Tag Archives: ball thrown from the top of a building

College Physics by Openstax Chapter 3 Problem 28


(a) A daredevil is attempting to jump his motorcycle over a line of buses parked end to end by driving up a 32º ramp at a speed of 40.0 m/s (144 km/h) . How many buses can he clear if the top of the takeoff ramp is at the same height as the bus tops and the buses are 20.0 m long? (b) Discuss what your answer implies about the margin of error in this act—that is, consider how much greater the range is than the horizontal distance he must travel to miss the end of the last bus. (Neglect air resistance.)


Solution:

To illustrate the problem, consider the following figure:

The projectile path of the daredevil from the ramp

Part A

To determine the number of buses that the daredevil can clear, we will divide the range of the projectile path by 20 m, the length of 1 bus. That is

\text{no. of bus}=\frac{\text{Range}}{\text{bus length}}

First, we need to solve for the range.

\begin{align*}
\text{Range} & =\frac{\text{v}_{\text{o}}^2\:\sin 2\theta }{\text{g}} \\
\text{Range} & =\frac{\left(40.0\:\text{m/s}\right)^2\sin \left[2\left(32^{\circ} \right)\right]}{9.81\:\text{m/s}^2} \\
\text{Range} & =146.7\:\text{m} \\

\end{align*}

Therefore, the number of buses cleared is

\begin{align*}
\text{no. of buses} & =\frac{146.7\:\text{m}}{20\:\text{m}} \\
\text{no. of buses} & =7.34\:\text{buses} \\
\text{no. of buses} & =7\:\text{buses}

\qquad \qquad{\color{DarkOrange} \left( \text{Answer} \right)} \\
\end{align*}

Therefore, he can only clear 7 buses. 

Part B

He clears the last bus by 6.7 m, which seems to be a large margin of error, but since we neglected air resistance, it really isn’t that much room for error.


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College Physics by Openstax Chapter 3 Problem 27


A ball is thrown horizontally from the top of a 60.0-m building and lands 100.0 m from the base of the building. Ignore air resistance. (a) How long is the ball in the air? (b) What must have been the initial horizontal component of the velocity? (c) What is the vertical component of the velocity just before the ball hits the ground? (d) What is the velocity (including both the horizontal and vertical components) of the ball just before it hits the ground?


Solution:

To illustrate the problem, consider the following figure:

The path of the ball thrown at the top of a 60 m building.

Part A

The problem states that the initial velocity is horizontal, this means that the initial vertical velocity is zero. We are also given the height of the building (which is a downward displacement), so we can solve for the time of flight using the formula y=voyt+1/2at2. That is,

\begin{align*}
\text{y} & =\text{v}_{\text{oy}}\text{t}+\frac{1}{2}\text{a}\text{t}^2 \\
 -60\:\text{m}&=0+\frac{1}{2}\left(-9.81\:\text{m/s}^2\right)\text{t}^2 \\
\text{t}^2 & =\dfrac{-60\:\text{m}}{-4.905\:\text{m/s}^2} \\
\text{t}^2 & =12.2324\:\text{s}^2 \\
\text{t} & =3.50\:\text{s} \ \qquad \ {\color{DarkOrange} \left( \text{Answer} \right)}

\end{align*}

Part B

To solve for the vox, we will use the formula \text{v}_{\text{ox}}=\frac{\Delta \:\text{x}}{\text{t}}.

\begin{align*}
\text{v}_{\text{ox}} & =\frac{100\:\text{m}}{3.50\:\text{s}} \\
\text{v}_{\text{ox}} & =28.6\:\text{m/s} \ \qquad \ {\color{DarkOrange} \left( \text{Answer} \right)}
\end{align*}

Part C

To solve for the velocity as the ball hits the ground, we shall consider two points: (1) at the beginning of the flight, and (2) when the ball hits the ground.

We know that the initial velocity, voy, is zero. To solve for the final velocity, we will use the formula \text{v}_{\text{f}}=\text{v}_{\text{o}}+\text{at}.

\begin{align*}
\text{v}_{\text{f}} & =0+\left(-9.81\:\text{m/s}^2\right)\left(3.50\:\text{s}\right) \\
\text{v}_{\text{f}} & =-34.3\:\text{m/s}

\ \qquad \ {\color{DarkOrange} \left( \text{Answer} \right)}
\end{align*}

The negative velocity indicates that the motion is downward.

Part D

Since we already know the horizontal and vertical components of the velocity when it hits the ground, we can find the resultant.

\begin{align*}
\text{v} & =\sqrt{\text{v}_{\text{x}}^2+\text{v}_{\text{y}}^2} \\
\text{v} & =\sqrt{\left(28.57\:\text{m/s}\right)^2+\left(-34.34\:\text{m/s}\right)^2} \\
\text{v} & =44.7\:\text{m/s}

\ \qquad \ {\color{DarkOrange} \left( \text{Answer} \right)}
\end{align*}

The direction of the velocity is

\begin{align*}
\theta_{\text{x}} & =\tan ^{-1}\left|\frac{\text{v}_{\text{y}}}{\text{v}_{\text{x}}}\right| \\
\theta _{\text{x}} & =\tan ^{-1}\left|\frac{-34.34}{28.57}\right| \\
\theta _{\text{x}} & =50.2^{\circ}

\ \qquad \ {\color{DarkOrange} \left( \text{Answer} \right)}
\end{align*}

The velocity is directed 50.2° down the x-axis.


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