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WorksheetsRotation Unit (Team Trivia)
Total questions: 12
Worksheet time: 36mins
A point on the edge of a disk rotates around the center of the disk with an initial angular velocity of 3rad/s3rad/s clockwise. The graph shows the point’s angular acceleration as a function of time. The positive direction is considered to be counterclockwise. All frictional forces are considered to be negligible.
How can the graph be used to determine the angular speed of the disk after 2s2s? Justify your selection.
Determine the area bound by the line and the horizontal axis from 0s to 2s , because this area represents the final angular velocity of the point on disk.
Determine the area bound by the line and the horizontal axis from 0s to 2s , because this area represents the change in the angular velocity of the point on disk.
Determine the vertical-axis intercept, because this value represents the final angular velocity of the point on disk.
Determine the slope of the line, because this value represents the change in the angular velocity of the point on disk.
A point on a disk rotates around the center axle of the disk. The table shows the angular speed of the point as a function of time. Which of the following graphs could represent the angular position of the point as a function of time?
A disk is fixed to a horizontal axle that extends between two supports, as shown in the figure. Frictional forces between the axle and the supports is not negligible. At time ts , the disk rotates about the center axle with an initial angular speed ωd . A student measures the angular displacement Δθo of a point on the edge of the disk from time ts until the disk no longer rotates. The angular acceleration of the disk is determined to be αd , and this value remains constant. Based on the data, if possible, how could the student predict the angular displacement of a point on the edge of the disk from time ts until the disk no longer rotates if the initial angular speed is increased to 2ωd ? Justify your selection.
Use the equation ω2=ωo2+2α(θ−θo) because the disk comes to rest, ωo=2ωd and α=αd . Solve for θ−θo
Use the equation ω2=ωo2+2α(θ−θo) because the disk comes to rest, ωo=2ωd and α=2αd . Solve for θ−θo
An equation is not necessary, because the point on the edge of the disk will have the same angular displacement regardless of its initial angular velocity.
The angular displacement cannot be determined because an equation that includes a term for time must be used.
A group of students must conduct an experiment to determine how the location of an applied force on a classroom door affects the rotational motion of the door. The rotational inertia of the door about its hinges is known. The initial angular velocity of the door is zero.
Which of the following lists what measuring devices the students need and the measurements they should take to collect the necessary data to test the relationship between a torque exerted on the door and the change in angular velocity of that object about the hinges of the door? Justify your selection.
A protractor to measure the angular displacement of the door and a meterstick to measure the radial distance from the door's hinges to the location where the force is applied.
A stopwatch to measure the time interval during which the force is applied and a meterstick to measure the radial distance from the door's hinges to the location where the force is applied.
A force probe to measure the applied force on the door, and a stopwatch to measure the time interval during which the force is applied, and a meterstick to measure the radial distance from the door's hinges to the location where the force is applied.
A stopwatch to measure the time interval during which the force is applied, a force probe to measure the applied force on the door, a protractor to measure the angular displacement of the door, and a meterstick to measure the radial distance from the door's hinges to the location where the force is applied.
An object of mass M hangs from a string that is looped around a pulley of negligible friction, as shown. The pulley has a mass 0.5M. The object is released from rest and it falls to the floor at time t1 . Which of the following pairs of graphs best represents the angular speed as a function of time for the pulley and the vertical speed as a function of time for the falling object for a short time after it is released from rest?
A net torque is applied to the edge of a spinning object as it rotates about its internal axis. The table shows the net torque exerted on the object at different instants in time. How can a student use the data table to determine the change in angular momentum of the object from 0s to 6s? Justify your selection.
Multiply the maximum net torque by 6s6s, because ΔL=τΔt
Devide the maximum net torque by 6s, because ΔL=τΔt
Create a graph of net torque as a function of time and graph four points of data by using the table. Determine the slope of the curve from 0s to 6s, because the shape of the curve on the graph will be a right triangle and the slope can be directly determined.
Create a graph of net torque as a function of time and graph four points of data by using the table. Determine the area bound by the curve and the horizontal axis from 0s0s to 6s6s, because the shape of the curve on the graph will be a right triangle and the area can be directly determined.
A uniform disk with mass Mo and radius R is mounted on a vertical axis so that it can rotate freely in a horizontal plane. The rotational inertia of the disk is Io. The disk is initially at rest. If force Fo is exerted tangentially to the rim of the disk for time interval Δt, the final angular momentum of the disk is Lo.
