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A \(0.100-\mathrm{kg}\) ball is thrown straight up into the air with an initial speed of \(15.0 \mathrm{m} / \mathrm{s} .\) Find the momentum of the ball (a) at its maximum height and (b) halfway up to its maximum height.

Short Answer

Expert verified
The momentum of the ball at its maximum height is \( 0 \, \mathrm{kgm/s} \), and halfway up to its maximum height is \( 0.745 \, \mathrm{kgm/s} \).

Step by step solution

01

Find the Velocity at Maximum Height

Using the principle of conservation of energy, when the ball reaches its maximum height, its velocity will be zero because all the kinetic energy would have been converted to potential energy. Thus, the velocity \( v_{max} = 0 \mathrm{m/s} \) .
02

Compute the Momentum at Maximum Height

The momentum of an object is computed as the product of its mass and velocity. Therefore, the momentum \( p_{max} \) at maximum height is given by \( p_{max} = m \cdot v_{max} = 0.100 \cdot 0 = 0 \mathrm{kgm/s} \) . The momentum is zero because the ball has lost all its speed at maximum height.
03

Find the Velocity Halfway to Maximum Height

The time it takes for the ball to reach its maximum height is given by \( t_{max} = v_{i} / g \) , where \( v_{i} = 15.0 \mathrm{m/s} \) is the initial velocity and \( g = 9.8 \mathrm{m/s^{2}} \) is the acceleration due to gravity. Therefore, \( t_{max} = 15.0 / 9.8 = 1.53 s \) . Halfway up would be at \( t_{half} = 0.5 \cdot t_{max} = 0.5 \cdot 1.53 = 0.77 s \) . The velocity \( v_{half} \) at this moment can be computed using the equation \( v_{half} = v_{i} - g \cdot t_{half} = 15 - 9.8 \cdot 0.77 = 7.45 \mathrm{m/s} \) .
04

Compute the Momentum Halfway to Maximum Height

The momentum \( p_{half} \) halfway up to maximum height is given by \( p_{half} = m \cdot v_{half} = 0.100 \cdot 7.45 = 0.745 \mathrm{kgm/s} \) .
05

Interpret the Results

The momentum of the ball decreases as it travels upward due to the opposing force of gravity. At maximum height, the ball loses all its speed and thus the momentum is zero. Halfway up to maximum height, the ball still has some speed, hence some momentum.

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Key Concepts

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

Conservation of Energy
The principle of conservation of energy is critical in solving problems involving objects in motion, like our ball being thrown into the air. According to this principle, the energy within a closed system must remain constant. In simpler terms, energy can change forms but it can never be created or destroyed.

In the context of the ball being thrown, the energy the ball possesses at launch is all kinetic energy due to its motion. As it travels upward, this kinetic energy is gradually converted into potential energy, which is energy stored due to its height above the ground.

When the ball reaches its maximum height, all of its initial kinetic energy has been transformed into potential energy. At this very point, the velocity of the ball is zero, meaning it temporarily pauses before it starts descending. This is why at the maximum height, the velocity is zero, leading to zero momentum at this point.

  • Initial Energy: Kinetic
  • Energy Transformation: Kinetic to Potential
  • Final Energy at Max Height: All Potential
Kinematics
Kinematics deals with the motion of objects without considering the causes of this motion, like forces. It gives us the tools to analyze how the ball moves upwards and what happens at different points in its journey.

When analyzing the ball's motion, we focus on its velocity at different stages:
  • At launch, the initial velocity is given, as it's thrown up with 15 m/s.
  • Halfway up, the velocity changes due to gravitational deceleration.
This is where kinematic equations come into play, specifically \[ v = v_i - gt \]where:
  • \( v \) is the velocity at any point in time.
  • \( v_i \) is the initial velocity.
  • \( g \) is the acceleration due to gravity (a constant \( 9.8 \ m/s^2 \)).
  • \( t \) is the time elapsed.
The ball's velocity halfway is found by inserting the halfway time into the equation. It becomes clear how the velocity reduces as it climbs, impacted by gravity.
Momentum Calculation
Momentum is a measure of the motion of an object expressed as the product of its mass and velocity. In our exercise of the ball thrown upward, momentum shifts as the ball ascends.

