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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

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

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

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

\({\varvec{K}}^{{1..4}}\)

\({\varvec{G}}^{{1..4}}\)

\(\alpha \)

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

\(1\,\hbox {GPa}\)

\(\left\{ 0.75, 0.75^2, -, {-}\right\} \times K^{\alpha ,0}\)

\(\left\{ 0.75, 0.75^2, -, {-}\right\} \times G^{\alpha ,0}\)

\(\beta \)

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

\(1\,\hbox {GPa}\)

\(\left\{ 1.50, 1.50^2, 1.50^3, 1.50^4 \right\} \times K^{\beta , 0}\)

\(\left\{ 1.50, 1.50^2, 1.50^3, 1.50^4 \right\} \times G^{\beta , 0}\)

\(\phi \)

\(\eta ^{1..4}\)

\(\alpha \)

\(\left\{ 0.75, 0.75^2, -, {-}\right\} \times 1\,\hbox {GPa s}\)

\(\beta \)

\(\left\{ 1.50^4, 1.50^3, 1.50^2, 1.50 \right\} \times 1\,\hbox {GPa s}\)