PHYSICS · ROTATIONAL MECHANICS

Moments & Torque

Forces don't only move objects. They can turn them.

Explore moments, torque, lever arms, couples, rotational equilibrium, and the physics of forces acting around a pivot.

Remember

Moment and torque describe the rotational effect of a force.

Single Force

τ = rF sin θ

Couple

M_couple = Fd

The crucial difference: a single force has a net force, while an ideal couple has zero net force but a nonzero moment. That is why a couple produces a pure turning effect.

SECTION 2

Key Definitions

SECTION 3

Moment vs. Torque

Moment

Torque

Describes the turning effect of a force about a point or axis.
Describes the tendency of a force to rotate an object.
Frequently used in statics and engineering mechanics.
Frequently used for rotating machinery, shafts, motors, engines, and rotational dynamics.
Depends on force and perpendicular distance.
Depends on force, distance, and angle.
Measured in N·m.
Measured in N·m.

There is not a fundamentally different equation for moment and torque. Both are based on the vector relationship:

M = r × Fτ = r × F

The terminology usually reflects the physical situation being discussed. Do not teach students that moment and torque are completely different physical quantities.

SECTION 4

Ordinary Torque vs. Torque of a Couple

1F

Single Force

Imagine pushing horizontally on the handle of a door. The door rotates because the force acts some distance from its hinges.

Result

Net Force ≠ 0 + Moment ≠ 0

The calculated moment depends on the reference point chosen.

2F

Couple

Imagine turning a steering wheel with two hands. One hand pushes upward while the other pushes downward with equal force on the opposite side.

Result

ΣF = 0 but ΣM ≠ 0

The result is a pure turning effect.

The crucial difference: A single force can produce both translation and rotation. A couple produces rotation without a net translational force.

SECTION 5

Moment & Torque Calculator

Drag the force arrow or application point to update the torque in real time.

d⊥=0.50mr=0.50mθ=90°F=80NPivot
Drag orange dot = angle, blue dot = distance
Direction
Torque40.00 N·m
DirectionCCW
Effective lever arm0.50 m
Tangential force80.00 N

τ = rF sin θ = (0.50)(80)(sin 90°) = 40.00 N·m

EXAMPLE

Force: 80 N, Distance: 0.50 m, Angle: 90°

τ = (0.50)(80)(sin 90°) = 40 N·m

Because the force is perpendicular to the lever arm, the torque is at its maximum possible value.

SECTION 6

Angle Explorer

Keep F and r constant while changing θ. See how torque varies with angle.

0°90°180°τ40.00 N·m

0°

τ = 0

30°

τ = 0.5rF

90°

τ = max

150°

τ = 0.5rF

180°

τ = 0

A large force does not necessarily produce a large torque. The direction of the force matters. Only the component of force perpendicular to the position vector contributes to the torque.

SECTION 7

Torque of a Couple

d = 0.40 mF=25NF=25N
Couple Torque10.00 N·m
Net Force0 N
RotationCounterclockwise

M_couple = Fd = (25)(0.40) = 10.00 N·m

Because this is a couple, its moment is independent of the reference point used to calculate it.

COUPLE EXAMPLE

Two equal and opposite forces of 25 N act on a steering wheel. Perpendicular distance: 0.40 m.

M_couple = Fd = (25)(0.40) = 10 N·m

You do not multiply by two — the separation distance already accounts for both forces.

SECTION 8

Why Is a Couple Different?

A

Single Force

Net force ≠ 0

Net moment ≠ 0

The object both moves and rotates.

B

Couple

Net force = 0

Net moment ≠ 0

The object rotates without its center of mass accelerating sideways.

A couple creates pure rotational loading.

SECTIONS 9–11

Sign Convention, Multiple Forces & Equilibrium

Sign Convention

Counterclockwise = Positive (+)

M = +12 N·m

Clockwise = Negative (−)

M = −7 N·m

A different sign convention may be used if it is clearly defined and used consistently.

Multiple Forces

When several forces act on an object: ΣM = M₁ + M₂ + M₃ + ...Clockwise and counterclockwise moments must be assigned opposite signs.

Force A+24 N·m
Force B−15 N·m
Force C−4 N·m
ΣM=24 − 15 − 4 = +5 N·m

Net counterclockwise moment of 5 N·m.

Rotational Equilibrium

An object is in rotational equilibrium when ΣM = 0.

ΣF = 0

No translational acceleration

ΣM = 0

No angular acceleration

For complete static equilibrium, both conditions must be satisfied simultaneously.

SECTION 12

Real-World Examples

Opening a Door

Pushing near the doorknob produces much more torque than pushing near the hinges. The farther the force is from the hinge, the larger the torque.

Using a Wrench

A longer wrench produces more torque for the same applied force. A force applied perpendicular to the wrench is most effective.

Riding a Bicycle

Force applied to a bicycle pedal creates torque about the crankshaft. The amount of torque changes as the pedal rotates because the angle between the crank arm and the applied force changes.

Seesaw

The effect of each person's weight depends on both their weight and their distance from the pivot. A lighter person can balance a heavier person by sitting farther from the pivot.

Steering Wheel

Two hands applying approximately equal and opposite tangential forces can produce a couple. The net force can be nearly zero while a substantial torque remains.

Turning a Jar Lid

Forces from the fingers and thumb can combine to create a couple that twists the lid.

Electric Motor

Electromagnetic forces generate torque on a rotor. This torque causes the motor shaft to rotate.

Car Engine

Combustion forces act through connecting rods and the crankshaft to generate torque. Engine torque describes the rotational output available at the crankshaft.

SECTION 13

Zul'Elkoen Applications

Starship Airlock

A crew member applies force to a manual emergency airlock handle. Users calculate how much torque is produced about the handle's pivot.

Gulliver Maintenance

A technician uses a long tool to loosen a seized fastener in the Gulliver's machinery bay. Users determine whether increasing force or increasing lever-arm length is more effective.

Attitude Control

Opposing thrusters positioned on different sides of a spacecraft can create a turning effect resembling a couple. The net linear force can be minimized while the spacecraft rotates.

SECTION 14

Common Mistakes

SECTIONS 15–16

Try It Yourself

A force of 49 N is applied at 0.3 m from a pivot, at 61° to the lever arm, acting clockwise. Calculate the torque.

SECTION 17

Quick Knowledge Check

Question 1 of 5Score: 0

A force acts directly toward a pivot. What torque does it produce?

SECTION 18

Advanced View

τ = rF sin θ

Basic mode uses the scalar relationship between force, distance, and angle. This is sufficient for most two-dimensional problems involving a single pivot.

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