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The Longest Home Run. According to the Guinness Book of World Records, the longest home run ever measured was hit by Roy "Dizzy" Carlyle in a minor league game. The ball traveled 188 \(\mathrm{m}(618 \mathrm{ft})\) before landing on the ground outside the ballpark. (a) Assuming the ball's initial velocity was in a direction \(45^{\circ}\) above the horizontal and ignoring air resistance, what did the initial speed of the ball need to be to produce such a home run if the ball was hit at a point 0.9 \(\mathrm{m}(3.0 \mathrm{ft})\) above ground level? Assume that the ground was perfectly flat. (b) How far would the ball be above a fence 3.0 \(\mathrm{m}(10 \mathrm{ft})\) high if the fence was 116 \(\mathrm{m}(380 \mathrm{ft})\) from home plate?

Short Answer

Expert verified
(a) Approx. 42.9 m/s (b) Approx. 40.86 m above the fence.

Step by step solution

01

Convert angle to radians

Given that the angle is \(45^{\circ}\), we can convert it to radians for calculations. Using the conversion \(1^{\circ} = \frac{\pi}{180}\) radians, we have:\[\theta = 45^{\circ} \times \frac{\pi}{180} = \frac{\pi}{4} \text{ rad}\]
02

Implement kinematic equation for range

The range \( R \) of a projectile is given by the formula:\[R = \frac{v_0^2 \sin 2\theta}{g}\]where \( v_0 \) is the initial speed, \( g = 9.8 \, \text{m/s}^2 \) is the acceleration due to gravity, and \( \theta \) is the launch angle. Since \( R = 188 \, \text{m} \) and \( \theta = \frac{\pi}{4} \):\[188 = \frac{v_0^2 \sin(\frac{\pi}{2})}{9.8}\]Since \( \sin(\frac{\pi}{2}) = 1 \), we simplify to:\[188 = \frac{v_0^2}{9.8}\]
03

Solve for initial speed

Rearrange the equation from the previous step to solve for \( v_0 \):\[v_0^2 = 188 \times 9.8\]\[v_0^2 = 1842.4\]\[v_0 = \sqrt{1842.4} \approx 42.9 \, \text{m/s}\]Thus, the initial speed required was approximately 42.9 m/s.
04

Find time to reach 116 m

Next, find the time \( t \) it takes for the ball to travel 116 m horizontally:\[x = v_{0x} \, t \Rightarrow t = \frac{x}{v_{0x}}\]Given \( v_{0x} = v_0 \cos \theta = 42.9 \cos(\frac{\pi}{4}) \approx 30.3 \, \text{m/s} \), and \( x = 116 \, \text{m} \):\[t = \frac{116}{30.3} \approx 3.83 \, \text{s}\]
05

Calculate vertical position at 116 m

Using the vertical motion equation, find the height \( y \) of the ball after 3.83 s:\[y = v_{0y}t - \frac{1}{2}gt^2\]where \( v_{0y} = v_0 \sin \theta = 42.9 \sin(\frac{\pi}{4}) \approx 30.3 \, \text{m/s} \).Substitute the values:\[y = 30.3 \times 3.83 - \frac{1}{2} \times 9.8 \times (3.83)^2\]\[y \approx 115.95 - 72.09 \approx 43.86 \, \text{m}\]
06

Determine the height above the fence

The height of the ball above the ground 116 m away is 43.86 m. Given the fence is 3.0 m, the ball is:\[43.86 - 3.0 = 40.86 \, \text{m}\]Therefore, the ball is approximately 40.86 m above the fence.

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Key Concepts

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

kinematic equations
Kinematic equations are crucial when analyzing projectile motion, such as the impressive 188 m home run hit by Roy "Dizzy" Carlyle. These equations connect an object's position, velocity, acceleration, and time.

For projectile motion, kinematic equations allow us to calculate important elements like range, time of flight, and final velocity. In the context of Carlyle's home run, we specifically used the equation for the range of a projectile:
  • \( R = \frac{v_0^2 \sin 2\theta}{g} \)
Where \( R \) is the range, \( v_0 \) is the initial velocity or speed, \( \theta \) is the launch angle, and \( g \) is the gravitational acceleration ( \( 9.8 \text{ m/s}^2 \) ).

By applying this equation, we determined the initial velocity needed to achieve the record-breaking home run distance. Here, knowing the distance the ball traveled and the gravitational pull on the ball, we could reverse engineer to find the initial launch speed, an essential part of understanding projectile dynamics.
launch angle
The launch angle is a significant factor in projectile motion as it influences how far and how high a projectile will travel. In the case of the remarkable 188 m home run, the launch angle was given as \( 45^\circ \). This specific angle is often chosen for calculations because it maximizes the range of a projectile when air resistance is negligible.

When solving problems involving projectile motion, angles must often be converted from degrees to radians. This conversion is necessary because many mathematical formulas, especially in physics, utilize radians for trigonometric functions. The conversion used is:
  • \( 1^\circ = \frac{\pi}{180} \text{ radians} \)
  • So, for a \( 45^\circ \) angle: \( \theta = \frac{\pi}{4} \text{ radians} \)
With the launch angle known, you can then determine how the initial velocity breaks into horizontal and vertical components, which is crucial for calculations on range and height.
vertical motion
Understanding vertical motion in projectile problems aids in fully analyzing the trajectory of objects like Roy "Dizzy" Carlyle's legendary home run. Vertical motion involves the initial vertical component of velocity and the impact of gravitational acceleration on it.

For vertical motion, the equation used is:
  • \( y = v_{0y}t - \frac{1}{2}gt^2 \)
Where \( y \) is the vertical displacement, \( v_{0y} \) is the initial vertical velocity (\( v_0 \sin \theta \) ), \( g \) is acceleration due to gravity, and \( t \) is time.

In this problem, the height of the ball at a specific distance was calculated using this equation. Starting with a time found from horizontal motion calculations, we can use the vertical motion equation to determine how high the ball traveled and by how much it’s height surpassed objects like fences. By finding that the ball reached 43.86 m at 116 m horizontally, we better grasp the upward and downward journey of the ball, demonstrating the symbiotic relationship between horizontal and vertical motion in projectiles.

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Most popular questions from this chapter

A projectile is fired from point \(A\) at an angle above thehorizontal. At its highest point, after having traveled a horizontal distance \(D\) from its launch point, it suddenly explodes into two identical fragments that travel horizontally with equal but opposite velocities as measured relative to the projectile just before it exploded. If one fragment lands back at point \(A,\) how far from \(A\) (in terms of \(D\) ) does the other fragment land?

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The earth has a radius of 6380 \(\mathrm{km}\) and turns around once on its axis in 24 \(\mathrm{h}\) . (a) What is the radial acceleration of an object at the earth's equator? Give your answer in \(\mathrm{m} / \mathrm{s}^{2}\) and as a fraction of \(g .\) (b) If \(a_{\text { rad }}\) at the equator is greater than \(g,\) objects will fly off the earth's surface and into space. (We will see the reason for this in Chapter 5.) What would the period of the earth's rotation have to be for this to occur?

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