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A large wooden turntable in the shape of a flat uniform disk has a radius of \(2.00 \mathrm{~m}\) and a total mass of \(120 \mathrm{~kg}\). The turntable is initially rotating at \(3.00 \mathrm{rad} / \mathrm{s}\) about a vertical axis through its center. Suddenly, a \(70.0 \mathrm{~kg}\) parachutist makes a soft landing on the turntable at a point near the outer edge. (a) Find the angular speed of the turntable after the parachutist lands. (Assume that you can treat the parachutist as a particle.) (b) Compute the kinetic energy of the system before and after the parachutist lands. Why are these kinetic energies not equal?

Short Answer

Expert verified
The final angular speed of the turntable after the parachutist lands is calculated by applying angular momentum conservation. The kinetic energy before and after the landing are different due to the external work done by the parachutist when landing.

Step by step solution

01

Compute initial angular momentum

Calculate the initial angular momentum of the turntable. The moment of inertia \(I\) of a disk is given by \(I = \frac{1}{2} m r^2\), where \(m\) is the mass and \(r\) is the radius of the disk. The initial angular momentum \(L_i\) can be obtained from \(L_i = I \omega_i\), where \(\omega_i\) is the initial angular speed. So, first compute the moment of inertia of the disk and then use it to find the initial angular momentum.
02

Compute final angular momentum

Find the final angular momentum after the parachutist lands. The parachutist can be considered as a particle with mass \(m_p\) at radius \(r\) from the centre of the turntable. So, the moment of inertia of the parachutist- turntable system after landing is \(I_f = I + m_p r^2\) . The final angular momentum \(L_f\) is equal to the initial angular momentum \(L_i\) because of the conservation of angular momentum. At this stage, you calculate the final angular momentum.
03

Compute final angular speed

Calculate the final angular speed \(\omega_f\) using \(\omega_f = \frac{L_f}{I_f}\). At this point, you can solve this equation to find the final angular speed after the parachutist landing.
04

Calculate initial and final kinetic energy

Finally, calculate the initial and final kinetic energy of the system using the formula for rotational kinetic energy \(KE = \frac{1}{2} I \omega^2\). Plug the values of initial and final moment of inertia and angular speed for initial and final energy.
05

Explain energy non-conservation

The values of initial and final kinetic energy will not be the same. The reason for this is the external work done by the parachutist when landing on the turntable. This energy has gone into rotating the turntable. Therefore, the conservation of energy does not apply in this case.

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Key Concepts

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

Moment of Inertia
The moment of inertia is a measure of an object’s resistance to changes in its rotation rate. When you think about mass in linear motion, it's about the resistance to changes in velocity, and similarly, the moment of inertia is the rotational analog. It depends not just on the mass of an object but also on how that mass is distributed relative to the axis of rotation.

For a solid disk like the turntable described in the exercise, the moment of inertia is calculated using the formula \(I = \frac{1}{2} m r^2\), where \(m\) is the mass and \(r\) is the radius. A larger radius or mass will increase the moment of inertia, making it harder to spin or stop the disk. Since adding the parachutist changes the distribution of mass, it also changes the system's moment of inertia, influencing how it rotates thereafter.

It’s important to remember the physical interpretation of the moment of inertia when facing problems about rotational motion, as it dictates how the velocity of rotation changes when an external force or torque is applied.
Angular Speed
Angular speed is how fast something rotates or revolves relative to another point, namely, how fast the angular position or orientation of an object is changing with time. It is usually measured in radians per second (rad/s).

Imagine you're on a carousel that’s turning; your angular speed would be how quickly you're going around in a circle. The initial angular speed of the turntable in the exercise is given as \(3.00 \mathrm{rad/s}\). When the parachutist lands on the turntable, it will affect the overall angular speed due to the conservation of angular momentum, which is a crucial concept when dealing with these systems. Even though the angular momentum remains constant (if no external torque acts), the angular speed can change if the moment of inertia changes.
Rotational Kinetic Energy
Rotational kinetic energy is the energy an object possesses due to its rotation. It is given by the formula \(KE = \frac{1}{2} I \omega^2\), where \(I\) is the moment of inertia and \(\omega\) is the angular speed. When an ice skater pulls in her arms, she reduces her moment of inertia but her rotational kinetic energy remains constant if no external forces act. This conservation leads to an increase in her spinning speed.

In our example, the final rotational kinetic energy of the system changes when the parachutist lands because an external force has acted (the force exerted by the parachutist during the landing), which is not considered in the isolated system of the rotational kinetic energy. Hence, the energy is not conserved, and this difference can help us understand the work done by external forces in similar situations.
Physical Systems and Energy Conservation
In physics, energy conservation is a fundamental concept stating that the total energy of an isolated system remains constant over time. This principle can be applied to many types of energy, including kinetic, potential, thermal, and various others. However, the conservation of energy within a physical system assumes there are no external forces acting upon it.

In the case of the turntable and parachutist, energy conservation is not observed because the parachutist performs work on the system, thereby adding energy to it. As a result, we see a discrepancy between the initial and final kinetic energies. This teaches us an important lesson: when solving problems related to energy conservation, always consider whether external forces or work could be influencing the system's total energy, which might lead to a non-conservation situation as seen in this exercise.

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Most popular questions from this chapter

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