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🎡AP Physics 1 Unit 5 Review

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5.3 Torque

5.3 Torque

Written by the Fiveable Content Team • Last updated August 2025
Verified for the 2026 exam
Verified for the 2026 examWritten by the Fiveable Content Team • Last updated August 2025
🎡AP Physics 1
Unit & Topic Study Guides
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Torque is a fundamental concept in physics, describing the rotational force applied to an object. It's crucial for understanding how forces cause objects to rotate, from simple machines to complex mechanical systems.

The magnitude of torque depends on the force applied, the distance from the rotation axis, and the angle between them. Force diagrams help visualize torques, while equations like τ = rF sin θ allow for precise calculations.

Torques on rigid systems

Perpendicular force component

Static friction is an "adjustable" force that matches the applied force up to its maximum value.

  • Torque is generated solely by the force component perpendicular to the position vector extending from the axis of rotation to the force's application point
  • When forces are applied at angles, only the perpendicular component contributes to rotation
  • The parallel component has no rotational effect

Lever arm

The lever arm is what gives mechanical advantage to many tools and machines we use daily.

  • Lever arm refers to the perpendicular distance between the axis of rotation and the line along which the force is exerted
  • Increasing the lever arm amplifies the torque produced by a given force
  • Torque is maximized when the force is applied at a 90° angle to the lever arm
  • This explains why wrenches have long handles and why door handles are placed far from hinges

Description of torques

Force diagrams

Force diagrams serve as the primary visual tool for analyzing rotational problems.

  • Force diagrams provide a visual representation of the torques acting on a rigid system
  • They are analogous to free-body diagrams but focus on rotational effects
  • Force diagrams illustrate the relative magnitude and direction of the forces acting on a rigid system
  • They show points of application in relation to the axis of rotation
  • Curved arrows typically indicate the direction of rotation that would result from each force

Magnitude of torque

The mathematical relationship between force, distance, and angle determines the torque value.

  • The magnitude of the torque (τ\tau) exerted on a rigid system by a force is given by the equation: τ=rFsinθ\tau = rF\sin\theta
  • rr represents the distance from the axis of rotation to the point where the force is applied
  • FF denotes the magnitude of the applied force
  • θ\theta is the angle between the force vector and the position vector from the axis of rotation to the force's application point
  • When the force is perpendicular to the position vector (θ=90°\theta = 90°), the torque reaches its maximum value: τmax=rF\tau_{max} = rF
  • Conversely, when the force is parallel to the position vector (θ=0°\theta = 0° or 180°180°), the torque is zero: τ=0\tau = 0

🚫 Boundary Statements

AP Physics 1 requires students to mathematically manipulate the magnitude of torque using vector conventions. However, the direction of torque is not covered on the exam.

Practice Problem 1: Torque Calculation

A student pushes perpendicular to a door with a force of 15 N at a distance of 0.75 m from the hinges. Calculate the torque applied to the door.

Solution:

  1. Identify the given values:
  • Force (F) = 15 N
  • Distance from axis of rotation (r) = 0.75 m
  • Angle (θ) = 90° (perpendicular force)
  1. Apply the torque equation: τ=rFsinθ\tau = rF\sin\theta τ=(0.75 m)(15 N)(sin90°)\tau = (0.75 \text{ m})(15 \text{ N})(\sin 90°) τ=(0.75 m)(15 N)(1)\tau = (0.75 \text{ m})(15 \text{ N})(1) τ=11.25 N\cdotpm\tau = 11.25 \text{ N·m} with τ=11.25 Nm\tau = 11.25 \text{ N}\cdot\text{m}

  2. The torque applied to the door is 11.25 N·m.

Practice Problem 2: Lever Arm Analysis

A 50 N force is applied at a 30° angle to a wrench handle that is 0.3 m long. Calculate (a) the torque produced and (b) how much the torque would increase if the force were applied perpendicularly.

Solution:

  1. For part (a):
  • Force (F) = 50 N
  • Distance (r) = 0.3 m
  • Angle (θ) = 30° τ=rFsinθ\tau = rF\sin\theta τ=(0.3 m)(50 N)(sin30°)\tau = (0.3 \text{ m})(50 \text{ N})(\sin 30°) τ=(0.3 m)(50 N)(0.5)\tau = (0.3 \text{ m})(50 \text{ N})(0.5) τ=7.5 N\cdotpm\tau = 7.5 \text{ N·m}
  1. For part (b) - perpendicular force (θ = 90°): τmax=rF\tau_{max} = rF τmax=(0.3 m)(50 N)\tau_{max} = (0.3 \text{ m})(50 \text{ N}) τmax=15 N\cdotpm\tau_{max} = 15 \text{ N·m}

  2. The increase in torque would be: Δτ=15 N\cdotpm7.5 N\cdotpm=7.5 N\cdotpm\Delta\tau = 15 \text{ N·m} - 7.5 \text{ N·m} = 7.5 \text{ N·m}

  3. The torque would double (increase by 100%) if applied perpendicularly.

Practice Problem 3: Multiple Torques

A seesaw has a length of 4 m with its pivot at the center. A 30 kg child sits 1.5 m from the pivot, while another child of unknown mass sits at the opposite end, 2 m from the pivot. If the seesaw is balanced, what is the mass of the second child?

Solution:

  1. When a system is balanced, the sum of clockwise torques equals the sum of counterclockwise torques.

  2. Calculate the torque from the first child:

  • Mass = 30 kg
  • Weight = mg = (30 kg)(9.8 m/s²) = 294 N
  • Distance from pivot = 1.5 m
  • τ1=(1.5 m)(294 N)=441 N\cdotpm\tau_1 = (1.5 \text{ m})(294 \text{ N}) = 441 \text{ N·m}
  1. For the second child:
  • Mass = m (unknown)
  • Weight = mg = m(9.8 m/s²) = 9.8m N
  • Distance from pivot = 2 m
  • τ2=(2 m)(9.8m N)=19.6m N\cdotpm\tau_2 = (2 \text{ m})(9.8m \text{ N}) = 19.6m \text{ N·m}
  1. Set up the balance equation: τ1=τ2\tau_1 = \tau_2 441 N\cdotpm=19.6m N\cdotpm441 \text{ N·m} = 19.6m \text{ N·m} m=44119.6=22.5 kgm = \frac{441}{19.6} = 22.5 \text{ kg}

  2. The mass of the second child is 22.5 kg.

Vocabulary

The following words are mentioned explicitly in the College Board Course and Exam Description for this topic.

Term

Definition

axis of rotation

The fixed line about which a system rotates.

force component perpendicular

The portion of an applied force that acts at a right angle to the position vector from the axis of rotation.

force diagram

A diagram used to represent and analyze the forces and torques exerted on a rigid system, showing the magnitude, direction, and point of application of each force relative to the axis of rotation.

free-body diagram

A visual representation that shows all forces exerted on an object or system, with each force drawn as a vector originating from the object's center of mass.

lever arm

The perpendicular distance from the axis of rotation to the line of action of an applied force.

line of action

The straight line along which a force acts, extending infinitely in both directions.

perpendicular force

The component of a force that is perpendicular to the position vector, which directly contributes to torque production.

position vector

A vector drawn from the axis of rotation to the point where a force is applied on a rigid system.

rigid system

A system that holds its shape but in which different points on the system move in different directions during rotation.

torque

A measure of the rotational effect of a force on a rigid system, calculated as the product of the force and its perpendicular distance from the axis of rotation.

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