Torque and Work

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AP Physics C: Mechanics › Torque and Work

Questions 1 - 10
1

A gyroscope with its axis tilted precesses with a constant angular speed about a vertical axis. The gravitational force exerts a torque on the gyroscope, causing the precession. What is the work done by this gravitational torque during one complete precession cycle?

It cannot be determined without knowing the gyroscope's spin and precession speeds.

Positive, because the torque is required to maintain the precession against dissipative forces.

Negative, because the potential energy of the gyroscope's center of mass does not change.

Zero, because the torque vector is always perpendicular to the angular displacement of precession.

Explanation

The work done by a torque is given by $$W = \int \vec{\tau} \cdot d\vec{\theta}$$. For a precessing gyroscope, the gravitational torque vector is horizontal. The angular displacement vector for the precession is along the vertical axis of precession. Since the torque vector is always perpendicular to the angular displacement vector, their dot product is zero, and the work done is zero. This torque changes the direction of the angular momentum but not its magnitude.

2

A net torque given by $$\tau = \tau_0 \sin(\theta)$$ is applied to a rotor, where $$\tau_0$$ is a positive constant. What is the work done by this torque as the rotor moves from an angular position of $$\theta = 0$$ to $$\theta = \pi$$ radians?

$$0$$

$$\tau_0$$

$$2\tau_0$$

$$\pi \tau_0$$

Explanation

The work done is the integral of the torque over the angular displacement: $$W = \int_{0}^{\pi} \tau_0 \sin(\theta) d\theta = \tau_0 [-\cos(\theta)]_{0}^{\pi} = -\tau_0 (\cos(\pi) - \cos(0)) = -\tau_0 (-1 - 1) = 2\tau_0$$.

3

What is the total work done by the net torque on the flywheel as it rotates from $$\theta = 0$$ to $$\theta = 5.0 , \text{rad}$$?

$$75 , \text{J}$$

$$25 , \text{J}$$

$$100 , \text{J}$$

$$50 , \text{J}$$

Explanation

The work done is the area under the torque versus angular position graph. Since the torque decreases linearly, the graph is a triangle. The area of the triangle is $$W = \frac{1}{2} \times \text{base} \times \text{height} = \frac{1}{2} (5.0 , \text{rad})(20 , \text{N} \cdot \text{m}) = 50 , \text{J}$$.

4

A spinning flywheel is slowing down due to a constant frictional torque. Which of the following correctly describes the work done by the frictional torque and the work done by the net torque on the flywheel during one revolution?

Work by frictional torque is positive; work by net torque is negative.

Work by frictional torque is negative; work by net torque is negative.

Work by frictional torque is zero; work by net torque is zero.

Work by frictional torque is negative; work by net torque is positive.

Explanation

The frictional torque opposes the angular velocity, so the angle between the torque vector and the infinitesimal angular displacement vector is $$\pi$$ radians. Thus, the work done by friction is negative. Since friction is the only torque mentioned that causes it to slow down, it is the net torque. Therefore, the net work done is also negative, consistent with the decrease in rotational kinetic energy.

5

A pulley of radius $r=0.10,\text{m}$ is rotated by a constant tangential pull on a rope. The applied force has magnitude $F=60,\text{N}$ and stays perpendicular to the radius as the pulley turns. The axle is frictionless, and the pulley rotates in its plane. The force is applied while the pulley rotates through $\Delta\theta=4.0,\text{rad}$. Assume no slipping and no dissipative losses. The torque is constant with magnitude $\tau=rF$. The work done by the torque is $W=\tau\Delta\theta$. Using the given information, calculate the total work done by the applied force.

$W=24,\text{N,m}$

$W=240,\text{J}$

$W=24,\text{J}$

$W=6.0,\text{J}$

Explanation

This question tests AP Physics C: Mechanics, specifically the concepts of torque and work in rotating systems. Torque is the rotational equivalent of force, calculated as τ = rFsinθ, where r is the distance from the pivot, F is the force, and θ is the angle between force and lever arm. Work in rotation is given by W = τθ, where θ is the angular displacement. In this scenario, a tangential force of 60 N at radius 0.10 m rotates a pulley through 4.0 rad. Choice A is correct because the torque is τ = rF = (0.10 m)(60 N) = 6.0 N·m, and the work is W = τΔθ = (6.0 N·m)(4.0 rad) = 24 J. Choice B incorrectly multiplies by an extra factor of 10, possibly from a decimal error. To help students, emphasize careful unit tracking and decimal placement. Practice with small radii to ensure students don't automatically assume meters when given centimeters.

