JEE · Physics

Elasticity

Explain how a solid resists deformation using stress, strain and the elastic moduli, choose the correct modulus and formula condition for a given loading, and diagnose common stress-strain mistakes.

Subject
Physics
Syllabus unit
Properties of Solids and Liquids
Updated
8 September 2026
  • Mapped to JEE Main 2026 and JEE Advanced 2026
  • Formulas carry their conditions
  • No invented weightage, question counts or trend percentages

Content status: draft. Verified academic content for this page has not been loaded yet, so the page is excluded from search indexing and the sitemap.

In short

Elasticity describes how a solid deforms under load and returns to its original shape when the load is removed, provided the deformation stays within the elastic limit. Stress is the internal restoring force per unit area, strain is the fractional deformation, and the elastic modulus is the ratio of stress to strain for a given type of deformation.

A correct solution first identifies the type of deformation (length, volume or shape), then picks the matching modulus (Young's, bulk or shear) and checks that the load stays within the region where Hooke's law holds.

Syllabus mapping

  • Unit
    Properties of Solids and Liquids
    Topics
    Elastic behaviour of solids, Stress and strain, Hooke's law and the elastic limit, Young's modulus, Bulk modulus, Modulus of rigidity (shear modulus), Stress-strain curve, Poisson's ratio, Compressibility, Elastic potential energy in a stretched wire, Thermal stress

What this chapter contains and why it matters

  • Question
    What is the chapter about?
    Direct answer
    How a solid responds to deforming forces through stress, strain, Hooke's law and the elastic moduli, and how the stress-strain curve describes elastic and plastic behaviour.
  • Question
    What is the central method choice?
    Direct answer
    Identify the type of deformation (length, volume or shape), select the matching modulus (Young's, bulk or shear), and confirm the load stays within the elastic limit before using a linear stress-strain relation.
  • Question
    Where do most mistakes begin?
    Direct answer
    Applying Hooke's law beyond the elastic limit, confusing stress with applied force, mixing up which modulus applies to which deformation, and dropping units when combining stress and strain.
  • Question
    What should come before Elasticity?
    Direct answer
    SI units and dimensions, and force and equilibrium reasoning from Laws of Motion.
  • Question
    What comes after it?
    Direct answer
    Fluid Mechanics uses bulk modulus and pressure ideas in a fluid context, and Surface Tension develops a related but separate surface-force topic.

The official JEE documents define content scope. They do not publish chapter weightage, so none is asserted here.

Official JEE syllabus mapping for Elasticity

Verified against the current JEE Main 2026 syllabus (Unit 7, Properties of Solids and Liquids) and JEE Advanced 2026 syllabus on 8 September 2026. This is a wording and scope mapping, not a claim about question difficulty or frequency.

  • Concept group
    Elastic behaviour and stress-strain relationship
    JEE Main 2026
    Elastic behaviour and stress-strain relationship are explicitly listed in Unit 7.
    JEE Advanced 2026
    Not stated as a separate line, but assumed for Hooke's law and Young's modulus.
    Preparation note
    Learn the stress-strain curve as the basis for every modulus.
  • Concept group
    Hooke's law and Young's modulus
    JEE Main 2026
    Hooke's law and Young's modulus are explicitly listed.
    JEE Advanced 2026
    Hooke's law and Young's modulus are explicitly listed in the Mechanics section.
    Preparation note
    Confirm the elastic-limit condition before every use of Hooke's law.
  • Concept group
    Bulk modulus and modulus of rigidity
    JEE Main 2026
    Bulk modulus and modulus of rigidity are explicitly listed.
    JEE Advanced 2026
    Modulus of rigidity and bulk modulus are explicitly listed, described within the fluids paragraph as 'in mechanics'.
    Preparation note
    Match bulk modulus to uniform-pressure loading and shear modulus to tangential loading.
  • Concept group
    Poisson's ratio, compressibility, elastic potential energy, thermal stress
    JEE Main 2026
    Not named as separate line items in the current official document.
    JEE Advanced 2026
    Not named as separate line items in the current official document.
    Preparation note
    Treated here as standard supporting NCERT-level concepts, not as independently notified syllabus topics. Verify directly against the official PDFs before assuming exam-specific emphasis.

Sources: JEE Main 2026 syllabus and JEE (Advanced) 2026 syllabus, both linked in the sources section below.

Before this chapter

Prerequisites: what you should know before Elasticity

  • Prerequisite
    SI units and dimensions
    You are ready if you can…
    Recognise that stress carries pressure units and strain is dimensionless.
    If not, repair this first
    Revise base units, dimensional formulas and unit conversion.
  • Prerequisite
    Force and equilibrium
    You are ready if you can…
    Draw a free-body diagram and identify internal restoring forces.
    If not, repair this first
    Revise Newton's third law and equilibrium of a deformable body.
  • Prerequisite
    Graph reading
    You are ready if you can…
    Read slope as a ratio on a stress-strain curve.
    If not, repair this first
    Revise slope as rate of change on a graph.
  • Prerequisite
    Basic algebra
    You are ready if you can…
    Rearrange ratio-based formulas for an unknown quantity.
    If not, repair this first
    Practise solving for stress, strain or modulus given the other two.

