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In the vertical jump, an athlete starts from a crouch and jumps upward to reach as high as possible. Even the best athletes spend little more than 1.00 \(\mathrm{s}\) in the air (their "hang time"). Treat the athlete as a particle and let \(y_{\text { max }}\) be his maximum height above the floor. To explain why he seems to hang in the air, calculate the ratio of the time he is above \(y_{\max } / 2\) to the time it takes him to go from the floor to that height. You may ignore air resistance.

Short Answer

Expert verified
The ratio is approximately 2.8.

Step by step solution

01

Understand the Problem

The problem requires us to find the time ratio of an athlete's hang time above half his maximum jump height, compared to the time it takes to reach that height from the ground.
02

Set up Known Equations for Motion

Use the kinematic equations for motion. For vertical motion under gravity, the equations are: 1. \[ v = u + at \]2. \[ s = ut + \frac{1}{2}at^2 \]3. \[ v^2 = u^2 + 2as \]Where:- \(u\) is the initial velocity,- \(v\) is the final velocity,- \(a\) is the acceleration (gravity here, \(-9.8\, m/s^2\)),- \(t\) is time,- \(s\) is displacement.
03

Maximum Height Calculation

At maximum height \(y_{\text{max}}\), the final velocity \(v = 0\). Using equation \(v^2 = u^2 + 2as\), simplify:\[ 0 = u^2 - 2g y_{\text{max}} \]Thus,\[ y_{\text{max}} = \frac{u^2}{2g} \]
04

Time to Reach \( y_{\max} / 2 \)

For \( y = y_{\max} / 2 \), substitute in equation \(s = ut + \frac{1}{2}at^2\):\[ \frac{u^2}{4g} = ut_1 - \frac{gt_1^2}{2} \]This quadratic equation for \(t_1\) (time to reach \( y_{\max} / 2\)) must be solved.
05

Solve the Quadratic Equation

Rearrange:\[ 0 = \frac{gt_1^2}{2} - ut_1 + \frac{u^2}{4g} \]Using the quadratic formula \(t = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}\), set \(a = \frac{g}{2}, b = -u, c = \frac{u^2}{4g}\). Solve for \(t_1\).
06

Total Hang Time Calculation

For total time \( T \) up and down, the upward motion: \[ T/2 = \frac{u}{g} \]From earlier results,\[ T = \frac{2u}{g} \] is the total hang time.
07

Calculate Time Above \( y_{max}/2 \)

The athlete is above \( y_{\max}/2\) on the way up and down. Total time above \( y_{\max}/2 \) is \[ T - 2t_1 \].
08

Final Time Ratio Calculation

The time ratio is \( \frac{T - 2t_1}{t_1} \). Simplifying gives:\[ \text{Ratio} = \frac{\sqrt{2}}{\frac{1}{2}} = 2.828.\]
09

Conclusion

The time ratio of the time spent above half the max height to the time reaching that height is approximately 2.8.

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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 fundamental tools used in the study of motion. These equations allow us to calculate various aspects of a moving object, such as its velocity, displacement, and time under constant acceleration. In the context of projectile motion and vertical jumps, we focus on objects moving under the influence of gravity.

Here are the basic kinematic equations:
  • Velocity: \( v = u + at \)
  • Displacement: \( s = ut + \frac{1}{2}at^2 \)
  • Velocity squared: \( v^2 = u^2 + 2as \)
In these equations:
  • \( u \) represents the initial velocity of the object.
  • \( v \) is the final velocity at a particular point in time.
  • \( a \) denotes the constant acceleration, which, in the case of gravity, is \(-9.8 \text{ m/s}^2\) towards the Earth.
  • \( t \) is the time elapsed during the motion.
  • \( s \) indicates the displacement from the initial position.


Understanding these equations allows us to analyze different parts of an athlete's jump, such as how high they can reach and how much time they spend above a certain height.
Vertical Jump Analysis
Analyzing a vertical jump involves breaking down the motion into measurable parts. Imagine an athlete crouching before leaping upward into the air. To fully understand this motion, we apply kinematic equations to calculate the maximum height (\( y_{\text{max}} \)) and other key metrics.

### Finding the Maximum HeightWhen the athlete reaches their peak height, their vertical velocity is zero. Using the equation \( v^2 = u^2 + 2as \), we know at the maximum height \( v = 0 \):
  • \( 0 = u^2 - 2gy_{\text{max}} \)
  • Solving gives \( y_{\text{max}} = \frac{u^2}{2g} \)
This expression tells us that the maximum height is directly related to the square of the initial velocity and inversely related to gravity.

### Evaluating Hang Time"Hang time" refers to the total time the athlete is airborne. By evaluating the equations, we can determine how much time is spent above half the maximum height \( y_{\max} / 2 \).

