A force of acts at a point from a fixed axis. The angle between the force and the radius from the axis is .
What is the magnitude of the torque about the axis?
Two equal and opposite forces of magnitude act on a rigid body. Their parallel lines of action are separated by a perpendicular distance of .
The resultant force and the magnitude of the torque of the couple are
and
and
and
and
A uniform horizontal beam of length and weight is pivoted at its left-hand end. A downward force of acts at the right-hand end. A vertical upward force acts at a point from the pivot.
The magnitude of required for rotational equilibrium is

A wheel has an initial angular speed of and a uniform angular acceleration of .
The angular displacement after is
A rigid disc rotates with constant angular speed . Point P is from the axis and point Q is from the axis.
The correct comparison of the centripetal accelerations of P and Q is
A flywheel has moment of inertia . A constant resultant torque of acts on it from rest for .
The angular speed after is
A rotating skater has moment of inertia and angular speed . The skater pulls in their arms so that the moment of inertia becomes . No external torque acts.
The final angular speed is
A student pushes on a door at a point from the hinge. The force has magnitude and acts at to the line from the hinge to the point of application.

Calculate the magnitude of the torque about the hinge.
State the condition on the angle for this force to produce maximum torque about the hinge.
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Two parallel forces of magnitude act on a rigid plate. The forces are opposite in direction and their lines of action are separated by .

Explain why this pair of forces can cause rotation without causing translational acceleration of the centre of mass.
Calculate the magnitude of the torque of the couple.
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Three small masses are fixed to a light rod that rotates about an axis perpendicular to the rod through its centre. The masses are arranged along the rod as follows.
The moment of inertia of the system about the axis is
A rigid body of moment of inertia is initially at rest. A torque of acts for in the positive sense. A torque of then acts for in the opposite sense.
The final angular speed is
A body rotates with angular momentum . Its moment of inertia decreases from to while no external torque acts.
The rotational kinetic energy changes by a factor of
A uniform horizontal beam of weight is supported by a pivot at its left end and a vertical cable at its right end. The beam is long. A load of weight is placed from the pivot.

State the condition for the beam to be in rotational equilibrium.
Determine the tension in the cable.
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A point on the rim of a rotating disc is from the axis. The disc rotates at .
Calculate the angular speed of the disc in .
Calculate the linear speed of the point on the rim.
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The graph shows the variation of angular velocity with time for a motor shaft. The angular acceleration is uniform over the interval shown.

State the physical quantity represented by the gradient of the graph.
The angular velocity increases from to in . Determine the angular displacement during this interval.
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Three small masses are fixed to a light rigid frame that rotates about an axis perpendicular to the frame. Their distances from the axis are shown.

Calculate the moment of inertia of the system about the axis.
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A flywheel of moment of inertia is initially at rest. A constant resultant torque of acts on it for .
Determine the angular acceleration of the flywheel.
Determine the angular speed after .
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A student investigates the torque produced on a light gate by applying the same force at the handle at different angles to the radius line from the hinge.

Use the data to determine the torque when the angle between the force and the radius line is .
State the angle at which the torque is greatest.
Explain why the torque becomes zero when the force is directed through the hinge.
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Two equal and opposite tangential forces are applied to a steering wheel to turn it while its centre remains fixed.

State the resultant force on the steering wheel due to the two applied forces.
Calculate the torque of the couple.
Explain why the wheel can have angular acceleration even though the resultant force is zero.
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Two coaxial discs are free to rotate without external torque. Disc 1 has moment of inertia and rotates clockwise at . Disc 2 has moment of inertia and rotates counter-clockwise at . The discs are then clamped together.
Taking clockwise as positive, the common final angular velocity is
clockwise
counter-clockwise
clockwise
clockwise
A solid cylinder of mass and radius rolls without slipping from rest down a slope. The vertical drop of its centre of mass is . The moment of inertia of the cylinder about its central axis is .
The speed of the centre of mass at the bottom of the slope is

Two coaxial turntables are initially separate. Turntable A has moment of inertia and angular velocity . Turntable B has moment of inertia and angular velocity . The turntables are brought into contact and rotate together with common angular velocity . External torque is negligible.

