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In most [[electrical circuit]]s the signal is transferred by a differential voltage between two [[Electrical conductor|conductors]]. If the voltages on these conductors are {{math|''U''<sub>1</sub>}} and {{math|''U''<sub>2</sub>}}, the common-mode signal is the [[Arithmetic mean|average]] of the voltages:
:<math>U_\text{cm} = \frac{U_1 + U_2}{2}</math>▼
When referenced to the local common or ground, a common-mode signal appears on both lines of a two-wire cable, in phase and with equal amplitudes. Technically, a common-mode voltage is one-half the vector sum of the voltages from each conductor of a balanced circuit to local ground or common. Such signals can arise from one or more of the following sources:▼
▲When referenced to the local common or [[Ground (electricity)|ground]], a common-mode signal appears on both lines of a two-wire cable, [[in phase]] and with equal amplitudes. Technically, a common-mode voltage is one-half the [[vector sum]] of the voltages from each conductor of a [[balanced circuit]] to local ground or common. Such signals can arise from one or more of the following sources:
* Radiated signals coupled equally to both lines,
* An offset from signal common created in the driver circuit, or
* A ground differential between the transmitting and receiving locations.
[[Noise (electronics)|Noise]] induced into a cable, or transmitted from a cable, usually occurs in the common mode, as the same signal tends to be picked up by both conductors in a two-wire cable. Likewise, RF noise transmitted from a cable tends to emanate from both conductors. Elimination of common-mode signals on cables entering or leaving electronic equipment is important to ensure [[electromagnetic compatibility]]. Unless the intention is to transmit or receive radio signals, an electronic designer generally designs electronic circuits to minimise or eliminate common-mode effects.
==Methods of eliminating common-mode signals==
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