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Table 5 \(\hbox {Four phases, straight and curved interfaces: Material properties}\)

From: Phase-inherent linear visco-elasticity model for infinitesimal deformations in the multiphase-field context

\(\phi \)

\(\alpha \)

\(\beta \)

\(\gamma \)

\(\delta \)

\(K^0\)

\(3.00\,\hbox {GPa}\)

\(13.00\,\hbox {GPa}\)

\(0.50\,\hbox {GPa}\)

\(70.00\,\hbox {GPa}\)

\(G^0\)

\(1.00\,\hbox {GPa}\)

\(4.00\,\hbox {GPa}\)

\(0.35\,\hbox {GPa}\)

\(10.00\,\hbox {GPa}\)

\(K^1\)

\(1.25 \times K^{\alpha , 0}\)

\(0.50 \times K^{\beta , 0}\)

\(1.15 \times K^{\gamma , 0}\)

–

\(G^1\)

\(1.25 \times G^{\alpha , 0}\)

\(0.50 \times G^{\beta , 0}\)

\(1.15 \times G^{\gamma , 0}\)

–

\(\eta ^1\)

\(2.50 \times 1.0\,\hbox {GPa s}\)

\(1.75 \times 1.5\,\hbox {GPa s}\)

\(2.00 \times 0.5\,\hbox {GPa s}\)

–

\(K^2\)

\(1.25^2 \times K^{\alpha , 0}\)

\(0.50^2 \times K^{\beta , 0}\)

\(1.15^2 \times K^{\gamma , 0}\)

–

\(G^2\)

\(1.25^2 \times G^{\alpha , 0}\)

\(0.50^2 \times G^{\beta , 0}\)

\(1.15^2 \times G^{\gamma , 0}\)

–

\(\eta ^2\)

\(2.50^2 \times \eta ^{\alpha ,1}\)

\(1.75^2 \times \eta ^{\beta ,1}\)

\(2.00 \times \eta ^{\gamma ,1}\)

–

\(K^3\)

\(1.25^3 \times K^{\alpha , 0}\)

–

\(1.15^3 \times K^{\gamma , 0}\)

–

\(G^3\)

\(1.25^3 \times G^{\alpha , 0}\)

–

\(1.15^3 \times G^{\gamma , 0}\)

–

\(\eta ^3\)

\(2.50^2 \times \eta ^{\alpha ,1}\)

–

\(2.00 \times \eta ^{\gamma ,1}\)

–

\(K^4\)

–

–

\(1.15^4 \times K^{\gamma , 0}\)

–

\(G^4\)

–

–

\(1.15^4 \times G^{\gamma , 0}\)

–

\(\eta ^4\)

–

–

\(2.00 \times \eta ^{\gamma ,1}\)

–