Average lifetime of a radioactive atom
Posted by David Zaslavsky on — EditedSome time ago I posted about the theoretical justification for exponential decay. In that post, I showed that you can quantify exponential decay with this equation:
where \(N(t)\) is the number of undecayed atoms at time \(t\) and \(\lambda\) is a constant representing the decay rate. If you plug in \(N(t) = \frac{1}{2}N(0)\), the condition for the half-life, you can find that
But physicists usually write the formula like this,
where \(\tau\) is called the time constant. We prefer this to using the decay rate because, as I wrote in Calculating Terminal Speed, it’s often best to write a physics question in terms of dimensionless ratios like \(\frac{t}{T}\), where \(T\) is some time characteristic of the physical system you’re studying. We could use the half-life for \(T\), but the time constant \(\tau\) is more appealing for a couple of reasons: it keeps that ugly factor of \(\ln 2\) out of the formula, and more importantly, \(\tau\) is physically meaningful because it’s the average lifetime of an individual atom …