This analysis involves understanding the symmetry of projectile motion. The time ascending to \( y_{\text{max}} / 2 \) and the time descending from it back to the same height are equal, thus giving insight into the athlete's capabilities.
Motion Under Gravity
When talking about projectiles, gravity is a crucial factor. It influences all objects in free fall, pulling them towards the Earth at a constant rate. For an athlete's vertical jump, this means their motion can be dissected into two phases: upwards against gravity and downwards with gravity.

### Upwards Motion During the jump's ascent, gravity decelerates the athlete until they reach their peak height, where vertical velocity is zero. This is where the athlete "hangs" momentarily before falling back down.
### Downwards Motion Once at the peak, the athlete begins descending, accelerating under the pull of gravity. This symmetrical motion ensures that the time taken to ascend to half the maximum height is the same as the time to descend back from it.
Understanding motion under gravity is vital not only for solving physics problems but also for practical applications like optimizing athletic performance. It provides the foundational principles necessary for calculating trajectories, understanding flight paths, and improving exercise training.

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Most popular questions from this chapter

The position of a particle between \(t=0\) and \(t=2.00 \mathrm{s}\) is given by \(x(t)=\left(3.00 \mathrm{m} / \mathrm{s}^{3}\right) t^{3}-\left(10.0 \mathrm{m} / \mathrm{s}^{2}\right) t^{2}+(9.00 \mathrm{m} / \mathrm{s}) t\) (a) Draw the \(x-t, v_{x}-t,\) and \(a_{x}-t\) graphs of this particle. (b) At what time(s) between \(t=0\) and \(t=2.00 \mathrm{s}\) is the particle instantaneously at rest? Does your numerical result agree with the \(v_{x}-t\) graph in part \((a) ?\) At each time calculated in part \((b)\) is the acceleration of the particle positive or negative? Show that in each case the same answer is deduced from \(a_{x}(t)\) and from the \(v_{x}-t\) graph. (d) At what time(s) between \(t=0\) and \(t=2.00 \mathrm{s}\) is the velocity of the particle instantancously not changing? Locate this point on the \(v_{x} t\) and \(a_{x}-t\) graphs of part (a). (e) What is the particle's greatest distance from the origin \((x=0)\) between \(t=0\) and \(t=2.00 \mathrm{s} ?(\mathrm{f})\) At what time(s) between \(t=0\) and \(t=2.00 \mathrm{s}\) is the particle speeding \(u p\) at the greatest rate? At what time(s) between \(t=0\) and \(t=2.00 \mathrm{s}\) is the particle slowing down at the greatest rate? Locate these points on the \(v_{x}-t\) and \(a_{x}-t\) graphs of part (a).

Launch of the Space Shuttle. At launch the space shuttle weighs 4.5 million pounds. When it is launched from rest, it takes 8.00 \(\mathrm{s}\) to reach \(161 \mathrm{km} / \mathrm{h},\) and at the end of the first 1.00 \(\mathrm{min}\) its speed is 1610 \(\mathrm{km} / \mathrm{h}\) . (a) What is the average acceleration (in \(\mathrm{m} / \mathrm{s}^{2} )\) of the shuttle (i) during the first 8.00 \(\mathrm{s}\) , and (ii) between 8.00 \(\mathrm{s}\) and the end of the first 1.00 \(\mathrm{min} 7\) (b) Assuming the acceleration is constant during each time interval (but not necessarily the same in both intervals), what distance does the shuttle travel (i) during the first \(8.00 \mathrm{s},\) and (ii) during the interval from 8.00 \(\mathrm{s}\) to 1.00 \(\mathrm{min}\) ?

A painter is standing on scaffolding that is raised at constant speed. As he travels upward, he accidentally nudges a paint can off the scaffolding and it falls 15.0 \(\mathrm{m}\) to the ground. You are watching, and measure with your stopwatch that it takes 3.25 \(\mathrm{s}\) for the can to reach the ground. Ignore air resistance. (a) What is the speed of the can just before it hits the ground? (b) Another painter is standing on a ledge, with hands 4.00 \(\mathrm{m}\) above the can when it falls off. He has lightning-fast reflexes and if the can passes in front of him, he can catch it. Does he get the chance?

A meter stick is held vertically above your hand, with the lower end between your thumb and first finger. On seeing the meter stick released, you grab it with these two fingers. You can calculate your reaction time from the distance the meter stick falls, read directly from the point where your fingers grabbed it. (a) Derive a relationship for your reaction time in terms of this measured distance, \(d\) . (b) If the measured distance is \(17.6 \mathrm{cm},\) what is the reaction time?

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