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Mathematics · 术语表

什么是 Arc length?

又称: arc-length function

Definition 18.6 University Mathematics — Year 2 · 第 18 章 — 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)=∫ab∥γ′(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)=∫t0t∥γ′(u)∥  ⁣dus(t) = \int_{t_0}^t \norm{\gamma'(u)}\,\dd u.

示例

Example 18.8 (Archimedes and the inscribed polygons)

For the unit circle, the inscribed regular nn-gon has length Ln=2nsin⁡πnL_n = 2n\sin\frac\pi n, and the expansion sin⁡x=x−x36+O(x5)\sin x = x - \frac{x^3}6 + O(x^5) gives

Ln=2π−π33n2+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=192sin⁡π96≈6.28206L_{96} = 192\sin\frac{\pi}{96} \approx 6.28206 against 2π≈6.283192\pi \approx 6.28319 — the error 0.001130.00113 agrees with the predicted π3/(3⋅962)≈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)=(Rcos⁡t,Rsin⁡t)\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)=(acos⁡t, asin⁡t, 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)=(rcos⁡θ, rsin⁡θ)\gamma(\theta) = (r\cos\theta,\ r\sin\theta), with

γ′(θ)=(r′cos⁡θ−rsin⁡θ, r′sin⁡θ+rcos⁡θ),∥γ′(θ)∥2=r′2+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+r′2  ⁣dθ\sqrt{r^2 + r'^2}\,\dd\theta. For the cardioid r=1+cos⁡θr = 1 + \cos\theta:

r2+r′2=(1+cos⁡θ)2+sin⁡2θ=2+2cos⁡θ=4cos⁡2θ2,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=∫−ππ2cos⁡θ2  ⁣dθ=[4sin⁡θ2]−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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