Show that when \(\alpha\) is small, \(\cos(\theta + \alpha) - \cos\theta \approx -\alpha\sin\theta - \frac{1}{2}\alpha^2\cos\theta\).
Find the limit as \(\alpha \to 0\) of
\[ \frac{\sin(\theta+\alpha) - \sin\theta}{\cos(\theta+\alpha) - \cos\theta} \qquad (*) \]
in the case \(\sin\theta \neq 0\).
In the case \(\sin\theta = 0\), what happens to the value of expression \((*)\) when \(\alpha \to 0\)?
A circle \(C_1\) of radius \(a\) rolls without slipping in an anti-clockwise direction on a fixed circle \(C_2\) with centre at the origin \(O\) and radius \((n-1)a\), where \(n\) is an integer greater than \(2\). The point \(P\) is fixed on \(C_1\). Initially the centre of \(C_1\) is at \((na, 0)\) and \(P\) is at \(\big((n+1)a, 0\big)\).
Let \(Q\) be the point of contact of \(C_1\) and \(C_2\) at any time in the rolling motion. Show that when \(OQ\) makes an angle \(\theta\), measured anticlockwise, with the positive \(x\)-axis, the \(x\)-coordinate of \(P\) is \(x(\theta) = a(n\cos\theta + \cos n\theta)\), and find the corresponding expression for the \(y\)-coordinate, \(y(\theta)\), of \(P\).
Find the values of \(\theta\) for which the distance \(OP\) is \((n-1)a\).
Let \(\theta_0 = \dfrac{1}{n-1}\pi\). Find the limit as \(\alpha \to 0\) of
\[ \frac{y(\theta_0 + \alpha) - y(\theta_0)}{x(\theta_0 + \alpha) - x(\theta_0)}\,. \]
Hence show that, at the point \(\big(x(\theta_0),\, y(\theta_0)\big)\), the tangent to the curve traced out by \(P\) is parallel to \(OP\).
The curve \(C\) has equation
\[
y= a^{\sin (\pi \e^ x)}\,,
\]
where \(a>1\).
Find the coordinates of the stationary points on \(C\).
Use the approximations \(\e^t \approx 1+t\) and \(\sin t \approx t\)
(both valid for small values of \(t\))
to show that
\[
y\approx 1-\pi x \ln a \;
\]
for small values of \(x\).
Sketch \(C\).
By approximating \(C\) by means of straight lines joining consecutive
stationary points, show that the area between \(C\) and the \(x\)-axis
between the \(k\)th and \((k+1)\)th maxima is approximately
\[
\Big( \frac {a^2+1}{2a} \Big)
\ln \Big ( 1+ \big( k-\tfrac34)^{-1} \Big)\,.
\]
The lengths of the sides \(BC\), \(CA\), \(AB\) of the triangle
\(ABC\) are denoted by \(a\), \(b\), \(c\), respectively. Given that
$$
b = 8+{\epsilon}_1, \,
c=3+{\epsilon}_2,\,
A=\tfrac{1}{3}\pi + {\epsilon}_3,
$$
where \({\epsilon}_1\), \({\epsilon}_2\), and \( {\epsilon}_3\) are small, show that
\(a \approx 7 + {\eta}\), where
${\eta}= {\left(13 \, {{\epsilon}_1}-2\,{\epsilon}_2
+ 24{\sqrt 3} \;{{\epsilon}_3}\right)}/14$.
Given now that
$$
{\vert {\epsilon}_1} \vert
\le 2 \times 10^{-3}, \ \ \
{\vert {\epsilon}_2} \vert \le 4\cdot 9\times 10^{-2}, \ \ \
{\vert {\epsilon}_3} \vert \le \sqrt3 \times 10^{-3},
$$
find the range of possible values of \({\eta}\).
For this question, you may use the following
approximations, valid if \(\theta \) is small: \
\(\sin\theta \approx \theta\) and \(\cos\theta \approx 1-\theta^2/2\,\).
A satellite \(X\) is directly above the point \(Y\)
on the Earth's surface and can just be seen
(on the horizon) from
another point \(Z\) on the Earth's surface.
The radius of the Earth is \(R\) and the height of
the satellite above the Earth is \(h\).
Find the distance \(d\)
of \(Z\) from \(Y\) along the Earth's surface.
If the satellite is in low orbit (so that \(h\) is
small compared with \(R\)),
show that
$$d \approx k(Rh)^{1/2},$$ where \(k\) is to be found.
If the satellite is very distant from the Earth (so that \(R\) is small
compared with \(h\)), show that
$$d\approx aR+b(R^2/h),$$
where \(a\) and \(b\) are to be found.
