Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 4 - Motion in Two and Three Dimensions - Problems - Page 84: 17

Answer

$v=(32m/s)\hat{i}$

Work Step by Step

We observe two components of the cart's motion. Vertically, moving up, it reaches a $y_{max}$, stops (going up) for an instant, and then moves down. In the meantime, it is accelerating horizontally. The accelerations are constant in either direction, so the Table 1 formulas apply. $\left[\begin{array}{ll} v=v_{0}+at, & (2- 11)\\ x-x_{0}=v_{0}t+21at^{2}, & (2- 15) \\ v^{2}=v_{0}^{2}+2a(x-x_{0}) , & (2- 16) \\ x-x_{0}=\frac{1}{2}(v_{0}+v)t, & (2- 17) \\ x-x_{0}=vt-\frac{1}{2}at^{2} & (2- 18) \end{array}\right]$ Concentrate first on the vertical component. At the apex (at the greatest y-coordinate $y_{max}$), the $v_{y}$ component of velocity is zero. Using Table 2-1, we apply $v=v_{0}+at$ to the y-direction in order to find the time needed to reach the apex. $v_{y}=v_{y0}+a_{y}t$ $0=(12m/s)+(-2.0m/\mathrm{s}^{2})t$ $t=\displaystyle \frac{12m/s}{2.0m/\mathrm{s}^{2}}=6.0s$ In the x-direction, we also apply $v=v_{0}+at$ , , knowing that the time passed is $t=6.0s:$ $v_{x}=v_{x0}+a_{y}t=(8.0m/s)+(4.0m/\mathrm{s}^{2})(6.0s)=32m/s$ Thus (at the greatest y-coordinate $y_{max}$), $v=v_{x}\hat{i}+v_{y}\hat{j}=(32m/s)\hat{i}+0$ $v=(32m/s)\hat{i}$
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