AQA · A-Level · Physics

    Course version: 7408 · Version from Sept 2016

    Bulk properties of solids: Elastic strain energy, breaking stress.

    When a material is stretched elastically, work is done against the interatomic forces and stored as elastic strain energy; on unloading, this energy is recovered.

    Checked against the AQA 7408 specification (opens in a new tab) on .

    • Point 3 of 8
    • 4 key terms

    Study notes

    From the checked teaching notes for this specification point.

    The idea

    When a material is stretched elastically, work is done against the interatomic forces and stored as elastic strain energy; on unloading, this energy is recovered. For a wire obeying Hooke's law, the stored energy equals the area under the force–extension graph, which for a straight-line region is ½FΔL, or equivalently ½k(ΔL)². Beyond the elastic limit, energy is dissipated as heat and permanent deformation. Breaking stress is the stress at which a material fractures; it depends on the material and on flaws, and is not the same as the ultimate tensile stress, which is the maximum stress the material can withstand before necking. A brittle material such as glass breaks at its elastic limit with little plastic deformation, whereas a ductile material such as copper extends and necks before fracture.

    What earns the marks

    • Elastic strain energy is the energy stored in a stretched or compressed material when it is deformed elastically and is recovered when the deforming force is removed.
    • For a material obeying Hooke's law, the stored energy equals the area under the force–extension graph, which is ½FΔL or ½k(ΔL)².
    • Work done in stretching a wire is stored as elastic strain energy; beyond the elastic limit, some energy is dissipated as thermal energy and permanent deformation remains.
    • Breaking stress is the stress at which a material fractures; it is a property of the material and is affected by surface flaws and internal defects.
    • Breaking stress is distinct from ultimate tensile stress: the ultimate tensile stress is the maximum stress reached before necking, while breaking stress is the stress at fracture.
    • A brittle material fractures with little plastic deformation, so its force–extension graph is approximately linear up to a sudden break.
    • A ductile material shows plastic deformation and necking before fracture, so its force–extension graph curves and extends well beyond the elastic limit.

    Common mistakes and how to put them right

    • Confusing elastic strain energy with the total work done when the material is stretched beyond its elastic limit.

      Put it right: Only the elastic part is recoverable, while plastic deformation dissipates energy.

    • Assuming breaking stress always equals ultimate tensile stress.

      Put it right: The ultimate tensile stress is the maximum stress before necking, whereas breaking stress is the stress at fracture, which can be lower.

    • Using ½FΔL for a non-linear force–extension graph.

      Put it right: The area under the graph must be found, and ½FΔL applies only to the straight-line Hooke's law region.

    Exam tips

    • Sketch the force–extension graph and shade the area representing stored energy before substituting values, so the correct region is used.
    • State clearly whether the material is brittle or ductile and link this to the shape of the force–extension graph and the fracture behaviour.
    • When comparing breaking stress with ultimate tensile stress, refer to the stress–strain graph and identify the fracture point and the maximum point separately.

    Try the lesson

    The start of the Bulk properties of solids: Elastic strain energy, breaking stress. lesson, made from checked teaching notes for this specification point.

    Have a go first

    A spring is stretched by a force of 20 N and its extension is 0.10 m. Calculate the elastic strain energy stored in the spring.

    Listen

    When a material is stretched elastically, work is done against the interatomic forces and stored as elastic strain energy; on unloading, this energy is recovered. For a wire obeying Hooke's law, the stored energy equals the area under the force–extension graph, which for a straight-line region is ½FΔL, or equivalently ½k(ΔL)². Beyond the elastic limit, energy is dissipated as heat and permanent deformation. Breaking stress is the stress at which a material fractures; it depends on the material and on flaws, and is not the same as the ultimate tensile stress, which is the maximum stress the material can withstand before necking. A brittle material such as glass breaks at its elastic limit with little plastic deformation, whereas a ductile material such as copper extends and necks before fracture. A strong answer earns marks for these points. Elastic strain energy is the energy stored in a stretched or compressed material when it is deformed elastically and is recovered when the deforming force is removed. For a material obeying Hooke's law, the stored energy equals the area under the force–extension graph, which is ½FΔL or ½k(ΔL)². Work done in stretching a wire is stored as elastic strain energy; beyond the elastic limit, some energy is dissipated as thermal energy and permanent deformation remains. Breaking stress is the stress at which a material fractures; it is a property of the material and is affected by surface flaws and internal defects. A common slip: Confusing elastic strain energy with the total work done when the material is stretched beyond its elastic limit. Instead, only the elastic part is recoverable, while plastic deformation dissipates energy. Exam tip: Sketch the force–extension graph and shade the area representing stored energy before substituting values, so the correct region is used.

    See it

    A top-down flowchart. The top node, 'Material stretched elastically', leads to 'Work done against interatomic forces', which leads to 'Energy stored as elastic strain energy'. From there, one arrow goes to 'Unloading: energy recovered' and another goes to 'Hooke's law: energy = area under force–extension graph', which leads to 'Straight-line region: ½FΔL or ½k(ΔL)²'. A separate branch from the top node, 'Stretched beyond elastic limit', leads to two nodes: 'Energy dissipated as heat' and 'Permanent deformation remains'.
    It shows how work done in stretching a material is stored as recoverable elastic strain energy, how that energy is calculated for a Hooke's law material, and what happens beyond the elastic limit.

    Key words

    Say what each word means before you turn the card.

    Elastic strain energy

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    Area under force–extension graph

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    Breaking stress

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    Ultimate tensile stress

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    See every definition
    Elastic strain energy
    The energy stored in a stretched or compressed material when it is deformed elastically, which is recovered when the deforming force is removed.
    Area under force–extension graph
    For a material obeying Hooke's law, the stored energy equals this, which for a straight-line region is ½FΔL or ½k(ΔL)².
    Breaking stress
    The stress at which a material fractures, depending on the material and on flaws, and not the same as the ultimate tensile stress.
    Ultimate tensile stress
    The maximum stress the material can withstand before necking, distinct from the stress at which it fractures.

    Label the diagram

    Some boxes have lost their names. Pick the right name for each number.

    The diagram again, with 3 boxes numbered instead of named. A top-down flowchart. The top node, 'Material stretched elastically', leads to 'Work done against interatomic forces', which leads to 'Energy stored as elastic strain energy'. From there, one arrow goes to 'Unloading: energy recovered' and another goes to 'Hooke's law: energy = area under force–extension graph', which leads to 'Straight-line region: ½FΔL or ½k(ΔL)²'. A separate branch from the top node, 'Stretched beyond elastic limit', leads to two nodes: 'Energy dissipated as heat' and 'Permanent deformation remains'.
    • 1Box 1

    • 2Box 2

    • 3Box 3

    0 of 3 labelled

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