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Strength of Materials
Standard Equation

Torsional Shear Stress in Circular Shafts

Calculates the shear stress at any radial location in a circular solid or hollow shaft under torsional load.

Primary Mathematical Expression

\tau = T * r / J

Design Schematic

Bearing ABearing BPulley 1F1Gear SeatF_mesh (Bending)KeywayTorque (T)Fillet Shoulders

Nomenclature & Variables

SymbolVariable NameMetric UnitImperial UnitDescription
TApplied torqueN·min·lbThe torsional moment load twisting the bar.
rRadial distancemminRadial distance from center axis to the point of interest.
JPolar moment of inertiamm⁴in⁴The geometric torsional resistance property of the cross-section.
\tauTorsional shear stressMPapsiThe resulting shear stress at radius r.

Step-by-Step Derivation

  1. 1

    A circular bar is subjected to pure torsion, causing cross-sections to rotate relative to each other about the longitudinal axis.

  2. 2

    Shear strain \gamma is proportional to radial distance r: \gamma = r * \phi, where \phi is the twist rate per unit length.

  3. 3

    Assuming elastic behavior, Hooke's Law for shear applies: \tau = G * \gamma = G * r * \phi.

  4. 4

    The resisting internal torque must balance the external torque: T = \int \tau * r * dA = \int (G * r² * \phi) * dA = (G * \phi) * J.

  5. 5

    Substituting G * \phi = T / J back into the stress equation yields the torsional shear stress formula: \tau = T * r / J.

Worked Example Calculation

Problem Statement

A solid circular shaft of radius 15 mm is subjected to a torque of 450 N·m. The polar moment of inertia J is 7.95 \times 10^4 mm⁴. Calculate the maximum torsional shear stress.

Calculation Steps
  • Identify input parameters: T = 450 N·m = 450,000 N·mm, r = 15 mm, J = 79,500 mm⁴.
  • Apply the Torsional Shear Stress Formula: \tau = T * r / J.
  • Compute: \tau = (450,000 * 15) / 79,500 = 6,750,000 / 79,500 = 84.9 MPa.
Final ResultShear Stress = 84.9 MPa

Engineering Assumptions

  • The bar has a circular cross-section (solid or hollow).
  • The material is homogeneous, isotropic, and obeys Hooke's Law in shear.
  • Cross-sections remain plane and do not warp during twisting.

Design Limitations

  • Not applicable to non-circular cross-sections (which undergo warping, requiring Prandtl stress function analysis).
  • Underestimates stress if twisting exceeds the elastic limit of the material.

Academic References & Standards

Shigley Ch 3textbook

Shigley's Mechanical Engineering Design, 11th Edition

Textbook covering torsional stresses and shafts.