INGENIA

CIV-07

Circular shaft torsion

Shear τ = T r / J and twist θ = T L /(G J).

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TorsionCoulomb / NavierEN 1993-1-1

Governing equation

τ=TrJ,J=πd432\tau=\dfrac{T r}{J},\quad J=\dfrac{\pi d^4}{32}

where

T
Torque (kN·m)
d
Diameter (mm)
L
Length (m)
G
Shear modulus (GPa)
\tau
Max shear (MPa)
\theta
Twist (°)

Lecture brief

Historical brief

From Euler’s 1744 elastica and Navier’s beam theory to Mohr’s circle and transformed-section RC, structural mechanics grew as a closed-form craft before finite elements. The lab keeps those governing lines for buckling, flexure, joints and influence. This sheet (CIV-07 — Circular shaft torsion) is the form associated with Coulomb / Navier · EN 1993-1-1. Working symbols: TT, dd, LL, GG \rightarrow τ\tau, θ\theta. For circular sections Saint-Venant torsion reduces to a linear stress field; J = π d⁴/32 is the polar moment.

Purpose

Purpose: compute τ\tau, θ\theta from TT, dd, LL, GG in Structural & civil via τ=TrJ,J=πd432\tau=\dfrac{T r}{J},\quad J=\dfrac{\pi d^4}{32} Shear τ = T r / J and twist θ = T L /(G J). Use it when a real structural & civil question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given T=12.000kNmT = 12.000\,\mathrm{kN·m}, d=80.000mmd = 80.000\,\mathrm{mm}, L=2.000mL = 2.000\,\mathrm{m}, G=80.000GPaG = 80.000\,\mathrm{GPa}, the governing relation τ=TrJ,J=πd432\tau=\dfrac{T r}{J},\quad J=\dfrac{\pi d^4}{32} yields τ=119.366MPa\tau = 119.366\,\mathrm{MPa}, θ=4.274\theta = 4.274\,\mathrm{^{\circ}}. Solid circular shaft, elastic, uniform T. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Max shear \tau119.366 MPa
  • Twist \theta4.274 °
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CIV-07 · beam
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Narration of this film

Solid circular shaft, elastic, uniform T.

For circular sections Saint-Venant torsion reduces to a linear stress field; J = π d⁴/32 is the polar moment.

Reading speed

Watch on YouTube