Mechanical Properties of Solids

Physics · Class 11

Lesson 9 of 9 · 17 min

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Must-know facts

22 facts

  1. 1Stress = restoring force per unit area = F/A; unit N m⁻² = Pa; dimensions [ML⁻¹T⁻²].
  2. 2Strain is a ratio of lengths or volumes: no unit, no dimensions.
  3. 3Three strains: longitudinal ΔL/L, shearing Δx/L = tan θ ≈ θ, volume ΔV/V.
  4. 4Hooke's law: stress ∝ strain for small deformations; the constant is the modulus of elasticity.
  5. 5Stress-strain curve: O-A proportional (Hooke's law), B yield point or elastic limit (σy), C permanent set if unloaded, D ultimate tensile strength (σu), E fracture.
  6. 6D and E close: brittle. D and E far apart: ductile.
  7. 7Elastomers (rubber, aorta tissue): large elastic region, no Hooke's law over most of it, no well-defined plastic region.
  8. 8Y = FL/(AΔL); G = F/(Aθ); B = −p/(ΔV/V); all three have the unit Pa.
  9. 9Y and G apply only to solids; B applies to solids, liquids and gases.
  10. 10For most materials G ≈ Y/3.
  11. 11Y: steel 2.0 × 10¹¹, copper 1.1 × 10¹¹, bone 9.4 × 10⁹ N m⁻² (values used in NCERT's examples).
  12. 12Same 0.1% strain in a 0.1 cm² wire: steel 2000 N, copper 1100 N, brass 900 N, aluminium 690 N; steel is the most elastic.
  13. 13Compressibility k = 1/B; a gas squeezes roughly a million times more easily than a solid.
  14. 14Bulk modulus of water 2.2 × 10⁹ N m⁻²; air at STP 1.0 × 10⁵ N m⁻² (1.0 × 10⁻⁴ GPa).
  15. 15Water at 3000 m ocean depth (g = 10) is compressed by 1.36%.
  16. 16Poisson's ratio = lateral strain/longitudinal strain; unitless; steels 0.28-0.30, aluminium alloys about 0.33.
  17. 17Elastic energy U = ½ × stress × strain × volume; per unit volume u = ½σε = ½Y(strain)².
  18. 18Beam sag δ = Wl³/(4bd³Y): depth counts as d³, breadth only as b.
  19. 19Crane rope for 10 t: A ≥ Mg/σy = 3.3 × 10⁻⁴ m² (radius about 1 cm); with a safety factor of 10, radius about 3 cm, made of braided thin wires.
  20. 20Mountain height limit: hρg = 30 × 10⁷ N m⁻² with ρ = 3 × 10³ kg m⁻³ gives about 10 km.
  21. 21A wire hung from a ceiling with weight F at its end has tension F, not 2F, at every section, so the stress is F/A.
  22. 22Stress is not a vector: no single direction can be assigned to it.

Common traps

Where marks are lost

Saying rubber is more elastic than steel because it stretches more.

More elastic means less strain for a given stress, that is, a larger modulus. Steel's Y is far larger, so steel is more elastic.

Using the diameter as the radius when finding A = πr².

Halve the diameter first. A 3.0 mm wire has r = 1.5 × 10⁻³ m and A = 7.07 × 10⁻⁶ m².

Leaving areas in mm² or cm² in Y = FL/(AΔL).

1 mm² = 10⁻⁶ m² and 1 cm² = 10⁻⁴ m². Convert before substituting.

Taking the tension in a hanging wire as 2F because the ceiling also pulls with F.

The tension at any cross-section is F, so the tensile stress is F/A.

Thinking a body loaded beyond the proportional limit A is permanently deformed.

Between A and B Hooke's law fails but the body still recovers. Permanent set appears only beyond the yield point B.

Giving bulk modulus a negative value because of the minus sign in B = −p/(ΔV/V).

ΔV is negative when p is positive, so B comes out positive. The sign only says volume falls as pressure rises.

Applying Young's or shear modulus to a liquid.

Liquids and gases have no shape or length of their own; only the bulk modulus applies to them.

Widening a beam to stop it sagging.

δ ∝ 1/(bd³): doubling the depth cuts the sag eightfold, doubling the breadth only halves it.

Treating Poisson's ratio or strain as having units.

Both are ratios of like quantities and are pure numbers.

Formulas

12 to know

Stress

σ = F/A

Unit N m⁻² = Pa; [ML⁻¹T⁻²].

Strains

longitudinal ΔL/L; shearing Δx/L = tan θ ≈ θ; volume ΔV/V

All dimensionless.

Hooke's law

stress = k × strain

Valid only in the linear part OA.

Young's modulus

Y = σ/ε = (F/A)/(ΔL/L) = FL/(AΔL)

So ΔL = FL/(AY).

Shear modulus

G = (F/A)/(Δx/L) = FL/(AΔx) = F/(Aθ); σs = Gθ

G ≈ Y/3 for most materials.

Bulk modulus

B = −p/(ΔV/V)

Positive; applies to solids, liquids and gases.

Compressibility

k = 1/B = −(1/Δp)(ΔV/V)

Largest for gases.

Poisson's ratio

(Δd/d)/(ΔL/L) = (Δd/ΔL)(L/d)

Pure number; steels 0.28-0.30.

Elastic energy

U = ½ × stress × strain × volume = ½ Y A l²/L

Per unit volume u = ½σε.

Beam sag

δ = Wl³/(4bd³Y)

Beam supported near its ends, load W at the centre.

Minimum rope area

A ≥ Mg/σy

Keeps the rope within its elastic limit.

Mountain height limit

hρg = elastic limit of rock

30 × 10⁷ N m⁻², ρ = 3 × 10³ kg m⁻³, g = 10 m s⁻² give h = 10 km.

Key terms

15 terms

Elasticity
The tendency of a body to recover its original size and shape once the deforming force is removed.
Plasticity
The behaviour of a body that stays deformed after the force is removed, as putty and mud do.
Stress
Internal restoring force per unit area of a deformed body; equal in size to the applied force per unit area.
Strain
Change in a dimension divided by the original dimension; a pure number.
Hydraulic stress
Uniform normal stress from a surrounding fluid; equal to the fluid pressure and changing only volume.
Elastic limit (yield point)
Point B of the stress-strain curve, the largest stress after which the body still recovers fully.
Permanent set
The strain left in a body after unloading from beyond its yield point.
Ultimate tensile strength
The highest stress on the stress-strain curve, point D; past it the wire keeps stretching under a smaller force until it breaks.
Brittle
A material whose fracture point lies close to its ultimate strength.
Ductile
A material that strains a long way between its ultimate strength and fracture.
Elastomer
A substance such as rubber or aorta tissue that can take large strains and recover, without following Hooke's law.
Modulus of rigidity
Another name for the shear modulus G.
Compressibility
Reciprocal of bulk modulus; fractional volume change per unit rise in pressure.
Poisson's ratio
Lateral strain divided by longitudinal strain for a stretched wire.
Buckling
Sideways bending of a deep, thin bar under a load that is not exactly placed.
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