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JEE · NEET Physics

Class 11 · Chapter 9

Mechanical Properties of Solids

Overview, notes, short notes, formula sheet, daily practice problems, previous year questions, and videos for this chapter — all in one place.

Mechanical Properties of Solids Formula Sheet

9 formulas across 3 topics in Mechanical Properties of Solids.

1 min read

Updated 2026-07-03 · v1.0.0

Stress & Strain

Stress is the internal restoring force per unit area; strain is the fractional deformation. Their ratio — within the elastic limit — defines the material.

Stress = F / A

Stress

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Finternal restoring force (equals applied force in equilibrium)N[MLT⁻²]
Across-sectional area[L²]

Valid when

  • Unit N/m² (pascal) — same unit and dimensions as pressure, but stress is not a scalar like pressure

Common mistakes

  • Longitudinal (tensile/compressive), shear (tangential) and volumetric stress are three different animals — identify which before picking a modulus

Strain = ΔL / L (longitudinal); ΔV/V (volumetric); tanφ ≈ φ (shear)

Strain (three types)

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
ΔLchange in lengthm[L]
Loriginal lengthm[L]
φshear anglerad[M⁰L⁰T⁰]

Valid when

  • Dimensionless — it is a ratio

Worth remembering

  • Hooke's law (stress ∝ strain) holds only up to the proportional limit — the stress-strain curve then bends through elastic limit, yield point, and fracture
  • Elastomers (rubber) stretch enormously WITHOUT obeying Hooke's law and without permanent set

Elastic Moduli

Three moduli for three deformation modes: Young's for stretching, bulk for squeezing, shear for twisting. All share the unit of stress.

Y = (F/A) / (ΔL/L) = FL / (A ΔL)

Young's modulus

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
YYoung's modulus of the materialsteel ≈ 2 × 10¹¹ N/m² — property of MATERIAL, not of the wireN/m²[ML⁻¹T⁻²]

Valid when

  • Within the proportional limit
  • Solids only

Common mistakes

  • A thicker or longer wire has the SAME Y — geometry changes ΔL, never Y
  • Y(steel) > Y(copper) > Y(rubber): larger Y means HARDER to stretch, so steel is more elastic than rubber in physics language

ΔL = FL / (AY) = MgL / (πr²Y)

Elongation of a loaded wire

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Rearranging the Young's modulus definition

Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
ΔLextensionm[L]
rwire radiusm[L]

Valid when

  • Wire stretching under its OWN weight: ΔL = ρgL²/2Y (half the naive value, because tension varies along the wire)

Common mistakes

  • Same load, wire of double radius → ΔL becomes ¼ (A ∝ r²) — ratio questions live here

B = −ΔP / (ΔV/V); compressibility k = 1/B

Bulk modulus & compressibility

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Bbulk modulusN/m²[ML⁻¹T⁻²]
ΔPchange in pressureN/m²[ML⁻¹T⁻²]
ΔV/Vfractional volume changedimensionless[M⁰L⁰T⁰]

Valid when

  • Minus sign keeps B positive (pressure up, volume down)
  • Defined for solids, liquids AND gases

Common mistakes

  • For gases B depends on the process: isothermal B = P, adiabatic B = γP

η = (F/A) / φ

Shear modulus (modulus of rigidity)

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
ηshear modulusN/m²[ML⁻¹T⁻²]
φshear anglerad[M⁰L⁰T⁰]

Valid when

  • Solids only — fluids cannot sustain shear stress at rest (that is what makes them fluids)

σ = − (lateral strain) / (longitudinal strain)

Poisson's ratio

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
σPoisson's ratiotheoretical range −1 to 0.5; most metals ≈ 0.3dimensionless[M⁰L⁰T⁰]

Valid when

  • σ = 0.5 means volume stays constant on stretching (ideal rubber)

Worth remembering

  • Y, B and η exist only within elastic behaviour; beyond the yield point the material flows plastically and no modulus applies

Elastic Potential Energy

Stretching a wire stores energy exactly like compressing a spring — the wire IS a very stiff spring with k = YA/L.

u = ½ × stress × strain = ½ Y (strain)²

Elastic energy density

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Work done per unit volume = area under the stress-strain curve

Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
uenergy stored per unit volumeJ/m³[ML⁻¹T⁻²]

Common mistakes

  • The factor ½ exists because force GROWS from zero — using full F × ΔL doubles the answer

k(wire) = YA / L

Effective spring constant of a wire

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Comparing F = (YA/L)ΔL with F = kx

Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
k(wire)equivalent spring constantN/m[MT⁻²]

Valid when

  • Wires in series/parallel combine exactly like springs

Worth remembering

  • Breaking force depends on AREA only, not length — a longer rope is not weaker; breaking STRESS is the material property

NEET keeps to direct modulus and energy-density substitutions; JEE builds composite rods and wire-block oscillation systems from k = YA/L.

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