6

A pulley of radius $r=0.20,\text{m}$ is turned by pulling on a light rope wrapped around its rim. A constant tangential force $F=50,\text{N}$ is applied to the rope so the force stays perpendicular to the radius. The axle is frictionless, and the pulley rotates in its plane. The force is applied while the pulley turns through an angle $\Delta\theta=2.5,\text{rad}$. Assume the rope does not slip on the rim. The torque from the pull is constant, so rotational work is $W=\tau\Delta\theta$. Using the given information, calculate the total work done by the applied force on the pulley during this rotation.

$W=2.0,\text{N,m}$

$W=5.0,\text{J}$

$W=25,\text{J}$

$W=125,\text{J}$

Explanation

This question tests AP Physics C: Mechanics, specifically the concepts of torque and work in rotating systems. Torque is the rotational equivalent of force, calculated as τ = rFsinθ, where r is the distance from the pivot, F is the force, and θ is the angle between force and lever arm. Work in rotation is given by W = τθ, where θ is the angular displacement. In this scenario, a tangential force of 50 N is applied to a pulley of radius 0.20 m through an angle of 2.5 rad. Choice A is correct because the torque is τ = rF = (0.20 m)(50 N) = 10 N·m (tangential force means sin90° = 1), and the work is W = τΔθ = (10 N·m)(2.5 rad) = 25 J. Choice D incorrectly gives units of N·m instead of J, showing confusion between torque and work units. To help students, stress that work always has units of energy (joules), while torque has units of N·m. Practice dimensional analysis to verify that τΔθ gives units of energy.

7

A mechanical arm rotates about a pivot, and a force $F=25,\text{N}$ is applied at a point $r=0.40,\text{m}$ from the pivot. The force is applied at an angle $\phi=45^\circ$ relative to the arm (the radius vector), in the plane of rotation. Assume the pivot is frictionless and the force magnitude remains constant at that instant. Only the torque from this applied force is considered. The torque magnitude is $\tau=rF\sin\phi$. Using the given information, determine the torque produced about the pivot.

$\tau=10,\text{N,m}$

$\tau=0.28,\text{N,m}$

$\tau=14,\text{N,m}$

$\tau=7.1,\text{N,m}$

Explanation

This question tests AP Physics C: Mechanics, specifically the concepts of torque and work in rotating systems. Torque is the rotational equivalent of force, calculated as τ = rFsinθ, where r is the distance from the pivot, F is the force, and θ is the angle between force and lever arm. Work in rotation is given by W = τθ, where θ is the angular displacement. In this scenario, a 25 N force is applied at 0.40 m from the pivot at a 45° angle. Choice A is correct because τ = rFsinφ = (0.40 m)(25 N)sin(45°) = (0.40)(25)(0.707) = 7.1 N·m. Choice B incorrectly calculates τ = rF without the angle factor, yielding 10 N·m. To help students, use the mnemonic that torque depends on the 'perpendicular' component of force. Practice with 45° angles specifically, as sin(45°) = cos(45°) = 0.707 is a common value students should memorize.

8

A balancing beam of negligible mass is pivoted at one end and initially held horizontal. A single weight of magnitude $W=50,\text{N}$ hangs from the beam at a distance $r=0.60,\text{m}$ from the pivot. The weight pulls vertically downward, and the beam rotates in a vertical plane. Consider the instant when the beam is horizontal so the angle between $\vec r$ and the weight is $90^\circ$. Ignore friction at the pivot and assume the weight remains attached at the same point. The torque magnitude from the weight is $\tau=rW\sin 90^\circ$. Using the given information, what is the torque about the pivot due to the hanging weight at this instant?

