Unit 6, lesson 82

Arc Lengths and Surfaces for Parametric Curves

How the speed of a moving point gives the length of a parametric curve and the area of the surface it sweeps out when rotated, and when these integrals count a piece twice.

  • Theory part 163
  • Practice part 164
  • Calculus of Parametric Curves

A bike odometer does not know the shape of the road. It adds up speed times time, and that sum is the distance travelled. Length along a parametric curve works the same way. Integrate the speed of the moving point and you get the length of its path, and a small change to that integral gives the area of a surface of revolution.

Key terms

Parametric speed

Definition Let x=x(t)x = x(t) and y=y(t)y = y(t) be differentiable at tt. The velocity of the point at time tt is the vector ⟨x′(t),y′(t)⟩\langle x'(t), y'(t) \rangle, and its speed is the length of that vector,

dsdt=x′(t)2+y′(t)2.\frac{ds}{dt} = \sqrt{x'(t)^2 + y'(t)^2}.

In plain words In a short time dtdt the point moves about x′ dtx'\,dt sideways and y′ dty'\,dt up, so by the Pythagorean theorem it covers about x′2+y′2 dt\sqrt{x'^2 + y'^2}\,dt of path.

Example For x=t2x = t^2, y=t3y = t^3 the speed is

dsdt=4t2+9t4=∣t∣4+9t2.\frac{ds}{dt} = \sqrt{4t^2 + 9t^4} = \lvert t \rvert \sqrt{4 + 9t^2}.

At t=1t = 1 it equals 13≈3.61\sqrt{13} \approx 3.61, and at t=0t = 0 it equals 00.

Regularity

Definition A parametrization x=x(t)x = x(t), y=y(t)y = y(t) on an interval II is smooth, or regular, if x′x' and y′y' are continuous on II and are never both zero there, that is, the speed is positive at every tt in II.

In plain words A regular parametrization never stops. Where the point comes to rest, the curve can form a sharp corner or cusp even though x(t)x(t) and y(t)y(t) are perfectly smooth functions.

Example For x=t2x = t^2, y=t3y = t^3 both derivatives 2t2t and 3t23t^2 vanish at t=0t = 0. The curve is y=±x3/2y = \pm x^{3/2}, which has a cusp at the origin. On any interval that avoids t=0t = 0 the parametrization is regular.

Arc length

Definition Let a curve CC be given by x=x(t)x = x(t), y=y(t)y = y(t) for α≤t≤β\alpha \le t \le \beta, where x′x' and y′y' are continuous on [α,β][\alpha, \beta] and CC is traversed exactly once as tt increases from α\alpha to β\beta. Then the length of CC is

L=∫αβx′(t)2+y′(t)2 dt.L = \int_{\alpha}^{\beta} \sqrt{x'(t)^2 + y'(t)^2}\, dt.

In plain words Length is the integral of speed over the time interval, as long as no part of the path is run over twice.

Example One arch of the cycloid x=r(θ−sin⁡θ)x = r(\theta - \sin\theta), y=r(1−cos⁡θ)y = r(1 - \cos\theta) with r>0r > 0 and 0≤θ≤2π0 \le \theta \le 2\pi has

x′2+y′2=r2(1−cos⁡θ)2+r2sin⁡2θ=2r2(1−cos⁡θ)=4r2sin⁡2θ2.x'^2 + y'^2 = r^2(1 - \cos\theta)^2 + r^2 \sin^2\theta = 2r^2(1 - \cos\theta) = 4r^2 \sin^2\frac{\theta}{2}.

Since sin⁡(θ/2)≥0\sin(\theta/2) \ge 0 on [0,2π][0, 2\pi], the square root is 2rsin⁡(θ/2)2r\sin(\theta/2) and the length is

L=∫02π2rsin⁡θ2 dθ=[−4rcos⁡θ2]02π=8r.L = \int_0^{2\pi} 2r\sin\frac{\theta}{2}\, d\theta = \left[-4r\cos\frac{\theta}{2}\right]_0^{2\pi} = 8r.

Piecewise smooth curves

Definition A curve x=x(t)x = x(t), y=y(t)y = y(t), α≤t≤β\alpha \le t \le \beta, is piecewise smooth if xx and yy are continuous on [α,β][\alpha, \beta] and there is a partition α=t0<t1<⋯<tn=β\alpha = t_0 < t_1 < \dots < t_n = \beta such that on each closed piece [tk−1,tk][t_{k-1}, t_k] the functions xx and yy have continuous derivatives (one-sided at the ends) that are never both zero. So each piece is smooth in the sense above, and corners or cusps can occur only at the points tkt_k. If the curve is traced exactly once, its length is the sum of the lengths of the pieces,

L=∑k=1n∫tk−1tkx′(t)2+y′(t)2 dt.L = \sum_{k=1}^{n} \int_{t_{k-1}}^{t_k} \sqrt{x'(t)^2 + y'(t)^2}\, dt.

In plain words Corners are allowed. Measure each smooth stretch between corners and add.

Example The curve x=tx = t, y=∣t∣y = \lvert t \rvert for −1≤t≤1-1 \le t \le 1 is a V with a corner at t=0t = 0. On each half the speed is 1+1=2\sqrt{1 + 1} = \sqrt{2}, so L=2+2=22L = \sqrt{2} + \sqrt{2} = 2\sqrt{2}, the two legs of length 2\sqrt{2} each.

