- Calculus, Volume 1: One Variable Calculus, with an Introduction to Linear Algebra
- Tom M. Apostol
- Second Edition
- 1967
- 978-1-119-49673-1
14.15 Exercises
-
A particle moves along a plane curve with constant speed 2. The motion starts at the origin when $t = 0$ and the initial velocity $\mathbf{v}(0)$ is $2\,\mathbf{i}.$ At every instant it is known that the curvature $\kappa(t) = 4t.$ Find the velocity $\mathbf{v}(t)$ when $t = \frac{1}{4}\sqrt{\pi}$ if the curve never goes below the $x$-axis.
-
Use the same setup as Exercise 11, but note this time that the starting angle is $0$ and that the particle moves away from the $x$-axis. What does this imply about the angle of inclination $\alpha(t)$ in relation to the curvature?
-
As discussed in Example 2 of Section 14.14, the angle of inclination $\alpha(t)$ between the tangent vector and the positive $x$-axis is related to curvature as follows:
$$
\begin{align*}
\\
\kappa(t) &= \left|\frac{d\alpha}{ds}\right|
\end{align*}
$$
Using the chain rule, noting that $v(t) = ds/dt,$ we can deduce that
$$
\begin{align*}
\\
|\alpha'(t)| &= \left|\frac{d\alpha}{dt}\right|
\\
&= \left|\frac{d\alpha}{ds}\right|\frac{ds}{dt}
\\
&= \left|\frac{d\alpha}{ds}\right|v(t)
\\
&= \kappa(t)v(t)
\end{align*}
$$
Given that the velocity has a starting angle of $0$ and that the particle never crosses the $x$-axis, this implies that the angle of inclination always moves towards $\pi/2.$ In other words, $\alpha'(t) = \kappa(t)v(t).$
Plugging in our values for speed and curvature, and noting that the starting angle is $0,$ we can express the angle of inclination explicitly as a function of $t$ by integrating its derivative from $0$ to $t$
$$
\begin{align*}
\\
\alpha(t) &= \int_0^t \alpha'(u)\,du
\\
\\
&=\int_0^t 8u\,du
\\
\\
&= 4u^2\Biggr|_0^t
\\
&= 4t^2
\end{align*}
$$
Then, we recall from Section 14.8 that the unit tangent $T(t)$ can be expressed in terms of the angle of inclination as follows:
$$
\begin{align*}
\\
T(t) &= \cos\alpha(t)\mathbf{i} + \sin\alpha(t)\mathbf{j}
\end{align*}
$$
In other words:
$$
\begin{align*}
\\
T(t) &= \cos \left(4t^2\right)\mathbf{i} + \sin\left(4t^2\right)\mathbf{j}
\end{align*}
$$
Multiplying by speed gives us the velocity in terms of $\mathbf{i}$ and $\mathbf{j}$
$$
\begin{align*}
\\
\mathbf{v}(t) &= 2\cos \left(4t^2\right)\mathbf{i} + 2\sin\left(4t^2\right)\mathbf{j}
\end{align*}
$$
Evaluating at time $t = \frac{1}{4}\sqrt{\pi}$
$$
\begin{align*}
\\
\mathbf{v}\left(\frac{1}{4}\sqrt{\pi}\right) &= 2\cos \left(\frac{\pi}{4}\right)\mathbf{i} + 2\sin\left(\frac{\pi}{4}\right)\mathbf{j}
\\
&= \sqrt{2}\,\mathbf{i} + \sqrt{2}\,\mathbf{j}
\quad
\blacksquare
\end{align*}
$$