The common-mode rejection ratio (CMRR) measures how well a differential amplifier amplifies the differential signal while ignoring the common-mode signal. It is the ratio of differential gain to common-mode gain:
is the gain the amplifier applies to the differential input ; is the (unwanted) gain it applies to the common-mode input . An ideal op-amp has , so its CMRR is infinite. A real op-amp leaks a little common-mode through, so CMRR is large but finite.
For a 741, CMRR . Convert: means . The differential gain is about thirty thousand times the common-mode gain. [Background from general knowledge, not the source PDF] The decibel form is standard because CMRR spans many orders of magnitude; a precision Instrumentation amplifier reaches well over ().
Why it matters
The whole reason to use a differential front end is to pull a small wanted difference out of a large unwanted common pedestal. Picture an ECG electrode pair: the heart signal is about differential, but both leads pick up roughly of 60 Hz mains hum in common. Suppose . The wanted output is . With CMRR , the common-mode gain is , so the hum at the output is — small enough to live with. Drop CMRR to () and the same hum becomes -equivalent at the input: the signal is buried. High CMRR is the single specification that makes sensor measurement — strain gauges, thermocouples, biopotentials — possible.
For a single-op-amp Difference amplifier, CMRR is not set by the op-amp at all but by how precisely the four external resistors are matched; any mismatch converts common-mode into a differential error. That fragility is exactly why the Instrumentation amplifier exists: its input stage amplifies only the differential signal before any resistor matching is relied upon, so realistic resistor tolerances still yield CMRR above .