$\tau=30,\text{N,m}$

$\tau=15,\text{N,m}$

$\tau=30,\text{J}$

$\tau=300,\text{N,m}$

Explanation

This question tests AP Physics C: Mechanics, specifically the concepts of torque and work in rotating systems. Torque is the rotational equivalent of force, calculated as τ = rFsinθ, where r is the distance from the pivot, F is the force, and θ is the angle between force and lever arm. Work in rotation is given by W = τθ, where θ is the angular displacement. In this scenario, a 50 N weight hangs 0.60 m from a pivot on a horizontal beam, creating maximum torque. Choice A is correct because τ = rWsin(90°) = (0.60 m)(50 N)(1) = 30 N·m, since the weight acts vertically and the beam is horizontal. Choice D incorrectly labels the torque with units of joules instead of N·m, confusing torque with work. To help students, emphasize that hanging weights on horizontal beams always produce maximum torque (sin90° = 1). Practice identifying when forces are perpendicular to position vectors for simplified calculations.

9

A uniform disc of radius $r=0.40,\text{m}$ is mounted on a low-friction axle. A force of magnitude $F=30,\text{N}$ is applied at the rim but not tangentially; instead, it makes an angle of $30^\circ$ with the radius. The force lies in the plane of the disc and stays at this angle with respect to the radius at the point of application. Air resistance is negligible, and the disc remains rigid. The torque magnitude about the center is given by $\tau=rF\sin\phi$, where $\phi$ is the angle between $\vec r$ and $\vec F$. Using the given information, what is the torque exerted by the force about the disc’s center?

$\tau=12,\text{N,m}$

$\tau=24,\text{N,m}$

$\tau=6.0,\text{N,m}$

$\tau=10.4,\text{N,m}$

Explanation

This question tests AP Physics C: Mechanics, specifically the concepts of torque and work in rotating systems. Torque is the rotational equivalent of force, calculated as τ = rFsinθ, where r is the distance from the pivot, F is the force, and θ is the angle between force and lever arm. Work in rotation is given by W = τθ, where θ is the angular displacement. In this scenario, a 30 N force is applied at the rim (0.40 m) at a 30° angle to the radius. Choice C is correct because τ = rFsinφ = (0.40 m)(30 N)sin(30°) = (0.40)(30)(0.5) = 6.0 N·m. Choice A incorrectly uses sin(90°) instead of sin(30°), yielding 12 N·m, which would be the torque if the force were tangential. To help students, use diagrams showing the force vector and its angle relative to the position vector. Emphasize that the angle in the torque formula is between the force and position vectors, not the force and some reference direction.

10

A disc of radius $r=0.25,\text{m}$ rotates about its center on a frictionless axle. A constant tangential force $F=16,\text{N}$ is applied at the rim so that the force stays perpendicular to the radius. The disc rotates through an angular displacement of $\Delta\theta=\pi,\text{rad}$. Ignore any losses so all work is due to the applied torque. The torque magnitude is constant and equals $\tau=rF$. The rotational work done is $W=\tau\Delta\theta$. Using the given information, how much work is done by the force during this rotation?

$W=2\pi,\text{J}$

$W=4\pi,\text{J}$

$W=4\pi,\text{N,m}$

$W=8\pi,\text{J}$

Explanation

This question tests AP Physics C: Mechanics, specifically the concepts of torque and work in rotating systems. Torque is the rotational equivalent of force, calculated as τ = rFsinθ, where r is the distance from the pivot, F is the force, and θ is the angle between force and lever arm. Work in rotation is given by W = τθ, where θ is the angular displacement. In this scenario, a tangential force of 16 N at radius 0.25 m rotates a disc through π rad. Choice A is correct because the torque is τ = rF = (0.25 m)(16 N) = 4.0 N·m, and the work is W = τΔθ = (4.0 N·m)(π rad) = 4π J. Choice D incorrectly gives units of N·m instead of J, confusing torque with work. To help students, practice problems using π in angular measurements, ensuring comfort with symbolic answers. Emphasize dimensional analysis: torque (N·m) × angle (rad) = work (J).

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