# Wheatstone bridge

Wheatstone bridge circuit diagram. The unknown resistance Rx is to be measured; resistances R1, R2 and R3 are known and R2 is adjustable. If the measured voltage VG is 0, then R2/R1Rx/R3.

A Wheatstone bridge is an electrical circuit used to measure an unknown electrical resistance by balancing two legs of a bridge circuit, one leg of which includes the unknown component. The primary benefit of the circuit is its ability to provide extremely accurate measurements (in contrast with something like a simple voltage divider).[1] Its operation is similar to the original potentiometer.

The Wheatstone bridge was invented by Samuel Hunter Christie in 1833 and improved and popularized by Sir Charles Wheatstone in 1843. One of the Wheatstone bridge's initial uses was for the purpose of soils analysis and comparison.[2]

## Operation

In the figure, ${\displaystyle \scriptstyle R_{x}}$  is the fixed, yet unknown, resistance to be measured.

${\displaystyle \scriptstyle R_{1},}$  ${\displaystyle \scriptstyle R_{2},}$  and ${\displaystyle \scriptstyle R_{3}}$  are resistors of known resistance and the resistance of ${\displaystyle \scriptstyle R_{2}}$  is adjustable. The resistance ${\displaystyle \scriptstyle R_{2}}$  is adjusted until the bridge is "balanced" and no current flows through the galvanometer ${\displaystyle \scriptstyle V_{g}}$ . At this point, the voltage between the two midpoints (B and D) will be zero. Therefore the ratio of the two resistances in the known leg ${\displaystyle \scriptstyle (R_{2}/R_{1})}$  is equal to the ratio of the two resistances in the unknown leg ${\displaystyle \scriptstyle (R_{x}/R_{3})}$ . If the bridge is unbalanced, the direction of the current indicates whether ${\displaystyle \scriptstyle R_{2}}$  is too high or too low.

At the point of balance,

{\displaystyle {\begin{aligned}{\frac {R_{2}}{R_{1}}}&={\frac {R_{x}}{R_{3}}}\\[4pt]\Rightarrow R_{x}&={\frac {R_{2}}{R_{1}}}\cdot R_{3}\end{aligned}}}

Detecting zero current with a galvanometer can be done to extremely high precision. Therefore, if ${\displaystyle \scriptstyle R_{1},}$  ${\displaystyle \scriptstyle R_{2},}$  and ${\displaystyle \scriptstyle R_{3}}$  are known to high precision, then ${\displaystyle \scriptstyle R_{x}}$  can be measured to high precision. Very small changes in ${\displaystyle \scriptstyle R_{x}}$  disrupt the balance and are readily detected.

Alternatively, if ${\displaystyle \scriptstyle R_{1},}$  ${\displaystyle \scriptstyle R_{2},}$  and ${\displaystyle \scriptstyle R_{3}}$  are known, but ${\displaystyle \scriptstyle R_{2}}$  is not adjustable, the voltage difference across or current flow through the meter can be used to calculate the value of ${\displaystyle \scriptstyle R_{x},}$  using Kirchhoff's circuit laws. This setup is frequently used in strain gauge and resistance thermometer measurements, as it is usually faster to read a voltage level off a meter than to adjust a resistance to zero the voltage.

## Derivation

Directions of currents arbitrarily assigned

First, Kirchhoff's first law is used to find the currents in junctions B and D:

{\displaystyle {\begin{aligned}I_{3}-I_{x}+I_{G}&=0\\I_{1}-I_{2}-I_{G}&=0\end{aligned}}}

Then, Kirchhoff's second law is used for finding the voltage in the loops ABD and BCD:

{\displaystyle {\begin{aligned}(I_{3}\cdot R_{3})-(I_{G}\cdot R_{G})-(I_{1}\cdot R_{1})&=0\\(I_{x}\cdot R_{x})-(I_{2}\cdot R_{2})+(I_{G}\cdot R_{G})&=0\end{aligned}}}

When the bridge is balanced, then IG = 0, so the second set of equations can be rewritten as:

{\displaystyle {\begin{aligned}I_{3}\cdot R_{3}&=I_{1}\cdot R_{1}\quad {\text{(1)}}\\I_{x}\cdot R_{x}&=I_{2}\cdot R_{2}\quad {\text{(2)}}\end{aligned}}}

Then, equation (1) is divided by equation (2) and the resulting equation is rearranged, giving:

${\displaystyle R_{x}={{R_{2}\cdot I_{2}\cdot I_{3}\cdot R_{3}} \over {R_{1}\cdot I_{1}\cdot I_{x}}}}$

Due to: I3 = Ix and I1 = I2 being proportional from Kirchhoff's First Law in the above equation I3 I2 over I1 Ix cancel out of the above equation. The desired value of Rx is now known to be given as:

${\displaystyle R_{x}={{R_{3}\cdot R_{2}} \over {R_{1}}}}$

On the other hand, if the resistance of the galvanometer is high enough that IG is negligible, it is possible to compute Rx from the three other resistor values and the supply voltage (VS), or the supply voltage from all four resistor values. To do so, one has to work out the voltage from each potential divider and subtract one from the other. The equations for this are:

{\displaystyle {\begin{aligned}V_{G}&=\left({R_{2} \over {R_{1}+R_{2}}}-{R_{x} \over {R_{x}+R_{3}}}\right)V_{s}\\[6pt]R_{x}&={{R_{2}\cdot V_{s}-(R_{1}+R_{2})\cdot V_{G}} \over {R_{1}\cdot V_{s}+(R_{1}+R_{2})\cdot V_{G}}}R_{3}\end{aligned}}}

where VG is the voltage of node D relative to node B.

## Significance

The Wheatstone bridge illustrates the concept of a difference measurement, which can be extremely accurate. Variations on the Wheatstone bridge can be used to measure capacitance, inductance, impedance and other quantities, such as the amount of combustible gases in a sample, with an explosimeter. The Kelvin bridge was specially adapted from the Wheatstone bridge for measuring very low resistances. In many cases, the significance of measuring the unknown resistance is related to measuring the impact of some physical phenomenon (such as force, temperature, pressure, etc.) which thereby allows the use of Wheatstone bridge in measuring those elements indirectly.

The concept was extended to alternating current measurements by James Clerk Maxwell in 1865 and further improved as Blumlein bridge by Alan Blumlein around 1926.[citation needed]

## Modifications of the fundamental bridge

The Wheatstone bridge is the fundamental bridge, but there are other modifications that can be made to measure various kinds of resistances when the fundamental Wheatstone bridge is not suitable. Some of the modifications are: