Let and treat the quencher concentration as a constant reservoir. Weak steady excitation, one emitting population, and the three specified processes give
Dividing the fluorescence photon-production rate by the absorbed photon rate therefore gives
This assumes no saturation, photochemical loss, reabsorption, static association or additional excited-state decay, and that each counted absorbed photon reaches the stated population. In this restricted scheme and the unquenched lifetime is .

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