Open Access
Table 2
Quantities returned by computeHomogeneous.
| Key | Units | Description |
|---|---|---|
| kE | dimensionless | Elastic Love number kE |
| kf | dimensionless | Fluid Love number kf |
| k2Re | dimensionless | Real part of k2(iω) |
| k2Im | dimensionless | Imaginary part of k2(iω) |
| gamma | Pa | Gravitational rigidity γ |
| alpha | Pa | Elastic rigidity α |
| eta | Pa s | Viscosity of the isolated dashpot |
| prefactor | s−2 | Mapping prefactor Θ = 3I°G/R5 |
| Fconv | Pa s2 | Conversion factor to physical units |
| nPoles | integer | Number of secular poles (equal to n + 1 in the notation of Section 2.3) |
| poles | s−1 | Secular pole locations {sj} |
| residues | dimensionless | Residues {rj} in the mode decomposition of k2(s) |
| nVoigt | integer | Number of Kelvin–Voigt elements (equal to n in the notation of Section 2.3) |
| tauV | s | Relaxation times {τi} of the Voigt elements |
| alphaV | Pa | Spring rigidities {αi} of the Voigt elements |
| etaV | Pa s | Dashpot viscosities {ηi} of the Voigt elements |
Notes. The routine returns both the intermediate mode information of the layered model and the parameters of the equivalent homogeneous generalized Voigt rheology.
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