- Mooney-Rivlin solid
In
continuum mechanics , a Mooney-Rivlin solid is a generalization of theNeo-Hookean solid model, where the strain energy W is a linear combination of two invariants ofFinger tensor mathbf{B}::W = C_{10} (overline{I}_1-3) + C_{01} (overline{I}_2-3)+ frac{1}{d}(J_{el}-1)^2,
where overline{I}_1 and overline{I}_2 are the first and the second invariant of
deviatoric component of theFinger tensor : [The characteristic polynomial of the linear operator corresponding to the second rank three-dimensional Finger tensor is usually written:p_B (lambda) = lambda^3 - a_1 , lambda^2 + a_2 , lambda - a_3In this article, the trace a_1 is written I_1, the next coefficient a_2 is written I_2, and the determinant a_3 would be written I_3.]:I_1 = lambda_1^2 + lambda_2 ^2+ lambda_3 ^2,
:I_2 = lambda_1^2 lambda_2^2 + lambda_2^2 lambda_3^2 + lambda_3^2 lambda_1^2,
:I_3 = lambda_1^2 lambda_2^2 lambda_3^2,
where: overline{I_p} = J^{-2/3}I_p.
and C_{10}, C_{01}, and d are constants.
If C_1= frac {1} {2} G (where G is the
shear modulus ) and C_2=0, we obtain aNeo-Hookean solid , a special case of a Mooney-Rivlin solid.The stress tensor mathbf{T} depends upon Finger tensor mathbf{B} by the following equation:
:mathbf{T} = -pmathbf{I} +2C_1 mathbf{B} +2C_2 mathbf{B}^{-1}
The model was proposed by
Melvin Mooney andRonald Rivlin in two independent papers in1952 .Uniaxial extension
For the case of uniaxial elongation, true stress can be calculated as:
:T_{11} = left(2C_1 - frac {2C_2} {alpha_1} ight) left( alpha_1^2 - alpha_1^{-1} ight)
and
engineering stress can be calculated as::T_{11eng} = left(2C_1 - frac {2C_2} {alpha_1} ight) left( alpha_1 - alpha_1^{-2} ight)
The Mooney-Rivlin solid model usually fits experimental data better than
Neo-Hookean solid does, but requires an additional empirical constant.Brain tissues
Elastic response of soft tissues like that in the brain is often modelled based on the Mooney--Rivlin model.
ource
*C. W. Macosko Rheology: principles, measurement and applications, VCH Publishers, 1994, ISBN 1-56081-579-5
Notes and References
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