Compute Poisson's ratio (ν) using lateral and axial strain. Understand material compressibility, elasticity limits, and the fundamental Poisson effect.
In continuum mechanics, Poisson's ratio (ν) is the negative ratio of transverse (lateral) strain to axial (longitudinal) strain. When a material is stretched in one direction, it tends to contract in the perpendicular directions. This fundamental property, named after French mathematician Siméon Denis Poisson, quantifies the degree of this lateral contraction. For isotropic linear elastic materials, ν is a key parameter linking elastic moduli (Young's modulus, shear modulus, bulk modulus).
ν = – εlateral / εaxial
where εlateral = Δd / d₀ (change in width/original width) and εaxial = ΔL / L₀.
Siméon Denis Poisson first derived the existence of the lateral contraction effect in 1829 using molecular theory. Initially, he predicted ν = 0.25 for all isotropic materials, but later experiments showed variations. The theoretical bounds for isotropic materials are -1 ≤ ν ≤ 0.5 for thermodynamic stability. Materials with ν = 0.5 (e.g., rubber, some polymers) are perfectly incompressible (no volume change under uniaxial stress). Negative Poisson's ratio materials ("auxetics") expand laterally when stretched, exhibiting unique mechanical properties used in advanced composites and biomedical devices.
Given lateral strain (εlat) and axial strain (εax), the tool computes ν = – εlat / εax. For uniaxial loading, both strains are directly measured or derived. The sign convention: tensile axial strain > 0, corresponding lateral strain typically negative (contraction). A positive ν results. For negative ν, the lateral strain has the same sign as axial (auxetic behavior). The calculator also checks for near-incompressible materials (ν → 0.5) and theoretical stability limits. Additional classification: ν < 0 (auxetic), 0 ≤ ν < 0.3 (brittle materials), 0.3 ≤ ν < 0.45 (ductile metals and polymers), ν ≥ 0.45 (elastomers).
| Material | Poisson's Ratio (ν) | Remarks |
|---|---|---|
| Steel (structural) | 0.27 – 0.30 | Ductile metal, standard construction |
| Aluminum alloys | 0.32 – 0.35 | Lightweight, good formability |
| Concrete | 0.15 – 0.25 | Brittle, lower lateral contraction |
| Natural rubber | 0.49 – 0.50 | Nearly incompressible |
| Cork | ≈ 0.00 | Zero lateral contraction, used for bottle stoppers |
| Auxetic foam | -0.2 to -0.8 | Negative ratio, expands laterally under tension |
| Titanium | 0.34 | High strength-to-weight ratio |
An automotive engineer selects a rubber gasket material to maintain sealing pressure under thermal expansion. Using Poisson's ratio, the team estimates lateral squeeze when the gasket is compressed axially. For a synthetic elastomer with ν = 0.49, the lateral expansion is significant, ensuring tight sealing. The Poisson's Ratio Calculator helped quickly validate that with axial compression of 10%, lateral expansion reaches nearly 4.9% – meeting design requirements without leakage.
From thermodynamic constraints for isotropic linear elastic materials, the bulk modulus K and shear modulus G must be positive, leading to -1 < ν < 0.5. For ν = 0.5, the bulk modulus becomes infinite (ideal incompressibility). Auxetic materials (ν < 0) challenge conventional design and offer enhanced shear resistance, fracture toughness, and energy absorption. This calculator flags results near boundaries for educational clarity.