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Nearly linear elastic region up to fracture; negligible plasticity. Ultimate strength ≈ fracture strength; sudden break after elastic limit. Examples: glass, ceramics, high-carbon steel (quenched).
Ratio of lateral strain to longitudinal strain within elastic limit.
ν = − (εlat / εlong)
Minus sign: tension ⇒ lateral contraction. Dimensionless.
Two wide flanges joined by a thin web. Most bending stress occurs at outer fibers → flanges carry bending; web carries shear → high strength-to-weight for beams.
Within elastic limit, stress ∝ strain.
σ = E ε
Here E = Young’s modulus. Linear region on stress–strain plot.
Rotational resistance about an axis; depends on mass and its distribution.
I = Σ mi ri2 or I = ∫ r² dm
Parallel-axis: I = Icm + M d².
Bending due to localized loads (e.g., point load on simply supported beam or cantilever tip load) where bending moment and shear vary along length → curvature not constant; strain energy distribution non-uniform.
Two equal, opposite, parallel forces with different lines of action → zero net force but finite moment (pure rotation).
M = F × d⊥
Tendency of a force to rotate a body about an axis.
⃗τ = ⃗r × ⃗F , |τ| = r F sinθ
Property by which a material recovers its original shape after removal of load (within elastic limit). Beyond limit ⇒ plastic (permanent) deformation.
Internal restoring force per unit area.
σ = F / A
SI unit: Pascal (Pa = N m⁻²). Types: tensile, compressive, shear.
Rotational analogue of Newton’s 2nd law.
⃗τ = d⃗L/dt
If external τ = 0 ⇒ ⃗L is conserved.
Repeated bending causes internal friction and dislocation motion (plastic work). Mechanical energy dissipates as heat (elastic hysteresis) → wire becomes warm.
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