Physical Models
Overview
SeisSol includes various physical models to simulate realistic earthquake scenarios.
Elastic
This is the standard model in SeisSol and it implements isotropic elastic materials. The constitutive behaviour is \(\sigma_{ij} = \lambda \delta_{ij} \epsilon_{kk} + 2\mu \epsilon_{ij}\) with stress \(\sigma\) and strain \(\epsilon\). Elastic materials can be extended to elastoplastic materials (see SCEC TPV13).
Anisotropic
This is an extension of the elastic material, where directiondependent effects also play a role.
The stress strain relation is given by the \(\sigma_{ij} = c_{ijkl} \epsilon_{kl}\).
Whereas isotropic materials are described by two material parameters, the tensor \(c\) has \(81\) entries.
Due to symmetry considerations there are only \(21\) independent parameters, which have to be specified in the material file:
c11
, c12
, c13
, c14
, c15
, c16
, c22
, c23
, c24
, c25
, c26
, c33
, c34
, c35
, c36
, c44
, c45
, c46
, c55
, c56
, c66
.
For more details about the anisotropic stiffness tensor, see: https://en.wikipedia.org/wiki/Hooke%27s_law#Anisotropic_materials.
All parameters have to be set, even if they are zero.
If only the two Lamé parameters are provided, SeisSol assumes isotropic behaviour.
Example of an material file for a homogeneous anisotropic fullspace. The material describes the tilted transversally isotropic medium from chapter 5.4 in https://link.springer.com/chapter/10.1007/9783030504205_3.
!ConstantMap
map:
rho: 2590
c11: 6.66000000000000e10
c12: 2.46250000000000e10
c13: 3.44750000000000e10
c14: 8.53035022727672e9
c15: 0.0
c16: 0.0
c22: 6.29062500000000e10
c23: 3.64187500000000e10
c24: 4.05949408023955e9
c25: 0.0
c26: 0.0
c33: 4.95562500000000e10
c34: 7.50194506028270e9
c35: 0.0
c36: 0.0
c44: 7.91875000000000e9
c45: 0.0
c46: 0.0
c55: 1.40375000000000e10
c56: 5.43430940874735e9
c66: 2.03125000000000e10
Anisotropy together with plasticity and dynamic rupture is not tested yet. You can define a dynamic rupture fault embedded in an isotropic material and have anisotropic regions elsewhere in the domain.
Poroelastic
In poroelastic materials a fluid and a solid phase interact with each other. The material model introduces the pressure \(p\) and the relative fluid velocities \(u_f, v_f, w_f\) to the model, so that we observe 13 quantities in total. A poroelastic material is characterised by the following material parameters:
Parameter 
SeisSol name 
Abbreviation 
Unit 

Solid Bulk modulus 

\(K_S\) 
\(Pa\) 
Solid density 

\(\rho_S\) 
\(kg \cdot m^{3}\) 
Matrix \(1^{st}\) Lamé parameter 

\(\lambda_M\) 
\(Pa\) 
Matrix \(2^{nd}\) Lamé parameter 

\(\mu_M\) 
\(Pa\) 
Matrix permeability 

\(\kappa\) 
\(m^2\) 
Matrix porosity 

\(\phi\) 

Matrix tortuosity 

\(T\) 

Fluid bulk modulus 

\(K_F\) 
\(Pa\) 
Fluid density 

\(\rho_F\) 
\(kg \cdot m^{3}\) 
Fluid viscosity 

\(\nu\) 
\(Pa \cdot s\) 
The implementation of poroelasticity is tested for point sources, material interfaces and freesurfaces. Plasticity and dynamic rupture together with poroelasticity are not tested.
Viscoelastic
Viscoelasticity is used to model the dissipation of wave energy over time. A full documentation can be found in Attenuation.