/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 20 As drawn in Fig. 2-7, a ball is ... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

As drawn in Fig. 2-7, a ball is thrown from the top of one building toward a tall building \(50 \mathrm{~m}\) away. The initial velocity of the ball is \(20 \mathrm{~m} / \mathrm{s}-40^{\circ}\) above horizontal. How far above or below its original level will the ball strike the opposite wall? We have $$ \begin{array}{l} v_{i x}=(20 \mathrm{~m} / \mathrm{s}) \cos 40^{\circ}=15.3 \mathrm{~m} / \mathrm{s} \\ v_{i x}=(20 \mathrm{~m} / \mathrm{s}) \cos 40^{\circ}=12.9 \mathrm{~m} / \mathrm{s} \end{array} $$ Consider first the horizontal motion. For it, $$ v_{i x}=v_{f x}=v_{x} 15.3 \mathrm{~m} / \mathrm{s} $$ Then \(x=v_{x} t\) gives $$ 50 \mathrm{~m}=(15.3 \mathrm{~m} / \mathrm{s}) t \quad \text { or } \quad t=3.27 \mathrm{~s} $$ For the vertical motion, taking down as positive, $$ y=v_{i j} t+\frac{1}{2} a_{y} t^{2}=(-12.9 \mathrm{~m} / \mathrm{s})(3.27 \mathrm{~s})+\frac{1}{2}\left(9.81 \mathrm{~m} / \mathrm{s}^{2}\right)(3.27 \mathrm{~s})^{2}=10.3 \mathrm{~m} $$ and to two significant figures, \(y=10 \mathrm{~m}\). Since \(y\) is positive, and since down is positive, the ball will hit at \(10 \mathrm{~m}\) below the original level.

Short Answer

Expert verified
The ball strikes 10 m below its original level.

Step by step solution

01

Identify the Known Horizontal Components

We start by identifying the horizontal component of the initial velocity. Given the initial velocity of the ball is 20 m/s at an angle of 40° above the horizontal, the horizontal component is calculated using: \( v_{i x} = v_i \cos \theta = (20 \, \text{m/s}) \cos 40^\circ = 15.3 \, \text{m/s} \).
02

Identify the Known Vertical Components

Next, we identify the vertical component of the initial velocity. Use the following equation: \( v_{i y} = v_i \sin \theta = (20 \, \text{m/s}) \sin 40^\circ = 12.9 \, \text{m/s} \). Note that the sign is negative because the vertical motion is being considered downwards as positive.
03

Determine Time of Flight

Considering horizontal motion and knowing the ball is thrown across a 50 m wide gap, use the equation: \( x = v_{x} t \) to find time \( t \). Substitute the known values: \( 50 \, \text{m} = (15.3 \, \text{m/s}) t \), solving for \( t \) gives: \( t = 3.27 \, \text{s} \).
04

Calculate Vertical Displacement

Now consider the vertical motion. Use the equation for vertical displacement: \( y = v_{i y} t + \frac{1}{2} a_{y} t^2 \). Substitute \( v_{i y} = -12.9 \, \text{m/s} \), \( a_y = 9.81 \, \text{m/s}^2 \), and \( t = 3.27 \, \text{s} \): \( y = (-12.9 \, \text{m/s})(3.27 \, \text{s}) + \frac{1}{2}(9.81 \, \text{m/s}^2)(3.27 \, \text{s})^2 = 10.3 \, \text{m} \).
05

Interpret the Result

Since \( y = 10.3 \, \text{m} \) is positive and was calculated with downward motion considered positive, the ball strikes the opposite building 10 meters below its original level.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

These are the key concepts you need to understand to accurately answer the question.

