Academy

Torque

Torque is the rotational analogue of force. It is the moment of force about an axis.
Class 11Class JEE
Derivation

What torque is

Torque is the rotational effect of a force — it is what causes angular acceleration, just as force causes linear acceleration.

τ=r×F\vec{\tau} = \vec{r} \times \vec{F}

In magnitude:

τ=rFsinθ\tau = rF\sin\theta

where rr is the distance from the axis to the point of application, FF is the force, and θ\theta is the angle between r\vec{r} and F\vec{F}.

The cross product

The torque vector τ=r×F\vec{\tau} = \vec{r} \times \vec{F} has:

  • Magnitude: rFsinθ=rFsinθ|\vec{r}||\vec{F}|\sin\theta = rF\sin\theta
  • Direction: perpendicular to both r\vec{r} and F\vec{F}, given by the right-hand rule

Right-hand rule: point fingers along r\vec{r}, curl toward F\vec{F}, thumb points along τ\vec{\tau}.

The lever arm

τ=rFsinθ\tau = rF\sin\theta can be rewritten as:

τ=F(rsinθ)=Fl\tau = F \cdot (r\sin\theta) = F \cdot l

where l=rsinθl = r\sin\theta is the lever arm (perpendicular distance from the axis to the line of action of the force).

Or:

τ=r(Fsinθ)=rF\tau = r \cdot (F\sin\theta) = r \cdot F_\perp

where F=FsinθF_\perp = F\sin\theta is the component of force perpendicular to r\vec{r}.

Both interpretations give the same result.

When is torque zero?

τ=rFsinθ=0\tau = rF\sin\theta = 0 when:

  • r=0r = 0: force applied at the axis — no lever arm, no torque
  • F=0F = 0: no force
  • θ=0°\theta = 0° or 180°180°: force along the line from axis to point of application — no perpendicular component

Units

[τ]=[r][F]=mN=Nm[\tau] = [r][F] = \text{m} \cdot \text{N} = \text{N} \cdot \text{m}

Note: Nm\text{N} \cdot \text{m} for torque is kept distinct from J\text{J} (Joule) for energy, even though numerically they are the same. Torque and energy are different physical quantities.

Sign convention

Counterclockwise torque: positive (by convention, in 2D) Clockwise torque: negative

In 3D, the sign is determined by the direction of τ\vec{\tau} relative to the chosen axis direction.

Torque and door

A door is more easily opened by pushing far from the hinges (large rr) and perpendicular to the door (maximum sinθ=1\sin\theta = 1). Pushing near the hinge requires much more force for the same torque — this is why door handles are placed at the far edge.

Key Idea
Torque depends on the choice of origin (or axis). The same force produces different torques about different axes. Always specify which axis you are computing the torque about.