Torque Calculator
Calculate torque (rotational force), applied force, or lever arm length using τ = r·F·sin(θ).
What Is Torque?
Torque (τ, tau) is the rotational equivalent of force. Just as a linear force causes linear acceleration (F = ma), torque causes angular acceleration (τ = Iα). It measures the tendency of a force to rotate an object about a pivot point. The formula is τ = r · F · sin(θ), where r is the distance from the pivot to the point of force application (the lever arm), F is the applied force, and θ is the angle between the force vector and the lever arm.
The SI unit of torque is the newton-meter (N·m). Note this is dimensionally the same as joules (J = N·m), but torque is not energy — it is a tendency to rotate, not an energy transfer. When θ = 90° (force perpendicular to the lever arm), sin(90°) = 1 and torque is maximized: τ = r·F. This is why engineers make wrenches long — a longer r produces more torque for the same force.
Torque is ubiquitous in engineering: engine output is rated in N·m (or lb·ft in imperial); steering systems specify rack torque; structural bolts have torque specifications; electric motors are characterized by their rated torque. The torque-speed relationship P = τ·ω (power = torque × angular velocity) governs all rotating machinery design.
When multiple torques act on an object, they sum algebraically (clockwise negative, counterclockwise positive by convention). For a rigid body in rotational equilibrium (not accelerating rotationally), the net torque = 0: Στ = 0. This principle, along with ΣF = 0, allows engineers to solve static problems involving beams, levers, and structures.
Formula Reference Table
| Quantity | Formula | Notes |
|---|---|---|
| Torque (τ) | τ = r · F · sin θ | N·m; θ = angle between F and r |
| Force (F) | F = τ / (r · sin θ) | sin θ ≠ 0 |
| Lever arm (r) | r = τ / (F · sin θ) | Perpendicular distance from pivot |
| Rotational 2nd Law | τ = I · α | I = moment of inertia, α = angular accel |
| Power (rotating) | P = τ · ω | ω in rad/s |
| Equilibrium | Σ τ = 0 | No net rotation |
3 Worked Examples
A 40 cm (0.4 m) wrench is turned with 75 N of force perpendicular to the handle. Find torque.
- θ = 90° so sin(90°) = 1
- τ = r × F × sin θ = 0.4 × 75 × 1
- τ = 30 N·m
An engine produces 250 N·m torque via a 0.05 m crankshaft radius. What tangential force is generated?
- F = τ / (r × sin θ) = 250 / (0.05 × 1)
- F = 250 / 0.05 = 5,000 N
- This force drives the piston connecting rod
A 0.6 m lever has a 200 N force at 30° to the bar. Find torque.
- sin(30°) = 0.5
- τ = 0.6 × 200 × 0.5 = 60 N·m
- Compared to 90°: 0.6 × 200 × 1 = 120 N·m — angle halves effectiveness
Real-World Applications
Common Mistakes to Avoid
τ = r·F·sin θ uses r = distance from pivot to force point. If you're given a diameter (e.g., a 60 mm bolt circle), use r = 30 mm = 0.030 m. Using the diameter gives twice the torque.
τ = r·F only when force is perfectly perpendicular (θ = 90°). Any other angle reduces effective torque. A force at 30° gives sin(30°) = 0.5 — half the maximum torque.
Both torque (N·m) and work (J = N·m) have the same SI units, but they are different quantities. Torque is a rotational tendency; work is energy transferred. Never add them or treat them as equivalent.
Convention: counterclockwise torques are positive, clockwise negative. Mixing this up when applying Στ = 0 gives wrong answers for unknown forces or distances.
Only the component of force perpendicular to the lever arm produces torque. A force parallel to the lever arm (θ = 0°) produces zero torque regardless of magnitude.
Frequently Asked Questions
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Interpretation: This formula is the rotational counterpart of linear mechanics, relating angle, angular motion, torque, inertia or rotational energy. Assumption: Define the rotation axis and sign convention. Rigid-body behavior, no slipping, steady rotation or negligible bearing losses may be assumed.