Mathematics · Glossary

What is Arc length?

Also known as: arc-length function

Definition 18.6 University Mathematics — Year 2 · Chapter 18 — Curves

Let γ ⁣:[a,b]Rn\gamma \colon [a, b] \to \R^n be a C1\mathcal{C}^1 arc. Its length is

L(γ)=abγ(t) ⁣dt,L(\gamma) = \int_a^b \norm{\gamma'(t)}\, \dd t ,

where \norm{\cdot} is the Euclidean norm. The arc-length function based at t0t_0 is s(t)=t0tγ(u) ⁣dus(t) = \int_{t_0}^t \norm{\gamma'(u)}\,\dd u.

Examples

Example 18.8 (Archimedes and the inscribed polygons)

For the unit circle, the inscribed regular nn-gon has length Ln=2nsinπnL_n = 2n\sin\frac\pi n, and the expansion sinx=xx36+O(x5)\sin x = x - \frac{x^3}6 + O(x^5) gives

Ln=2ππ33n2+O(1n4):L_n = 2\pi - \frac{\pi^3}{3n^2} + O\Bigl(\frac1{n^4}\Bigr) :

the polygonal lengths of Theorem 18.7 converge quadratically. Numerically: L6=6L_6 = 6 (the hexagon, giving the crude π>3\pi > 3), while L96=192sinπ966.28206L_{96} = 192\sin\frac{\pi}{96} \approx 6.28206 against 2π6.283192\pi \approx 6.28319 — the error 0.001130.00113 agrees with the predicted π3/(3962)0.00112\pi^3/(3\cdot96^2) \approx 0.00112. This is why Archimedes, doubling the hexagon five times to 9696 sides, could bracket π\pi to three digits by hand: each doubling divides the error by four. The supremum in the polygonal characterization is not just attained in the limit; it is attained fast, because a smooth curve separates from its chords only at second order.

Example 18.11 (Circle and helix)

For the circle γ(t)=(Rcost,Rsint)\gamma(t) = (R\cos t, R\sin t), γ=R\norm{\gamma'} = R, so s=Rts = Rt and the length of a full turn is 2πR2\pi R. For the helix γ(t)=(acost, asint, bt)\gamma(t) = (a\cos t,\ a\sin t,\ bt) with a>0a > 0, γ(t)=a2+b2\norm{\gamma'(t)} = \sqrt{a^2 + b^2} is constant: the helix is traversed at constant speed, and s=ta2+b2s = t\sqrt{a^2 + b^2}.

Example 18.12 (Arc length in polar coordinates)

A polar curve r=r(θ)r = r(\theta) is the arc γ(θ)=(rcosθ, rsinθ)\gamma(\theta) = (r\cos\theta,\ r\sin\theta), with

γ(θ)=(rcosθrsinθ, rsinθ+rcosθ),γ(θ)2=r2+r2\gamma'(\theta) = (r'\cos\theta - r\sin\theta,\ r'\sin\theta + r\cos\theta), \qquad \norm{\gamma'(\theta)}^2 = r'^2 + r^2

(the cross terms cancel): the polar length element is r2+r2 ⁣dθ\sqrt{r^2 + r'^2}\,\dd\theta. For the cardioid r=1+cosθr = 1 + \cos\theta:

r2+r2=(1+cosθ)2+sin2θ=2+2cosθ=4cos2θ2,r^2 + r'^2 = (1 + \cos\theta)^2 + \sin^2\theta = 2 + 2\cos\theta = 4\cos^2\tfrac\theta2,

and on [π,π]\intcc{-\pi}{\pi} the half-angle cosine is nonnegative, so

L=ππ2cosθ2 ⁣dθ=[4sinθ2]ππ=4(4)=8:L = \int_{-\pi}^{\pi}2\cos\tfrac\theta2\,\dd\theta = \Bigl[4\sin\tfrac\theta2\Bigr]_{-\pi}^{\pi} = 4 - (-4) = 8 :

like the cycloid arch of Exercise 18.1, a curve built from circles has a rational length, with no π\pi anywhere. The half-angle factorization is the standard trick for lengths of circle-generated curves; when it fails (the ellipse), the length is a genuinely new function — an elliptic integral, beyond elementary closed forms.

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