horizontal motion
In projectile motion, understanding horizontal motion is crucial. When a projectile is launched, its horizontal component is independent of its vertical component.
The key aspect to remember is that the horizontal velocity remains constant throughout the flight.
This is because, in the absence of air resistance, there are no horizontal forces acting on the projectile, meaning that the projectile's horizontal acceleration is zero.
Hence, the horizontal motion can be described by the simple equation:
  • \( x = v_{x} t \)
Where \( x \) is the horizontal distance traveled, \( v_x \) is the initial horizontal velocity, and \( t \) is the time.
This equation represents that the displacement in horizontal motion is directly proportional to time, with the constant of proportionality being the horizontal velocity.
For instance, if our projectile is to cross a horizontal distance of 50 m with a constant horizontal velocity of 15.3 m/s, we utilize the equation \( 50 \, \text{m} = (15.3 \, \text{m/s}) t \) to find the time duration, which is 3.27 seconds.
vertical motion
Vertical motion in projectile scenarios is influenced by gravity, making it quite dynamic compared to horizontal motion.
The vertical component is affected by acceleration due to gravity, which we denote as \( g = 9.81 \, \text{m/s}^2 \).
This means that as the projectile moves upwards, it decelerates, and on its way down, it accelerates. In this sense,
we can determine the vertical displacement using the formula:
  • \( y = v_{i y} t + \frac{1}{2} a_{y} t^2 \)

In this equation, \( y \) represents the vertical displacement, \( v_{i y} \) is the initial vertical velocity, and \( a_y \) is the acceleration of gravity, which is always acting downward.
In the given exercise, considering the ball's launch, we used this formula to determine how the ball's position changes vertically and found it goes 10.3 meters below its starting height when it hits the wall.
initial velocity
Initial velocity is a critical factor in projectile motion as it determines how the projectile will travel.
It consists of two components: horizontal and vertical, which can be calculated using trigonometric functions if the launch angle is known.
The process involves the following calculations:
  • The horizontal component: \( v_{i x} = v_i \cos \theta \)
  • The vertical component: \( v_{i y} = v_i \sin \theta \)

Where \( v_i \) is the initial speed and \( \theta \) is the angle above the horizontal.
For example, in the exercise, we have an initial velocity of 20 m/s at an angle of 40°.
This results in a horizontal component of 15.3 m/s and a vertical component of 12.9 m/s.
Such a separation allows us to individually address horizontal and vertical motions, building a complete picture of the projectile's path.
time of flight
Time of flight is the duration for which a projectile remains in motion until it reaches a specific point.
It helps in determining both how long the projectile will be traveling and where it will land.
The time of flight can be found from either the horizontal or vertical motion analysis.
For horizontal motion, since the horizontal velocity is constant, it helps us easily find time by rearranging the equation \( x = v_{x} t \).
For example, in the exercise, knowing that the ball must travel 50 m horizontally with a constant velocity of 15.3 m/s,
we solve the equation to find the time of flight, which is approximately 3.27 seconds.
This time is crucial for further calculations regarding the vertical displacement, helping in predicting key outcomes of the projectile's flight.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A marble dropped from a bridge strikes the water in \(5.0 \mathrm{~s}\). Calculate ( \(a\) ) the speed with which it strikes and \((b)\) the height of the bridge.

A body is projected downward at an angle of \(30.0^{\circ}\) with the horizontal from the top of a building \(170 \mathrm{~m}\) high. Its initial speed is \(40.0 \mathrm{~m} / \mathrm{s}\). (a) How long will it take before striking the ground? (b) How far from the foot of the building will it strike? (c) At what angle with the horizontal will it strike?