Explain briefly, by means of a diagram, or otherwise, why
\[
\mathrm{f}(\theta+\delta\theta)\approx\mathrm{f}(\theta)+\mathrm{f}'(\theta)\delta\theta,
\]
when \(\delta\theta\) is small.
Two powerful telescopes are placed at points \(A\) and \(B\) which are
a distance \(a\) apart. A very distant point \(C\) is such that \(AC\)
makes an angle \(\theta\) with \(AB\) and \(BC\) makes an angle \(\theta+\phi\)
with \(AB\) produced. (A sketch of the arrangement is given in the
diagram.)
\noindent
If the perpendicular distance \(h\) of \(C\) from \(AB\) is very large
compared with \(a\) show that \(h\) is approximately \((a\sin^{2}\theta)/\phi\)
and find the approximate value of \(AC\) in terms of \(a,\theta\) and
\(\phi.\)
It is easy to show (but you are not asked to show it) that errors
in measuring \(\phi\) are much more important than errors in measuring
\(\theta.\) If we make an error of \(\delta\phi\) in measuring \(\phi\)
(but measure \(\theta\) correctly) what is the approximate error in
our estimate of \(AC\) and, roughly, in what proportion is it reduced
by doubling the distance between \(A\) and \(B\)?
First note that \(\displaystyle \lim_{x \to 0} \frac{\sin x}{x} \to 1\), then \(\frac1n\) is a sequence converging to zero, therefore \(\frac{\sin 1/n}{1/n}\) also must tend to \(1\).
Note that \(\lim_{x \to \infty} \tan^{-1} x = \frac{\pi}{2}\) and since \(n\) is a sequence tending to infinity we must have \(\lim_{n \to \infty} \tan^{-1} n = \frac{\pi}{2}\)
Show that
\[
\cos\left(\frac{\alpha}{2}\right)\cos\left(\frac{\alpha}{4}\right)=\frac{\sin\alpha}{4\sin\left(\dfrac{\alpha}{4}\right)}\,,
\]
where \(\alpha\neq k\pi\), \(k\) is an integer.
Prove that, for such \(\alpha\),
\[
\cos\left(\frac{\alpha}{2}\right)\cos\left(\frac{\alpha}{4}\right)\cdots\cos\left(\frac{\alpha}{2^{n}}\right)=\frac{\sin\alpha}{2^{n}\sin\left(\dfrac{\alpha}{2^{n}}\right)}\,,
\]
where \(n\) is a positive integer.
Deduce that
\[
\alpha=\frac{\sin\alpha}{\cos\left(\dfrac{\alpha}{2}\right)\cos\left(\dfrac{\alpha}{4}\right)\cos\left(\dfrac{\alpha}{8}\right)\cdots}\,,
\]
and hence that
\[
\frac{\pi}{2}=\frac{1}{\sqrt{\frac{1}{2}}\sqrt{\frac{1}{2}+\frac{1}{2}\sqrt{\frac{1}{2}}}\sqrt{\frac{1}{2}+\frac{1}{2}\sqrt{\frac{1}{2}+\frac{1}{2}\sqrt{\frac{1}{2}}}}\cdots}\,.
\]
\begin{align*}
&&\sin \alpha &= 2 \sin \frac{\alpha}{2} \cos \frac{\alpha}{2} \\
&&&= 4 \sin \frac{\alpha}{4} \cos \frac{\alpha}{4} \cos \frac{\alpha}{2} \\
\Rightarrow && \frac{\sin \alpha}{4 \sin \frac{\alpha}{4}} &= \cos \frac{\alpha}{2} \cos \frac{\alpha}{4}
\end{align*}
We proceed by induction on \(n\). Clearly this is true for \(n = 1\) (as we just established). Assume it is true for \(n=k\). Then:
\begin{align*}
&& \frac{\sin \alpha}{2^n \sin \frac{\alpha}{2^n}} &= \cos\left(\frac{\alpha}{2}\right)\cos\left(\frac{\alpha}{4}\right)\cdots\cos\left(\frac{\alpha}{2^{n}}\right) \\
\Rightarrow && \frac{\sin \alpha}{2^{n+1} \sin \frac{\alpha}{2^{n+1}} \cos \frac{\alpha}{2^{n+1}}} &= \cos\left(\frac{\alpha}{2}\right)\cos\left(\frac{\alpha}{4}\right)\cdots\cos\left(\frac{\alpha}{2^{n}}\right) \\
\Rightarrow && \frac{\sin \alpha}{2^{n+1} \sin \frac{\alpha}{2^{n+1}} } &= \cos\left(\frac{\alpha}{2}\right)\cos\left(\frac{\alpha}{4}\right)\cdots\cos\left(\frac{\alpha}{2^{n}}\right)\cos \left ( \frac{\alpha}{2^{n+1}} \right) \\
\end{align*}
Therefore it is true for \(n=k+1\) Therefore since it is true for \(n=1\) and if it is true for \(n=k\) it is also true for \(n=k+1\) by the principle of mathematical induction it is true for all \(n \geq 1\)
\begin{align*}
\lim_{n \to \infty} \frac{\sin \alpha}{\cos\left(\frac{\alpha}{2}\right)\cdots\cos\left(\frac{\alpha}{2^{n}}\right)} &= \lim_{n \to \infty} 2^n \sin \frac{\alpha}{2^n} \\
&= \lim_{n \to \infty} \alpha \frac{\sin \frac{\alpha}{2^n}}{\frac{\alpha}{2^n}} \\
&= \alpha \lim_{t \to 0} \frac{\sin t}{t} \\
&= \alpha
\end{align*}
When \(\alpha = \frac{\pi}{2}\) notice that \(\sin \alpha =1\), \(\cos \frac{\alpha}{2} = \sqrt{\frac12}\) and \(2\cos^2 \frac{\alpha}{2^{n+1}}-1 = \cos \frac{\alpha}{2} \Rightarrow \cos \frac{\alpha}{2^{n+1}} = \sqrt{\frac12 + \cos \frac{\alpha}{2^n}}\) exactly the series we see.
