\documentclass[12pt]{report} \usepackage{palatino}\usepackage{epsfig}\pagestyle{empty} %%% this results in no pagenumbers (footer is empty}\addtolength{\oddsidemargin}{-1.0in}\addtolength{\evensidemargin}{-1.0in}\addtolength{\textwidth}{1.5in}\addtolength{\topmargin}{-0.5in}\addtolength{\textheight}{1.0in}\baselineskip=20pt\newcommand{\dsps}{\displaystyle}\newcommand{\pp}{\par \noindent}\newcommand{\newp}{\vfil \eject}%\newcommand{\newp}{\bigskip}\begin{document}\noindent\vfil \noindent\large\hfil Math 126 C - Winter 2006 \hfil \pp\hfil Mid-Term Exam Number Two\hfil  \pp\hfil Solutions \hfil \pp\hfil February 16, 2006 \hfil \pp\normalsize\begin{enumerate}\item {\textit{Eliminate the parameter in the following parametric equation pairto get a Cartesian equation for the curve that involves no trigonometric functions.}}\[x = \cos t, y = \sin t - \cos t\]There are many different ways to solve this.  Here's one:We know \[\sin^2 t + \cos^2 t = 1\]and\[\cos t = x\]and \[\sin t = y + \cos t = y + x\]so that\[(y+x)^2 +x^2 = 1\]and we're done.Here's another way: notice that we can write\[\sin t = \pm \sqrt{1-\cos^2 t} = \pm \sqrt{1- x^2}\]so that \[y = \pm \sqrt{1-x^2} - x.\]\item {\textit{Consider the curve defined parametrically by the parametric equations}}\[x = \ln \ln t, y = \ln t - (\ln t)^2.\]{\textit{Find the equation of the tangent line to the curve at thepoint $t=e$.}}If $t=e$ then $x=0$, and $y=0$. We have\[\frac{dx}{dt} = \frac{1}{t \ln t} = \frac{1}{e}\]when $t=e$,and\[\frac{dy}{dt} = \frac{1}{t} - 2 \left( \ln t \right) \frac{1}{t} = \frac{1}{e} - \frac{2}{e} = -\frac{1}{e}\]when $t=e$.Thus, when $t=e$,\[\frac{dy}{dx} = \frac{\frac{dy}{dt}}{\frac{dx}{dt}} = -1\]so the tangent line has equation $y=-x$.%\item Find all points of intersection between the curve defined by the%polar equation %\[%r = 4 \csc \theta%\]%and the line $y=x$.  %\newp%\item Find the unit tangent vector $\vec{T}(t)$ at the point given by%$\dsps t=\frac{\pi}{2}$ on the curve defined by the vector function%\[%\vec{r}(t) = 3 \sin t \vec{i} + 5 \cos t \vec{j} + 7 \sin^2 t \vec{k}%\]%\vfil\item {\textit{Find the parametric equations for the tangent line to thecurve defined by\[x = t^3-t, y = t^6+t^2+1, z = \frac{1}{2}t^2+5t\]at the point $(0,1,0)$.}}We find \[\frac{dx}{dt} = 3t^2-1\]\[\frac{dy}{dt} = 6t^5+2t\]\[\frac{dz}{dt} = t+5\]The point $(0,1,0)$ corresponds to $t=0$.  To see this, note that we need\[t^3-t=0\]which tells us\[t(t^2-1)=0\]so we know $t=0$, $t=1$ or $t=-1$.  Checking these values with$y=t^6+t^2+1$, we find that only $t=0$ works.Plugging $t=0$ into the derivatives above, and using the point $(0,1,0)$, we have the tangent line equations\[x = -t, y=1, z = 5t.\]\item {\textit{At what point does the curve $y=e^x$ have maximum curvature?}}We have a formula to find the curvature function $\kappa(x)$ for the graph of a given function $f(x)=e^x$:\[\kappa(x) = \frac{|f''(x)|}{(1+(f'(x))^2)^{3/2}}= \frac{e^x}{(1+e^{2x})^{3/2}}\]Note that we have used the fact that $e^x>0$ for all $x$ to remove theabsolute value symbol.Now we want to find out how large this function $\kappa(x)$ can get.We can start our search for maxima of this function be studying the function's first derivative.\[\kappa'(x) = \frac{e^x (1+e^{2x})^{3/2} - e^x \frac{3}{2}(1+e^{2x})^{1/2}2x}{(1+e^{2x})^3}\]\[=\frac{e^x(1+e^{2x})^{1/2}\left( (1+e^{2x}) - 3e^{2x} \right)}{(1+e^{2x})^3}=\frac{e^x(1+e^{2x})^{1/2}(1-2e^{2x})}{(1+e^{2x})^3}\]We note that this is defined for all $x$, so the only critical points will occurwhere this is zero.  If this is zero, then\[1-2e^{2x}=0\]since $e^x>0$ for all $x$, and $(1+e^{2x})^{1/2}>0$ for all $x$.Hence, the only critical point is at\[x = \frac{1}{2}\ln \frac{1}{2}.\]Since $2e^{2x}$ is a strictly increasing function, we can see that that $\kappa'(x)$ is going to be negative for $x$ greater than the valuewe just found, and it will be positive for $x$ less than that value.In other words, we can conclude that this value of $x$ gives us themaximum value of $\kappa(x)$.The point on the curve where curvature is maximum is thus\[\left( \frac{1}{2}\ln \frac{1}{2}, \frac{1}{\sqrt{2}} \right)\]\item Find the length of the curve defined by\[\vec{r}(t) = \left\langle \frac{2\sqrt{2}}{3} t^{3/2},t, \frac{1}{2}t^2 \right\rangle,0 \le t \le 4\]Conveniently,\[\left(\frac{d}{dt} \frac{2\sqrt{2}}{3} t^{3/2}\right)^2+\left(\frac{d}{dt}t\right)^2+\left(\frac{d}{dt}\frac{1}{2}t^2\right)^2= (t+1)^2\]so the arc length is just\[\int_0^4 (t+1) \, dt = 12.\]\item {\textit{Find the curvature of the curve defined by\[\vec{r}(t) = \left\langle \frac{1}{2}t^2-2t,t^2-t,t^2+t \right\rangle\]at the point $t=0$.}}We have two useful formulas for finding the curvature of a 3D curve.  One is\[\kappa(t) = \frac{|\vec{T}'(t)|}{|r'(t)|}\]and the other is\[\kappa(t) = \frac{|\vec{r}\,'(t) \times \vec{r}\,''(t)}{|\vec{r}\,'(t)|^3}\]For this problem, the second equation is {\textbf{much}} easier to use.I really can't think of a time when it would be preferable to use the first one,expect in that rare occasion where you are given $\vec{T}'(t)$ anddon't have to derive it from $\vec{r}(t)$.So we use the second formula.  Since we are interested in $\kappa(0)$,we need only find $\vec{r}\,'(0)$ and $\vec{r}\,''(0)$ and plug them intothe formula:\[\vec{r}\,'(t) = \langle t-2,2t-1,2t+1 \rangle\]\[\vec{r}\,'(0) = \langle -2,-1,1 \rangle\]\[\vec{r}\,''(t) = \langle 1,2,2 \rangle\]\[\vec{r}\,''(0) = \langle 1,2,2 \rangle\]Plugging these into our formula gives us\[\kappa(0) = \frac{\sqrt{50}}{(\sqrt{6})^3} = \frac{5}{6 \sqrt{3}}.\]\end{enumerate}\end{document}% \epsfig{file=enclosure01.eps, % width=11cm,% angle=0 } 
