Calculate torsional spring rate, deflection angle, bending stress, and stored energy. Built-in wire material database with safety factor analysis.
The torsional spring calculator computes the rate, deflection, stress, and stored energy of helical torsion springs — the type that applies a rotational torque rather than a linear force. These springs are found in clothespins, door hinges, mousetraps, garage doors, clock mechanisms, and countless other devices where rotational force is needed.
Unlike compression or extension springs that resist linear loads, torsion springs resist angular rotation. They are wound as helical coils and have straight legs that transmit torque. When one leg is held stationary and the other is rotated, the spring stores energy as bending stress in the wire. The spring rate is expressed in torque per unit angle (N·m/rad or mN·m/degree).
This calculator includes a database of 7 common spring wire materials with their shear modulus and tensile strength values. It calculates the stress concentration factor (Ki), checks against the allowable bending stress (0.78 × Sut for static loading), and provides a torque-vs-deflection table showing at which angle the spring will exceed its stress limit.
Torsion springs are deceptively simple components that require careful engineering to ensure they meet torque requirements without exceeding stress limits. This calculator eliminates the need for manual calculations and provides instant feedback on the stress, safety factor, and operating range.
The torque-deflection table is particularly useful — it shows exactly where the spring transitions from safe (green) to marginal (yellow) to overstressed (red) as the angle increases, allowing you to set proper mechanical stops and define the operating range.
Torsion Spring Rate: k = πd⁴G / (64DNa + 64×2×L_leg), where d = wire diameter, D = mean coil diameter, Na = active turns, G = shear modulus, L_leg = leg length. Stress concentration factor: Ki = (4C²−C−1) / (4C(C−1)), where C = D/d. Bending stress: σ = Ki × 32M / (πd³). Stored energy: U = ½kθ². Allowable stress: σ_allow = 0.78 × Sut (static).
Result: Spring rate = 6.68 mN·m/°, deflection = 149.7°, stress = 1458 MPa, SF = 1.16
With d = 2 mm, D = 15 mm, and Na = 6: C = 7.5, Ki = 1.08. Rate ≈ 0.00668 N·m/°. At 1 N·m torque, angle = 1/0.00668 = 149.7°. Bending stress = 1.08 × 32 × 1 / (π × 0.002³) = 1458 MPa. Allowable = 0.78 × 2170 = 1693 MPa, so SF = 1.16.
A torsion spring is a helical coil of wire with straight legs extending from each end. When one leg is held fixed and a torque is applied to the other, the coil winds tighter (or, less commonly, looser), storing energy as bending stress in the wire material. Unlike the name suggests, the wire itself is not in torsion — it's in bending.
The spring rate is determined by the wire diameter (d), coil diameter (D), number of active turns (Na), and the elastic modulus of the wire material. The relationship is approximately linear: doubling the applied torque doubles the angular deflection. This linearity holds until the stress approaches the yield point and the wire begins to take a permanent set.
**Spring index (C):** The ratio D/d controls both the stress concentration and manufacturability. Spring indexes below 4 are extremely difficult to wind and have very high stress concentrations. Indexes above 12 produce springs that tend to buckle or tangle. The sweet spot of C = 6-10 provides good performance and reasonable manufacturing cost.
**Leg design:** The straight legs are often the most critical design element. Their length, attachment angle, and connection method determine how torque is transmitted. Longer legs reduce the effective spring rate and change the angular relationship between the fixed and loaded ends.
**Operating range:** Every torsion spring has a maximum safe deflection angle determined by the point where bending stress reaches the allowable limit. The torque-vs-deflection table in this calculator makes it easy to identify this limit and design appropriate mechanical stops.
Torsion springs are ubiquitous in mechanical design. Common applications include door closers (returning doors to closed position), counterbalance mechanisms (garage doors, laptop hinges), trigger mechanisms (mousetraps, spring-loaded devices), and constant-torque applications (clock mainsprings, retractable reels). In each case, the spring must deliver the right torque over the right angular range for the required number of cycles.
C = D/d (mean coil diameter divided by wire diameter). A spring index of 4-12 is generally manufacturable. Below 4, the wire is hard to form; above 12, the coil may tangle or buckle. C also affects the stress concentration factor.
Reducing the coil diameter (D) increases the spring rate proportionally (k ∝ 1/D). However, tighter coils (lower C) increase the stress concentration factor and make manufacturing more difficult.
Longer legs act as additional lever arms that deflect under load, effectively reducing the spring rate. The simplified formula (without legs) gives a higher rate than reality. Always include leg lengths for accurate results.
Static loading assumes the torque is applied slowly and held. Dynamic or cyclic loading requires much lower allowable stresses (typically 0.53-0.60 × Sut) and fatigue analysis, especially if the spring cycles millions of times.
Torsion springs are loaded in bending, not torsion (despite the name). The wire experiences bending stress across its cross section, unlike compression springs which experience torsional shear in the wire.
Music wire (A228) has the highest strength and is the most common. Use stainless steel for corrosion resistance, phosphor bronze for electrical conductivity, and chrome silicon for high-temperature applications.