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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

\({\varvec{\phi }}\) \({\varvec{K}}^{\mathbf{0}}\) \({\varvec{G}}^{\mathbf{0}}\) \({\varvec{K}}^{\mathbf{1}}\) \({\varvec{G}}^{\mathbf{1}}\) \({\varvec{\eta }}^{\mathbf{1}}\)
\(\alpha \) \(\frac{125}{3}\,\hbox {GPa}\) \(\frac{250}{13}\,\hbox {GPa}\)
\(\beta \) \(\frac{25}{6} \,\hbox {GPa}\) \(\frac{25}{13} \,\hbox {GPa}\) \(\frac{25}{3}\,\hbox {GPa}\) \(\frac{50}{13}\,\hbox {GPa}\) \(\frac{50}{13}\,\hbox {GPa s}\)