- Calculus, Volume 2: Multi-Variable Calculus and Linear Algebra with Applications to Differential Equations and Probability
- Tom M. Apostol
- Second Edition
- 1991
- 978-1-119-49676-2
1.13 Exercises
-
In the real linear space $C(-1, 1)$, let $(f, g) = \int_{-1}^1 f(t) g(t) \, dt$. Consider the three functions $u_1, u_2, u_3$ given by
$$u_1(t) = 1, \quad u_2(t) = t, \quad u_3(t) = 1 + t.$$
Prove that two of them are orthogonal, two make an angle $\pi/3$ with each other, and two make an angle $\pi/6$ with each other.
-
Recall from Section 11:
$1. \quad$For an element $x$ in a Euclidean space $V$ with inner product $(x, x),$ the nonnegative number $\|x\| = (x, x)^{1/2}$ is called the norm of $x.$
$2.\quad$ In a real Euclidean space $V,$ the angle between two nonzero elements $x$ and $y$ is defined to be that number $\theta$ in the interval $0 \leq \theta \leq \pi$ which satisfies the equation
\begin{align*}
\cos \theta &= \frac{(x, y)}{\|x\|\|y\|}.
\end{align*}
-
$\quad 1. \quad u_1$ and $u_2$ are orthogonal.
$\quad 2. \quad u_1$ and $u_3$ form angle $\pi/6.$
$\quad 3. \quad u_2$ and $u_3$ form angle $\pi/3.$
Proof.$\quad (u_1, u_2)$ is given by
\begin{align*}
(u_1, u_2) &= \int_{-1}^{1}u_1(t)u_2(t)\,dt
\\
&= \int_{-1}^{1}t\,dt
\\
&= \frac{t^2}{2}\Biggr|_{-1}^{1}
\\
&= 0.
\end{align*}
So by definition, $u_1$ and $u_2$ are orthogonal. $\quad \blacksquare$
To find the elements that make an angle of $\pi/3$ and $\pi/6$ with one-another, we first note that as a result of the Cauchy-Schwarz inequality, the angles $\pi/3$ and $\pi/6$ are the only values in the interval $[0, \pi]$ whose cosines are $1/2$ and $\sqrt{3}/2,$ respectively.
To calculate the cosine of the angle between $u_1$ and $u_3,$ we first find the inner product of the two elements:
\begin{align*}
(u_1, u_3) &= \int_{-1}^{1}1 + t\,dt
\\
&= t + \frac{t^2}{2}\,\Biggr|_{-1}^1
\\
&= 2
\end{align*}
Then, we calculate the norms $\|u_1\|$ and $\|u_3\|:$
\begin{align*}
\|u_1\| &= (u_1, u_1)^{1/2}
\\
&=\left(\int_{-1}^{1}\,dt\right)^{1/2}
\\
&= \left(t\,|_{-1}^1\right)^{1/2}
\\
&= \sqrt{2}
\\
\\
\|u_3\| &= (u_3, u_3)^{1/2}
\\
&=\left(\int_{-1}^{1}1 + 2t + t^2\,dt\right)^{1/2}
\\
&= \left(t + t^2 + \frac{t^3}{3}\,\biggr|_{-1}^1\right)^{1/2}
\\
&= \left(2 + \frac{2}{3}\right)^{1/2}
\\
&= \frac{2\sqrt{2}}{\sqrt{3}}
\end{align*}
Combining these values, we get the cosine of the angle $\theta$ between $u_1$ and $u_3:$
\begin{align*}
\cos \theta &= \frac{(u_1, u_3)}{\|u_1\|\|u_3\|}
\\
&= \frac{2}{4/\sqrt{3}}
\\
&= \frac{\sqrt{3}}{2}
\end{align*}
As noted previously, $\pi/6$ is the only angle in the interval $[0, \pi]$ with cosine $\sqrt{3}/2.$ Thus, we can conclude that $u_1$ and $u_3$ make an angle of $\pi/6. \quad \blacksquare$
To calculate the cosine of the angle between $u_2$ and $u_3,$ we first find the inner product of the two elements:
\begin{align*}
(u_2, u_3) &= \int_{-1}^{1}t + t^2\,dt
\\
&= \frac{t^2}{2} + \frac{t^3}{3}\,\Biggr|_{-1}^1
\\
&= \frac{2}{3}
\end{align*}
Then, we calculate the norms $\|u_2\|$ and $\|u_3\|:$
\begin{align*}
\|u_2\| &= (u_2, u_2)^{1/2}
\\
&=\left(\int_{-1}^{1}t^2\,dt\right)^{1/2}
\\
&= \left(\frac{t^3}{3}\,\biggr|_{-1}^1\right)^{1/2}
\\
&= \frac{\sqrt{2}}{\sqrt{3}}
\\
\\
\|u_3\| &= (u_3, u_3)^{1/2}
\\
&=\left(\int_{-1}^{1}1 + 2t + t^2\,dt\right)^{1/2}
\\
&= \left(t + t^2 + \frac{t^3}{3}\,\biggr|_{-1}^1\right)^{1/2}
\\
&= \left(2 + \frac{2}{3}\right)^{1/2}
\\
&= \frac{2\sqrt{2}}{\sqrt{3}}
\end{align*}
Combining these values, we get the cosine of the angle $\theta$ between $u_2$ and $u_3:$
\begin{align*}
\cos \theta &= \frac{(u_2, u_3)}{\|u_1\|\|u_3\|}
\\
&= \frac{(2/3)}{(4/3)}
\\
&= \frac{1}{2}
\end{align*}
And as noted previously, $\pi/3$ is the only angle in the interval $[0, \pi]$ with cosine $1/2.$ As such, we can conclude that $u_2$ and $u_3$ make an angle of $\pi/3.\quad \blacksquare$
This completes the proof.