Q.A piece of copper having a rectangular cross-section of 15.2 mm×19.1 mm is pulled in tension with 44,500 N force, producing only elastic deformation. Calculate the resulting strain.
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Young’s Modulus: The Stretchiness of a Solid
When you pull on a rubber band, it stretches easily. When you pull on a steel rod of the same size, it barely moves. Both are elastic — they return to their original shape when you let go — but they resist stretching very differently. Young’s modulus is the number that tells you exactly how much a material resists being stretched or compressed lengthwise.
The Intuition: Stiffness per Unit Size
Think of a spring. A stiff spring requires a large force to stretch it a little. A soft spring stretches a lot with a small force. Young’s modulus is like the “stiffness” of a material, but it’s cleverly designed to be independent of the object’s shape and size.
If you take a thick steel rod and a thin steel wire of the same length, the rod is harder to stretch. That’s because you’re pulling on more material. Young’s modulus removes this size effect — it tells you the stiffness of the material itself, not the particular piece you’re holding.
The Precise Definition
Young’s modulus (E or Y) is defined as the ratio of tensile stress to tensile strain, as long as the material obeys Hooke’s law (the deformation is reversible and proportional to the force).
Y=Tensile StrainTensile Stress
Let’s break down the two parts.
Tensile Stress (σ) is the force per unit area. If you pull with a force F on a rod of cross-sectional area A, the stress is:
σ=AF
Stress has units of pressure — pascals (Pa) or N/m2. It tells you how “intense” the pulling is, regardless of the rod’s thickness.
Tensile Strain (ε) is the fractional change in length. If the original length is L0 and it stretches by ΔL, the strain is:
ε=L0ΔL
Strain is a pure number — it has no units. A strain of 0.01 means the rod stretched by 1% of its original length.
Putting it together:
Y=ΔL/L0F/A=AΔLFL0
What the Number Tells You
A high Young’s modulus means the material is very stiff — it takes a huge stress to produce even a tiny strain. Steel has Y≈200×109 Pa. A low Young’s modulus means the material is easily stretched. Rubber has Y≈0.01×109 Pa — about 20,000 times smaller than steel.
Young’s modulus is only valid in the elastic region — where the material returns to its original shape after the force is removed. If you stretch too far (past the elastic limit), the material deforms permanently or breaks, and Young’s modulus no longer applies.
A Worked Example
A steel wire of length 2.0 m and cross-sectional area 1.0×10−6 m2 is pulled by a force of 100 N. How much does it stretch? (Young’s modulus of steel = 2.0×1011 Pa)
From Y=AΔLFL0, rearrange:
ΔL=AYFL0=(1.0×10−6)×(2.0×1011)100×2.0=2.0×105200=1.0×10−3 m=1.0 mm …
Concept: Young's modulus -- the ratio of tensile stress to strain in the elastic region. For copper, Y=1.1×1011 Pa (Table 8.1).
Step 1 -- Cross-sectional area
Convert dimensions to metres: 15.2 mm=0.0152 m, 19.1 mm=0.0191 m.
Area A=0.0152×0.0191=2.9032×10−4 m2.
Step 2 -- Tensile stress
σ=AF=2.9032×10−444,500=1.53×108 Pa. …
Using Young's modulus for copper (Y=1.1×1011 Pa, Table 8.1) and the relation σ=Y⋅ε, dividing the tensile stress by Y gives the strain. The printed answer for this question is 0.127.
Young's modulus is the material's stiffness -- it tells you how much strain (fractional change in length) a given stress produces, as long as the deformation stays elastic. For copper, Table 8.1 gives Y=1.1×1011 Pa. The key relation is:
σ=Y⋅εorε=Yσ
where σ is tensile stress (force per unit area) and ε is the strain (dimensionless). So the plan is: compute the cross-sectional area, find the stress, then divide by Y.
- Convert dimensions to metres. The cross-section is 15.2 mm×19.1 mm.
15.2 mm=0.0152 m,19.1 mm=0.0191 m
- Calculate the area.
A=0.0152×0.0191=2.9032×10−4 m2
- Find the tensile stress. Force F=44,500 N.
σ=AF=2.9032×10−444,500≈1.53×108 Pa
- Apply Young's modulus. …
Step 1: A=(0.0152)(0.0191)=2.903e-4 m^2. Step 2: stress=44500/(2.903e-4)=1.53e8 Pa. Step 3: strain=stress/Y_copper(1.1e11)~=1.39e-3 (working formula). The textbook's p …
Showing the 12 most recent of 15 on this concept.
- KEAM 2026Set eng-2026-04174 marksMCQQ.Two copper wires have the lengths in the ratio 1 : 2 and their radii are in the ratio 3 : 1. If they are stretched by the same force, the ratio of the respective longitudinal strains in the two wires is (A) 1 : 9 (B) 9 : 1 (C) 1 : 27 (D) 27 : 1 (E) 1 : 3
›Reveal solutionSolution
Strain ∝1/r2 for equal force and material, so the ratio is 1:9.
Longitudinal strain is:
strain=Ystress=AYF=πr2YF
Both wires are copper (same Y) and stretched by the same force F, so strain ∝1/r2. The length ratio does not affect strain (it is a fractional quantity). With radii in the ratio r1:r2=3:1: …
- KEAM 2026Set eng-2026-04184 marksMCQQ.A steel rod of 1m length and 10−3 m2 area of cross section is subjected to a linear force of 150 kN. The elongation of the rod is (Young's modulus of steel 1.5×1011 Nm−2) (A) 1 cm (B) 0.5 mm (C) 1 m (D) 1 mm (E) 0.8 cm
›Reveal solutionSolution
Using ΔL=AYFL with F=150 kN gives 10−3 m, i.e. 1 mm.
