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Factor Of Safety Ultimate⚠ unverified

Mechanical / Stress Analysis · Compute the factor of safety against ultimate (fracture) failure

Parameters

InputSymbolUnitDefaultDescription
SutSutPa1.0Material ultimate tensile strength
sigma_maxσmaxPa1.0Maximum applied stress
OutputSymbolUnitDescription
resultnDimensionless factor of safety against ultimate failure

The science & history

Understanding the Parameters

Derivation (Approaching a Proof)

Fracture is taken to occur when the maximum stress reaches the ultimate strength:

$$\sigma_{max} = S_{ut} \quad\text{(fracture)}.$$

The factor of safety is the ratio of that capacity to the applied peak stress — equivalently, the factor by which the (proportional) load may be scaled before fracture:

$$n = \frac{S_{ut}}{\sigma_{max}}.$$

At $n = 1$ the peak stress equals the ultimate strength; $n > 1$ leaves margin. For brittle materials, using the maximum principal stress for $\sigma_{max}$ makes this the maximum-normal-stress (Rankine) failure check.

Dimensional check. $n = \dfrac{S_{ut}}{\sigma_{max}} = \dfrac{\text{Pa}}{\text{Pa}}$ = dimensionless — a pure factor, as required.

History and Development

The maximum-normal-stress theory pairing with an ultimate-strength margin is the classical Rankine criterion (W.J.M. Rankine, 19th century), appropriate for brittle materials such as cast iron, ceramics, and glass that fracture on the plane of maximum tensile stress. The distinction between yield-based and ultimate-based factors of safety — and choosing the right one for the material's failure mode — is a cornerstone of design practice.

Related Concepts: Factor of Safety yield, Max Principal Stress, Stress Concentration, Principal Stresses, Static Failure Theories, Von Mises Stress

Notes: Guards fracture (use for brittle materials); ductile parts usually governed by yield (Factor of Safety yield). For brittle/stress-raiser cases use the peak principal stress $K_t\sigma_{nom}$ (brittle materials don't redistribute). Maximum-normal-stress (Rankine) theory.

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