At its maximum height, the ball's velocity is zero, since it stops momentarily before starting to fall back down. This gives it a momentum of zero at this point, as calculated by the equation:\[ p = m imes v \]where:
  • \( p \) denotes momentum
  • \( m \) is mass
  • \( v \) signifies velocity
Halfway up the flight, the ball retains some velocity despite losing part of its initial speed to gravity. Hence, its momentum at halfway point is calculated with the velocity at halfway.

It's insightful to observe how momentum behaves along the ball's path:
  • At the base or initial point, momentum is at its peak due to maximum velocity.
  • It diminishes as the ball climbs higher and slows down.
  • At maximum height, momentum reaches zero since the speed is zero.
  • Halfway momentum reflects partial velocity reduction.
Understanding these shifts in momentum offers a solid grasp of how mass and velocity interplay to influence momentum in any moving body.

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Most popular questions from this chapter

A billiard ball moving at \(5.00 \mathrm{m} / \mathrm{s}\) strikes a stationary ball of the same mass. After the collision, the first ball moves, at \(4.33 \mathrm{m} / \mathrm{s},\) at an angle of \(30.0^{\circ}\) with respect to the original line of motion. Assuming an elastic collision (and ignoring friction and rotational motion), find the struck ball's velocity after the collision.

A neutron in a nuclear reactor makes an elastic head-on collision with the nucleus of a carbon atom initially at rest. (a) What fraction of the neutron's kinetic energy is transferred to the carbon nucleus? (b) If the initial kinetic energy of the neutron is \(1.60 \times 10^{-13} \mathrm{J},\) find its final kinetic energy and the kinetic energy of the carbon nucleus after the collision. (The mass of the carbon nucleus is nearly 12.0 times the mass of the neutron.)

Sand from a stationary hopper falls onto a moving conveyor belt at the rate of \(5.00 \mathrm{kg} / \mathrm{s}\) as in Figure \(\mathrm{P} 9.72 .\) The conveyor belt is supported by frictionless rollers and moves at a constant speed of \(0.750 \mathrm{m} / \mathrm{s}\) under the action of a constant horizontal external force \(\mathbf{F}_{\text {ext }}\) supplied by the motor that drives the belt. Find (a) the sand's rate of change of momentum in the horizontal direction, (b) the force of friction exerted by the belt on the sand, (c) the external force \(\mathbf{F}_{\mathrm{ext}},\) (d) the work done by \(\mathbf{F}_{\mathrm{ext}}\) in \(1 \mathrm{s},\) and \((\mathrm{e})\) the kinetic energy acquired by the falling sand each second due to the change in its horizontal motion. (f) Why are the answers to \((\mathrm{d})\) and \((\mathrm{e})\) different?

Rocket Science. A rocket has total mass \(M_{i}=360 \mathrm{kg}\) including \(330 \mathrm{kg}\) of fuel and oxidizer. In interstellar space it starts from rest, turns on its engine at time \(t=0\) and puts out exhaust with relative speed \(v_{e}=1500 \mathrm{m} / \mathrm{s}\) at the constant rate \(k=2.50 \mathrm{kg} / \mathrm{s} .\) The fuel will last for an actual burn time of \(330 \mathrm{kg} /(2.5 \mathrm{kg} / \mathrm{s})=132 \mathrm{s},\) but define a "projected depletion time" as \(T_{p}=M_{i} / k=\) 144 s. (This would be the burn time if the rocket could use its payload and fuel tanks as fuel, and even the walls of the combustion chamber.) (a) Show that during the burn the velocity of the rocket is given as a function of time by $$v(t)=-v_{e} \ln \left[1-\left(t / T_{p}\right)\right]$$ (b) Make a graph of the velocity of the rocket as a function of time for times running from 0 to 132 s. (c) Show that the acceleration of the rocket is $$ a(t)=v_{e} /\left(T_{p}-t\right) $$ (d) Graph the acceleration as a function of time. (e) Show that the position of the rocket is $$ x(t)=v_{e}\left(T_{p}-t\right) \ln \left[1-\left(t / T_{p}\right)\right]+v_{e} t $$ (f) Graph the position during the burn.

A golf club consists of a shaft connected to a club head. The golf club can be modeled as a uniform rod of length \(\ell\) and mass \(m_{1}\) extending radially from the surface of a sphere of radius \(R\) and mass \(m_{2} .\) Find the location of the club's center of mass, measured from the center of the club head.

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