Revision Notes
OCR A Level Physics A: Springs, stress, strain and the Young modulus (H556) – Revision Notes
Revision notes on springs, Hooke's law, elastic energy, stress, strain, the Young modulus and stress-strain graphs for OCR A Level Physics A (H556).
- Subject
- Physics
- Level
- A LEVELS
- Topic
- Springs, stress, strain and the Young modulus
- Author
- Marlbridge Academic Team
- Updated
Aligned to OCR A Level Physics (H556), Version 3.0 (March 2026), for first assessment in 2017. Official specification .
Syllabus page (what it covers and how it is assessed): OCR A Level Physics.
Syllabus points this page covers
H556
- 3.4 Materials
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These notes condense sections 3.4.1 (Springs) and 3.4.2 (Mechanical properties of matter) of the OCR Advanced GCE in Physics A specification (H556), Version 3.0 (March 2026), for first assessment in 2017. Longer explanations and fuller worked examples are in the study guide.
Related pages: the practice questions, the OCR A Level Physics hub, the printable checklist and the free diagnostics.
Definitions to recall
- Tensile deformation: pulling forces make an object longer; the change is the extension.
- Compressive deformation: pushing forces make an object shorter; the change is the compression.
- Hooke’s law: below the limit of proportionality, a spring’s extension doubles when the force doubles.
- Force constant k: force per unit extension for a given spring or wire, in N m⁻¹.
- Limit of proportionality: the point beyond which force-extension is no longer a straight line through the origin.
- Elastic deformation: the object returns to its original size and shape when the force is removed.
- Plastic deformation: a permanent change in size or shape remains after the force is removed.
- Tensile stress: force per unit cross-sectional area.
- Tensile strain: extension divided by original length.
- Ultimate tensile strength (UTS): the maximum tensile stress a material can withstand before breaking.
- Young modulus: tensile stress divided by tensile strain, within the limit of proportionality.
Equations and units
| Quantity | Equation | Unit |
|---|---|---|
| Hooke’s law | F = kx | N |
| Force constant | k = F/x | N m⁻¹ |
| Work done / stored energy (linear) | E = ½Fx = ½kx² | J |
| Stress | σ = F/A | Pa (N m⁻²) |
| Strain | ε = x/L | none |
| Young modulus | E = σ/ε = FL/(Ax) | Pa |
| Link between k and E | k = EA/L | N m⁻¹ |
| Wire cross-section | A = πd²/4 | m² |
The symbol E is used for both elastic energy and the Young modulus. Use the context and units to tell them apart.
Graphs: what to read off
| Graph | Gradient | Area under graph |
|---|---|---|
| Force (y) against extension (x) | k | Work done / energy stored |
| Extension (y) against force (x) | 1/k | Not used |
| Stress (y) against strain (x), straight part | Young modulus | Not used |
| Extension (y) against force (x), wire | L/(EA) | Not used |
Force-extension features: straight through the origin means Hooke’s law holds; where it curves is the limit of proportionality; a steeper line (force on y) is a stiffer sample.
Method: work done from a graph
- Identify the force axis and the extension axis, and check the units (mm to m, kN to N).
- If the line is straight through the origin, use ½Fx.
- Otherwise split into triangles, rectangles and trapeziums, or count squares.
- Convert the area into joules: area = (force per square) × (extension per square) × number of squares.
Reminder. A force rises linearly from 0 to 12 N over the first 0.030 m, then stays at 12 N to 0.070 m. Work = ½ × 12 × 0.030 + 12 × 0.040 = 0.18 + 0.48 = 0.66 J.
Method: Young modulus of a metal wire
- Choose a long, thin wire, clamped firmly at the top, kept taut by a small weight.
- Measure the original length L with a metre rule or tape.
- Use a micrometer at several positions and in two perpendicular directions, then average the diameters and calculate A = πd²/4.
- Add equal masses in steps and record the extension at each, against a fixed scale. Unload too, to check the wire is elastic.
- Plot extension (y) against force (x). The gradient is L/(EA).
- E = L / (A × gradient).
Key points: the diameter is the largest source of uncertainty because A ∝ d², so a 2% uncertainty in d gives 4% in A. Wear eye protection and use sand or foam to catch falling masses. Keep extensions inside the elastic region.
Reminder. L = 1.50 m, d = 0.40 mm, gradient 7.0 × 10⁻⁵ m N⁻¹. A = π × (0.20 × 10⁻³)² = 1.26 × 10⁻⁷ m². E = 1.50 / (1.26 × 10⁻⁷ × 7.0 × 10⁻⁵) = 1.7 × 10¹¹ Pa.
Method: plastic deformation on a force-extension graph
- Find the area under the loading line for the total work done.
- Draw the unloading line from the maximum point, parallel to the original straight section.
- Where it meets zero force is the permanent extension.
