Calculate Young's modulus (elastic modulus) from stress and strain, or from force, area, and length change. Solve for stress, strain, or modulus when you know the other two.
Modulus — E = stress / strain
Applied stress in megapascals (1 MPa = 1 N/mm²).
Unitless ratio of change in length to original length (e.g. 0.001 for 0.1%).
From Dimensions — E = (F/A) / (ΔL/L)
Applied axial force in newtons.
Cross-sectional area the force acts over, in square millimetres.
Unloaded, starting length (gauge length), in millimetres.
How much the object stretched under the load, in millimetres.
Solve for modulus, stress, or strain
Known modulus in gigapascals.
Known stress in megapascals.
Known strain as a unitless ratio.
Result
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Enter values above to compute.
4 min read3 steps7 terms3 examples6 FAQsE = σ / ε
Young's modulus is the single number engineers reach for first when comparing how stiff two materials are.
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Walk-through
How to Use This Calculator
3 steps▸
1
Pick a tab for what you know
Use the Modulus tab when you already know stress and strain and want Young's modulus directly. Use the From Dimensions tab when you know the applied force, cross-sectional area, original length, and change in length instead. Use the Solve tab when you know two of {modulus, stress, strain} and need the third.
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Enter your known values
Stress is in megapascals (MPa), force is in newtons (N), area is in square millimetres (mm²), and length values are in millimetres (mm). Strain is always a unitless ratio (e.g. 0.001), not a percentage.
3
Read the modulus and the interpretation
The result card shows Young's modulus in gigapascals (GPa) alongside the stress and strain used to compute it. The interpretation line below explains what a higher or lower modulus means for material stiffness.
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Reference
Formula & Methodology
2 formulas▸
Young's Modulus from Stress and Strain
E = σ / ε
E is Young's modulus (also called the elastic modulus), σ (sigma) is stress in pascals, and ε (epsilon) is strain, a dimensionless ratio. The result is typically reported in gigapascals (GPa) since raw pascal values for most materials are extremely large. Example: σ = 200 MPa, ε = 0.001 → E = 200,000,000 Pa ÷ 0.001... expressed directly as 200 MPa / 0.001 = 200,000 MPa = 200 GPa.
Young's Modulus from Force and Dimensions
E = (F/A) / (ΔL/L)
This is the same formula expanded into its measurable components: F is the applied axial force, A is the cross-sectional area the force acts over, L is the original (unloaded) length, and ΔL is the change in length under load. F/A is stress and ΔL/L is strain, so this reduces to exactly E = σ/ε — the two tabs of this calculator always agree because they compute the same relationship from different starting inputs.
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Glossary
Key Terms Explained
7 terms▸
Young's Modulus ↗A measure of a material's stiffness in the elastic (non-permanent-deformation) region, defined as the ratio of stress to strain: E = σ/ε. Also called the elastic modulus or tensile modulus. Higher values mean the material deforms less under a given stress — steel (≈200 GPa) is far stiffer than rubber (≈0.01–0.1 GPa).
Stress ↗The internal force per unit area within a material, calculated as σ = F/A (force divided by cross-sectional area). Measured in pascals (Pa), commonly reported in megapascals (MPa) since raw Pa values are unwieldy for real materials.
Strain ↗The dimensionless ratio of how much a material's length changes relative to its original length: ε = ΔL/L. Because it's a length divided by a length, it has no units and is often expressed as a plain decimal (e.g. 0.001) or a percentage (0.1%).
Elastic Modulus ↗A general term for any ratio of stress to strain in the elastic region of a material — Young's modulus (tension/compression), shear modulus (shear stress), and bulk modulus (uniform pressure) are all elastic moduli measuring stiffness under different loading conditions.
Hooke's Law ↗The principle that, within the elastic region, stress is directly proportional to strain (F = kx for a spring, or σ = Eε for a material under axial load). Young's modulus is the proportionality constant for this relationship in tension or compression.
Elastic Region ↗The range of stress over which a material deforms proportionally and returns fully to its original shape once the load is removed. Young's modulus is only valid within this region — beyond the yield point, deformation becomes permanent and the stress-strain relationship is no longer linear.
GPa (Gigapascal) ↗A unit of pressure or stress equal to one billion pascals (1 GPa = 1,000 MPa = 1,000,000,000 Pa). Young's modulus values for structural materials are almost always reported in GPa because the raw pascal values are impractically large — e.g. steel is about 200,000,000,000 Pa, or simply 200 GPa.
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Scenarios
Real-World Examples
3 worked examples▸
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Structural Steel
Modulus from stress and strain
Stress (σ) 200 MPaStrain (ε) 0.001
E = σ/ε = 200 MPa / 0.001 = 200,000 MPa = 200 GPa. This matches the textbook modulus for structural steel, confirming a 200 MPa stress produces only a 0.1% strain in the elastic region — steel is very stiff.
