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PRINCIPAL STRESSES, MAX SHEAR, VON MISES, TRESCA YIELD
Stress analysis converts a multi-axial state of stress (σx, σy, τxy) into a single scalar that can be compared to a material yield strength. Two principal directions exist where shear vanishes and normal stress is maximum or minimum; these are the principal stresses σ1 and σ2. The maximum in-plane shear stress sits at 45° to those axes. Mohr's circle plots normal stress on the x-axis and shear stress on the y-axis, parameterizing the rotation of the stress tensor as you change reference frame.
σ_avg = (σx + σy)/2R = sqrt(((σx - σy)/2)² + τxy²)σ1, σ2 = σ_avg ± Rτ_max = Rσ_vM = sqrt(σ1² - σ1·σ2 + σ2²)FoS = Sy / σ_vMReferences & StandardsShigley 9.6, Norton 5.4, ASME BPVC VIII-1 UG-23
Use this module any time a part sees combined loading: a pressure-vessel wall (hoop + longitudinal + radial), a shaft under torque + bending, a weld throat under shear + tension, or a bolted bracket where eccentric load creates simultaneous tension and shear at the same fastener. The von Mises criterion gives a single number to compare to yield for ductile materials; the maximum-shear (Tresca) criterion is more conservative. For brittle materials, use the maximum principal-stress criterion instead.
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