A skier starts from rest and slides down a mountainside along a straight descending path \(9.0 \mathrm{~m}\) long in \(3.0 \mathrm{~s}\). In what time after starting will the skier acquire a speed of \(24 \mathrm{~m} / \mathrm{s}\) ? Assume that the acceleration is constant and the entire run is straight, at a fixed incline, and around \(1.0\) -km long. We must find the skier's acceleration from the data concerning the 3.0 s trip. Taking the direction of motion down the inclined path as the \(+x\) -direction, we have \(t=3.0 \mathrm{~s}, v_{i x}=0\), and \(x=9.0 \mathrm{~m} .\) Then \(x=v_{i x} t+\frac{1}{2} a t^{2}\) gives $$ a=\frac{2 x}{t^{2}}=\frac{18 \mathrm{~m}}{(3.0 \mathrm{~s})^{2}}=2.0 \mathrm{~m} / \mathrm{s}^{2} $$ We can now use this value of \(a\) for the longer trip, from the starting point to the place where \(v_{f x}=24 \mathrm{~m} / \mathrm{s}\). For this trip, \(v_{i x}=0\), \(u_{f x}=24 \mathrm{~m} / \mathrm{s}, a=2.0 \mathrm{~m} / \mathrm{s}^{2} .\) Then, from \(v_{f}=v_{i}+a t\) $$ t=\frac{v_{f x}-v_{i x}}{a}=\frac{24 \mathrm{~m} / \mathrm{s}}{2.0 \mathrm{~m} / \mathrm{s}^{2}}=12 \mathrm{~s} $$

A stone is thrown straight upward with a speed of \(20 \mathrm{~m} / \mathrm{s}\). It is caught on its way down at a point \(5.0 \mathrm{~m}\) above where it was thrown. (a) How fast was it going when it was caught? ( \(b\) ) How long did the trip take? The situation is shown in Fig. 2-3. Take up as positive. Then, for the trip that lasts from the instant after throwing to the instant before catching, \(v_{i y}=20 \mathrm{~m} / \mathrm{s}, y=+5.0 \mathrm{~m}\) (since it is an upward displacement), \(a=-9.81 \mathrm{~m} / \mathrm{s}^{2}\) (a) Use \(v_{f y}^{2}=v_{i y}^{2}+2 a y\) to compute $$ \begin{array}{l} v_{f j}^{2}=(20 \mathrm{~m} / \mathrm{s})^{2}+2\left(-9.81 \mathrm{~m} / \mathrm{s}^{2}\right)(5.0 \mathrm{~m})=302 \mathrm{~m}^{2} / \mathrm{s}^{2} \\\ v_{f j}=\pm \sqrt{302 \mathrm{~m}^{2} / \mathrm{s}^{2}}=-17 \mathrm{~m} / \mathrm{s} \end{array} $$ Take the negative sign because the stone is moving downward, in the negative direction, at the final instant. (b) To find the time, use \(a=\left(v_{f y}-v_{i y}\right) / t\) and so $$ t=\frac{(-17.4-20) \mathrm{m} / \mathrm{s}}{-9.81 \mathrm{~m} / \mathrm{s}^{2}}=3.8 \mathrm{~s} $$ Notice that we retain the minus sign on \(v_{f y}\). You can check your work by dividing the problem into two parts, the trip up to peak altitude and the trip down from peak. The peak altitude is given by Eq. (2.9); that is, \(y_{p}=-v_{i}^{2} / 2 g=-(20\) \(\mathrm{m} / \mathrm{s})^{2} / 2\left(-9.81 \mathrm{~m} / \mathrm{s}^{2}\right)=20.38736 \mathrm{~m}\). [Hint: Don't round off to two figures mid-calculation.] Now drop the stone from \(y_{p}\) so it falls a distance \((20.38736 \mathrm{~m})-(5.0 \mathrm{~m})=15.38736 \mathrm{~m}\), at which point it will be moving- - from Eq. (2.6) with down as plus-at \(v_{f}^{2}=2 g s=\) \(2\left(9.81 \mathrm{~m} / \mathrm{s}^{2}\right)(15.38736 \mathrm{~m})=301.900 \mathrm{~m}^{2} / \mathrm{s}^{2}\), and so \(v_{f}=17.4 \mathrm{~m} / \mathrm{s}=\) \(17 \mathrm{~m} / \mathrm{s}\). Similarly, you can calculate the total time of flight, which equals the time to reach peak altitude plus the time to fall \(15.387\) \(\mathrm{m} .\)

If a vehicle accelerates at \(10.0 \mathrm{~m} / \mathrm{s}^{2}\) from rest for \(20.0 \mathrm{~s}\), how far will it travel in the process? [Hint: You are given \(a, u_{i}\), and \(t\), and you need to find s.]

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.