Example 1
Wrench: a force of 20 N acts at a right angle on an arm of 0.3 m. This is the reference example on this page.
M = 6.000 N·m, F⊥ = 20.00 N
Enter force F in newtons, arm r in meters, and angle α in degrees. The calculator finds torque from M = F·r·sin α and also reports the perpendicular component F⊥. At 20 N, 0.3 m, and 90° the torque is 6 N·m, and at 30° it is 3 N·m. The model does not sum several forces for ΣM = 0 or compute rotational power P = τω.
Enter force F, arm r, and angle α. The torque, the perpendicular component, and the chart appear here.
The balance of two arms is on the F₁·r₁ = F₂·r₂ calculator. For point-mass moment of inertia, use the I = m·r² calculator. For rotational kinetic energy, use the Eₖ = ½Iω² calculator.
Torque measures how strongly a force turns a body about an axis. The magnitude is M = F·r·sin α, the length of the cross product r × F. F is the force, r is the distance from the axis to the point of application, and α is the angle between the force vector and the arm. At 20 N, 0.3 m, and 90° the sine is 1, so M = 20·0.3·1 = 6 N·m. The same F and r at 30° give 3 N·m, because sin 30° = 1/2.
The calculator uses the three numbers you enter: force F in newtons, arm r in meters, and angle α in degrees. The result is in N·m. The panel shows three decimal places, so 6 N·m appears as 6.000 N·m. Beside the torque, the calculator reports the perpendicular component F⊥ = F·sin α, the sine of the angle, the torque at 90° equal to F·r, and the perpendicular arm r⊥ = r·sin α. The chart plots M against α from 0° to 180° at the F and r you entered.
What the panel shows. At 90° the component F⊥ equals the whole force, and r⊥ equals r. At 30°, with 20 N and 0.3 m, the panel shows F⊥ = 10.00 N, r⊥ = 0.150 m, and M = 3.000 N·m, while the torque at a right angle stays 6.000 N·m. At 0° and at 180° the sine is zero, so the torque is zero: the line of action lies along the arm and the body does not turn. The calculator reports the magnitude of the torque, not a direction. From 0° to 180° the sine is non-negative, and the force and the arm are non-negative as well, so the result is not negative.
Limits of the model. One force, one arm, one angle. The calculator does not add several forces and does not check the balance of two arms. The balance F₁·r₁ = F₂·r₂ is on the lever equilibrium page, and the angle there is a right angle. This page also does not compute angular acceleration from M = I·ε or rotational kinetic energy. A newton-meter of torque has the same dimension as a joule, but a joule measures work W = F·s, not a twist. This page does not compute that work.
F and r must be non-negative. Zero is allowed and gives a torque of zero: a zero force, or a force applied at the axis. A negative number is rejected. The angle must lie from 0° to 180° inclusive. The angle is measured from the arm to the force vector, not from the floor. A comma and a period mean the same value: 0,3 and 0.3. After you switch the header to US units, force is in lbf, the arm is in feet, and the torque is in ft·lbf. The panel then also shows the SI value. The text on this page stays in SI units. The calculator converts with 1 lbf = 4.4482216 N, 1 m = 3.2808399 ft, and 1 ft·lbf = 1.3558179 N·m.
Examples on this page: a wrench with 20 N on 0.3 m at a right angle gives 6 N·m, and the same arrangement at 30° gives 3 N·m. A force of 10 N on an arm of 0.6 m at a right angle gives 6 N·m again. A door handle with 5 N at 0.8 m gives 4 N·m. A force of 25 N along an arm of 0.5 m gives 0 N·m. The button “Fill this example” enters those numbers into the fields and refreshes the panel and the chart.
M = F·r·sin α
F⊥ = F sin α r⊥ = r sin α [M] = N·m
Model: torque, the magnitude of the cross product r × F. At a right angle the sine is 1 and the formula reduces to M = F·r, as in Archimedes’ law of the lever. The calculator computes one force. It does not combine two arms and it does not report a direction.
The torque about an axis is the cross product of the position vector and the force. The position vector r runs from the axis to the point where the force is applied. The magnitude is M = F·r·sin α, where α is the angle between those two vectors. The unit is N·m. In a workshop the same quantity is called a moment of force. This page computes that quantity for one force.
