Applications of Integration

Computing areas between curves, volumes of solids of revolution, arc lengths, and other accumulated quantities.

Area between curves: subtract bottom from top over the interval
-0.303.300123402468f(x) = -xÂē + 4x + 1g(x) = xA = 7.812

Area = integral of [f(x) - g(x)] from x = -0.30 to x = 3.30.

Definition

The integral is a measuring machine. The same operation that computes area can compute length, volume, mass, work, probability — anything that can be expressed as an accumulation of infinitely thin slices.

Area between two curves: the area between f(x)f(x) and g(x)g(x) over [a,b][a, b] (where fâ‰Ĩgf \geq g):

A=âˆŦab[f(x)−g(x)] dxA = \int_a^b [f(x) - g(x)]\,dx

Displacement and distance: if v(t)v(t) is velocity, then:

  • Displacement (signed): âˆŦabv(t) dt\int_a^b v(t)\,dt
  • Distance traveled (always positive): âˆŦabâˆĢv(t)âˆĢ dt\int_a^b |v(t)|\,dt
Key properties
  • Every application here follows the same template: identify an infinitesimal contribution, write it as f(x) dxf(x)\,dx, integrate
  • Displacement and distance traveled coincide exactly when velocity never changes sign
  • All these formulas reduce to ordinary area/length/volume formulas in the simplest cases (e.g. revolving a rectangle gives a cylinder's volume)
  • Units work out automatically: integrating a rate (velocity, force, density) over its variable yields the corresponding total quantity
Common mistakes
  • Confusing displacement with distance traveled: if velocity changes sign, âˆŦv dt\int v\,dt (signed) underestimates how far the particle actually moved — split at the sign changes and integrate âˆĢv(t)âˆĢ|v(t)|
  • Squaring the difference instead of differencing the squares in the washer method: (R−r)2≠R2−r2(R-r)^2 \neq R^2 - r^2 except when r=0r=0 or r=Rr=R
Area between two curves

Find the area between y=x2y = x^2 and y=xy = x on [0,1][0, 1].

Since xâ‰Ĩx2x \geq x^2 on this interval: A=âˆŦ01(x−x2) dx=[x22−x33]01=12−13=16A = \int_0^1 (x - x^2)\,dx = \left[\frac{x^2}{2} - \frac{x^3}{3}\right]_0^1 = \frac{1}{2} - \frac{1}{3} = \frac{1}{6}.

Try it

A particle has velocity v(t)=t2−4v(t) = t^2 - 4 for 0â‰Ītâ‰Ī30 \leq t \leq 3. Find the distance traveled.

Solution

v(t)=0v(t) = 0 when t=2t = 2. On [0,2][0,2], v<0v < 0; on [2,3][2,3], v>0v > 0.

Distance =âˆŦ02(4−t2) dt+âˆŦ23(t2−4) dt= \int_0^2 (4-t^2)\,dt + \int_2^3 (t^2-4)\,dt

On [0,2][0,2]: [4t−t33]02=8−83=163\left[4t - \frac{t^3}{3}\right]_0^2 = 8 - \frac{8}{3} = \frac{16}{3}.

On [2,3][2,3]: [t33−4t]23=(9−12)−(83−8)=−3+163=73\left[\frac{t^3}{3} - 4t\right]_2^3 = (9-12) - \left(\frac{8}{3}-8\right) = -3 + \frac{16}{3} = \frac{7}{3}.

Total distance =163+73=233= \frac{16}{3} + \frac{7}{3} = \frac{23}{3}.

Related concepts

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