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
``
R1 R2
V R R IR
S 3 4
||
R3 Rx
``
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
``
A BC D
| | |
E X-Y F
| | |
G | |
||
J K
||
R1 Rx
||
``
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
Formula for Balancing Length
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