At a right angle the sine is 1, so the formula reduces to M = F·r. That is the moment in Archimedes’ law of the lever: two such magnitudes balance when F₁·r₁ = F₂·r₂. Archimedes stated that condition for weights in the treatise On the Equilibrium of Planes. The sine in the general formula is the later way of writing the length of the cross product r × F. This calculator does not check the balance of two sides.
The same product can be read in two ways. The perpendicular component is F⊥ = F·sin α, and then M = F⊥·r. The perpendicular arm is r⊥ = r·sin α, the distance from the axis to the line of action, and then M = F·r⊥. In this calculator the field r is the distance to the point of application, not the perpendicular arm already. The calculator computes the perpendicular arm separately.
For 20 N, 0.3 m, and 90° both forms agree: F⊥ = 20 N, r⊥ = 0.3 m, and M = 6 N·m. At 30° the sine is 1/2, so F⊥ = 10 N, r⊥ = 0.15 m, and M = 3 N·m. The torque at a right angle, which is F·r alone, stays 6 N·m. The panel shows these numbers with decimal places: 3.000 N·m, 10.00 N, and 0.150 m.
Step 1. Convert the angle to radians only in order to compute the sine: degrees times π/180. Step 2. Multiply F·r·sin α. Step 3. For 20 N, 0.3 m, and 90°: sin 90° = 1, M = 6 N·m, and the panel shows 6.000 N·m. Step 4. For 30°: sin 30° = 0.5, M = 3 N·m, and the panel shows 3.000 N·m. Step 5. A force of 10 N on an arm of 0.6 m at a right angle gives the same product, 6 N·m. Step 6. At 60°, with 30 N and 0.2 m, the sine on the panel is 0.8660 and the torque is 5.196 N·m. At 10°, with 40 N and 0.4 m, the sine is 0.1736, the torque is 2.778 N·m, and r⊥ = 0.069 m.
The sine rises from 0 to 1 between 0° and 90° and falls from 1 to 0 between 90° and 180°. At a fixed F and r the torque is therefore largest at a right angle and equals F·r. At 0° and at 180° the torque is zero. The chart on this page plots that curve for the F and r you entered, at 0°, 30°, 45°, 60°, 90°, 120°, 150°, and 180°.
The calculator does not report whether the body turns clockwise or counterclockwise. In the allowed range the sine is not negative, and F and r are not negative either, so the result does not fall below zero. The direction belongs on the diagram. The calculator rejects 181° and a negative angle.
One force does not replace a system of forces. Varignon’s theorem says that the torque of the resultant equals the sum of the torques of the components, but this page does not form that sum. The balance of two arms is on the lever calculator and requires a right angle. Angular acceleration from M = I·ε and the energy ½Iω² are on separate pages. Work W = F·s has the dimension of a joule. The same written unit N·m does not turn a torque into energy.
The model leaves out thread friction, flex in the wrench, and the fact that a hand may not grip the end of the arm. The number on this page is the torque of the force you entered about the axis you entered. It is not the tightening torque from a bolt specification.
Enter the force in newtons, the arm in meters, and the angle in degrees. The torque comes out in N·m. A centimeter is 0.01 m. After you switch the header units, force is in lbf, the arm is in feet, and the torque is in ft·lbf. The SI value stays beside it. The factors in the page code are 1 lbf = 4.4482216 N, 1 m = 3.2808399 ft, and 1 ft·lbf = 1.3558179 N·m.
M, F, r, and α describe one torque. For 20 N, 0.3 m, and 90° the torque is 6 N·m. At 30° it is 3 N·m. N·m here means a twist, not a joule of work.
Wrench: a force of 20 N acts at a right angle on an arm of 0.3 m. This is the reference example on this page.
M = 6.000 N·m, F⊥ = 20.00 N
The same wrench, 20 N and 0.3 m, but the force is at 30° instead of a right angle. The sine is 1/2.
M = 3.000 N·m, F⊥ = 10.00 N
Half the force and twice the arm: 10 N on 0.6 m at a right angle. The product stays the same.
M = 6.000 N·m, F⊥ = 10.00 N
Door handle: 5 N perpendicular to the door, 0.8 m from the hinge.
