Wheatstone’s Bridge, Meter Bridge and Potentiometer
Finding Unknown Resistance using Wheatstone Bridge
Wheatstone’s Bridge
- Developed by Sir Charles Wheatstone in 1843
- Use of a bridge circuit to measure unknown resistance
- Consists of 4 resistors arranged in a diamond shape
Wheatstone’s Bridge Circuit
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R3 Rx
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Working Principle of Wheatstone’s Bridge
- Condition for balanced bridge:
(R1/R2) = (R3/Rx)
- When the bridge is balanced:
- No current flows through the galvanometer
- Ratio of resistances is equal
Applications of Wheatstone’s Bridge
- Determining unknown resistance
- Measuring small variations in resistance
- Null detection in sensitive laboratory instruments
Meter Bridge
- Also known as slide wire bridge or potentiometer
- Consists of a long uniform wire stretched over a wooden board
- Used to find the unknown resistance and verify Ohm’s law
Circuit Diagram of Meter Bridge
P - Q | | R1 X | | - J | | R2 Y | | - K | | G M N H
Working of Meter Bridge
- Jockey is moved along the wire until the null point is obtained
- No current flows through the galvanometer when balanced
- Ratio of resistances is equal:
(R1/X) = (R2/Y)
Potentiometer
- Device used to measure emf and potential difference
- Consists of a long uniform wire
- Comparing unknown emf with a known standard cell emf
Circuit Diagram of Potentiometer
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A BC D
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E X-Y F
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G | |
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J K
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R1 Rx
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Properties of a Potentiometer
- Measures potential difference accurately
- No current flows in the potentiometer wire
- Can measure emf of a cell directly
Balancing Length in Potentiometer
- Balancing length is the position on the wire where no current flows through the galvanometer
- At a balanced point, potential drop across a length is equal to the emf of the cell being measured
- Balancing length (L) is given by:
L = (E × l) / V
where,
E is the emf of the cell,
l is the length of the potentiometer wire,
V is the potential gradient of the potentiometer wire
Wheatstone Bridge Vs. Potentiometer
Wheatstone Bridge:
- Measures unknown resistance
- Comparison of resistances
- Needs a known resistance
Potentiometer:
- Measures potential difference or emf
- Does not require a known resistance
- No power loss in the circuit
Advantages of Wheatstone’s Bridge
- Highly accurate method of measuring resistance
- Can be used for both high and low resistances
- Easy to use and portable
Advantages of Meter Bridge
- High sensitivity and accuracy in measuring unknown resistances
- Directly verifies Ohm’s law
- Can be used for both DC and AC circuits
Advantages of Potentiometer
- Highly accurate in measuring potential difference and emf
- No current flow through the wire, reducing errors
- Can be used with different cells or batteries
Limitations of Wheatstone’s Bridge
- Requires a known resistance for comparison
- Works only if the galvanometer has high sensitivity
Limitations of Meter Bridge
- Difficult to obtain exact null point due to thermal effects
- Not suitable for low resistance measurements
Limitations of Potentiometer
- Requires a long wire, limiting portability
- Measurement errors can occur due to wire resistivity and faults in connections
Slide 21:
- Example: Determine the value of the unknown resistance Rx in a Wheatstone bridge circuit having R1 = 100 ohms, R2 = 200 ohms, and R3 = 150 ohms.
- Equation: (R1/R2) = (R3/Rx)
- Substituting the given values, we have (100/200) = (150/Rx)
- Solving for Rx, we find Rx = 300 ohms
Slide 22:
- Example: A meter bridge has a wire of length 100 cm. The resistances R1 and R2 are 10 ohms and 20 ohms respectively. Find the balancing length when the unknown resistance X is 5 ohms.
- Equation: (R1/X) = (R2/Y), where Y is the length from one end of the wire to the null point
- Substituting the given values, we have (10/5) = (20/Y)
- Solving for Y, we find Y = 10 cm, which is the balancing length
Slide 23:
- Example: A potentiometer has a wire of length 200 cm and a potential gradient of 0.1 V/cm. If the emf of a cell being measured is 1.5 V, find the balancing length.
- Equation: L = (E × l) / V, where L is the balancing length, E is the emf, l is the length of the wire, and V is the potential gradient
- Substituting the given values, we have L = (1.5 × 200) / 0.1 = 300 cm
Slide 24:
- Example: A student measures the balancing length of a potentiometer wire to be 40 cm. If the potential gradient is 0.2 V/cm, determine the emf of the cell being measured.
- Equation: E = (L × V) / l, where E is the emf, L is the balancing length, V is the potential gradient, and l is the length of the wire
- Substituting the given values, we have E = (40 × 0.2) / 100 = 0.08 V
Slide 25:
- Example: In a Wheatstone bridge circuit, if R1 = 5 ohms and R2 = 10 ohms, what should be the value of R3 to balance the bridge when the unknown resistance Rx is 15 ohms?
- Equation: (R1/R2) = (R3/Rx)
- Substituting the given values, we have (5/10) = (R3/15)
- Solving for R3, we find R3 = 7.5 ohms
Slide 26:
- Example: A meter bridge has a wire of length 50 cm. The resistances R1 and R2 are 5 ohms and 10 ohms respectively. Find the balancing length when the unknown resistance X is 8 ohms.
- Equation: (R1/X) = (R2/Y), where Y is the length from one end of the wire to the null point
- Substituting the given values, we have (5/8) = (10/Y)
- Solving for Y, we find Y = 16.7 cm, which is the balancing length
Slide 27:
- Example: A potentiometer has a wire of length 150 cm and a potential gradient of 0.05 V/cm. If the emf of a cell being measured is 2 V, find the balancing length.
- Equation: L = (E × l) / V, where L is the balancing length, E is the emf, l is the length of the wire, and V is the potential gradient
- Substituting the given values, we have L = (2 × 150) / 0.05 = 600 cm
Slide 28:
- Example: A student measures the balancing length of a potentiometer wire to be 30 cm. If the potential gradient is 0.3 V/cm, determine the emf of the cell being measured.
- Equation: E = (L × V) / l, where E is the emf, L is the balancing length, V is the potential gradient, and l is the length of the wire
- Substituting the given values, we have E = (30 × 0.3) / 100 = 0.09 V
Slide 29:
- Applications of Wheatstone Bridge:
- Measurement of unknown resistance
- Determination of unknown resistivity of a material
- Calibration of resistance measuring instruments
Slide 30:
- Applications of Meter Bridge:
- Verification of Ohm’s law
- Measurement of small resistances
- Measurement of unknown resistance by null deflection technique