State why angular momentum is conserved during the contact process.
Calculate the common angular velocity after contact.
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A variable resultant torque acts on a rotor. The graph shows torque against time . Counter-clockwise torque is taken as positive.

State the quantity represented by the signed area under the torque-time graph.
The positive triangular area is and the negative triangular area is . Determine the change in angular momentum of the rotor.
The rotor has moment of inertia and is initially at rest. Calculate its final angular velocity.
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A skater rotates with angular speed and moment of inertia . The skater pulls in their arms so that the moment of inertia becomes . External torque is negligible.
Calculate the final angular speed of the skater.
Explain why the rotational kinetic energy changes even though angular momentum is conserved.
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A rigid block floats on a nearly frictionless air table. Two different horizontal forces of the same magnitude may be applied to the block. Force A acts through the centre of mass. Force B acts along a line that does not pass through the centre of mass.

Compare the translational acceleration of the centre of mass produced by the two forces.
Suggest why force B, but not force A, also produces angular acceleration about the centre of mass.
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A uniform horizontal beam is hinged to a wall and supported by a cable. A lamp is attached to the beam. The beam is stationary.

State the condition for rotational equilibrium of the beam.
Calculate the tension in the cable.
Explain why the force exerted by the hinge does not appear in the torque equation used in part (b).
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The angular speed of a cooling fan is recorded as it speeds up uniformly and then rotates at constant angular speed.

Determine the angular acceleration during the speeding-up interval.
Calculate the angular displacement during the first .
Calculate the linear speed of the indicated point on the blade at the end of the speeding-up interval.
Explain why the indicated point still has acceleration when the angular speed is constant.
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A skater rotates with negligible external torque while pulling their arms closer to the rotation axis. At , the skater's angular speed is . The graph shows how the skater's moment of inertia changes with time.

Calculate the final angular speed of the skater.
Determine the increase in rotational kinetic energy.
Explain why the rotational kinetic energy can increase even though angular momentum is conserved.
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A torsion wire exerts a restoring torque on a rigid disc when the disc is rotated through a small angular displacement. The graph shows torque as a function of angular displacement. The moment of inertia of the disc is .

Determine the torsion constant of the wire.
Calculate the angular acceleration when the angular displacement is .
Explain why this torque can produce angular simple harmonic motion.
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A uniform solid cylinder rolls without slipping from rest down a slope. The vertical drop of its centre of mass is . For a solid cylinder about its central axis, . Air resistance is negligible.

Show that the final speed of the centre of mass satisfies .
Calculate the final speed of the centre of mass.
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A variable resultant torque acts on a turntable. The graph shows the torque as a function of time. The turntable has moment of inertia and initial angular speed in the positive sense.

Determine the angular impulse delivered to the turntable over the time interval shown.
Calculate the final angular speed of the turntable.
Explain the significance of a negative region on the graph.
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Four small masses are fixed to a light rotating frame. The frame itself has negligible moment of inertia. A constant resultant torque is then applied about the central axis.
| Quantity | Mass / kg | Radius from axis / m | Resultant torque / N m |
|---|---|---|---|
| Mass 1 | 0.20 | 0.25 | â |
| Mass 2 | 0.20 | 0.25 | â |
| Mass 3 | 0.30 | 0.10 | â |
| Mass 4 | 0.10 | 0.40 | â |
| Applied torque | â | â | 0.132 |
Calculate the moment of inertia of the system about the central axis.
Calculate the angular acceleration produced by the applied torque.
The system starts from rest. Calculate its angular speed after .
One mass is moved closer to the axis while the same torque is applied. Suggest the effect on the angular acceleration.
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Two coaxial discs rotate freely with opposite senses and are then clamped together. Friction in the clamp is internal to the two-disc system.
| Disc | Moment of inertia / kg m^2 | Initial angular velocity / rad s^-1 |
|---|---|---|
| Disc 1 | 0.060 | 24 |
| Disc 2 | 0.040 | -12 |
State which conservation law should be applied during the clamping process.
Calculate the common final angular speed, including its rotational sense.
Calculate the change in rotational kinetic energy and explain why it occurs.
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A motor exerts a net driving torque on a flywheel as it turns through an angular displacement. The flywheel has moment of inertia and initial angular speed .

