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Engineering reference

Mechanical Properties & Failure: theory, method, and sources

This materials science workspace publishes 12 governing equations, 6 stated assumptions, 1 documented boundary, and 2 sources so the numbers it returns can be checked rather than taken on trust.

Calculations run locallyCalculation & source methodology

How this tool works

Eleven modules cover engineering and true stress–strain, isotropic elastic constants, modulus of resilience, toughness by curve integration, Vickers hardness, Charpy impact energy, critical crack stress, Paris law fatigue crack growth, Basquin high-cycle fatigue, Norton creep, and Hall–Petch strengthening.

Fracture, fatigue, and creep are treated with the same stress basis, so a design stress can be checked against fast fracture, cyclic life, and time-dependent deformation in sequence.

Calculators and topics covered

  • stress strain
  • fracture
  • fatigue
  • creep
  • hardness
  • tensile test
  • Vickers
  • Hall Petch
  • Basquin
  • fracture toughness

Core equations

engineering stress and strain:σ=FA0,  ε=ΔLL0\text{engineering stress and strain:}\quad \sigma = \frac{F}{A_{0}},\; \varepsilon = \frac{\Delta L}{L_{0}}true stress and strain:σt=σ(1+ε),  εt=ln(1+ε)\text{true stress and strain:}\quad \sigma _{t} = \sigma \left(1 + \varepsilon \right),\; \varepsilon _{t} = \ln \left(1 + \varepsilon \right)isotropic elasticity:G=E2(1+ν),  K=E3(12ν)\text{isotropic elasticity:}\quad G = \frac{E}{2 \left(1 + \nu \right)},\; K = \frac{E}{3 \left(1 - 2 \nu \right)}modulus of resilience:Ur=σy22E\text{modulus of resilience:}\quad U_{r} = \frac{\sigma _{y}^{2}}{2 E}toughness:Ut=σ  dε  (trapezoidal  integration  of  the  curve)\text{toughness:}\quad U_{t} = \int \sigma \; d\varepsilon \; \left(\text{trapezoidal}\; \text{integration}\; of\; the\; \text{curve}\right)Vickers hardness:HV=1.854Fd2\text{Vickers hardness:}\quad HV = \frac{1.854 F}{d^{2}}Charpy impact energy:E=mg(h1h2),  impact  toughness=EA\text{Charpy impact energy:}\quad E = \mathrm{mg} \left(h_{1} - h_{2}\right),\; \text{impact}\; \text{toughness} = \frac{E}{A}critical crack stress:σc=KICYπa\text{critical crack stress:}\quad \sigma _{c} = \frac{K_{IC}}{Y \sqrt{\pi a}}Paris law:dadN=C(ΔK)m,  integrated  from  a0  to  a1\text{Paris law:}\quad \frac{da}{dN} = C \left(\Delta K\right)^{m},\; \text{integrated}\; \text{from}\; a_{0}\; to\; a_{1}Basquin relation:σa=σf(2Nf)b\text{Basquin relation:}\quad \sigma _{a} = \sigma ^{\prime}_{f} \left(2 N_{f}\right)^{b}Norton creep:ε˙=Aσnexp(QkT)\text{Norton creep:}\quad \dot{\varepsilon } = A\sigma ^{n} \exp \left(\frac{- Q}{kT}\right)Hall–Petch:σy=σ0+kd12\text{Hall–Petch:}\quad \sigma _{y} = \sigma _{0} + k \cdot d^{\frac{- 1}{2}}

Method and assumptions

Assumptions

  • Materials are homogeneous, isotropic, and free of residual stress unless stated.
  • Engineering stress uses the original cross-sectional area, so it diverges from true stress after necking begins.
  • Linear elastic fracture mechanics applies, which requires small-scale yielding at the crack tip.
  • Paris law integration assumes constant amplitude loading with no crack closure, overload retardation, or threshold effects.
  • Basquin and Norton coefficients are material- and temperature-specific and must come from test data for the exact condition.
  • Fatigue and creep predictions are order-of-magnitude estimates, not certified life.

Limitations and design boundaries

  • Educational screening models only. Material certification, process qualification, applicable standards, statistical variability, environmental conditioning, and professional engineering judgment are required for real selection or design.

Sources and references

Primary sources are preferred for ratings, standards, manufacturer data, and externally defined constants.

Source policy
  • Callister and Rethwisch, Materials Science and Engineering: An Introduction
  • Askeland and Wright, The Science and Engineering of Materials