Strain energy in torsion: for a hollow circular shaft (outer diameter D, inner diameter d) under elastic torsion, the total strain energy expressed using the maximum shear stress τ_max at the outer surface equals which of the following?

Difficulty: Medium

Correct Answer: (τ_max^2 / 4G) × Volume of shaft

Explanation:


Introduction / Context:
Strain energy in torsion is vital for shock and fatigue considerations. For circular shafts, the shear stress varies linearly with radius, so the average energy density differs from the simple τ^2 / (2G) expression that assumes uniform shear. A compact and widely used result expresses total strain energy in terms of τ_max and the volume.



Given Data / Assumptions:

  • Hollow circular shaft, outer diameter D, inner diameter d.
  • Linear elastic torsion, Saint-Venant assumptions.
  • Maximum shear stress τ_max occurs at r = D/2.


Concept / Approach:
Total strain energy U in torsion is U = (T * θ) / 2. Also, U = ∫(τ^2 / 2G) dV, but τ varies with r. Carrying out the radial integration for a circular shaft shows that the average energy density equals τ_max^2 / (4G), so the total is U = (τ_max^2 / 4G) * Volume.



Step-by-Step Solution:

Shear distribution: τ(r) = (τ_max / R) * r with R = D/2.Energy density: u(r) = τ(r)^2 / (2G) = (τ_max^2 / (2G R^2)) * r^2.Integrate over annulus: U = ∫ u(r) dV = ∫_{r_i}^{r_o} (τ_max^2 / (2G R^2)) * r^2 * (2π r L) dr.Simplify integration ⇒ U = (τ_max^2 / 4G) * (π (r_o^2 − r_i^2) L) = (τ_max^2 / 4G) × Volume.


Verification / Alternative check:
From U = T^2 L / (2 G J) and τ_max = T R / J; eliminate T and J to recover U = (τ_max^2 / 4G) × Volume.



Why Other Options Are Wrong:
(τ^2 / 2G) × Volume assumes uniform τ; not valid for circular torsion.Other coefficients (1/6, 1/8, 1) do not match the correct radial integration.



Common Pitfalls:
Using solid-shaft intuition incorrectly; forgetting τ varies with r; confusing τ_max with average shear.



Final Answer:

(τ_max^2 / 4G) × Volume of shaft

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