This is a readiness check, not a weightage or scoring-priority list.

Concepts in this chapter

1. Treat stress as an internal restoring force per unit area

Stress is force divided by the area over which it acts internally, not the external applied force by itself.

When an external force deforms a solid, internal forces resist the deformation. Stress is this internal restoring force divided by the cross-sectional area over which it acts. Its SI unit is the same as pressure, newton per square metre.

2. Strain is a dimensionless ratio

Strain compares the change caused by deformation to the original undeformed value.

Longitudinal strain is change in length divided by original length. Volume strain is change in volume divided by original volume. Shear strain is the angle of deformation, measured in radians. All three are ratios of like quantities, so strain has no unit.

3. Apply Hooke's law only within the elastic limit

Stress is proportional to strain only up to the proportional limit on the stress-strain curve.

Hooke's law states that stress is proportional to strain for small deformations. Beyond the proportional limit the material can still be elastic for a short range, but the linear relationship no longer holds, and beyond the elastic limit the deformation becomes permanent.

4. Match the deformation type to its modulus

Young's modulus is for length change under longitudinal stress, bulk modulus is for volume change under uniform pressure, shear modulus is for shape change under tangential stress.

Young's modulus applies to a rod or wire stretched or compressed along its length. Bulk modulus applies to a body under uniform pressure from all sides, such as a fluid or a submerged solid. Shear modulus (modulus of rigidity) applies when tangential stress changes shape without changing volume.

5. Read the stress-strain curve as a sequence of regions

Proportional region, elastic limit, yield point, plastic region, and fracture point occur in order.

A tensile test produces a stress-strain curve with a straight proportional region, followed by a region where the material remains elastic but the relation is no longer linear, a yield point where plastic deformation begins, a plastic region, and finally fracture. Only the region up to the elastic limit is described by Hooke's law.

6. Poisson's ratio links lateral and longitudinal strain

Poisson's ratio is the negative ratio of lateral strain to longitudinal strain, within elastic limits.

When a wire is stretched, it also contracts sideways. Poisson's ratio compares this lateral contraction strain to the longitudinal extension strain. It is a material property used alongside the elastic moduli in NCERT-level treatment of elasticity, and it is not named as a separate line item in the current official JEE Main or JEE Advanced syllabus documents.

7. Compressibility is the reciprocal of bulk modulus

Compressibility measures how readily a substance's volume changes under pressure and is defined as the reciprocal of the bulk modulus. It is a standard supporting idea for bulk modulus problems rather than a separately notified syllabus topic.

8. Elastic potential energy is stored work done during deformation

Energy stored in a stretched wire equals the work done against the internal restoring force.

As a wire is stretched gradually within the elastic limit, work is done against the internal restoring force, and this work is stored as elastic potential energy. It can be recovered as the wire returns to its natural length, provided the elastic limit was not exceeded.

9. Thermal stress arises when constrained expansion is prevented

If a rod that would otherwise expand or contract with a temperature change is rigidly constrained at both ends, an internal thermal stress develops instead of a length change. This connects thermal expansion to Young's modulus and is treated as an application of the same stress-strain framework.

Method selector: choose the modulus before calculating

Match the type of deformation to the correct modulus before any algebra.

  • Information given
    Wire or rod stretched or compressed along its length
    First method
    Young's modulus
    Validation
    Confirm the load stays within the elastic limit
  • Information given
    Body under uniform pressure from all sides
    First method
    Bulk modulus
    Validation
    Check that only volume, not shape, changes
  • Information given
    Tangential force changing the shape of a block
    First method
    Shear modulus (modulus of rigidity)
    Validation
    Confirm volume stays constant
  • Information given
    Given bulk modulus, asked for volume response to pressure
    First method
    Compressibility as the reciprocal of bulk modulus
    Validation
    Keep pressure and volume change in consistent units
  • Information given
    Wire stretched, asked for stored energy
    First method
    Elastic potential energy from work done against restoring force
    Validation
    Confirm deformation stayed within the elastic limit
  • Information given
    Rod rigidly constrained and heated or cooled
    First method
    Thermal stress from prevented thermal expansion
    Validation
    Use the unconstrained expansion that would have occurred as the reference strain

Formula sheet

  • Stress equals force divided by area.

    Internal restoring force per unit cross-sectional area.

    F
    internal restoring force (N)
    A
    cross-sectional area (m^2)

    Use whenA deforming force acts on a defined cross-sectional area within the elastic limit.

