Multivariable Calculus, 7th Edition

Published by Brooks Cole
ISBN 10: 0-53849-787-4
ISBN 13: 978-0-53849-787-9

Chapter 10 - Parametric Equations and Polar Coordinates - 10.2 Exercises - Page 675: 14

Answer

$\frac{dy}{dx} = \frac{e^{t}}{2t}$ $\frac{d²y}{dx²} = \frac {e^{t}(t – 1)}{4t³}$ The curve is concave up for $t$ in $(–\infty, 0)$ and $(1, \infty)$.

Work Step by Step

We differentiate both equations with respect to $t$: $x = t² + 1$ $\frac{dx}{dt} = 2t$ $y = e^{t} – 1$ $\frac{dy}{dt} = e^{t}$ Now, we know that $\frac{dy}{dx} = \frac{\frac{dy}{dt}}{\frac{dx}{dt}}$, so: $\frac{dy}{dx} = \frac{e^{t}}{2t}$ To find $\frac{d²y}{dx²}$, we differentiate $\frac{dy}{dx}$ using the chain rule: $\frac{dy}{dx} = \frac{e^{t}}{2t}$ $\frac{d²y}{dx²} = \frac {\frac{d}{dt} (\frac{e^{t}}{2t})}{\frac{dx}{dt}}$ $= \frac {\frac{2t(e^{t}) – 2(e^{t})}{4t²}}{2t}$ $= \frac {e^{t}(2t – 2)}{8t³}$ $= \frac {e^{t}(t – 1)}{4t³}$ The curve will be concave up whenever $\frac{d²y}{dx²} \gt 0$, which will happen if $t – 1$ and $t³$ have the same sign (we don’t need to worry about $e^{t}$ because it is always positive). Since $t – 1 \gt 0$ when $t \gt 1$ and $t³ \gt 0$ when $t\gt 0$: For $t$ in ($–\infty$ , 0), both expressions are negative and therefore $\frac{d²y}{dx²}$ is positive. For $t$ in (0 , 1), the expressions have opposite signs and therefore $\frac{d²y}{dx²}$ is negative. For $t$ in (1 , $\infty$), both expressions are positive and therefore $\frac{d²y}{dx²}$ is positive. Thus the curve is concave up for $t$ in $(–\infty, 0)$ and $(1, \infty)$.
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