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MEC-38

Castigliano axial deflection

δ = ∂U/∂P = P L /(A E) for an axial bar. U = P² L /(2 A E).

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EnergyCastigliano 1873

Governing equation

δ=UP=PLAE\delta=\dfrac{\partial U}{\partial P}=\dfrac{PL}{AE}

where

P
Axial load (kN)
L
Length (m)
A
Area (cm^2)
E
Modulus (GPa)
\delta
Extension (mm)

Lecture brief

Historical brief

Machine design grew from Coulomb torsion and Hertz contact (1881) through Soderberg fatigue and the heat-engine cycle. The lab writes shaft, bearing, contact and thermodynamic limits in SI. This sheet (MEC-38 — Castigliano axial deflection) is the form associated with Castigliano 1873. Working symbols: PP, LL, AA, EE \rightarrow δ\delta. Castigliano's second theorem: displacement conjugate to a force is the derivative of complementary energy.

Purpose

Purpose: compute δ\delta from PP, LL, AA, EE in Mechanical via δ=UP=PLAE\delta=\dfrac{\partial U}{\partial P}=\dfrac{PL}{AE} δ = ∂U/∂P = P L /(A E) for an axial bar. U = P² L /(2 A E). Use it when a real mechanical question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given P=80.000kNP = 80.000\,\mathrm{kN}, L=2.000mL = 2.000\,\mathrm{m}, A=12.000cm2A = 12.000\,\mathrm{cm^2}, E=200.000GPaE = 200.000\,\mathrm{GPa}, the governing relation δ=UP=PLAE\delta=\dfrac{\partial U}{\partial P}=\dfrac{PL}{AE} yields δ=0.6667mm\delta = 0.6667\,\mathrm{mm}. A bar, an axial P, a stretch. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Extension \delta0.6667 mm
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Narration of this film

A bar, an axial P, a stretch.

Castigliano's second theorem: displacement conjugate to a force is the derivative of complementary energy.

Reading speed

Watch on YouTube