Exponential Models with Differential Equations

When a quantity changes at a rate proportional to its own size, the differential equation is dydt=ky\frac{dy}{dt} = ky. Its solutions are exponential functions, and they model growth and decay in many settings.

The model

The formula comes from separation of variables. For y≠0y \ne 0,
∫1y dy=∫k dtln⁡∣y∣=kt+C,\begin{aligned} \int \frac{1}{y}\,dy &= \int k\,dt \\[4pt] \ln|y| &= kt + C, \end{aligned}
so y=Aekty = Ae^{kt} with A=±eCA = \pm e^C. Setting t=0t = 0 gives A=y0A = y_0. The constant solution y=0y = 0 is the case y0=0y_0 = 0. When a free-response question asks for the solution, show these separation steps. The scoring guides give no points to an answer that only quotes y0ekty_0e^{kt}.
Dividing the equation by yy gives k=dy/dtyk = \frac{dy/dt}{y}, the rate of change as a fraction of the current amount. So kk has units of 1/time1/\text{time}. A value of k=0.03k = 0.03 per year means the quantity is growing at 3%3\% of its current size per year at every instant.

Half-life and doubling time

For decay, the half-life TT is the time for the quantity to fall to half its value. Taking logarithms in ekT=12e^{kT} = \frac{1}{2} gives the half-life T=ln⁡2−kT = \frac{\ln 2}{-k}. It doesn't depend on the starting amount. For growth, the doubling time is ln⁡2k\frac{\ln 2}{k}, from ekT=2e^{kT} = 2.

Motion along a line

In motion along a line, the same equation describes a velocity proportional to the position. Differentiating once more gives the acceleration.