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Physics · Ch 8 — Mechanical Properties of Solids

Summary

Summary

This chapter developed the mechanics of elastic solids from first principles, along exactly the topics WBCHSE's Unit 7 SUB TOPIC 1 lists:

  • Elastic and plastic behaviour (Section 8.1): a body is elastic if it fully recovers its original shape once a deforming force is removed, and plastic if it does not.
  • Stress and strain (Section 8.2): stress is the internal restoring force per unit area, F/AF/A (SI unit Pa\text{Pa}); strain is the resulting fractional deformation (dimensionless). Three kinds of each were distinguished: tensile/compressive (longitudinal), shearing (tangential), and hydraulic (volume).
  • Hooke's law (Section 8.3): within the proportional limit, stress ∝\propto strain, with the constant of proportionality called the modulus of elasticity.
  • The stress-strain curve (Section 8.4): read for a ductile metal from the proportional limit, through the elastic limit and yield point, up to the ultimate tensile strength and finally the fracture point; contrasted with a brittle material's short, steep curve.
  • The three elastic moduli: Young's modulus Y=FLA ΔLY = \dfrac{FL}{A\,\Delta L} for longitudinal deformation (Section 8.5), the shear modulus of rigidity η=F/Aθ\eta = \dfrac{F/A}{\theta} for shape-changing deformation, with η=0\eta = 0 identically for any fluid (Section 8.6), and the bulk modulus K=−ΔPΔV/VK = -\dfrac{\Delta P}{\Delta V/V} for volume-changing deformation, with compressibility =1/K= 1/K (Section 8.7).
  • Poisson's ratio σ=−lateral strainlongitudinal strain\sigma = -\dfrac{\text{lateral strain}}{\text{longitudinal strain}} (Section 8.8), a dimensionless number typically between 0.20.2 and 0.40.4 for ordinary solids, with a theoretical upper limit of 0.50.5. …