By considering the graphs of \(y=kx\) and \(y=\sin x,\) show that the
equation \(kx=\sin x,\) where \(k>0,\) may have \(0,1,2\) or \(3\) roots
in the interval \((4n+1)\frac{\pi}{2} < x < (4n+5)\frac{\pi}{2},\)
where \(n\) is a positive integer.
For a certain given value of \(n\), the equation has exactly one root
in this interval. Show that \(k\) lies in an interval which may be
written \(\sin\delta < k < \dfrac{2}{(4n+1)\pi},\) where \(0 < \delta < \frac{1}{2}\pi\)
and
\[
\cos\delta=\left((4n+5)\frac{\pi}{2}-\delta\right)\sin\delta.
\]
Show that, if \(n\) is large, then \(\delta\approx\dfrac{2}{(4n+5)\pi}\)
and obtain a second, improved, approximation.
Clearly we can achieve \(0\), \(1\), and \(2\) intersections by never entering the range, entering too flat, or entering before hitting the second branch. To achieve \(3\) we can go at a flat enough slope that we hit somewhere near the top of the second branch, and since the gradient there will be \(\approx 0\), and our gradient is positive, we must intersect before that point as well, ie \(3\) intersections. Clearly we cannot intersect the second branch \(3\) times or the first branch twice, therefore there are at most \(3\) intersections.
To intersect the graph only once, we need to:
be below \(((4n+1)\tfrac{\pi}{2}, 1)\) and
not touch the second gradient
The first condition means that \(k (4n+1)\tfrac{\pi}{2} < 1 \Rightarrow k < \frac{2}{(4n+1)\pi}\). For the second condition, consider a point on the curve \(\sin x\) whose tangent line goes through the origin, ie \(\frac{y - \sin t}{x - t} = \cos t \Rightarrow y = (\cos t)x - t \cos t+\sin t\) ie \(\sin t = t \cos t\). For this point \(t\) to be in the required interval, we need \((4n+5) \tfrac{\pi}{2} -t \in (0, \frac{\pi}{2})\), so let's call this value \(\delta\). Then our result is:
The gradient needs to be steeper than \(\cos t = \cos \left ( (4n+5) \tfrac{\pi}{2} - \delta \right) = \sin \delta\) and \(\cos \delta =\left ( (4n+5) \tfrac{\pi}{2} - \delta \right) \sin \delta \).
If \(n\) is large, then,
\begin{align*}
&& 1 &\approx \left ( (4n+5) \tfrac{\pi}{2} - \delta \right) \delta \\
\Rightarrow && 1 &\approx (4n+5) \tfrac{\pi}{2} \delta \\
\Rightarrow && \delta &\approx \frac{2}{(4n+5)\pi}
\end{align*}.
To higher order:
\begin{align*}
&& 1-\frac12 \delta^2 &\approx \left ( (4n+5) \tfrac{\pi}{2} - \delta \right) \delta \\
\Rightarrow && 1-\frac12 \delta^2 &\approx (4n+5) \tfrac{\pi}{2} \delta - \delta^2 \\
\Rightarrow && 0 &\approx 1 - (4n + 5)\tfrac{\pi}{2} \delta + \frac12 \delta^2 \\
\Rightarrow && \delta &\approx (4n+5) \tfrac{\pi}{2} - \sqrt{(4n+5)^2 \frac{\pi^2}{4} - 2} \\
&&&= \frac{2}{(4n+5) \tfrac{\pi}{2} + \sqrt{(4n+5)^2 \frac{\pi^2}{4} - 2}}
\end{align*}.