- The area under the unloading line is the energy recovered. Total work minus energy recovered is dissipated as thermal energy.
Reminder. A strip has initial slope 400 N m⁻¹. It is loaded to 24 N at 0.090 m. The unloading line reaches zero force at 0.090 - 24/400 = 0.030 m, so the permanent extension is 0.030 m. Energy recovered = ½ × 24 × 0.060 = 0.72 J.
Stress-strain graph shapes
| Material | Graph features | Behaviour at the end |
|---|---|---|
| Ductile (for example copper) | Straight line, then curve; possible yield point; peak at UTS; wire necks | Large plastic deformation, then breaks |
| Brittle (for example glass) | Straight line almost to the end | Fractures suddenly, little plastic deformation |
| Polymeric: rubber | Curve, not straight; loading and unloading curves differ | Returns to original length; the loop is energy dissipated as thermal energy |
| Polymeric: polythene | Initial rise, then yields and extends a long way | Permanent extension |
For a metal loaded past its elastic limit, the unloading line is approximately parallel to the original straight section and the graph ends at a non-zero extension: the permanent extension.
Must-know distinctions
- Stiffness k and Young modulus E. k depends on the sample’s size; E depends only on the material. k = EA/L.
- Elastic and plastic. Elastic: returns when unloaded. Plastic: does not.
- Limit of proportionality and elastic limit. One is about the graph being straight, the other about returning to the original size.
- Stress and strain. Stress has unit Pa; strain has no unit.
- UTS and breaking force. UTS is a stress. Breaking force is a force and depends on the area.
- Tensile and compressive. Both can be handled with F = kx, using the size of the change in length.
Quick self-test
- State Hooke’s law.
- A force of 18 N stretches a spring by 0.24 m. Find k.
- The same spring is extended by 0.12 m. How much energy is stored?
- A spring with k = 300 N m⁻¹ is compressed by 5.0 cm. What force acts on it?
- A force of 300 N acts on a wire of cross-sectional area 1.5 mm². Find the stress.
- A wire of length 1.25 m extends by 1.5 mm. Find the strain.
- A material has stress 75 MPa at strain 1.25 × 10⁻³ in the elastic region. Find the Young modulus.
- A rod of cross-section 4.0 mm² breaks under 1.6 kN. Find the UTS.
- A spring with k = 250 N m⁻¹ stores 0.20 J. What is its extension?
- A wire has E = 1.2 × 10¹¹ Pa, A = 0.80 mm² and L = 3.0 m. Find k.
- Why is the wire’s diameter measured at several places?
- How does a rubber band’s graph differ from a spring’s, and what does the enclosed loop between its loading and unloading curves represent?
Answers
- Within the limit of proportionality, extension is proportional to force.
- k = 18 / 0.24 = 75 N m⁻¹.
- E = ½ × 75 × 0.12² = 0.54 J.
- F = 300 × 0.050 = 15 N.
- 1.5 mm² = 1.5 × 10⁻⁶ m². Stress = 300 / 1.5 × 10⁻⁶ = 2.0 × 10⁸ Pa.
- Strain = 1.5 × 10⁻³ / 1.25 = 1.2 × 10⁻³.
- E = 75 × 10⁶ / 1.25 × 10⁻³ = 6.0 × 10¹⁰ Pa.
- UTS = 1600 / 4.0 × 10⁻⁶ = 4.0 × 10⁸ Pa.
- x = √(2E/k) = √(2 × 0.20 / 250) = 0.040 m.
- k = EA/L = 1.2 × 10¹¹ × 0.80 × 10⁻⁶ / 3.0 = 3.2 × 10⁴ N m⁻¹.
- The wire may not be uniform or perfectly circular. A is proportional to d², so any error in d is doubled in A. Averaging reduces this.
- The rubber band’s graph is a curve, not a straight line, and the unloading curve lies below the loading curve. The loop between them represents energy dissipated as thermal energy.
Where marks are usually lost
- Using the total length of a spring or wire as the extension.
- Leaving mm, mm² or kN in the equation and not converting to m, m² or N.
- Squaring the diameter without halving it first for the radius, or using the diameter as the radius.
- Quoting E = σ/ε without saying it only applies within the limit of proportionality.
- Describing plastic and elastic deformation without referring to what happens when the force is removed.
- Using ½Fx when the graph is not a straight line through the origin.
- Saying “the graph is a straight line” for a rubber band, or forgetting that its loading and unloading curves differ.
- Calling the gradient of an extension-force graph k, when it is 1/k.
- In practical answers, giving a single diameter reading, or measuring the extension of a wire over a short length, which makes the percentage uncertainty large.
Official syllabus
OCR Advanced GCE in Physics A (H556) specification, Version 3.0 (March 2026), for first assessment in 2017, published by OCR. Sections 3.4.1 Springs and 3.4.2 Mechanical properties of matter.
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