M = 4.000 N·m, F⊥ = 5.00 N
A short lug wrench: 150 N at a right angle on 0.15 m.
M = 22.500 N·m, F⊥ = 150.00 N
A force nearly along the arm: 40 N, 0.4 m, angle 10°. The panel rounds the sine to 0.1736.
M = 2.778 N·m, F⊥ = 6.95 N
A force along the arm: 25 N on 0.5 m at 0°. The torque is zero. At 90° it would be 12.5 N·m.
M = 0.000 N·m, F⊥ = 0.00 N
Pedal: 50 N at a right angle, 0.25 m from the crank axis.
M = 12.500 N·m, F⊥ = 50.00 N
A door pushed at 60°: 30 N at 0.2 m from the hinge. The panel shows a sine of 0.8660.
M = 5.196 N·m, F⊥ = 25.98 N
The calculator computes the torque of one force from M = F·r·sin α and the perpendicular component F⊥ = F·sin α. For 20 N, 0.3 m, and 90° the torque is 6 N·m. At 30° it is 3 N·m, because the sine of 30° is 1/2.
Enter the force in newtons, the arm in meters, and the angle in degrees. The torque is in N·m. Enter a centimeter as 0.01 m. After you switch the header to US units, force is in lbf, the arm is in feet, and the torque is in ft·lbf. The panel also shows the SI value.
The angle must lie from 0° to 180° inclusive. The force and the arm must be non-negative. Zero is allowed and gives a torque of zero. A negative number and an angle outside that range are rejected. An empty field is not enough either: all three numbers are required.
The sine of both angles is zero, so the torque is 0 N·m. The line of action lies along the arm and the body does not turn. The panel shows 0.000 N·m. The torque at 90° for the same F and r stays in its own field and equals F·r.
The sine of the angle is then 1, and from 0° to 180° it does not rise higher. At a fixed F and r the torque then equals F·r. Between 0° and 90° the sine rises, and between 90° and 180° it falls back to zero.
The perpendicular component F⊥ = F·sin α is the part of the force perpendicular to the arm. The perpendicular arm r⊥ = r·sin α is the distance from the axis to the line of action. Both forms give the same torque: M = F⊥·r = F·r⊥. At 20 N, 0.3 m, and 30° the results are F⊥ = 10 N and r⊥ = 0.15 m.
No. In this calculator r is the distance from the axis to the point where the force is applied. The perpendicular arm, the distance from the axis to the line of action, is computed as r·sin α. Entering r⊥ in the r field together with an angle other than 90° would apply the sine a second time.
No. The result is the magnitude of the torque. From 0° to 180° the sine is non-negative, so the number does not fall below zero. Clockwise or counterclockwise is marked on the diagram. The calculator does not decide it.
Here there is one moment, M = F·r·sin α, and the angle may be other than a right angle. On the lever equilibrium page two moments balance: F₁·r₁ = F₂·r₂, and the angle is a right angle. This page does not solve for a missing force on the other side of the axis.
The dimension is the same, because 1 N·m = 1 J when the quantity is work. For torque the unit stays N·m, so a twist is not confused with energy. This page does not compute the work W = F·s.
From the arm to the force vector, not from the floor. 90° means the force is perpendicular to the segment from the axis to the point of application. An angle measured from a horizontal floor gives a different sine if the arm is not itself horizontal.
It is, when the force is applied at the end of the handle and r is the distance from the nut axis to that point. If the hand grips the handle closer to the head, r is shorter than the whole wrench. The calculator does not infer where the hand grips.
Yes. 0.3 and 0,3 are the same arm in meters.
Multiply force by arm and by the sine of the angle between them. For 20 N, 0.3 m, and 90°: 20·0.3·1 = 6 N·m.
6 N·m. With the same F and r at α = 30° the result falls to 3 N·m, because sin 30° = 0.5.
Divide by 100: 30 cm = 0.3 m. The arm field expects meters.
No. The result is the torque magnitude M. Rotational power also needs angular speed ω and is not a mode on this page.
No. It finds the torque of one force about an axis. Summing several torques and the equilibrium condition belong on the lever-balance calculator.
The definition, the form with the sine, and the units come from standard mechanics sources.
Page updated November 3, 2026.