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A cylindrically shaped space station is rotating about the axis of the cylinder to create artificial gravity. The radius of the cylinder is \(82.5 \mathrm{~m}\). The moment of inertia of the station without people is \(3.00 \times 10^{9} \mathrm{~kg} \cdot \mathrm{m}^{2}\). Suppose 500 people, with an average mass of \(70.0 \mathrm{~kg}\) each, live on this station. As they move radially from the outer surface of the cylinder toward the axis, the angular speed of the station changes. What is the maximum possible percentage change in the station's angular speed due to the radial movement of the people?

Short Answer

Expert verified
The maximum percentage change in angular speed is approximately 7.94%.

Step by step solution

01

Determine Initial Moment of Inertia

The total initial moment of inertia, when all people are on the cylinder's surface, can be calculated as the sum of the cylinder's moment of inertia and the moment of inertia contributed by the people: \[ I_0 = I_{ ext{cylinder}} + n m r^2 \] where \( I_{ ext{cylinder}} = 3.00 \times 10^9 \ \text{kg} \cdot \text{m}^2 \), \( n = 500 \), \( m = 70.0 \ \text{kg} \), and \( r = 82.5 \ \text{m} \). Let's calculate \( I_0 \):\[ I_0 = 3.00 \times 10^9 + 500 \times 70.0 \times (82.5)^2 \text{ kg} \cdot \text{m}^2 \].
02

Calculate Initial Moment of Inertia Value

Perform the calculation for the initial moment of inertia:\[ I_0 = 3.00 \times 10^9 + 500 \times 70.0 \times 6806.25 \]\[ = 3.00 \times 10^9 + 238218750 \]\[ = 3.23821875 \times 10^9 \ \text{kg} \cdot \text{m}^2 \].
03

Determine Final Moment of Inertia

When the people move to the axis, their moment of inertia contribution becomes zero, so the final moment of inertia is just that of the cylinder:\[ I_{ ext{final}} = I_{ ext{cylinder}} = 3.00 \times 10^9 \ \text{kg} \cdot \text{m}^2 \].
04

Apply Conservation of Angular Momentum

According to the conservation of angular momentum, the initial angular momentum equals the final angular momentum:\[ I_0 \omega_0 = I_{ ext{final}} \omega_{ ext{final}} \].Rearrange to find the expression for the ratio of the final angular speed to initial angular speed:\[ \frac{\omega_{ ext{final}}}{\omega_0} = \frac{I_0}{I_{ ext{final}}} \].
05

Calculate Percentage Change in Angular Speed

Plug in values to calculate \( \frac{\omega_{ ext{final}}}{\omega_0} \):\[ \frac{\omega_{ ext{final}}}{\omega_0} = \frac{3.23821875 \times 10^9}{3.00 \times 10^9} \approx 1.0794 \].Calculate the percentage change:\[ \text{Percentage Change} = \left( \frac{\omega_{ ext{final}} - \omega_0}{\omega_0} \right) \times 100\% \approx (1.0794 - 1) \times 100\% = 7.94\% \].

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Key Concepts

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

Artificial Gravity
In a space environment where there is no natural gravity, creating an artificial version is crucial for the comfort and health of astronauts. But how do we achieve this seemingly impossible feat? One ingenious solution is using a rotating cylindrical space station. The rotation mimics the gravitational pull we experience on Earth by creating a centripetal force.

Imagine a giant cylinder spinning in space. As it rotates, the people inside experience a force pushing them against the outer wall. This force makes them feel like they are being pulled by gravity, thus creating the sensation of artificial gravity. Here's a simplified breakdown of the key ideas:
  • **Rotation:** The central concept is that the faster the cylinder spins, the stronger the artificial gravity feels.
  • **Centripetal Force:** This force is crucial as it acts towards the center of the circle, but to someone inside the cylinder, it feels like gravity.
  • **Design:** The size and speed of rotation are carefully calculated to mimic Earth's gravity, often targeting 9.8 m/s².
This clever design allows astronauts to move and live more normally in space, reducing the health issues associated with prolonged weightlessness.
Conservation of Angular Momentum
As people move around within the space station, the principles of physics ensure that some things remain constant. One such principle is the conservation of angular momentum, a fundamental concept in rotational dynamics.

Angular momentum can be thought of as the rotational counterpart to linear momentum. This means that when no external torques are acting on a system, its angular momentum remains constant. In our space station scenario:
  • When people move towards or away from the axis, the distribution of mass changes.
  • The moment of inertia adjusts because it depends on the mass distribution relative to the axis of rotation.
  • As a result, the angular speed compensates to conserve the overall angular momentum, unless acted upon by external forces.
This principle helps explain why the angular speed of the station changes when people move toward its center. It's a natural balancing act that keeps the rotational system stable.
Angular Speed
Angular speed is a measure of how quickly something rotates around an axis. When many of us first learn about speed, we think in terms of meters per second or miles per hour. But when it comes to rotation, angular speed uses angles, usually measured in radians, per unit of time.

