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Table 3 Two phases, straight interface: Material properties

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

\({\varvec{\phi }}\)

\({\varvec{K}}^{\mathbf{0}}\)

\({\varvec{G}}^{\mathbf{0}}\)

\({\varvec{K}}^{\mathbf{1}}\)

\({\varvec{G}}^{\mathbf{1}}\)

\({\varvec{\eta }}^{\mathbf{1}}\)

\(\alpha \)

\(\frac{125}{3}\,\hbox {GPa}\)

\(\frac{250}{13}\,\hbox {GPa}\)

–

–

–

\(\beta \)

\(\frac{25}{6} \,\hbox {GPa}\)

\(\frac{25}{13} \,\hbox {GPa}\)

\(\frac{25}{3}\,\hbox {GPa}\)

\(\frac{50}{13}\,\hbox {GPa}\)

\(\frac{50}{13}\,\hbox {GPa s}\)