ||||
3. | ||||
4. | ||||
5. |
Mean value of galvanometer resistance (G) = ________ Ω
Table 2: Determination of Figure of Merit
S.No. | Circuit resistance (R) Ω | Galvanometer resistance (G) Ω | Current (I = E/(R+G)) A | Deflection (n₁) divisions | Figure of merit (k = I/n₁) A/division |
---|---|---|---|---|---|
1. | |||||
2. | |||||
3. | |||||
4. | |||||
5. |
Mean value of figure of merit (k) = ________ A/division
8. Calculations
1. The resistance of the galvanometer is given by:
2. The current through the galvanometer is given by:
where E is the emf of the battery used (in volts)
3. The figure of merit is calculated as:
Sample calculation for the first reading:
- Let R = 1000 Ω
- Original deflection (n₁) = 20 divisions
- Shunt resistance for half-deflection (S) = 50 Ω
- EMF of battery (E) = 1.5 V
Therefore:
- Galvanometer resistance (G) = S = 50 Ω
- Current through galvanometer (I) = $\frac{1.5}{1000+50} = \frac{1.5}{1050} = 0.00143$ A
- Figure of merit (k) = $\frac{0.00143}{20} = 7.14 \times 10^{-5}$ A/division
9. Result
- The resistance of the given galvanometer is ________ Ω.
- The figure of merit of the given galvanometer is ________ A/division.
10. Precautions
- All connections should be tight and clean.
- The battery should have sufficient emf and should be in good condition.
- The galvanometer should be placed on a level surface, free from vibrations.
- The galvanometer should be properly adjusted to zero before taking readings.
- The resistance box should be handled carefully, and plugs should be inserted firmly.
- The key should be pressed gently to avoid any jerk.
- The current passing through the galvanometer should not exceed its maximum safe limit.
- Parallax error should be avoided while taking readings from the galvanometer scale.
- The resistance R should be adjusted to get a suitable deflection (about 3/4 of the full scale).
11. Sources of Error
- Zero error in the galvanometer.
- Error due to improper adjustment of the resistance box.
- Error due to improper connections or loose contacts.
- Error due to internal resistance of the battery.
- Error due to variations in battery voltage during the experiment.
- Error due to temperature variations affecting the resistance values.
- Parallax error while reading the galvanometer scale.
- Error due to fluctuations in the magnetic field around the galvanometer.
- Error due to the heating effect of current in the circuit components.