Determine the work done on the flywheel over the interval shown.
Calculate the final angular speed of the flywheel.
Explain why a positive area under this graph corresponds to an increase in rotational kinetic energy.
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A uniform horizontal beam is hinged to a vertical wall at one end. A cable attached to the other end of the beam makes an angle of above the beam. A box is suspended from the beam from the hinge.

The beam has length and mass . The box has mass and is suspended from the hinge.
State the expression for the torque of a force about an axis.
Calculate the tension in the cable when the beam is in rotational equilibrium.
The cable is reattached so that it makes a smaller angle with the horizontal beam, while the box remains at the same position. Explain the effect on the force exerted by the hinge on the beam.
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A centrifuge rotor starts from rest. Its angular velocity is increased uniformly, then kept constant, and finally reduced uniformly to rest.

During the first the angular velocity increases uniformly from to .
Determine the angular acceleration during this interval.
Determine the angular displacement of the rotor during this interval.
The rotor then spins at constant angular velocity for before being brought uniformly to rest in a further . Sketch the variation of angular acceleration with time for the complete motion. Numerical values should be shown on the angular acceleration axis.
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Four identical small masses, each of mass , are attached to a light rigid rectangular frame. The frame rotates about an axis through its centre and perpendicular to the plane of the frame.

Each mass is . The rectangle has sides and . A motor provides a torque of and friction provides an opposing torque of .
Calculate the moment of inertia of the four masses about the axis.
Calculate the angular acceleration of the frame.
The four masses are moved closer to the axis while the motor torque and friction torque remain unchanged. Discuss the effect on the angular acceleration and on the rotational kinetic energy at a given angular speed.
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A small satellite in deep space is initially at rest. Two thrusters fire simultaneously, producing a couple about the centre of mass of the satellite. The moment of inertia of the satellite about this axis is .

Each thruster produces a force of . The perpendicular separation of the two lines of action is . The thrusters fire for .
Calculate the torque of the couple.
Calculate the angular acceleration of the satellite.
Calculate the angular displacement of the satellite while the thrusters fire.
Explain why the centre of mass of the satellite does not accelerate even though the satellite rotates.
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A disc is suspended from a thin torsion wire. When the disc is twisted and released, the wire exerts a restoring torque on the disc given by , where is the angular displacement from equilibrium. For this question, , , and the disc is released from rest at .

The disc has moment of inertia . The torsion constant is . The disc is released from rest at angular displacement .
Calculate the initial angular acceleration of the disc, including its direction.
Explain why the motion can be described as angular simple harmonic motion.
Calculate the maximum angular velocity of the disc, assuming no energy is dissipated.
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A small satellite moves in an elliptical orbit around a planet. The planet is much more massive than the satellite. Air resistance is negligible.

