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Poisson's ratio

When a sample of material is stretched in one direction, it tends to get thinner in the other two directions. Poisson's ratio (ν) is a measure of this tendency. It is defined as the ratio of the strain in the direction of the applied load to the strain normal to the load. For a perfectly incompressible material, the Poisson's ratio would be exactly 0.5. Most practical engineering materials have ν between 0.0 and 0.5. Cork is close to 0.0, most steels are around 0.3, and rubber is almost 0.5.

Referenced By

Elastic | Elastic modulus | Fused quartz | Modulus of elasticity | Young's modulus

 

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This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "Poisson's ratio".

 

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