Math 2.0

Mechanics of deformable solids Definition

Fatigue

Builds on Stress

Definition

Let a specimen of a material be loaded cyclically, so that the stress at a point oscillates between σmin⁡\sigma_{\min} and σmax⁡\sigma_{\max}. The stress amplitude is σa=(σmax⁡−σmin⁡)/2\sigma_a = (\sigma_{\max} - \sigma_{\min})/2 and the mean stress is σm=(σmax⁡+σmin⁡)/2\sigma_m = (\sigma_{\max} + \sigma_{\min})/2. Fatigue is the progressive and localized damage of the material under such loading, by crack initiation and crack growth. It leads to fracture after a finite number of cycles, even when σmax⁡\sigma_{\max} is below the static tensile strength. The fatigue life Nf(σa,σm)N_f(\sigma_a, \sigma_m) is the number of cycles to failure, and the graph of NfN_f against σa\sigma_a at fixed σm\sigma_m is the S–N curve. The endurance limit, when it exists, is the amplitude below which Nf=∞N_f = \infty.

Remarks

Example: in the high-cycle regime many metals follow Basquin's law σa=σf′(2Nf)b\sigma_a = \sigma_f' (2 N_f)^b, with material constants σf′>0\sigma_f' > 0 and b<0b < 0; then halving the stress amplitude multiplies the life by 2−1/b2^{-1/b}. Non-example: failure of a bar under a single load above its tensile strength is static fracture, not fatigue, because no cycling is involved. Many steels show an endurance limit, while aluminium alloys do not, and their S–N curves keep decreasing.

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Further reading

  1. Web https://en.wikipedia.org/wiki/Fatigue_(material)
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Changed3 November 2026

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