MAT-00 · laboratory
Hooke, Hall–Petch, Arrhenius, Paris law and the lever rule.
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34 governing sheets
σ = E ε in the linear elastic regime.
Elasticityσy = σ0 + ky / √d.
Strengtheningk = A exp(−Ea /(R T)) for thermally activated processes.
Kineticsda/dN = C (ΔK)^m in the mid-ΔK regime.
FractureWα = (Cβ − C0)/(Cβ − Cα) for a two-phase alloy.
Phase diagramsσt = σe (1+εe) at constant volume.
Plasticityσf = √(2 E γ /(π a)) for a through crack.
Fractureτ = c + σ tan φ on the failure plane.
Failureσy = σ0 + ky / √d. Yield rises as grains shrink.
Strengtheningda/dN = C (ΔK)^m in the mid-ΔK regime.
FractureWα = (Cβ − C0)/(Cβ − Cα) for a two-phase alloy.
Phase diagramsσt = σe (1+εe), εt = ln(1+εe) at constant volume.
PlasticityFor Hollomon σ = K ε^n, necking starts at εt = n. Load maximum dP = 0.
Plasticityε̇ = A σ^n. Secondary (steady) creep rate.
CreepKIc = Y σ √(π a). Critical stress-intensity in mode I.
Fractureτ = α G b √ρ. Forest hardening from dislocation density.
Strengtheningn λ = 2 d sinθ. Constructive interference from crystal planes.
CrystallographyJ = −D (c2−c1)/Δx. Steady diffusion down a concentration gradient.
DiffusionΔL = α L ΔT. Length change from a temperature step.
Elasticityν = −εlat / εlong. Lateral contraction over axial stretch.
ElasticityK = E / [3(1−2ν)]. Volumetric stiffness of an isotropic solid.
ElasticityG = E / [2(1+ν)]. The isotropic relation between E, G and ν.
ElasticitySe ≈ 0.5 Sut · ka kb kc. Marin factors on a rotating-beam limit.
Fatigueσ = K ε^n. Power-law true stress–strain in the plastic range.
PlasticityP = T (C + log10 tr) / 1000. Time–temperature collapse of rupture data.
Creepτ = G b / λ. Bypass of impenetrable particles by dislocation loops.
StrengtheningLogarithmic strain.
GoverningNecking when n equals true strain for Hollomon.
GoverningSteady-state power-law creep.
GoverningBrittle fracture of a through-crack.
GoverningGrain-size strengthening.
GoverningIsostrain composite modulus.
Governingσ = E ε in the linear elastic range.
Mechanics of materialsk = A exp(−Ea / RT). Thermal activation over a barrier Ea.
Mechanics of materials