Length of Arc of Evolute equals Difference in Radii of Curvature
Theorem
Let $C$ be a curve defined by a real function which is twice differentiable.
Let the curvature of $C$ be non-constant.
The length of arc of the evolute $E$ of $C$ between any two points $Q_1$ and $Q_2$ of $C$ is equal to the difference between the radii of curvature at the corresponding points $P_1$ and $P_2$ of $C$.
Proof
Let $P = \tuple {x, y}$ be a general point on $C$.
Let $Q = \tuple {X, Y}$ be the center of curvature of $C$ at $P$.
From the above diagram:
- $(1): \quad \begin {cases} x - X = \pm \rho \sin \psi \\ Y - y = \pm \rho \cos \psi \end {cases}$
where:
- $\rho$ is the radius of curvature of $C$ at $P$
- $\psi$ is the angle between the tangent to $C$ at $P$ and the $x$-axis.
Whether the sign is plus or minus depends on whether the curve is convex or concave.
For simplicity, let it be assumed that the curvature $k$ at each point under consideration on $C$ is positive.
The case for $k < 0$ can then be treated similarly.
Thus we have $k > 0$ and so $(1)$ can be written:
- $(2): \quad \begin {cases} X = x - \rho \sin \psi \\ Y = y +\rho \cos \psi \end {cases}$
By definition of curvature:
- $k = \dfrac {\d \psi} {\d s}$
and:
- $\rho = \dfrac 1 k = \dfrac {\d s} {\d \psi}$
Hence:
\(\ds \rho \sin \psi\) | \(=\) | \(\ds \dfrac {\d s} {\d \psi} \dfrac {\d y} {\d s}\) | ||||||||||||
\(\text {(3)}: \quad\) | \(\ds \) | \(=\) | \(\ds \dfrac {\d y} {\d \psi}\) |
and:
\(\ds \rho \cos \psi\) | \(=\) | \(\ds \dfrac {\d s} {\d \psi} \dfrac {\d x} {\d s}\) | ||||||||||||
\(\text {(4)}: \quad\) | \(\ds \) | \(=\) | \(\ds \dfrac {\d x} {\d \psi}\) |
Differentiating $(2)$ with respect to $\psi$:
\(\ds \dfrac {\d X} {\d \psi}\) | \(=\) | \(\ds \dfrac {\d x} {\d \psi} - \rho \cos \psi - \dfrac {\d \rho} {\d \psi} \sin \psi\) | ||||||||||||
\(\text {(5)}: \quad\) | \(\ds \) | \(=\) | \(\ds - \dfrac {\d \rho} {\d \psi} \sin \psi\) | from $(3)$ |
and:
\(\ds \dfrac {\d Y} {\d \psi}\) | \(=\) | \(\ds \dfrac {\d y} {\d \psi} - \rho \sin \psi + \dfrac {\d \rho} {\d \psi} \cos \psi\) | ||||||||||||
\(\text {(6)}: \quad\) | \(\ds \) | \(=\) | \(\ds \dfrac {\d \rho} {\d \psi} \cos \psi\) | from $(4)$ |
Let $S$ be the length of arc of the evolute $E$ from a fixed point $Q_0$ on $E$ to the variable point $Q$ corresponding to $P$.
We have that:
- $\d S^2 = \d X^2 + \d Y^2$
and so:
\(\ds \paren {\dfrac {\d S} {\d \psi} }^2\) | \(=\) | \(\ds \paren {\dfrac {\d X} {\d \psi} }^2 + \paren {\dfrac {\d Y} {\d \psi} }^2\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \paren {- \dfrac {\d \rho} {\d \psi} \sin \psi}^2 + \paren {\dfrac {\d \rho} {\d \psi} \cos \psi}^2\) | from $(5)$ and $(6)$ | |||||||||||
\(\ds \) | \(=\) | \(\ds \paren {\dfrac {\d \rho} {\d \psi} }^2 \paren {\sin^2 \psi + \cos^2 \psi}\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \paren {\dfrac {\d \rho} {\d \psi} }^2\) | Sum of Squares of Sine and Cosine |
Choosing the direction of $S$ so that $S$ and $\rho$ increase together, this tells us:
- $\dfrac {\d S} {\d \psi} = \dfrac {\d \rho} {\d \psi}$
Integrating with respect to $\psi$ gives:
- $S = \rho + c$
where $c$ is a constant.
$\blacksquare$
Sources
- 1992: George F. Simmons: Calculus Gems ... (previous) ... (next): Chapter $\text {B}.23$: Evolutes and Involutes. The Evolute of a Cycloid