- The half-time "T" is the time during which the charge stored is decreased by two times : "Q_0 e^{-\\frac{T}{RC}} = \\frac{1}{2} Q_0". Thus "\\frac{T}{RC}=\\ln 2" and so "T = RC\\ln2".
- The characteristic time "\\tau" is defined such that "Q = Q_0 e^{-\\frac{t}{\\tau}}" and thus "\\tau = RC".
We see from these two relations that "T = \\tau \\ln 2". We can also verify that "RC" have the dimensions of a time.
Comments
Leave a comment