Calculus (3rd Edition)

Published by W. H. Freeman
ISBN 10: 1464125260
ISBN 13: 978-1-46412-526-3

Chapter 14 - Calculus of Vector-Valued Functions - 14.5 Motion in 3-Space - Exercises - Page 745: 25

Answer

(a) the position function of the ball $t$ seconds after it is thrown is ${\bf{r}}\left( t \right) = \left( {40t,35t, - 16{t^2} + 32t + 5} \right)$ (b) the player is in bounds when he receives the ball.

Work Step by Step

(a) We have the initial velocity: ${\bf{v}}\left( 0 \right) = 40{\bf{i}} + 35{\bf{j}} + 32{\bf{k}}$ Let the center of the field be the origin of the $xy$-plane. Since the ball leaves his hand at a height of $5$ ft, the initial position is ${\bf{r}}\left( 0 \right) = \left( {0,0,5} \right)$. The only force that acts on the ball is the gravitational force. So, the acceleration due to gravity is ${\bf{a}}\left( t \right) = - 32{\bf{k}}$ $ft/{s^2}$. 1. Find the velocity vector We have ${\bf{v}}\left( t \right) = \smallint {\bf{a}}\left( t \right){\rm{d}}t = \smallint \left( {0,0, - 32} \right){\rm{d}}t = \left( {0,0, - 32t} \right) + {{\bf{c}}_0}$ The initial condition ${\bf{v}}\left( 0 \right) = 40{\bf{i}} + 35{\bf{j}} + 32{\bf{k}}$ gives $\left( {40,35,32} \right) = \left( {0,0,0} \right) + {{\bf{c}}_0}$ ${{\bf{c}}_0} = \left( {40,35,32} \right)$ Thus, ${\bf{v}}\left( t \right) = \left( {0,0, - 32t} \right) + \left( {40,35,32} \right)$ ${\bf{v}}\left( t \right) = \left( {40,35, - 32t + 32} \right)$ 2. Find the position vector We have ${\bf{r}}\left( t \right) = \smallint {\bf{v}}\left( t \right){\rm{d}}t = \smallint \left( {40,35, - 32t + 32} \right){\rm{d}}t$ ${\bf{r}}\left( t \right) = \left( {40t,35t, - 16{t^2} + 32t} \right) + {{\bf{c}}_1}$ The initial condition ${\bf{r}}\left( 0 \right) = \left( {0,0,5} \right)$ gives $\left( {0,0,5} \right) = \left( {0,0,0} \right) + {{\bf{c}}_1}$ ${{\bf{c}}_1} = \left( {0,0,5} \right)$ Thus, the position function of the ball $t$ seconds after it is thrown is ${\bf{r}}\left( t \right) = \left( {40t,35t, - 16{t^2} + 32t} \right) + \left( {0,0,5} \right)$ ${\bf{r}}\left( t \right) = \left( {40t,35t, - 16{t^2} + 32t + 5} \right)$ (b) From part (a) we obtain the position function of the ball $t$ seconds after it is thrown: ${\bf{r}}\left( t \right) = \left( {40t,35t, - 16{t^2} + 32t + 5} \right)$ The ball is caught by a player $5$ ft above the ground. So, we have the equation for the $z$-component $5 = - 16{t^2} + 32t + 5$ $ - 16{t^2} + 32t = 0$ $t\left( { - 16t + 32} \right) = 0$ We obtain the solutions: $t=0$ and $t=2$. Now, $t=0$ corresponds to the time when the ball is thrown. Thus, we take the second solution $t=2$. At $t=2$, the position of the ball is ${\bf{r}}\left( 2 \right) = \left( {80,70,5} \right)$ from the center of the field. Since the field is $150$ ft in width (y-coordinate) and $300$ ft in length (x-coordinate), ${\bf{r}}\left( 2 \right) = \left( {80,70,5} \right)$ is still inside of the field. Hence, the player is in bounds when he receives the ball.
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