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CIRCUIT DIAGRAM EXAMPLE

Wheatstone Bridge Circuit Diagram and Formula

The Wheatstone bridge measures an unknown resistance by comparing it with known ones. The same circuit sits under strain gauges, load cells and many resistive temperature sensors.

Wheatstone bridgeWheatstone bridgeTwo dividers compared by a galvanometer+GB15 VR3470 ΩR4RxR11 kΩR22.2 kΩG1Balanced (VG = 0) whenR1 / R2 = R3 / RxUnknown at balanceRx = R2 × R3 / R1 = 2.2 kΩ × 470 Ω / 1 kΩ ≈ 1.03 kΩReading if Rx = 1.1 kΩVG = 5 V × (1.1 / 1.57 − 2.2 / 3.2) ≈ 66 mVMade with ProtoFlow · protoflow.ai
Each side of the bridge is a voltage divider. When the ratios match, both midpoints sit at the same voltage and the galvanometer reads zero, which gives the unknown resistance from the three known ones.

How this circuit works

The bridge is two voltage dividers across the same 5 V battery. R1 and R2 set the voltage at the left midpoint; R3 and Rx set the voltage at the right one. The galvanometer G1 between the midpoints shows any difference.

With these values the left midpoint sits at 5 V × 2.2 kΩ / 3.2 kΩ ≈ 3.44 V. The right midpoint matches it only when the right side divides in the same ratio, which happens when R1 / R2 = R3 / Rx. Then no current flows through G1 and it reads zero.

Rearranged, Rx = R2 × R3 / R1, so this bridge balances at Rx ≈ 1.03 kΩ. In a lab bridge R3 is adjustable: you turn it until the galvanometer reads zero, then work out Rx. The answer depends only on the known resistors, not on the battery voltage or the meter's calibration.

Off balance, the voltage between the midpoints grows with the mismatch; with Rx = 1.1 kΩ it is about 66 mV. Sensor bridges use that output: a strain gauge or RTD changes Rx slightly, and an instrumentation amplifier measures the small difference.

Formulas

Balance condition
R1 / R2 = R3 / Rx
Unknown resistance
Rx = R2 × R3 / R1 = 2.2 kΩ × 470 Ω / 1 kΩ ≈ 1.03 kΩ
Bridge output
VG = V × (Rx / (R3 + Rx) − R2 / (R1 + R2))

Open-circuit voltage between the midpoints. With Rx = 1.1 kΩ: 5 V × (0.701 − 0.688) ≈ 66 mV.

Parts list

RefPartValueWhat it does
B1Battery5 V5 V battery. The balance point does not depend on its voltage.
G1Meter—Galvanometer, or any sensitive meter, between the two midpoints.
R1Resistor1 kΩ1 kΩ, top of the left ratio arm.
R2Resistor2.2 kΩ2.2 kΩ, bottom of the left ratio arm.
R3Resistor470 Ω470 Ω reference arm; adjustable in a lab bridge.
R4ResistorRxThe unknown resistance, Rx.

Netlist

Recovered from the drawing itself: every pin on each net below is joined by a wire, a junction or a shared supply or ground symbol.

NetConnects
N1B1.-, R4.2, R2.2
N2B1.+, R3.1, R1.1
N3R3.2, R4.1, G1.2
N4R1.2, R2.1, G1.1

Common mistakes

  • Mixing up the ratio. The balance condition compares the two halves of each side: R1 / R2 on the left with R3 / Rx on the right.
  • Connecting the meter between the wrong nodes. It goes between the two midpoints, not across the battery or across one resistor.
  • Reading an unbalanced bridge with a low-resistance meter. It draws current and lowers the reading; at balance it makes no difference.
  • Ignoring lead resistance when Rx is small. Long leads add to Rx; three-wire and four-wire connections are the usual fix.

Frequently asked questions

What is a Wheatstone bridge used for?

Measuring an unknown resistance precisely, and reading resistive sensors such as strain gauges, load cells, RTDs and thermistors, where the sensor forms one arm of the bridge.

What is the balance condition of a Wheatstone bridge?

R1 / R2 = R3 / Rx. At balance both midpoints sit at the same voltage and no current flows through the galvanometer.

Why does the battery voltage not matter at balance?

Both sides divide the same voltage, so changing it moves both midpoints by the same fraction and their difference stays zero.

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