- Pulling force
- 1000N
- Cross-sectional area
- 0.0001m²
- Original length
- 2m
- Change in length
- 0.001m
20,000,000,000Pa
Open with these values20,000,000,000Pa
Result: 20,000,000,000 PaYoung's modulus is stress divided by strain: the force per square metre divided by the fraction of its length the sample gained. Strain goes in as a ratio, not a percentage — 1 mm on a 2 m bar is 0.0005, not 0.05. The answer is in pascals; steel sits near 200 GPa, that is 2e11 Pa.
20,000,000,000Pa
Open with these values15,000,000,000Pa
Open with these values36,250,000Pa
Open with these valuesE = stress ÷ strain = (F × L₀) ÷ (A × ΔL)
| Force, area, length, stretch | Stress on the sample | Modulus (Pa) |
|---|---|---|
| 0.145, 0.00002, 0.5, 0.0001 | 7250 Pa | 36250000 |
| 10000, 0.001, 5, 0.01 | 10 MPa | 5000000000 |
| 1500, 0.0003, 2.5, 0.0015 | 5 MPa | 8333333333.33 |
| 500, 0.00005, 3, 0.002 | 10 MPa | 15000000000 |
| 1000, 0.0001, 2, 0.001 | 10 MPa | 20000000000 |
| 2000, 0.0002, 1, 0.0005 | 10 MPa | 20000000000 |
Divide the tensile stress by the tensile strain: E = (F × L₀) ÷ (A × ΔL). Use newtons for force, square metres for area and metres for both lengths to get pascals. A 1000 N pull on a 0.0001 m² bar that stretches 0.001 m from an original 2 m gives 20 GPa.
Young's modulus, or the modulus of elasticity, measures how stiff a material is — how strongly it resists being stretched or compressed. It is the ratio of tensile stress, force per unit area, to tensile strain, the relative change in length. It is measured in pascals and usually quoted in gigapascals.
A ratio. A bar 2 m long that gains 1 mm has a strain of 0.001 ÷ 2 = 0.0005, not 0.05 percent. Entering a percentage here makes the modulus come out a hundred times too small.
Stress is the force spread over the cross-section, σ = F ÷ A, measured in pascals. Strain is the relative stretch, ε = ΔL ÷ L₀, and is a dimensionless ratio. Young's modulus is stress divided by strain, so it says how much stress a given amount of stretch costs.
Steel is roughly 200 GPa, copper about 110 GPa, aluminium around 69 GPa, glass near 70 GPa, and rubber only about 0.01 to 0.1 GPa. A higher modulus means the material stretches less under the same stress.
Only within the elastic region, where stress and strain stay proportional and the material springs back to its original shape. Beyond the elastic limit it deforms permanently and one modulus no longer describes it. This calculator assumes small, reversible deformations.
Information, not professional advice.
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