    Common trapUsing the externally applied force without confirming it equals the internal restoring force in equilibrium.

  • Longitudinal strain equals change in length divided by original length.

    Fractional change in length of a stretched or compressed rod or wire.

    ΔL
    change in length (m)
    L
    original length (m)

    Use whenThe deformation is along one dimension, such as a stretched wire.

    Common trapUsing the final length instead of the original length in the denominator.

  • Volume strain equals change in volume divided by original volume.

    Fractional change in volume under uniform pressure.

    ΔV
    change in volume (m^3)
    V
    original volume (m^3)

    Use whenA body is under uniform pressure from all sides.

    Common trapApplying volume strain to a deformation that only changes shape, not volume.

  • Shear strain equals the tangent of the shear angle, approximately the angle itself for small angles.

    Angular deformation produced by a tangential force, for small angles.

    theta
    angle of shear deformation (rad)

    Use whenA tangential stress changes the shape of a block without changing its volume, and the angle is small.

    Common trapTreating shear strain as a length ratio instead of an angle.

  • Stress equals a constant times strain, within the proportional limit.

    Stress is directly proportional to strain within the proportional limit.

    k
    constant of proportionality (a modulus) (same as stress)

    Use whenThe deformation is within the proportional (linear) part of the elastic region.

    Common trapExtending the linear relation beyond the elastic limit shown on the stress-strain curve.

  • Young's modulus equals longitudinal stress divided by longitudinal strain.

    Ratio of longitudinal stress to longitudinal strain for a stretched or compressed rod or wire.

    Y
    Young's modulus (N/m^2)

    Use whenThe deformation is along the length of a rod or wire, within the elastic limit.

    Common trapUsing Young's modulus for a volume or shape change instead of Young's, bulk or shear as appropriate.

  • Bulk modulus equals negative pressure change divided by fractional volume change.

    Ratio of pressure change to fractional volume change, for uniform compression or expansion.

    B
    bulk modulus (N/m^2)
    ΔP
    change in pressure (N/m^2)

    Use whenA body is under uniform pressure from all sides and only its volume changes.

    Common trapDropping the negative sign convention that reflects volume decreasing as pressure increases.

  • Shear modulus equals shear stress divided by shear strain.

    Ratio of tangential (shear) stress to shear strain.

    G
    shear modulus (modulus of rigidity) (N/m^2)

    Use whenA tangential force deforms the shape of a body without changing its volume, within the elastic limit.

    Common trapConfusing shear modulus with Young's modulus when the loading is tangential, not longitudinal.

  • Compressibility equals one divided by bulk modulus.

    Compressibility is the reciprocal of bulk modulus.

    k
    compressibility (m^2/N)

    Use whenBulk modulus is known and the ease of volume change under pressure is asked for.

    Common trapReporting compressibility with the same numerical value as bulk modulus instead of inverting it.

  • Poisson's ratio equals negative lateral strain divided by longitudinal strain.

    Ratio comparing sideways contraction strain to lengthwise extension strain.

    sigma_p
    Poisson's ratio (dimensionless)

    Use whenBoth lateral and longitudinal strains are given or asked for, within the elastic limit.

    Common trapDropping the sign convention that keeps Poisson's ratio positive for materials that contract sideways while stretched.

  • Elastic potential energy equals one half times force times extension, for gradual loading.

    Elastic potential energy stored in a wire stretched gradually within the elastic limit.

    U
    elastic potential energy (J)

    Use whenA wire or rod is stretched gradually (not suddenly) and stays within the elastic limit.

    Common trapUsing the final force F over the full extension instead of the average force during gradual loading.

  • Elastic energy per unit volume equals one half times stress times strain.

    Elastic potential energy stored per unit volume of a stretched wire.

    u
    elastic energy per unit volume (J/m^3)

    Use whenVolume of the stretched material is known and energy density is required instead of total energy.

    Common trapMixing stress and strain from different loading stages instead of the final elastic-limit values.

  • Thermal stress equals Young's modulus times the coefficient of linear expansion times the temperature change.

    Internal stress developed in a rigidly constrained rod when its free thermal expansion is prevented.

    alpha
    coefficient of linear thermal expansion (1/K)
    ΔT
    change in temperature (K)

    Use whenBoth ends of a rod are rigidly fixed so the rod cannot expand or contract with a temperature change.

    Common trapApplying this formula when the rod is free to expand, where no thermal stress develops.

Worked examples

A steel wire of length 2 m and cross-sectional area 1 mm^2 is stretched by 1 mm under a load. Given Young's modulus for steel, find the tensile force applied.

Answer: F = Y × A × (ΔL/L), evaluated with the given numerical values.

Compute longitudinal strain: ΔL / L = 0.001 m / 2 m.

