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Table 4 Two phases, curved interface: Material properties

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

\({\varvec{\phi }}\) \({\varvec{K}}^{\mathbf{0}}\) \({\varvec{G}}^{\mathbf{0}}\) \({\varvec{K}}^{{1..4}}\) \({\varvec{G}}^{{1..4}}\)
\(\alpha \) \(3\,\hbox {GPa}\) \(1\,\hbox {GPa}\) \(\left\{ 0.75, 0.75^2, -, {-}\right\} \times K^{\alpha ,0}\) \(\left\{ 0.75, 0.75^2, -, {-}\right\} \times G^{\alpha ,0}\)
\(\beta \) \(3\,\hbox {GPa}\) \(1\,\hbox {GPa}\) \(\left\{ 1.50, 1.50^2, 1.50^3, 1.50^4 \right\} \times K^{\beta , 0}\) \(\left\{ 1.50, 1.50^2, 1.50^3, 1.50^4 \right\} \times G^{\beta , 0}\)
\(\phi \) \(\eta ^{1..4}\)
\(\alpha \) \(\left\{ 0.75, 0.75^2, -, {-}\right\} \times 1\,\hbox {GPa s}\)
\(\beta \) \(\left\{ 1.50^4, 1.50^3, 1.50^2, 1.50 \right\} \times 1\,\hbox {GPa s}\)