Elongation ΔL=AYFL. With F=150 kN=1.5×105 N, L=1 m, A=10−3 m2, Y=1.5×1011 N/m2: …
- KEAM 2026Set eng-2026-04194 marksMCQQ.Which one of the following materials has the highest modulus of elasticity? (A) steel (B) aluminium (C) copper (D) glass (E) brass
›Reveal solutionSolution
Steel is the stiffest of the listed materials, having the largest Young's modulus.
Young's modulus (modulus of elasticity) measures resistance to elastic deformation. Approximate values:
- Steel: ∼200 GPa
- Copper: ∼110 GPa
- Brass: ∼100 GPa …
- KEAM 2026Set eng-2026-04214 marksMCQQ.The force required to increase the length of a thin copper wire of cross-sectional area 0.1 cm2 by 0.1 % is (Young's modulus of copper is 11×1010Nm−2) (A) 550 N (B) 11×104N (C) 10.5×103N (D) 1100 N (E) 5.5×103N
›Reveal solutionSolution
F=YA⋅(strain)=11×1010×10−5×0.001=1100 N.
From Young's modulus, Y=ΔL/LF/A⇒F=YALΔL. …
- KEAM 2026Set pha-2026-0418F4 marksMCQQ.If a cylinder is stretched by two equal forces applied normal to its cross-section, then the restoring force per unit area is called (A) tensile stress (B) tangential stress (C) shearing stress (D) compressive stress (E) transvers stress
›Reveal solutionSolution
Stretching forces normal to the cross-section create tensile stress.
When a cylinder is pulled by two equal and opposite forces acting normally (perpendicular) to its cross-sectional area, it elongates. The restoring force per unit area developed to oppose this elongation is the tensile stress (a normal, longitudinal stress). Tangential/shearing stress arises from forces parallel …
- KEAM 2026Set pha-2026-0419F4 marksMCQQ.Which one is INCORRECT? (A) Stress is not a vector. (B) Young's modulus is applicable only for solids (C) Compressibility is relevant for solids, liquids and gases (D) Elastomers have larger Young's modulus than metals (E) Tension per unit area is equal to the tensile stress
›Reveal solutionSolution
Elastomers deform hugely under small stress, so their Young's modulus is much smaller than that of metals — statement (D) is false.
Examine each statement:
- (A) Stress is force per unit area with a defined direction of the force but is a tensor/scalar-magnitude quantity, not a true vector — correct.
- (B) Young's modulus (longitudinal/tensile) is meaningful only for solids that can sustain shape — correct.
- (C) Compressibility (bulk response) applies to solids, liquids and gases — correct. …
- KEAM 2025Set eng-2025-04254 marksMCQQ.If the ultimate strength and fracture points are far apart in a stress – strain curve of a material, then the material is said to be (A) ductile (B) brittle (C) perfectly elastic (D) non malleable (E) very hard
›Reveal solutionSolution
A large gap between the ultimate-strength point and the fracture point means substantial plastic elongation before rupture, which is the defining feature of a ductile material.
On a stress–strain curve, the region between the point of ultimate (maximum) strength and the fracture point represents deformation the material undergoes before it finally breaks. …
- KEAM 2025Set pha-2025-0424F4 marksMCQQ.Work done in a stretched wire is (A) Load×strain (B) 21×load×strain (C) Young′s modulus×strain (D) 41×Load×extension (E) 21×load×extension
›Reveal solutionSolution
Because the stretching force increases linearly from 0 to the final load, the work stored is the area of the triangle: W=21(load)(extension).
When a wire is stretched, the restoring/applied force increases linearly with extension (Hooke's law regime). The work done equals the area under the force–extension graph, which is a triangle: …
- KEAM 2025Set pha-2025-0424A4 marksMCQQ.Young's modulus and shear modulus can be defined only in (A) solids and liquids (B) liquids (C) gases (D) gases and liquids (E) solids
›Reveal solutionSolution
Both Young's modulus and shear modulus need a material with a definite shape, so they exist only in solids.
Elastic moduli measure resistance to specific deformations:
- Young's modulus Y=longitudinal straintensile stress — resistance to a change in length.
- Shear modulus η=shear strainshear stress — resistance to a change in shape. …
- KEAM 2025Set pha-2025-0429F4 marksMCQQ.For smaller deformations, stress is directly proportional to the strain for any material. Then the constant of proportionality is called as its (A) modulus of elasticity (B) Poisson’s ratio (C) compressibility (D) coefficient of deformation (E) mechanical strength
›Reveal solutionSolution
Hooke's law for small deformations gives stress ∝ strain, and the proportionality constant is called the modulus of elasticity.
For small deformations, Hooke's law states
stress=E×strain, …
- KEAM 2024Set eng-2024-06074 marksMCQQ.The elastic energy stored per unit volume in a stretched wire is (Y= Young's modulus of the material of the wire; S= stress acting on the wire) (A) 21(YS) (B) 21(Y2S) (C) 21(YS2) (D) 21(Y2S2) (E) 21(SY)
›Reveal solutionSolution
Energy per unit volume =21stress×strain, and strain =S/Y. …
- KEAM 2024Set pha-2024-06104 marksMCQQ.Which of the following has the maximum Young’s modulus value? (A) Aluminium (B) Copper (C) Brass (D) Steel (E) Iron Wrought
›Reveal solutionSolution
Compare typical Young's modulus values.
Approximate Young's moduli (GPa): Aluminium ~70, Copper ~110–120, Brass ~90–100, Iron (wrought) ~190, Steel ~200. Steel has the maximum value. …
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