Use Y = (F/A) / (ΔL/L) rearranged to F = Y × A × (ΔL/L), substituting the known Young's modulus, area and strain.

Confirm the resulting stress is below the elastic limit of steel before accepting the answer.

A solid sphere of volume V is subjected to a uniform pressure increase ΔP, causing a fractional volume decrease. Express the bulk modulus and the compressibility.

Answer: B = -ΔP / (ΔV/V); compressibility k = 1/B.

Identify the loading as uniform pressure from all sides, so bulk modulus is the correct choice, not Young's or shear modulus.

Apply B = -ΔP / (ΔV/V) using the given pressure increase and fractional volume decrease.

Take the reciprocal of B to state the compressibility.

A metal rod is rigidly fixed at both ends and its temperature is raised by ΔT. Find the thermal stress developed, given Young's modulus Y and coefficient of linear expansion alpha.

Answer: Thermal stress = Y × alpha × ΔT.

Recognise that the rod would expand by alpha × L × ΔT if free, so the constraint imposes an equivalent compressive strain of alpha × ΔT.

Apply stress = Y × strain with this thermally imposed strain to get stress = Y × alpha × ΔT.

Common mistakes and what they actually indicate

  • Applying Hooke's law (stress proportional to strain) beyond the elastic limit shown on the stress-strain curve.

    Knowledge gap

    Why it happens

    The linear relation only holds up to the proportional limit; beyond the elastic limit deformation becomes permanent and non-linear.

    How it is corrected

    Check where the given deformation lies on the stress-strain curve before using a linear stress-strain formula.

  • Using Young's modulus for a problem that describes uniform pressure (volume change) or tangential force (shape change).

    Decision / selection error

    Why it happens

    Each modulus is defined for a specific type of deformation; they are not interchangeable.

    How it is corrected

    Identify whether length, volume or shape is changing before selecting Young's, bulk or shear modulus.

  • Treating stress as the applied external force rather than the internal restoring force per unit area.

    Recall gap

    Why it happens

    In equilibrium the two are numerically equal, but the physical meaning of stress is internal and distributed over area, not a single external force.

    How it is corrected

    Always divide by the correct cross-sectional area and confirm equilibrium before equating applied force to internal stress.

  • Dropping the negative sign in the bulk modulus formula and reporting a negative modulus.

    Execution error

    Why it happens

    Volume decreases as pressure increases, so the negative sign keeps bulk modulus a positive quantity.

    How it is corrected

    Track the sign of ΔV relative to ΔP explicitly before finalising the numerical answer.

  • Using the gradual-loading energy formula (1/2) F ΔL when a load is applied suddenly.

    Decision / selection error

    Why it happens

    Sudden loading involves a different work-energy relationship because the force is not built up gradually.

    How it is corrected

    Check whether the problem states gradual or sudden loading before applying the (1/2) F ΔL energy formula.

  • Computing shear strain as a length ratio instead of an angle.

    Knowledge gap

    Why it happens

    Shear strain is defined through the angular deformation of the body, not a change-in-length ratio.

    How it is corrected

    Identify the shear angle from the geometry of the deformed shape before computing shear modulus.

  • Calculating thermal stress for a rod that is free to expand, where no stress develops.

    Decision / selection error

    Why it happens

    Thermal stress requires a constraint that prevents the natural length change; a free rod simply changes length instead.

    How it is corrected

    Confirm the rod is rigidly constrained at both ends before applying the thermal stress formula.

  • Mixing units for force, area and length when computing a modulus, producing an inconsistent numerical answer.

    Execution error

    Why it happens

    Moduli combine force, area and a dimensionless strain; any unit inconsistency propagates directly into the result.

    How it is corrected

    Convert all quantities to consistent SI units before substituting into a modulus formula.

  • Assuming Poisson's ratio, compressibility, or thermal stress are heavily tested because they appear in coaching notes.

    Needs review

    Why it happens

    These are standard supporting concepts in NCERT-level treatment, but they are not named as separate line items in the current official JEE Main or JEE Advanced syllabus documents.

    How it is corrected

    Check the official syllabus mapping table on this page and the linked source documents before assuming exam-specific emphasis.

FAQ

Elasticity — questions

Straight answers about how Rank Sarthi fits into serious exam preparation.

No. This chapter covers how solids deform under stress and strain. Fluid Mechanics and Surface Tension are separate chapters that own pressure-in-fluids and surface-force intents respectively.

Sources and provenance

Evidence boundary: the syllabus mapping is tied to the official 2026 JEE Main and JEE Advanced documents. Poisson's ratio, compressibility, elastic potential energy and thermal stress are standard NCERT-level supporting concepts, not independently notified syllabus line items, and this page states that boundary explicitly. No chapter weightage, question frequency or forecast is asserted.

Last updated
8 September 2026

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