If we describe a system to be in a specific state $E_0$ at time $t=0$, but this state has a finite lifetime $\tau_b$, the state decays in time according to
$$ \psi(t)\sim e^{-t/2\tau_b}e^{iE_0t/\hbar}.$$
This state can be written as a superposition of states with a range of energies around $E_0$ according to
$$ \psi(t) \sim \frac{1}{2\pi\hbar}\int_{-\infty}^{+\infty}dE \frac{1}{1-2i(E-E_0)\tau_b/\hbar}e^{-i(E-E_0) t/\hbar}. $$
Note that this is essentially the Fourier transform of the exponential decay, if we use the Einstein relation between energy and frequency $E=\hbar\omega$.
The energy-uncertainty of this state, taken to be the FWHM $\Delta E$ of the Lorentzian energy distribution
$$ p(E)dE = \frac{dE}{1+(E-E_0)^2(2\tau_b)^2/\hbar^2}$$
obeys the equation
$$ (\Delta E/2)^2(2\tau_b)^2/\hbar^2 = 1 \Rightarrow \Delta E\tau_b = \hbar.$$
This shows how the decay time $\tau_b$ of an exponentially decaying state is related (via a Fourier-transform) to the energy uncertainty $\Delta E$ of the state.
I do not consider this explanation to be a rigorous derivation, and I am sure it can be formulated in a more rigorous way. However, I like it, because it exemplifies the relation between 'decay in time' and 'energy uncertainty' in a very transparent way.