DP Physics Questionbank
B.1 – Rigid bodies and rotational dynamics
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Description
Nature of science:
Modelling: The use of models has different purposes and has allowed scientists to identify, simplify and analyse a problem within a given context to tackle it successfully. The extension of the point particle model to actually consider the dimensions of an object led to many groundbreaking developments in engineering. (1.2)
Understandings:
- Torque
- Moment of inertia
- Rotational and translational equilibrium
- Angular acceleration
- Equations of rotational motion for uniform angular acceleration
- Newton’s second law applied to angular motion
- Conservation of angular momentum
Applications and skills:
- Calculating torque for single forces and couples
- Solving problems involving moment of inertia, torque and angular acceleration
- Solving problems in which objects are in both rotational and translational equilibrium
- Solving problems using rotational quantities analogous to linear quantities
- Sketching and interpreting graphs of rotational motion
- Solving problems involving rolling without slipping
Guidance:
- Analysis will be limited to basic geometric shapes
- The equation for the moment of inertia of a specific shape will be provided when necessary
- Graphs will be limited to angular displacement–time, angular velocity–time and torque–time
Data booklet reference:
Theory of knowledge:
- Models are always valid within a context and they are modified, expanded or replaced when that context is altered or considered differently. Are there examples of unchanging models in the natural sciences or in any other areas of knowledge?
Utilization:
- Structural design and civil engineering rely on the knowledge of how objects can move in all situations
Aims:
- Aim 7: technology has allowed for computer simulations that accurately model the complicated outcomes of actions on bodies
Directly related questions
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16N.3.SL.TZ0.8a:
The velocity of the falling object is 1.89 m s–1 at 3.98 s. Calculate the average angular acceleration of the flywheel.
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16N.3.SL.TZ0.8c:
(i) Calculate the tension in the string.
(ii) Determine the mass m of the falling object.
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16N.3.SL.TZ0.8b:
Show that the torque acting on the flywheel is about 0.3 Nm.
- 16N.3.SL.TZ0.9: The diagram shows two methods of pedalling a bicycle using a force F. In method 1 the pedal is...
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17M.3.SL.TZ1.5a.iii:
Hence, show that .
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17M.3.SL.TZ1.5b.ii:
Calculate the number of revolutions made by the system before it comes to rest.
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17M.3.SL.TZ1.5a.i:
Write down an expression, in terms of M, v and R, for the angular momentum of the system about the vertical axis just before the collision.
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17M.3.SL.TZ1.5a.ii:
Just after the collision the system begins to rotate about the vertical axis with angular velocity ω. Show that the angular momentum of the system is equal to .
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17M.3.SL.TZ1.5a.iv:
Determine in terms of M and v the energy lost during the collision.
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17M.3.SL.TZ1.5b.i:
Show that the angular deceleration of the system is 0.043 rads–2.
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17M.3.SL.TZ2.6c.i:
Determine the final angular speed of the probe–satellite system.
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17M.3.SL.TZ2.6a.i:
Deduce the linear acceleration of the centre of mass of the probe.
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17M.3.SL.TZ2.6a.ii:
Calculate the resultant torque about the axis of the probe.
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17M.3.SL.TZ2.6b:
The forces act for 2.00 s. Show that the final angular speed of the probe is about 16 rads–1.
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17M.3.SL.TZ2.6c.ii:
Calculate the loss of rotational kinetic energy due to the linking of the probe with the satellite.
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20N.3.SL.TZ0.6b:
Draw the variation with time of the angular displacement of the bar during the acceleration.
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20N.3.SL.TZ0.6d:
The torque is removed. The bar comes to rest in complete rotations with constant angular deceleration. Determine the time taken for the bar to come to rest.
- 20N.3.SL.TZ0.7b: Explain the changes to the rotational kinetic energy in the person-turntable system.
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20N.3.SL.TZ0.6c:
Calculate the torque acting on the bar while it is accelerating.
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20N.3.SL.TZ0.8:
A solid sphere of radius and mass is released from rest and rolls down a slope, without slipping. The vertical height of the slope is . The moment of inertia of this sphere about an axis through its centre is .
Show that the linear velocity of the sphere as it leaves the slope is .
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20N.3.SL.TZ0.6a:
Show that the final angular velocity of the bar is about .