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Tensile Test Specimen
Modulus from force and dimensions
Force (F) 10,000 NArea (A) 50 mm²Original length (L) 100 mmChange in length (ΔL) 0.1 mm
stress = F/A = 10,000 N / 50 mm² = 200 MPa. strain = ΔL/L = 0.1/100 = 0.001. E = 200 MPa / 0.001 = 200 GPa — the same result as the stress-and-strain example, because both paths compute the identical E = σ/ε relationship.
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Predicting the Stretch
Solving for a missing variable
Young's modulus (E) 200 GPaStress (σ) 150 MPa
On the Solve tab, solving for strain gives ε = σ/E = 150 MPa / 200,000 MPa = 0.00075. If you also know the original length — say L = 2,000 mm — you can then find the change in length by hand: ΔL = ε × L = 0.00075 × 2,000 = 1.5 mm. Solving in two steps like this lets you work backward from a known modulus and stress to a predicted stretch.
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Reference
Cite This Calculator
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Deep Dive
Understanding Young's Modulus — the Elastic Modulus
Young's modulus is the single number engineers reach for first when comparing how stiff two materials are. It tells you how much a material resists stretching or compressing under load, and it's the foundation for predicting deflection in beams, stretch in cables, and strain in structural members before anything is built.
Why Stress Divided by Strain Measures Stiffness
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Stress (force per unit area) describes how hard you're pulling or pushing on a material. Strain (change in length over original length) describes how much it actually deforms in response. Dividing the two cancels out the specific size of your test specimen and the specific force you applied, leaving a property of the material itself: Young's modulus. A material with a high E, like steel (≈200 GPa), barely stretches under a given stress. A material with a low E, like rubber (≈0.01–0.1 GPa), stretches dramatically under the same stress. This is why E is reported as a fixed material property in engineering handbooks rather than something you have to re-measure for every part.
Two Equivalent Ways to Compute It
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This calculator offers two input paths that compute the exact same quantity. The Modulus tab takes stress and strain directly — useful when you already have those numbers from a materials datasheet or a prior calculation (for example, from the Stress and Strain calculators). The From Dimensions tab takes the raw measurements from a tensile test — force, cross-sectional area, original length, and change in length — and derives stress and strain internally before computing E. Because F/A is stress and ΔL/L is strain, the two tabs are algebraically identical; they'll always agree for consistent inputs.
Limits: Elastic Region Only
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Young's modulus is only meaningful within a material's elastic region — the range of stress over which it deforms proportionally and springs back completely when the load is removed. Push a material past its yield point and the stress-strain relationship stops being linear; the material undergoes permanent (plastic) deformation, and a single E value no longer describes its behavior. This calculator assumes every input falls within the elastic region. It also assumes uniaxial loading (a simple pull or push along one axis) — more complex loading (shear, torsion, combined stresses) requires a different elastic modulus, such as the shear modulus or bulk modulus.
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Questions
Frequently Asked Questions
6 questions▸
What is the formula for Young's modulus?+
E = σ/ε, where σ is stress (force per unit area) and ε is strain (change in length divided by original length). Equivalently, E = (F/A) / (ΔL/L) using the raw force, area, and length measurements — both formulas give the same result.
What is Young's modulus for steel?+
Structural steel has a Young's modulus of approximately 200 GPa (200,000 MPa). Aluminum is around 69 GPa, copper around 110–130 GPa, and concrete around 17–30 GPa, all far below steel's stiffness.
What units does Young's modulus use?+
Young's modulus has units of pressure — pascals (Pa) in SI — but because raw Pa values for real materials are extremely large (steel is about 2×10¹¹ Pa), it's almost always reported in gigapascals (GPa). This calculator displays results in GPa and accepts stress inputs in MPa for practical, readable numbers.
What does a stiffer material mean?+
A higher Young's modulus means the material resists elastic deformation more strongly — it takes more stress to produce the same amount of strain. A stiffer material stretches or bends less under the same load, which is why steel beams deflect far less than wooden ones of the same size under equal loads.
Does Young's modulus apply outside the elastic region?+
No. Young's modulus only describes the linear, fully-reversible relationship between stress and strain in a material's elastic region. Once a material is stressed past its yield point, it deforms permanently and the stress-strain relationship is no longer linear, so a single E value can't describe that behavior.
What's the difference between Young's modulus and shear modulus?+
Young's modulus measures stiffness under tensile or compressive (axial) loading — a straight pull or push. Shear modulus measures stiffness under shear loading — forces that slide adjacent layers of material past each other. Both are elastic moduli, but they describe resistance to different kinds of deformation.
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