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Metre Bridge: Slide-Wire Bridge

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Estimated time: 9 minutes
CISCE: Class 12

Introduction

Think of the metre bridge like a see-saw. Just as a see-saw balances when torques on both sides are equal, the bridge "balances" (galvanometer shows zero deflection) when the ratio of resistances on both arms is equal — regardless of how much current flows through the circuit.

CISCE: Class 12

Definition: Metre Bridge

A metre bridge (slide-wire bridge) is a practical laboratory device based on the Wheatstone bridge principle, used to measure an unknown electrical resistance by achieving a null-point (balance) condition on a one-metre-long uniform resistance wire.

CISCE: Class 12
National Testing Agency: Class 12

Principle

The metre bridge works on the Wheatstone bridge principle: a bridge circuit is said to be balanced when no current flows through the galvanometer, i.e., points B and D are at the same potential.

Balance condition: \[\frac {P}{Q}\] = \[\frac {R}{S}\].
CISCE: Class 12
National Testing Agency: Class 12

Construction

Key components:

  • A 1-metre-long uniform wire (manganin or constantan) of uniform cross-section
  • Two thick copper strips creating three gaps on a wooden board
  • A resistance box (R) — known resistance
  • An unknown resistance (S) to be measured
  • A galvanometer (G) with a sliding jockey
  • A battery (Bt) with a key (K) and rheostat

CISCE: Class 12
National Testing Agency: Class 12

Working Procedure

Step Action
1 Connect known resistance R and unknown resistance S in adjacent gaps
2 Close the battery key and adjust R
3 Slide the jockey along the wire to locate the null point (zero deflection)
4 Note the balancing length l (from end A)
5 Apply the balance formula to calculate S
6 Repeat with different R values and take the mean for accuracy
CISCE: Class 12
National Testing Agency: Class 12

Derivation

Using the Wheatstone bridge balance condition, with the wire resistance proportional to length:

  • \[\frac {P}{Q}\] = \[\frac {R}{S}\] and \[\frac {P}{Q}\] = \[\frac {l}{100−l}\]

Equating both:

  • \[\frac {R}{S}\] = \[\frac {l}{100−l}\]

Solving for S:

  • S = R(\[\frac {100−l}{l}\])
CISCE: Class 12

Precautions

  • Keep the null point close to the midpoint (30–70 cm) of the wire for higher accuracy
  • Avoid prolonged current flow to prevent heating and resistance change
  • Use a galvanometer shunt initially to protect it from high currents
  • Do not rub the jockey against the wire — this damages the uniform cross-section
  • Account for end resistance at the copper strip junctions
  • Ensure the wire has uniform cross-section throughout its length
CISCE: Class 12
National Testing Agency: Class 12

Limitations

  • Not suitable for very low resistances (below ~1 Ω) due to end-resistance errors dominating the measurement
  • For low resistances, use Kelvin's Double Bridge or Cary Foster's Bridge instead
CISCE: Class 12

Example

Given: R = 6 Ω, balancing length l = 60 cm

Formula: S = R(\[\frac {100−l}{l}\])

Substitution: S = 6 × \[\frac {100−60}{60}\] = 6 × \[\frac {40}{60}\]

Answer: S = 4 Ω

(Battery current in this configuration ≈ 0.66 A, based on total circuit resistance.)

Video Tutorials

We have provided more than 1 series of video tutorials for some topics to help you get a better understanding of the topic.

Series 1


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