Bridge circuits were a common way of measuring component values by comparing them to known values. Often an unknown component would be put in one arm of a bridge, and then the bridge would be nulled by adjusting the other arms or changing the frequency of the voltage source. See, for example, the Wheatstone bridge.
The Wien bridge does not require equal values of R or C. At some frequency, the reactance of the series R2–C2 arm will be an exact multiple of the shunt Rx–Cx arm. If the two R3 and R4 arms are adjusted to the same ratio, then the bridge is balanced.
The bridge is balanced when:
The equations simplify if one chooses R2 = Rx and C2 = Cx; the result is R4 = 2 R3.
In practice, the values of R and C will never be exactly equal, but the equations above show that for fixed values in the 2 and x arms, the bridge will balance at some ω and some ratio of R4/R3.
- Ferguson, J. G.; Bartlett, B. W. (July 1928), The Measurement of Capacitance in Terms of Resistance and Frequency, Bell System Technical Journal 7 (3): 420–437, doi:10.1002/j.1538-7305.1928.tb01234.x
- Terman, Frederick (1943), Radio Engineers' Handbook, McGraw-Hill
- Wien, M. (1891), Messung der Inductionsconstanten mit dem "optischen Telephon" (Measurement of Inductive Constants with the "Optical Telephone"), Annalen der Physik und Chemie (in German) 280 (12): 689–712, Bibcode:1891AnP...280..689W, doi:10.1002/andp.18912801208