At perigee the orbital radius is and the speed is . At apogee the orbital radius is . At both positions the velocity is perpendicular to the radius line.
Explain why the angular momentum of the satellite about the planet is conserved.
Calculate the speed of the satellite at apogee.
Discuss how conservation of angular momentum accounts for the satellite sweeping out equal areas in equal times.
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Three objects of the same mass and radius roll without slipping down the same ramp. The expression may be used, where for a hoop, for a solid cylinder and for a solid sphere. The vertical drop of the centre of mass is .
| Run | Hoop / m s^-1 | Solid cylinder / m s^-1 | Solid sphere / m s^-1 |
|---|---|---|---|
| 1 | 1.84 | 2.10 | 2.18 |
| 2 | 1.85 | 2.14 | 2.21 |
| 3 | 1.87 | 2.18 | 2.24 |
| 4 | 1.89 | 2.20 | 2.28 |
Calculate the predicted final speed for the solid cylinder.
State which object is predicted to have the greatest final speed.
Evaluate whether the data distinguish between the solid cylinder and the solid sphere.
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A satellite moves in an elliptical orbit around a planet. The gravitational force acts along the line joining the satellite and the centre of the planet. The table gives data for the satellite at the closest and furthest points of the orbit.
| Point | Distance from planet centre / m | Speed / m s^-1 |
|---|---|---|
| Closest point | 7.0 Ă 10^6 | 9.2 Ă 10^3 |
| Furthest point | 1.4 Ă 10^7 | â |
Use conservation of angular momentum about the planet centre to calculate the speed at the furthest point.
Compare the angular speeds at the closest and furthest points.
Explain why the angular momentum of the satellite about the planet centre is conserved.
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Two coaxial flywheels can rotate freely about the same fixed axle. They are initially separate and are then clamped together. Friction in the clamp acts only between the two flywheels during the joining process.

Flywheel A has moment of inertia and angular velocity . Flywheel B has moment of inertia and angular velocity .
Calculate the common angular velocity immediately after the flywheels are clamped together.
Determine the loss of rotational kinetic energy during the clamping process.
Evaluate the statement: âBecause angular momentum is conserved in this process, rotational kinetic energy must also be conserved.â
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A turntable of moment of inertia rotates initially with angular velocity in the positive sense. A variable external torque is applied.

From to , the torque forms a triangular pulse with maximum value .
Determine the angular impulse delivered during the first interval, .
Calculate the angular velocity of the turntable at .
From to , a constant torque of acts on the turntable.
Determine the angular velocity at .
Explain why the final angular velocity is not equal to the initial angular velocity.
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A solid cylinder rolls without slipping from rest down a straight ramp. The moment of inertia of a solid cylinder about its central axis is .

The cylinder has mass and radius . The centre of mass descends through a vertical height of along a ramp of length .
Show that the speed of the centre of mass at the bottom of the ramp is about .
Calculate the average acceleration of the centre of mass along the ramp, assuming it is uniform.
hoop of the same mass and radius is released from the same height. For a hoop, . Compare the motion of the hoop with that of the cylinder.
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A student stands on a rotating platform and holds two identical dumbbells. The platform rotates freely except for a small constant frictional torque. Treat the student and platform, excluding the dumbbells, as having constant moment of inertia.

The platform and student have moment of inertia . Each dumbbell consists of two masses. Initially the dumbbells are from the axis and the angular velocity is . The dumbbells are pulled in to from the axis in . During this time the frictional torque is opposing the rotation.
Calculate the initial moment of inertia of the system.
Determine the final angular velocity of the system.
Evaluate the claim that âpulling the dumbbells in always conserves angular momentum and therefore must increase the angular speedâ.
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A light rigid rod is pivoted at its centre and can rotate freely in a horizontal plane. Two identical small masses are fixed to the ends of the rod. A small piece of clay moves horizontally and sticks to one end of the rod in an inelastic collision.

The rod has length . Each fixed mass is . The clay has mass and speed immediately before impact. The rod is initially at rest.
Calculate the angular momentum of the clay about the pivot immediately before impact.
Calculate the angular velocity immediately after the clay sticks to the rod.
The collision lasts for a very short time.
Determine the loss of kinetic energy in the collision.
Discuss why angular momentum can be conserved during the collision while kinetic energy is not conserved.
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Two masses are connected by a light inextensible string that passes over a pulley. The string does not slip on the pulley. The pulley rotates about a fixed axle with negligible axle friction.

The masses are and . The pulley has radius and moment of inertia .
Show that the acceleration of the masses is about .
Calculate the two tensions in the string.
Discuss why the two tensions are not equal, even though the string is light.
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