Applications of IntegrationTopic #32 of 32

Surface Area of Revolution

Finding surface areas of solids of revolution.

Formula for Rotation around x-axis

When y=f(x)y = f(x) is rotated around the x-axis from x=ax = a to x=bx = b:

S=2πabf(x)1+[f(x)]2dx=2πabydsS = 2\pi \int_a^b f(x) \sqrt{1 + [f'(x)]^2} \, dx = 2\pi \int_a^b y \, ds

where ds=1+(dy/dx)2dxds = \sqrt{1 + (dy/dx)^2} \, dx is the arc length element.

Formula for Rotation around y-axis

When y=f(x)y = f(x) is rotated around the y-axis from x=ax = a to x=bx = b:

S=2πabx1+[f(x)]2dx=2πabxdsS = 2\pi \int_a^b x \sqrt{1 + [f'(x)]^2} \, dx = 2\pi \int_a^b x \, ds

General Pattern

S=2π(radius)(arc length element)S = 2\pi \int (\text{radius})(\text{arc length element})

  • Radius is the distance from the curve to the axis of rotation
  • Arc length element is ds=1+(dy/dx)2dxds = \sqrt{1 + (dy/dx)^2} \, dx

Parametric Form

For x=x(t)x = x(t), y=y(t)y = y(t) rotated around x-axis:

S=2παβy(t)(dxdt)2+(dydt)2dtS = 2\pi \int_\alpha^\beta y(t) \sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2} \, dt

As a Function of y

For x=g(y)x = g(y) rotated around x-axis from y=cy = c to y=dy = d:

S=2πcdy1+[g(y)]2dyS = 2\pi \int_c^d y \sqrt{1 + [g'(y)]^2} \, dy

Examples

Example 1: Cone

Rotate y=xy = x from x=0x = 0 to x=hx = h around the x-axis.

dydx=1\frac{dy}{dx} = 1

ds=1+1dx=2dxds = \sqrt{1 + 1} \, dx = \sqrt{2} \, dx

S=2π0hx2dx=2π2[x22]0h=π2h2S = 2\pi \int_0^h x \cdot \sqrt{2} \, dx = 2\pi\sqrt{2} \left[\frac{x^2}{2}\right]_0^h = \pi\sqrt{2} \cdot h^2

Verify: For a cone with radius r=hr = h and slant height l=h2l = h\sqrt{2}:

S=πrl=πhh2=πh22S = \pi rl = \pi h \cdot h\sqrt{2} = \pi h^2\sqrt{2}

Example 2: Sphere

Rotate y=r2x2y = \sqrt{r^2 - x^2} from x=rx = -r to x=rx = r around x-axis.

dydx=xr2x2\frac{dy}{dx} = \frac{-x}{\sqrt{r^2 - x^2}}

1+(dydx)2=1+x2r2x2=r2r2x21 + \left(\frac{dy}{dx}\right)^2 = 1 + \frac{x^2}{r^2 - x^2} = \frac{r^2}{r^2 - x^2}

ds=rr2x2dxds = \frac{r}{\sqrt{r^2 - x^2}} \, dx

S=2πrrr2x2rr2x2dx=2πrrrdxS = 2\pi \int_{-r}^r \sqrt{r^2 - x^2} \cdot \frac{r}{\sqrt{r^2 - x^2}} \, dx = 2\pi \int_{-r}^r r \, dx

=2πr[x]rr=2πr2r=4πr2= 2\pi r [x]_{-r}^r = 2\pi r \cdot 2r = 4\pi r^2

Example 3: Paraboloid

Rotate y=x2y = x^2 from x=0x = 0 to x=1x = 1 around the y-axis.

dydx=2x\frac{dy}{dx} = 2x

ds=1+4x2dxds = \sqrt{1 + 4x^2} \, dx

S=2π01x1+4x2dxS = 2\pi \int_0^1 x \cdot \sqrt{1 + 4x^2} \, dx

Let u=1+4x2u = 1 + 4x^2, du=8xdxdu = 8x \, dx

=2π1815udu=π423[u3/2]15= 2\pi \cdot \frac{1}{8} \int_1^5 \sqrt{u} \, du = \frac{\pi}{4} \cdot \frac{2}{3} [u^{3/2}]_1^5

=π6[53/21]=π6[551]5.33= \frac{\pi}{6} [5^{3/2} - 1] = \frac{\pi}{6} [5\sqrt{5} - 1] \approx 5.33

Example 4: Using y as parameter

Rotate x=yx = \sqrt{y} from y=0y = 0 to y=4y = 4 around x-axis.

dxdy=12y\frac{dx}{dy} = \frac{1}{2\sqrt{y}}

ds=1+14ydy=4y+14ydyds = \sqrt{1 + \frac{1}{4y}} \, dy = \sqrt{\frac{4y + 1}{4y}} \, dy

S=2π04y4y+14ydy=2π04y4y+12dyS = 2\pi \int_0^4 y \cdot \sqrt{\frac{4y + 1}{4y}} \, dy = 2\pi \int_0^4 \sqrt{y} \cdot \frac{\sqrt{4y + 1}}{2} \, dy

=π044y2+ydy= \pi \int_0^4 \sqrt{4y^2 + y} \, dy

Let u=4y+1u = 4y + 1, then y=u14y = \frac{u-1}{4}:

=π8117(u1)u4du=π16117u2udu= \frac{\pi}{8} \int_1^{17} \sqrt{\frac{(u-1)u}{4}} \, du = \frac{\pi}{16} \int_1^{17} \sqrt{u^2 - u} \, du

Using substitution and formula: 30.85\approx 30.85

Example 5: Gabriel's Horn

Rotate y=1xy = \frac{1}{x} from x=1x = 1 to x=x = \infty around x-axis.

dydx=1x2\frac{dy}{dx} = -\frac{1}{x^2}

ds=1+1x4dxds = \sqrt{1 + \frac{1}{x^4}} \, dx

S=2π11x1+1x4dxS = 2\pi \int_1^\infty \frac{1}{x} \sqrt{1 + \frac{1}{x^4}} \, dx

Since 1+1x4>1\sqrt{1 + \frac{1}{x^4}} > 1:

S>2π11xdx=2π[lnx]1=S > 2\pi \int_1^\infty \frac{1}{x} \, dx = 2\pi [\ln x]_1^\infty = \infty

The surface area is infinite!

Note: Interestingly, the volume is finite:

V=π11x2dx=π[1x]1=πV = \pi \int_1^\infty \frac{1}{x^2} \, dx = \pi \left[-\frac{1}{x}\right]_1^\infty = \pi

This is the famous Gabriel's Horn paradox.

Example 6: Zone of sphere

Find surface area of sphere of radius rr between y=ay = a and y=by = b (where ra<br-r \leq a < b \leq r).

x=r2y2x = \sqrt{r^2 - y^2}

dxdy=yr2y2\frac{dx}{dy} = \frac{-y}{\sqrt{r^2 - y^2}}

ds=rr2y2dyds = \frac{r}{\sqrt{r^2 - y^2}} \, dy

S=2πabr2y2rr2y2dy=2πrabdy=2πr(ba)S = 2\pi \int_a^b \sqrt{r^2 - y^2} \cdot \frac{r}{\sqrt{r^2 - y^2}} \, dy = 2\pi r \int_a^b dy = 2\pi r(b - a)

The surface area depends only on the height of the zone, not its position!