Subsection 1.8.1 Arc Length
Consider a smooth curve in 3-space that is parametrically described by the vector-valued function
\(\vr\) defined by
\(\vr(t) = \langle x(t), y(t), z(t)
\rangle.\) Preview Activity 1.8.1 shows that to approximate the length of the curve defined by
\(\vr(t)\) as the values of
\(t\) run over an interval
\([a,b]\text{,}\) we partition the interval
\([a,b]\) into
\(n\) subintervals of equal length
\(\Delta t\text{,}\) with
\(a = t_0 \lt t_1 \lt \cdots
\lt t_n = b\) as the endpoints of the subintervals. On each subinterval, we approximate the length of the curve by the length of the line segment connecting the endpoints. The points on the curve corresponding to
\(t = t_{i-1}\) and
\(t = t_i\) are
\((x(t_{i-1}),
y(t_{i-1}), z(t_{i-1}))\) and
\((x(t_i), y(t_i), z(t_i))\text{,}\) respectively, so the length of the line segment connecting these points is
\begin{equation*}
\sqrt{(x(t_i) - x(t_{i-1}))^2 + (y(t_i) - y(t_{i-1}))^2 + (z(t_i) -
z(t_{i-1}))^2}.
\end{equation*}
Now we add all of these approximations together to obtain an approximation to the length \(L\) of the curve:
\begin{equation*}
L \approx \sum_{i=1}^n \sqrt{(x(t_i) - x(t_{i-1}))^2 + (y(t_i) -
y(t_{i-1}))^2 + (z(t_i) - z(t_{i-1}))^2}.
\end{equation*}
We now want to take the limit of this sum as \(n\) goes to infinity, but in its present form it might be difficult to see how. We first introduce \(\Delta t\) by multiplying by \(\frac{\Delta t}{\Delta t}\text{,}\) and see that
\begin{align*}
L \amp \approx \sum_{i=1}^n \sqrt{(x(t_i) - x(t_{i-1}))^2 + (y(t_i) - y(t_{i-1}))^2 + (z(t_i) - z(t_{i-1}))^2}\\
\amp = \sum_{i=1}^n \sqrt{(x(t_i) - x(t_{i-1}))^2 + (y(t_i) - y(t_{i-1}))^2 + (z(t_i) - z(t_{i-1}))^2} \frac{\Delta t}{\Delta t}\\
\amp = \sum_{i=1}^n \sqrt{(x(t_i) - x(t_{i-1}))^2 + (y(t_i) - y(t_{i-1}))^2 + (z(t_i) - z(t_{i-1}))^2} \frac{\Delta t}{\sqrt{(\Delta t)^2}}
\end{align*}
To get the difference quotients under the radical, we use properties of the square root function to see further that
\begin{align*}
L \amp \approx \sum_{i=1}^n \sqrt{\left[(x(t_i) - x(t_{i-1}))^2 + (y(t_i) - y(t_{i-1}))^2 + (z(t_i) - z(t_{i-1})^2\right] \frac{1}{(\Delta t)^2}} \Delta t\\
\amp = \sum_{i=1}^n \sqrt{\left(\frac{x(t_i) - x(t_{i-1})}{\Delta t}\right)^2 + \left(\frac{y(t_i) - y(t_{i-1})}{\Delta t}\right)^2 + \left(\frac{z(t_i) - z(t_{i-1})}{\Delta t}\right)^2} \Delta t.
\end{align*}
Recall that as \(n \to \infty\) we also have \(\Delta t \to 0\text{.}\) Since
\begin{align*}
x'(t) \amp = \lim_{\Delta t \to 0} \frac{x(t_i) - x(t_{i-1})}{\Delta t},\\
y'(t) \amp = \lim_{\Delta t \to 0} \frac{y(t_i) - y(t_{i-1})}{\Delta t}, \ \text{ and } \\
z'(t) \amp \lim_{\Delta t \to 0} \frac{z(t_i) - z(t_{i-1})}{\Delta t},
\end{align*}
we see that
\begin{equation*}
\lim_{n \to \infty} \sum_{i=1}^n \sqrt{\left(\frac{x(t_i) - x(t_{i-1})}{\Delta t}\right)^2 + \left(\frac{y(t_i) - y(t_{i-1})}{\Delta t}\right)^2 + \left(\frac{z(t_i) - z(t_{i-1})}{\Delta t}\right)^2} \Delta t
\end{equation*}
is equal to
\begin{equation*}
\int_a^b \sqrt{(x'(t))^2 + (y'(t))^2 + (z'(t))^2} \, dt.
\end{equation*}
Noting further that
\begin{equation*}
|\vr'(t)| = \sqrt{(x'(t))^2 + (y'(t))^2 + (z'(t))^2},
\end{equation*}
we can rewrite our arclength formula in a more succinct form as follows.
The length of a curve.
If \(\vr(t)\) defines a smooth curve \(C\) on an interval \([a,b]\text{,}\) then the length \(L\) of \(C\) is given by
\begin{equation}
L = \int_a^b |\vr'(t)| \, dt.\tag{1.8.1}
\end{equation}
Note that formula
(1.8.1) applies to curves in any dimensional space. Moreover, this formula has a natural interpretation: if
\(\vr(t)\) records the position of a moving object, then
\(\vr'(t)\) is the object’s velocity and
\(|\vr'(t)|\) its speed. Formula
(1.8.1) says that we simply integrate the speed of an object traveling over the curve to find the distance traveled by the object, which is the same as the length of the curve, just as in one-variable calculus.
Activity 1.8.2.
Here we calculate the arc length of two familiar curves.
-
Use Equation
(1.8.1) to calculate the circumference of a circle of radius
\(r\text{.}\)
-
Find the exact length of the spiral defined by
\(\vr(t) = \langle \cos(t), \sin(t), t \rangle\) on the interval
\([0,2\pi]\text{.}\)
We can adapt the arc length formula to curves in 2-space that define
\(y\) as a function of
\(x\) as the following activity shows.
Activity 1.8.3.
Let
\(y = f(x)\) define a smooth curve in 2-space. Parameterize this curve and use Equation
(1.8.1) to show that the length of the curve defined by
\(f\) on an interval
\([a,b]\) is
\begin{equation*}
\int_a^b \sqrt{1+[f'(t)]^2} \, dt.
\end{equation*}