University Calculus: Early Transcendentals (3rd Edition)

Published by Pearson
ISBN 10: 0321999584
ISBN 13: 978-0-32199-958-0

Chapter 7 - Section 7.3 - Hyperbolic Functions - Exercises - Page 419: 78

Answer

$ a.\quad$shown below $ b.\quad$shown below

Work Step by Step

$(y$ is proportional to $x $ if there is a constant $k$ such that $y=kx)$ $ a.\quad$ $s(t)=a\cos kt+b\sin ktx\qquad $... differrentiate (chain rule, twice) $\displaystyle \frac{ds}{dt}=-a\sin kt\cdot k+b\cos kt\cdot k$ $\displaystyle \frac{ds}{dt}=-ak\sin kt+bk\cos kt\qquad $... differrentiate (chain rule, twice) $\displaystyle \frac{d^{2}s}{dt^{2}}=-ak^{2}\cos kt-bk^{2}\sin kt$ $=-k^{2} (a \cos kt+b\sin kt)$ $=(-k^{2})\cdot s$ So, $\displaystyle \frac{d^{2}s}{dt^{2}}$ is proportional to $s$. The negative sign indicates that the acceleration is in the opposite direction of displacement (towards the origin). $ b.\quad$ $s(t)=a\cosh kt-\vdash b\sinh kt \qquad $... differrentiate $\displaystyle \frac{ds}{dt}=ak\sinh kt+bk\cosh kt \qquad $... once more, $\displaystyle \frac{d^{2}s}{dt^{2}}=ak^{2}\cosh kt+bk^{2}\sinh kt=k^{2}s$ Again, acceleration is proportional to displacement. This time, acceleration has the same sign (direction) as displacement (away from the origin).
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