Engineering Mechanics: Statics & Dynamics (14th Edition)

Published by Pearson
ISBN 10: 0133915425
ISBN 13: 978-0-13391-542-6

Chapter 12 - Kinematics of a Particle - Section 12.2 - Rectilinear Kinematics: Continuous Motion - Problems - Page 19: 34

Answer

$$ \begin{aligned} & v=-R \sqrt{\frac{2 g_0\left(y_0-y\right)}{(R+y)\left(R+y_0\right)}} \\ & v_{\text {imp }}=3.02 \mathrm{~km} / \mathrm{s} \end{aligned} $$

Work Step by Step

From Prob. 12-36, $(+\uparrow) \quad a=-g_0 \frac{R^2}{(R+y)^2}$ Since $a d y=v d v$ then $$ \begin{aligned} & -g_0 R^2 \int_{y_0}^y \frac{d y}{(R+y)^2}=\int_0^v v d v \\ & g_0 R^2\left[\frac{1}{R+y}\right]_{y_0}^y=\frac{v^2}{2} \\ & g_0 R^2\left[\frac{1}{R+y}-\frac{1}{R+y_0}\right]=\frac{v^2}{2} \end{aligned} $$ Thus $$ v=-R \sqrt{\frac{2 g_0\left(y_0-y\right)}{(R+y)\left(R+y_0\right)}} $$ When $y_0=500 \mathrm{~km}, \quad y=0$, $$ \begin{aligned} & v=-6356\left(10^3\right) \sqrt{\frac{2(9.81)(500)\left(10^3\right)}{6356(6356+500)\left(10^6\right)}} \\ & v=-3016 \mathrm{~m} / \mathrm{s}=3.02 \mathrm{~km} / \mathrm{s} \downarrow \end{aligned} $$
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