Repeated tracing

Definition Let x′x' and y′y' be continuous on [α,β][\alpha, \beta]. If the parametrization runs over some part of the curve more than once, the integral

∫αβx′(t)2+y′(t)2 dt\int_{\alpha}^{\beta} \sqrt{x'(t)^2 + y'(t)^2}\, dt

is the total distance travelled by the point, not the length of the curve. To get the length, restrict to an interval on which the curve is traced exactly once.

In plain words The integral is an odometer. Drive the same road back and forth and it keeps counting.

Example For x=sin⁡2tx = \sin^2 t, y=cos⁡2ty = \cos^2 t we have x+y=1x + y = 1 with 0≤x≤10 \le x \le 1, a segment of length 2\sqrt{2}. The speed is 2 ∣sin⁡2t∣\sqrt{2}\,\lvert \sin 2t \rvert, and

∫03π2 ∣sin⁡2t∣ dt=2⋅6=62,\int_0^{3\pi} \sqrt{2}\,\lvert \sin 2t \rvert\, dt = \sqrt{2} \cdot 6 = 6\sqrt{2},

because the point runs along the segment six times. The interval [0,π2][0, \frac{\pi}{2}] traces it once and gives 2\sqrt{2}.

Surface area of revolution

Definition Let CC be given by x=x(t)x = x(t), y=y(t)y = y(t) for α≤t≤β\alpha \le t \le \beta, with x′x' and y′y' continuous on [α,β][\alpha, \beta] and CC traversed exactly once. If y(t)≥0y(t) \ge 0 on [α,β][\alpha, \beta], the surface obtained by rotating CC about the xx-axis has area

S=∫αβ2π y(t)x′(t)2+y′(t)2 dt.S = \int_{\alpha}^{\beta} 2\pi\, y(t) \sqrt{x'(t)^2 + y'(t)^2}\, dt.

If instead x(t)≥0x(t) \ge 0 on [α,β][\alpha, \beta], rotating about the yy-axis gives

S=∫αβ2π x(t)x′(t)2+y′(t)2 dt.S = \int_{\alpha}^{\beta} 2\pi\, x(t) \sqrt{x'(t)^2 + y'(t)^2}\, dt.

In plain words Each tiny piece of curve of length dsds sweeps out a thin band. The band’s area is its circumference 2π×radius2\pi \times \text{radius} times its width dsds.

Example The upper half circle x=rcos⁡tx = r\cos t, y=rsin⁡ty = r\sin t, 0≤t≤π0 \le t \le \pi, with r>0r > 0 has speed rr. Rotating it about the xx-axis gives a sphere with

S=∫0π2π rsin⁡t⋅r dt=2πr2[−cos⁡t]0π=4πr2.S = \int_0^{\pi} 2\pi\, r\sin t \cdot r\, dt = 2\pi r^2 \left[-\cos t\right]_0^{\pi} = 4\pi r^2.

Distance to the axis

Definition In the surface area integral the factor in front of dsds is 2πρ(t)2\pi\rho(t), where ρ(t)\rho(t) is the distance from the point (x(t),y(t))(x(t), y(t)) to the axis of rotation. For the xx-axis ρ=∣y∣\rho = \lvert y \rvert, for the yy-axis ρ=∣x∣\rho = \lvert x \rvert, for the line y=ky = k it is ∣y−k∣\lvert y - k \rvert and for the line x=hx = h it is ∣x−h∣\lvert x - h \rvert. The curve must not cross the axis, because pieces on opposite sides can sweep over the same surface, which would then be counted twice.

In plain words The radius of each band is how far that bit of curve is from the axis, whatever the axis is.

Example Rotate the circle x=cos⁡tx = \cos t, y=2+sin⁡ty = 2 + \sin t, 0≤t≤2π0 \le t \le 2\pi, about the xx-axis. Its distance to the axis is 2+sin⁡t>02 + \sin t > 0 and its speed is 11, so the torus has area

S=∫02π2π(2+sin⁡t) dt=2π⋅4π=8π2.S = \int_0^{2\pi} 2\pi (2 + \sin t)\, dt = 2\pi \cdot 4\pi = 8\pi^2.

Check yourself

  1. Find the length of x=etcos⁡tx = e^t \cos t, y=etsin⁡ty = e^t \sin t for 0≤t≤10 \le t \le 1.
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The derivatives are x′=et(cos⁡t−sin⁡t)x' = e^t(\cos t - \sin t) and y′=et(sin⁡t+cos⁡t)y' = e^t(\sin t + \cos t), so

x′2+y′2=e2t((cos⁡t−sin⁡t)2+(sin⁡t+cos⁡t)2)=2e2t.x'^2 + y'^2 = e^{2t}\left((\cos t - \sin t)^2 + (\sin t + \cos t)^2\right) = 2e^{2t}.

The length is

L=∫012 et dt=2(e−1)≈2.43.L = \int_0^1 \sqrt{2}\, e^t\, dt = \sqrt{2}(e - 1) \approx 2.43.
  1. Rotate the segment x=3tx = 3t, y=4ty = 4t, 0≤t≤10 \le t \le 1, about the xx-axis. Find the surface area.
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The speed is 55 and the distance to the axis is 4t4t, so

S=∫012π⋅4t⋅5 dt=20π.S = \int_0^1 2\pi \cdot 4t \cdot 5\, dt = 20\pi.

This is the side of a cone with radius 44 and slant height 55, and π⋅4⋅5=20π\pi \cdot 4 \cdot 5 = 20\pi.

  1. For x=cos⁡tx = \cos t, y=sin⁡ty = \sin t, what does the speed integral over 0≤t≤6π0 \le t \le 6\pi give, and what is the length of the circle?
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The integral is 6π6\pi, the distance travelled in three laps. The circle has length 2π2\pi.

How this lesson connects