Consider a second disk that has the same mass Mo as the first disk, but its radius is 2R. The rotational inertia of this disk is 4Io. If the same force Fo is exerted tangentially to the rim of the disk for the same time interval Δt, then the final angular momentum of the second disk would be
Lo
2Lo
4Lo
8Lo
One end of a horizontal rod is connected to an axle that is connected to a motor that can be adjusted to change the angular speed of the rod as it rotates in a horizontal circle. Students must determine the change in angular momentum of the rod after 10s. The students use the following procedure.
1. Measure the length of the rod with a meterstick.
2. Ensure that the rod is at rest.
3. Start the stopwatch and simultaneously adjust the motor so that the rod rotates around the axle as the angular speed is slowly increased.
4. Record the angular speed of the rod when the stopwatch reads 10s.
The students are provided with the equation for the rotational inertia of the rod about one end, I=3ML2 . Which of the following steps should the students add to the procedure to ensure that the change in angular momentum of the rod can be determined?
Record the initial angular speed of the rod
Measure the thickness of the rod with a meterstick
Determine the net torque exerted on the rod from the axle by using a force probe
Measure the mass of the rod.
Three disks are concentrically attached to one another, and four rods of negligible mass are attached to the outer disk. Identical objects of mass Mo can be attached to the rods, and their positions on the rods can be adjusted. The disks, rods, and objects form a system that freely rotates around a central axis that is perpendicular to the plane of the page. The objects are initially a distance D away from the axis of rotation. A constant force Fo is applied tangent to the second disk, as shown in the figure. How can the system be changed so that the change in angular momentum of the system per unit of time is increased?
Move the objects of mass Mo farther away from the axis of rotation.
Move the objects of mass Mo closer to the axis of rotation.
Increase the magnitude of the net torque exerted on the system.
Decrease the magnitude of the net torque exerted on the system.
A uniform rod is at rest on a horizontal surface. A student may launch a sphere of clay toward the rod along one of the three paths shown in the figure. Path X and path Z are directed toward the center of mass of the rod. In each case, the sphere of clay is launched with the same linear speed and sticks to the rod. In each case, the time of collision between the sphere of clay and the rod is time to . A pivot is fixed to the end of the rod, representing the point at which the rod or clay-rod system may rotate. Frictional forces are considered to be negligible.
A sphere of clay travels toward the rod along path ZZ. A student must predict what will happen to the linear momentum and the angular momentum of the rod-sphere system as a result of the collision. Which of the following correctly predicts the change, if any, of these quantities?
Linear Momentum --> No Change
Angular Momentum
--> No Change
Linear Momentum --> No Change
Angular Momentum
--> Decreases
Linear Momentum --> Decreases
Angular Momentum
--> No Change
Linear Momentum --> Decreases
Angular Momentum
--> Decreases
A merry-go-round disk with a rotational inertia of Id about its center spins around its center axle with an initial angular velocity of ω0. A child is standing near the edge of the merry-go-round, as shown in Figure 1. The child’s rotational inertia about the center of the disk when near the edge is I0. As the merry-go-round spins, the child moves closer to the center, as shown in Figure 2, until the disk rotates with an angular velocity of ω1. Which of the following equations could a student use to determine the rotational inertia Is of the child-merry-go-round system about the center axle immediately after the child has moved to the location shown in Figure 2? Justify your selection.
Idω0=Isω1 because the initial momentum of the merry-go-round is equal to the final angular momentum of the system
Idω0=Isω1 because the initial angular momentum of the child is equal to the final angular momentum of the system.
(Id+I0)ω0=Isω1 because the sum of the initial angular momenta of the merry-go-round and the child is equal to the final angular momentum of the system.
(Id−I0)ω0=Isω1 because the difference between the initial angular momenta of the merry-go-round and the child is equal to the final angular momentum of the system.
An isolated spherical star of radius R0 rotates about an axis that passes through its center with an angular velocity of ω0. Gravitational forces within the star cause the star’s radius to collapse and decrease to a value r0 < R0, but the mass of the star remains constant. A graph of the star’s angular velocity as a function of time as it collapses is shown. Which of the following predictions is correct about the angular momentum L of the star immediately after the collapse?
L will be greater after the collapse
L will be less after the collapse
L will remain the same before and after the collapse
L will be the same after the collapse, but will change direction
