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P01D2017 – Relay Race

Relay Race

The Berkeley relay team is in the lead during the third leg of their race, but the Stanford team is close behind them. In order to win the race, the third runner on the Cal team must pass the baton successfully to the final runner while they are traveling side-by-side at the same velocity. Throughout this problem, the third runner is moving at a constant speed of $v=10\ m/s$. Throughout this entire exam, you may round quantities to one significant figure if you like; for example, you may approximate the magnitude of the acceleration of a projectile as $g=10\ m/s^2$.

View answer

We let $a$ denote the acceleration of the final runner whose kinematic equations are given by

\left\{ \begin{array}{c}
\displaystyle{x_f\left(t\right)=\frac{1}{2}at^2+D} \\
\\
v_x\left(t\right)=at \end{array}
\right.

In time $t_1$, the final runner reaches the speed $v=10\ m/s$ of the third runner and therefore his acceleration must satisfy

\begin{aligned}
v_x\left(t_1\right)=v\ \ \ \ &\Rightarrow \ \ \ \ \ at_1=v \\
\\
&\Rightarrow \ \ \ \ \ a=\frac{v}{t_1}
\end{aligned}

The acceleration of the final runner is equal to

\boxed{a=\frac{v}{t_1}=\frac{10}{5}=2\ m/s^2}
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The average speed of the final runner is equal to

\boxed{v_{avg}=\frac{v_{ini}+v_{fin}}{2}=\frac{0+10}{2}=5\ m/s}
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We set $x_0=0$ at the location of the third runner so that the final runner is initially located at $x=D$ from him.

The positions of the third runner and of the final runner are given respectively by

x_3\left(t\right)=vtx_f\left(t\right)=\frac{1}{2}at^2+D

It takes the final runner $t_1=5\ s$ to reach the speed $v=5\ m/s$ which he does when he is right beside the third runner. In other words, the third runner and the final runner both share the same position at time $t_1=5\ s$ and we have $x_3\left(t_1\right)=x_f\left(t_1\right)$. This allows us to solve for $t_1$ as follows

\begin{aligned}
x_3\left(t_1\right)=x_f\left(t_1\right)\ \ \ \ &\Rightarrow \ \ \ \ \ vt_1=\frac{1}{2}at^2_1+D \\
\\
&\Rightarrow \ \ \ \ \ D=vt_1-\frac{1}{2}at^2_1
\end{aligned}

The distance $D$ between the runners is therefore equal to

\boxed{D=vt_1-\frac{1}{2}at^2_1=10\cdot 5-\frac{1}{2}\cdot 2\cdot 5^2=50-25=25\ m}
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The blimp is moving with speed $v_{By}=7\ m/s$ to the North while the runners are moving with speed $v=10\ m/s$ to the North. This means that, to the runners, it is as if the blimp were moving at speed $v-v_{By}=3\ m/s$ to the South.

The blimp is moving with speed $v_{Bx}=4\ m/s$ to the West while the runners are not moving to the West whatsoever. This means that, to the runners, the blimp is moving with speed $v_{Bx}=4\ m/s$ to the West.

Thus, the velocity of the blimp relative to the runners is given by

\boxed{{\overrightarrow{v}}_{B/R}=4\hat{x}+3\hat{y}\ \ \ \ \ \left(m/s\right)}

where $\hat{y}$ points to the South as shown in the figure above.

View answer

The net displacement of the runner is zero if he runs around the whole track and therefore his average velocity is zero.