Differential signalling 2026-11-05
Differential signalling encodes a signal in the electric potential difference between two conductors, . Writing separates this information from the common-mode voltage . A receiver responds primarily to the difference, with finite common-mode rejection ratio in practice.[ref]
For a test, drive one conductor to V and the other to V, giving V. Adding the same 0.3 V disturbance to both preserves . If unequal coupling instead adds 0.30 V and 0.29 V, the receiver sees a 0.01 V differential error. This calculation explains why balanced path impedances matter: common exposure alone does not ensure common coupling. A useful bench measurement compares a shared disturbance with a deliberately unbalanced input path, recording both inputs and the output. Differential transmission also need not mean that either conductor is at zero potential relative to the receiver's reference.
Differential signal pair 2026-11-05
A differential signal pair carries information in the electric potential difference between two conductors. For conductor potentials and relative to a stated reference, define the differential and common-mode voltage components by
Equivalently and . A signal pair need not have zero common component; the receiver uses the difference while tolerating a specified range of common input potentials.[ref]
Equal added disturbances cancel in the ideal subtraction: replacing both potentials by leaves unchanged. For example, inputs at and volts have volts. Adding volts to each changes but preserves the difference.
Real receivers have finite common-mode rejection ratio, and unequal coupling or mismatched impedances can convert a common disturbance into a differential one. Thus differential signalling is a system property involving the source, both paths and the receiver. An original test applies the same disturbance to both inputs and compares the output with a deliberately unbalanced path; it separates ideal cancellation from sensitivity to mismatch.