Applications of Derivatives

A derivative is a rate of change

If yy depends on xx, then dydx\dfrac{dy}{dx} measures how fast yy changes as xx changes. This is the idea behind every physical rate-of-change problem, from growing areas to moving particles.

The applications at a glance

Every application below starts from the same derivative. Each has its own page with the method and worked examples.

Where the derivative is used, and the page that covers each use
ApplicationWhat the derivative tells you
Rates of change (this page)dydx\dfrac{dy}{dx} at a given value: how fast yy changes
Increasing and decreasing functionsThe sign of f′(x)f'(x): positive means rising, negative means falling
Tangents and normalsf′(x1)f'(x_1) is the tangent's slope at a point, −1f′(x1)-\dfrac{1}{f'(x_1)} the normal's
Maxima and minimaSolve f′(x)=0f'(x) = 0, then test the sign of f′f' or f′′f''
Approximationsdy=f′(x) dxdy = f'(x)\,dx estimates a small change in yy
Rolle's theoremGuarantees a point where f′(c)=0f'(c) = 0 (or equals the chord's slope)

Worked example: rate of change of an area

Find the rate of change of the area of a circle with respect to its radius rr, when r=4r=4 cm.

Solution: Area is A=πr2A = \pi r^2, so:

dAdr=2πr\dfrac{dA}{dr} = 2\pi r

At r=4r=4: dAdr=2π(4)=8π\dfrac{dA}{dr} = 2\pi(4) = 8\pi sq. cm per cm of radius.

Worked example: velocity and acceleration

A particle's position is s=4t3−2t2+3t+7s = 4t^3 - 2t^2 + 3t + 7. Find its velocity and acceleration at t=2t=2 seconds.

Solution: Velocity is the first derivative of position, and acceleration is the derivative of velocity:

v=dsdt=12t2−4t+3,a=dvdt=24t−4v = \dfrac{ds}{dt} = 12t^2 - 4t + 3, \qquad a = \dfrac{dv}{dt} = 24t - 4

At t=2t=2:

v=12(4)−4(2)+3=43 units/s,a=24(2)−4=44 units/s2v = 12(4) - 4(2) + 3 = 43 \text{ units/s}, \qquad a = 24(2) - 4 = 44 \text{ units/s}^2

Worked example: related rates

A spherical balloon is being inflated so that its radius increases at 0.50.5 cm/s. How fast is its volume increasing when the radius is 1010 cm?

Solution: Both VV and rr change with time, so differentiate V=43πr3V = \dfrac{4}{3}\pi r^3 with respect to tt using the chain rule:

dVdt=4πr2drdt=4π(10)2(0.5)=200π cm3/s\dfrac{dV}{dt} = 4\pi r^2\dfrac{dr}{dt} = 4\pi(10)^2(0.5) = 200\pi \text{ cm}^3\text{/s}

Common mistakes

  • Substituting the value too early. In the balloon example, putting r=10r = 10 into VV before differentiating gives a constant, whose derivative is 0. Differentiate first, then substitute.
  • Dropping the units. A rate's units are the output's units per input unit: cm2\text{cm}^2 per cm for area against radius, cm3\text{cm}^3 per second for volume against time.
  • Confusing velocity with speed. Velocity dsdt\dfrac{ds}{dt} can be negative (moving backwards). Speed is its absolute value.
  • Treating acceleration as a first derivative of position. Acceleration is d2sdt2\dfrac{d^2s}{dt^2}, the derivative of velocity.

Continue learning

Rate-of-change problems and optimization problems both start from the same derivative-as-rate idea: one asks how fast something changes, the other asks where that rate hits zero. The same derivative also drives approximating small changes directly, instead of an exact rate.