Audited 31 Jul 2026·Last updated 28 Oct 2026·3 citations·Tier 2·0 uses

Rotational Stiffness Calculator

Find rotational stiffness in N·m per radian by dividing an applied torque by the twist it produces, as measured on a shaft, coupling, spring or joint.

Rotational Stiffness Calculator

N·m
rad
Rotational stiffness
6,000
Torque needed per radian of twist, in newton-metres per radian, at the load you entered.
Model scope
Secant stiffness for the entered load point; it assumes a linear elastic torque-angle response and does not select a material or geometry.

Background.

Twist a shaft, a coupling or a bolted beam-to-column joint and it resists by turning back against you. How hard it resists for each unit of twist is its rotational stiffness — the turning-motion counterpart of a spring constant. A stiff drive shaft barely winds up under engine torque; a flexible coupling is designed to wind up noticeably so that shock loads are cushioned before they reach the gears and bearings.

The number is simply torque divided by the angle it produces. Apply 120 newton-metres and measure 0.02 radians of rotation, a little over one degree, and the stiffness is 6,000 N·m per radian. That one figure feeds straight into the questions engineers care about. In a drivetrain or a gauge it sets the torsional natural frequency, √(k/J) in radians per second for a rotor of inertia J, and so decides whether the system will resonate at a running speed. In a structure it decides how much a connection lets a beam end rotate, which shifts bending moments between members.

Two things are easy to get wrong. The angle must be in radians: one radian is about 57.3°, so a deflection read off in degrees and typed in as if it were radians makes the stiffness come out 57.3 times too small. And the ratio describes the component only while its response stays linear. Rubber couplings, slipping joints and anything approaching yield get softer as the load rises, so a stiffness worked out from a single load and angle is a secant value for that load. It may not hold at another.

For a solid round shaft, the stiffness can also be predicted from its geometry and material as G × J_p ÷ L, but that prediction is not made here; this page starts from a measured or specified torque and angle.

What is rotational stiffness calculator?

Rotational stiffness, also called torsional stiffness or a torsional spring constant, is the torque required per unit of angular deflection: k_θ = T ÷ θ. In SI units it is measured in newton-metres per radian. It describes how strongly a component resists being twisted, in the same way that a linear spring constant in newtons per metre describes resistance to being stretched.

How to use this calculator.

  1. Enter the applied torque in newton-metres. If you have force and lever arm, multiply them; 400 N on a 0.3 m arm is 120 N·m. To convert from pound-feet, multiply by 1.3558.
  2. Enter the rotation that torque produced, in radians. To convert from degrees, multiply by π ÷ 180, so 1.146° is 0.02 rad.
  3. Use the twist of the part you care about only. If your measurement includes slack in the clamps, keys or bolts, the result will describe the whole assembly, not the part.
  4. Read the stiffness in N·m/rad. For a per-degree figure, multiply it by π ÷ 180.

The formula.

k_θ = T / θ

k_θ = T ÷ θ, where T is the applied torque in newton-metres and θ the resulting angular deflection in radians. Because the radian is dimensionless, the unit N·m/rad is sometimes written simply as N·m; keeping the rad makes clear that the value is per radian rather than per degree. The relation is the rotational form of Hooke's law, T = k_θ θ, and holds while the material and joints respond elastically and in proportion. Doubling the torque for the same twist doubles the stiffness; doubling the twist for the same torque halves it. Two torsional springs in series combine as 1/k = 1/k₁ + 1/k₂, and in parallel their stiffnesses add. The energy stored in the twisted part is ½ k_θ θ².

A worked example.

Example

A shaft fixed at one end has 120 N·m applied at the other and twists by 0.02 rad, which is 0.02 × 180 ÷ π ≈ 1.146°. Dividing torque by angle gives 120 ÷ 0.02 = 6,000 N·m/rad. Per degree, that is 6,000 × π ÷ 180 ≈ 104.7 N·m. The energy stored in the twist is ½ × 6,000 × 0.02² = 1.2 J. Had the 1.146° reading been typed in as if it were radians, the result would have been 120 ÷ 1.146 ≈ 104.7 N·m/rad — numerically the per-degree value, about 57 times too low. Coupling two such shafts end to end, in series, would halve the stiffness of the pair to 3,000 N·m/rad.

angular Deflection Rad0.02
torque Nm120

Frequently asked questions.

How is rotational stiffness used to find a natural frequency?
For a rotor of polar moment of inertia J on a torsional spring of stiffness k_θ, the undamped natural frequency is √(k_θ ÷ J) in radians per second. A 6,000 N·m/rad shaft carrying a 0.5 kg·m² rotor would vibrate at about 17.43 Hz. Running a machine near that speed invites torsional resonance.
How do I convert between N·m per radian and N·m per degree?
Multiply a per-radian stiffness by π ÷ 180, about 0.01745, to get the per-degree value; divide to go the other way. A stiffness of 6,000 N·m/rad is about 104.7 N·m per degree. Product datasheets for couplings and joints use both, so check the unit before comparing.
What is the difference between secant and tangent stiffness?
Secant stiffness is torque divided by total angle at a given load, the straight line from zero to that point; it is what this page gives. Tangent stiffness is the slope of the torque–angle curve at that point. For a perfectly linear part they are equal; for rubber or a slipping joint they diverge.
How can I predict the stiffness of a round shaft before testing it?
For a solid or hollow circular shaft, k_θ = G × J_p ÷ L, where G is the material's shear modulus, J_p the polar second moment of area and L the length. For a solid shaft J_p = πd⁴ ÷ 32, so doubling the diameter makes the shaft sixteen times stiffer, and doubling the length halves it.
Why did my measured stiffness come out lower than the calculated value?
Any compliance in the test path adds in series with the part itself: keyways, splines, clamps, bolted flanges and the test rig all twist a little. Since series stiffnesses combine reciprocally, a soft clamp or rig can pull the measured value well below the part's true stiffness. Measure the angle as close to the part as you can.

References& sources.

  1. [1]Inman, Engineering Vibration, 4th ed. (PRINT), section 2.2, torsional spring stiffness and torque-displacement relation.
  2. [2]NPTEL, Mechanical Vibrations, torsional vibration model and torsional spring relation.
  3. [3]BIPM, The International System of Units (SI Brochure), 9th ed., version 3.01, coherent derived units and quantity equations.

How this page was produced

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Quanta Calculator
Primary sources
3 cited below
Method
k_θ = T / θ
Published
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