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20N.3.SL.TZ0.7a:
Explain the direction in which the person-turntable system starts to rotate.
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17N.3.SL.TZ0.7b:
Show that the linear acceleration a of the hoop is given by the equation shown.
a =
- 17N.3.SL.TZ0.7c: Calculate the acceleration of the hoop when θ = 20°. Assume that the hoop continues to roll...
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17N.3.SL.TZ0.7e:
The angle of the incline is slowly increased from zero. Determine the angle, in terms of the coefficient of friction, at which the hoop will begin to slip.
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17N.3.SL.TZ0.7d:
State the relationship between the force of friction and the angle of the incline.
- 17N.3.SL.TZ0.7a: On the diagram, draw and label the forces acting on the hoop.
- 17N.3.SL.TZ0.6a: Explain what is meant by proper length.
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18M.3.SL.TZ2.6a.ii:
In moving from point A to point B, the centre of mass of the wheel falls through a vertical distance of 0.36 m. Show that the translational speed of the wheel is about 1 m s–1 after its displacement.
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18M.3.SL.TZ2.6b.ii:
Describe the effect of F on the angular speed of the wheel.
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18M.3.SL.TZ2.6a.i:
The moment of inertia of the wheel is 1.3 × 10–4 kg m2. Outline what is meant by the moment of inertia.
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18M.3.SL.TZ2.6a.iii:
Determine the angular velocity of the wheel at B.
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18M.3.SL.TZ1.6a:
Show that the angular acceleration of the merry-go-round is 0.2 rad s–2.
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18M.3.SL.TZ1.6b.i:
Calculate, for the merry-go-round after one revolution, the angular speed.
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18M.3.SL.TZ1.6b.ii:
Calculate, for the merry-go-round after one revolution, the angular momentum.
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18M.3.SL.TZ1.6c:
Calculate the new angular speed of the rotating system.
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18M.3.SL.TZ1.6d.i:
Explain why the angular speed will increase.
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18M.3.SL.TZ1.6d.ii:
Calculate the work done by the child in moving from the edge to the centre.
- 18N.3.SL.TZ0.6c.ii: At the instant the rod becomes vertical calculate the angular momentum of the rod.
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18N.3.SL.TZ0.6c.i:
At the instant the rod becomes vertical show that the angular speed is ω = 2.43 rad s–1.
- 18N.3.SL.TZ0.6a: Calculate the force the support exerts on the rod.
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18N.3.SL.TZ0.6b.ii:
After time t the rod makes an angle θ with the horizontal. Outline why the equation cannot be used to find the time it takes θ to become (that is for the rod to become vertical for the first time).
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18N.3.SL.TZ0.6b.i:
Calculate, in rad s–2, the initial angular acceleration of the rod.
- 19M.3.SL.TZ2.8a: Outline why the normal force acting on the ladder at the point of contact with the wall is equal...
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19M.3.SL.TZ2.9a:
Show that the total kinetic energy Ek of the sphere when it rolls, without slipping, at speed v is .
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19M.3.SL.TZ2.9b:
A solid sphere of mass 1.5 kg is rolling, without slipping, on a horizontal surface with a speed of 0.50 m s-1. The sphere then rolls, without slipping, down a ramp to reach a horizontal surface that is 45 cm lower.
Calculate the speed of the sphere at the bottom of the ramp.
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19M.3.SL.TZ2.8b:
Calculate F.
- 19N.3.SL.TZ0.5b(i): Identify the physical quantity represented by the area under the graph.
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19N.3.SL.TZ0.5b(iii):
Calculate the maximum tension in the string.
- 19N.3.SL.TZ0.5b(ii): Show that the angular velocity of the flywheel at t = 5.00 s is 200 rad s–1.
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19N.3.SL.TZ0.5c(ii):
At t = 5.00 s the flywheel is spinning with angular velocity 200 rad s–1. The support bearings exert a constant frictional torque on the axle. The flywheel comes to rest after 8.00 × 103 revolutions. Calculate the magnitude of the frictional torque exerted on the flywheel.
- 19N.3.SL.TZ0.5a: State the torque provided by the force W about the axis of the flywheel.
- 19N.3.SL.TZ0.5c(i): The flywheel is in translational equilibrium. Distinguish between translational equilibrium and...