In the context of our space station, angular speed is affected by the distribution of mass within the station. Here's what happens:
  • Initially, people contribute to the overall moment of inertia when they are at the outer edge.
  • As people move inward, the moment of inertia decreases because the mass is closer to the rotation axis.
  • According to the conservation of angular momentum, when the moment of inertia decreases, the angular speed must increase to keep the system balanced.
The change in angular speed is a direct consequence of the spatial re-distribution of mass inside the station, offering a real-life application of rotational physics.
Cylindrical Space Station
The concept of a cylindrical space station is not just a fanciful idea from science fiction but a practical design that helps generate artificial gravity. The physics and technology behind this design incorporate some fundamental principles that allow it to function effectively in space.

Here are some key aspects of a cylindrical space station:
  • **Shape and Rotation:** The cylindrical shape is chosen specifically for its ability to create a uniform centripetal force as it rotates, making it more efficient at simulating gravity.
  • **Advantages of Design:** Cylinders can house large populations while maintaining structural integrity even at high speeds.
  • **Living Space:** The rotation creates artificial gravity along the outer walls, allowing standard living spaces for the crew, complete with floors, ceilings, and walls.
This design allows for a sustainable environment where astronauts can live and work for extended periods, significantly improving their quality of life in space.

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Most popular questions from this chapter

Concept Questions The drawing shows two identical systems of objects; each consists of three small balls (masses \(m_{1}, m_{2}\), and \(m_{3}\) ) connected by massless rods. In both systems the axis is perpendicular to the page, but it is located at a different place, as shown. (a) Do the systems necessarily have the same moments of inertia? If not, why not? (b) The same force of magnitude \(F\) is applied to the same ball in each system (see the drawing). Is the magnitude of the torque created by the applied force greater for system A or for system B? Or is the magnitude the same in the two cases? Explain. (c) The two systems start from rest. Will system A or system B have the greater angular speed at the same later time? Or will they have the same angular speeds? Justify your answer. Problem The masses of the balls are \(m_{1}=9.00 \mathrm{~kg}, m_{2}=6.00 \mathrm{~kg}\), and \(m_{3}=7.00 \mathrm{~kg}\). The magnitude of the force is \(F=424 \mathrm{~N}\). (a) For each of the two systems, determine the moment of inertia about the given axis of rotation. (b) Calculate the torque (magnitude and direction) acting on each system. (c) Both systems start from rest, and the direction of the force moves with the system and always points along the \(4.00-\mathrm{m}\) rod. What is the angular velocity of each system

A particle is located at each corner of an imaginary cube. Each edge of the cube is \(0.25 \mathrm{~m}\) long, and each particle has a mass of \(0.12 \mathrm{~kg}\). What is the moment of inertia of these particles with respect to an axis that lies along one edge of the cube?

A small \(0.500-\mathrm{kg}\) object moves on a frictionless horizontal table in a circular path of radius \(1.00 \mathrm{~m}\). The angular speed is \(6.28 \mathrm{rad} / \mathrm{s}\). The object is attached to a string of negligible mass that passes through a small hole in the table at the center of the circle. Someone under the table begins to pull the string downward to make the circle smaller. If the string will tolerate a tension of no more than \(105 \mathrm{~N}\), what is the radius of the smallest possible circle on which the object can move?

Interactive LearningWare 9.1 at reviews the concepts that are important in this problem. One end of a meter stick is pinned to a table, so the stick can rotate freely in a plane parallel to the tabletop (see the drawing). Two forces, both parallel to the tabletop, are applied to the stick in such a way that the net torque is zero. One force has a magnitude of \(4.00 \mathrm{~N}\) and is applied perpendicular to the stick at the free end. The other force has a magnitude of \(6.00 \mathrm{~N}\) and acts at a \(60.0^{\circ}\) angle with respect to the stick. Where along the stick is the 6.00 -N force applied? Express this distance with respect to the axis of rotation.

Concept Questions As seen from above, a playground carousel is rotating counterclockwise about its center on frictionless bearings. A person standing still on the ground grabs onto one of the bars on the carousel very close to its outer edge and climbs aboard. Thus, this person begins with an angular speed of zero and ends up with a nonzero angular speed, which means that he underwent a counterclockwise angular acceleration. (a) What applies the force to the person to create the torque causing this acceleration? What is the direction of this force? (b) According to Newton's actionreaction law, what can you say about the direction of the force applied to the carousel by the person and about the nature (clockwise or counterclockwise) of the torque that it creates? (c) Does the torque identified in part (b) increase or decrease the angular speed of the carousel? Problem The carousel has a radius of \(1.50 \mathrm{~m}\), an initial angular speed of \(3.14 \mathrm{rad} / \mathrm{s}\), and a moment of inertia of \(125 \mathrm{~kg} \cdot \mathrm{m}^{2}\). The mass of the person is \(40.0 \mathrm{~kg}\). Find the final angular speed of the carousel after the person climbs aboard. Verify that your answer is consistent with your answers to the Concept Questions.

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