Coding gain: Difference between revisions

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In [[linear elasticity]], the '''Lamé parameters''' are the two parameters
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* λ, also called ''Lamé's first parameter''
* μ, the [[shear modulus]] or ''Lamé's second parameter'' (also referred to as '''G''')
 
In homogenous and [[isotropic]] materials, these satisfy [[Hooke's law]] in 3D,
 
:<math>\sigma=2\mu \varepsilon +\lambda \; \mathrm{tr}(\varepsilon)I</math>
 
where σ is the [[Stress (physics)|stress]], ε the [[strain tensor]], <math>\scriptstyle I</math> the [[identity matrix]] and <math>\scriptstyle\mathrm{tr}(\cdot)</math> the [[Trace (linear algebra)|trace]] function.  
 
The first parameter λ is related to the bulk modulus and the shear modulus via <math>K = \lambda + (2/3) \mu</math> in three-dimensions and <math>K = \lambda + \mu</math> for two-dimensional solids, and serves to simplify the stiffness matrix in Hooke's law.  
Although the shear modulus, μ, must be positive, the Lamé's first parameter, λ, can be negative, in principle; however, for most materials it is also positive. The two parameters together constitute a parameterization of the elastic moduli for homogeneous isotropic media, popular in mathematical literature, and are thus related to the other elastic moduli.
 
The parameters are named after [[Gabriel Lamé]].
 
== References ==
* K. Feng, Z.-C. Shi, ''Mathematical Theory of Elastic Structures'', Springer New York, ISBN 0-387-51326-4, (1981)
* G. Mavko, T. Mukerji, J. Dvorkin, ''The Rock Physics Handbook'', Cambridge University Press (paperback), ISBN 0-521-54344-4, (2003)
 
 
{{Elastic moduli}}
 
{{DEFAULTSORT:Lame parameters}}
{{physics-stub}}
 
[[Category:Elasticity (physics)]]

Latest revision as of 02:09, 19 October 2014

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