Skip to main content
Ch 10: Dynamics of Rotational Motion
Young & Freedman Calc - University Physics 14th Edition
Young & Freedman Calc14th EditionUniversity PhysicsISBN: 9780321973610Not the one you use?Change textbook
Chapter 10, Problem 45b

A large wooden turntable in the shape of a flat uniform disk has a radius of 2.00 m and a total mass of 120 kg. The turntable is initially rotating at 3.00 rad/s about a vertical axis through its center. Suddenly, a 70.0-kg parachutist makes a soft landing on the turntable at a point near the outer edge. Compute the kinetic energy of the system before and after the parachutist lands. Why are these kinetic energies not equal?

Verified step by step guidance
1
First, calculate the initial kinetic energy of the turntable. The formula for the kinetic energy of a rotating object is \( KE = \frac{1}{2} I \omega^2 \), where \( I \) is the moment of inertia and \( \omega \) is the angular velocity. For a uniform disk, the moment of inertia \( I \) is given by \( I = \frac{1}{2} m r^2 \), where \( m \) is the mass and \( r \) is the radius.
Substitute the values for the turntable into the moment of inertia formula: \( I = \frac{1}{2} \times 120 \text{ kg} \times (2.00 \text{ m})^2 \). Then, use this \( I \) to find the initial kinetic energy using \( \omega = 3.00 \text{ rad/s} \).
Next, calculate the moment of inertia of the system after the parachutist lands. The parachutist can be treated as a point mass at a distance \( r \) from the axis of rotation. The new moment of inertia \( I' \) is the sum of the turntable's moment of inertia and the parachutist's contribution: \( I' = I + m_p r^2 \), where \( m_p \) is the parachutist's mass.
After the parachutist lands, the angular velocity \( \omega' \) changes due to conservation of angular momentum. The initial angular momentum \( L = I \omega \) must equal the final angular momentum \( L' = I' \omega' \). Solve for \( \omega' \) using \( \omega' = \frac{I \omega}{I'} \).
Finally, compute the kinetic energy of the system after the parachutist lands using \( KE' = \frac{1}{2} I' \omega'^2 \). The kinetic energies before and after are not equal because the parachutist landing on the turntable increases the moment of inertia, which decreases the angular velocity, leading to a lower kinetic energy despite the conservation of angular momentum.

Verified video answer for a similar problem:

This video solution was recommended by our tutors as helpful for the problem above.
Video duration:
11m
Was this helpful?

Key Concepts

Here are the essential concepts you must grasp in order to answer the question correctly.

Rotational Kinetic Energy

Rotational kinetic energy is the energy due to the rotation of an object and is given by the formula KE = 0.5 * I * ω², where I is the moment of inertia and ω is the angular velocity. For a uniform disk, the moment of inertia is I = 0.5 * m * r². Understanding this concept is crucial for calculating the kinetic energy of the turntable before and after the parachutist lands.
Recommended video:
Guided course
06:07
Intro to Rotational Kinetic Energy

Conservation of Angular Momentum

The conservation of angular momentum states that if no external torques act on a system, the total angular momentum remains constant. When the parachutist lands on the turntable, the system's angular momentum before and after the landing must be equal, allowing us to find the new angular velocity and subsequently the kinetic energy after the landing.
Recommended video:
Guided course
12:12
Conservation of Angular Momentum

Inelastic Collision

An inelastic collision is one in which kinetic energy is not conserved, although momentum is. When the parachutist lands on the turntable, the collision is inelastic because the parachutist and turntable move together afterward, leading to a loss of kinetic energy due to the conversion of some energy into other forms, such as heat or sound.
Recommended video:
Guided course
04:18
Completely Inelastic Collisions
Related Practice
Textbook Question

A solid wood door 1.00 m wide and 2.00 m high is hinged along one side and has a total mass of 40.0 kg. Initially open and at rest, the door is struck at its center by a handful of sticky mud with mass 0.500 kg, traveling perpendicular to the door at 12.0 m/s just before impact. Find the final angular speed of the door. Does the mud make a significant contribution to the moment of inertia?

Textbook Question

A thin uniform rod has a length of 0.500 m0.500\(\text{ m}\) and is rotating in a circle on a frictionless table. The axis of rotation is perpendicular to the length of the rod at one end and is stationary. The rod has an angular velocity of 0.400 rad/s0.400\(\text{ rad/s}\) and a moment of inertia about the axis of 3.00×103kg/m23.00\(\times\)10^{-3}\(\text{kg/m}\)^2. A bug initially standing on the rod at the axis of rotation decides to crawl out to the other end of the rod. When the bug has reached the end of the rod and sits there, its tangential speed is 0.160 m/s0.160\(\text{ m/s}\). The bug can be treated as a point mass. What is the mass of the rod.

2
views
Textbook Question

A small 10.0-g bug stands at one end of a thin uniform bar that is initially at rest on a smooth horizontal table. The other end of the bar pivots about a nail driven into the table and can rotate freely, without friction. The bar has mass 50.0 g and is 100 cm in length. The bug jumps off in the horizontal direction, perpendicular to the bar, with a speed of 20.0 cm/s relative to the table. What is the angular speed of the bar just after the frisky insect leaps?

Textbook Question

A large wooden turntable in the shape of a flat uniform disk has a radius of 2.00 m and a total mass of 120 kg. The turntable is initially rotating at 3.00 rad/s about a vertical axis through its center. Suddenly, a 70.0-kg parachutist makes a soft landing on the turntable at a point near the outer edge. Find the angular speed of the turntable after the parachutist lands. (Assume that you can treat the parachutist as a particle.)

1
views
Textbook Question

The Spinning Figure Skater. The outstretched hands and arms of a figure skater preparing for a spin can be considered a slender rod pivoting about an axis through its center (Fig. E10.43). When the skater's hands and arms are brought in and wrapped around his body to execute the spin, the hands and arms can be considered a thinwalled, hollow cylinder. His hands and arms have a combined mass of 8.0 kg. When outstretched, they span 1.8 m; when wrapped, they form a cylinder of radius 25 cm. The moment of inertia about the rotation axis of the remainder of his body is constant and equal to 0.40 kg m2 . If his original angular speed is 0.40 rev/s, what is his final angular speed?

3
views
Textbook Question

Suppose that an asteroid traveling straight toward the center of the earth were to collide with our planet at the equator and bury itself just below the surface. What would have to be the mass of this asteroid, in terms of the earth's mass M, for the day to become 25.0% longer than it presently is as a result of the collision? Assume that the asteroid is very small compared to the earth and that the earth is uniform throughout.

1
views