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Length of a Curve 📂Calculus

Length of a Curve

Length of a Plane Curve1

Buildup

1.PNG

Suppose we have a smooth function y=f(x)y=f(x) given as in figure (a) above, with n+1n+1 points on it. The total length ss of the curve can be obtained by summing up the lengths sks_{k} of each arc divided by points. Moreover, the length of each arc can be approximated by the length between two points as shown in figure (b). As the number of points increases, the sum of these approximated lengths will get closer to the actual length LL. Thus, we obtain the following equation.

L=limni=1nPi1Pi L = \lim \limits_{n \to \infty} \sum \limits_{i=1}^{n} \left| P_{i-1}P_{i} \right|

At this time, the length of each component is as follows, by the Pythagorean theorem.

Pi1Pi=(xixi1)2+(yiyi1)2=(Δxi)2+(Δyi)2 \left| P_{i-1}P_{i} \right| = \sqrt{(x_{i} - x_{i-1})^{2} + (y_{i} - y_{i-1})^{2}} = \left( \Delta x_{i} \right)^{2} + \left( \Delta y_{i} \right)^{2}

Furthermore, by the mean value theorem, we can know that there exists xi(xi1,xi)x_{i}^{\ast} \in (x_{i-1}, x_{i}) for which the following equation holds.

f(xi)f(xi1)= f(xi)(xixi1)Δyi= f(xi)Δxi \begin{align*} f(x_{i}) - f(x_{i-1}) =&\ f^{\prime} (x_{i}^{\ast}) \left( x_{i} - x_{i-1} \right) \\ \Delta y_{i} =&\ f^{\prime} (x_{i}^{\ast}) \Delta x_{i} \end{align*}

Therefore, the length of each segment is as follows.

Pi1Pi= (Δxi)2+(Δyi)2= (Δxi)2+[f(xi)]2(Δxi)2= 1+[f(xi)]2Δxi \begin{align*} \left| P_{i-1}P_{i} \right| =&\ \left( \Delta x_{i} \right)^{2} + \left( \Delta y_{i} \right)^{2} \\ =&\ \left( \Delta x_{i} \right)^{2} + \left[ f^{\prime} (x_{i}^{\ast}) \right]^{2} \left( \Delta x_{i} \right)^{2} \\ =&\ \sqrt{1 + \left[ f^{\prime} (x_{i}^{\ast}) \right]^{2}} \Delta x_{i} \end{align*}

Then, the length of the curve LL is as follows.

L=limni=1nPi1Pi=limni=1n1+[f(xi)]2Δxi L = \lim \limits_{n \to \infty} \sum \limits_{i=1}^{n} \left| P_{i-1}P_{i} \right| = \lim \limits_{n \to \infty} \sum \limits_{i=1}^{n} \sqrt{1 + \left[ f^{\prime} (x_{i}^{\ast}) \right]^{2}} \Delta x_{i}

Since 1+[f(x)]2\sqrt{1 + \left[ f^{\prime} (x) \right]^{2}} is continuous, the limit of the Riemann sum exists and it is integrable. Therefore, the length of the curve is defined as follows.

Definition

If ff^{\prime} is continuous at [a,b][a,b](If ff is a smooth function), the length LL of the curve y=f(x)y=f(x) is defined as follows.

L:=ab1+[f(x)]2dx=ab1+(dydx)2dx L := \int_{a}^{b} \sqrt{1 + \left[ f^{\prime} (x) \right]^{2}} dx = \int_{a}^{b} \sqrt{1 + \left( \dfrac{d y}{d x} \right)^{2}} dx

From this, the arc length function, which represents the length of the curve from the starting point P0(a,f(a))P_{0}(a, f(a)) to the point Q(x,f(x))Q(x,f(x)), is naturally defined as follows.

s(x)=ax1+[f(t)]2dt s(x) = \int_{a}^{x} \sqrt{1 + \left[ f^{\prime} (t) \right]^{2}} dt

Therefore, dsdx=1+[f(x)]2=1+(dydx)2\dfrac{d s}{d x} = \sqrt{1 + [f^{\prime}(x)]^{2}} = \sqrt{1 + \left( \dfrac{d y}{d x} \right)^{2}} holds, and the length of the curve can be indicated as follows.

L=Cds=ab1+(dydx)2dx L = \int_{C} ds = \int_{a}^{b} \sqrt{1 + \left( \dfrac{d y}{d x} \right)^{2}} dx

Theorem

Suppose curve CC is represented by the parametric equation x=f(t),y=g(t),αtβx = f(t), y=g(t), \alpha \le t \le \beta. If f,gf^{\prime}, g^{\prime} is continuous at [α,β][\alpha, \beta](If f,gf, g is a smooth function), the length of curve CC is as follows.

L=αβ(dxdt)2+(dydt)2dt L = \int_{\alpha}^{\beta} \sqrt{\left( \dfrac{d x}{d t} \right)^{2} + \left( \dfrac{d y}{d t} \right)^{2}} dt

Proof

Let’s assume a=x(α),b=x(β)a = x(\alpha), b = x(\beta). By assumption, dydx=dydtdxdt\dfrac{d y}{d x} = \dfrac{\dfrac{d y}{d t}}{\dfrac{d x}{d t}} holds. Therefore,

L=ab1+(dydx)2dx=αβ1+(dydtdxdt)2dxdtdt=αβ(dxdt)2+(dydt)2dt L = \int_{a}^{b} \sqrt{1 + \left( \dfrac{d y}{d x} \right)^{2}} dx = \int_{\alpha}^{\beta} \sqrt{1 + \left(\dfrac{\dfrac{d y}{d t}}{\dfrac{d x}{d t}} \right)^{2}} \dfrac{d x}{d t} dt = \int_{\alpha}^{\beta} \sqrt{\left(\dfrac{d x}{d t}\right)^{2} + \left(\dfrac{d y}{d t}\right)^{2}}dt

Length of a Space Curve2

Similarly to the buildup above, when a curve in a 3-dimensional space is expressed as r(t)=(f(t),g(t),h(t))\mathbf{r}(t) = \left( f(t), g(t), h(t) \right), the length of the curve is defined as follows.

L= ab[f(t)]2+[g(t)]2+[h(t)]2dt= ab(dxdt)2+(dydt)2+(dzdt)2dt= abr(t)dt \begin{align*} L =&\ \int_{a}^{b} \sqrt{\left[ f^{\prime}(t) \right]^{2} + \left[ g^{\prime}(t) \right]^{2} + \left[ h^{\prime}(t) \right]^{2}} dt \\ =&\ \int_{a}^{b} \sqrt{ \left( \dfrac{d x}{d t} \right)^{2} + \left( \dfrac{d y}{d t} \right)^{2} + \left( \dfrac{d z}{d t} \right)^{2} } dt \\ =&\ \int_{a}^{b} \left| \mathbf{r}^{\prime}(t) \right| dt \end{align*}

Likewise, the arc length function is as follows.

s(t)=atr(u)du=at(dxdu)2+(dydu)2+(dzdu)2du s(t) = \int_{a}^{t} \left| \mathbf{r}^{\prime}(u) \right| du = \int_{a}^{t} \sqrt{ \left( \dfrac{d x}{d u} \right)^{2} + \left( \dfrac{d y}{d u} \right)^{2} + \left( \dfrac{d z}{d u} \right)^{2} } du


  1. James Stewart, Daniel Clegg, and Saleem Watson, Calculus (early transcendentals, 9E), p547-551, 663-664 ↩︎

  2. James Stewart, Daniel Clegg, and Saleem Watson, Calculus (early transcendentals, 9E), p862-863 ↩︎