<p>The <i>comprehensive</i> incompressible strain energy function devised in a preceding contribution (J. Elast. 153:219–244, <CitationRef CitationID="CR1">2023</CitationRef>) is extended in this work for application to the finite deformation of isotropic <i>compressible</i> rubber-like materials. Based on the two established approaches in the literature for constructing a compressible strain energy function <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10659_2025_10122_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>W</mi> </math></EquationSource> <EquationSource Format="TEX">$W$</EquationSource> </InlineEquation> from the incompressible counterpart, two models are developed and presented: one model is developed on using a <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10659_2025_10122_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="99" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>J</mi> <mrow> <mo>(</mo> <mo>=</mo> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mspace width="0.2em" /> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mspace width="0.2em" /> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mo>)</mo> </mrow> </math></EquationSource> <EquationSource Format="TEX">$J\left (= \lambda _{1} \thinspace \lambda _{2} \thinspace \lambda _{3} \right )$</EquationSource> </InlineEquation> term added to the general functional form of the incompressible model; and the second model on using the isochoric, or modified, principal stretches <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10659_2025_10122_Article_IEq3.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mrow> <mo>(</mo> <msub> <mover accent="true"> <mi>λ</mi> <mo stretchy="false">¯</mo> </mover> <mi>a</mi> </msub> <mo>)</mo> </mrow> </math></EquationSource> <EquationSource Format="TEX">$\left (\bar{\lambda }_{a}\right )$</EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10659_2025_10122_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="71" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>a</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mn>2</mn> <mo>,</mo> <mn>3</mn> </math></EquationSource> <EquationSource Format="TEX">$a = 1,2,3$</EquationSource> </InlineEquation>, in the functional form of the incompressible model, to account for the deviatoric contribution <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10659_2025_10122_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="36" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>W</mi> <mrow> <mi>d</mi> <mi>e</mi> <mi>v</mi> </mrow> </msub> </math></EquationSource> <EquationSource Format="TEX">$W_{dev}$</EquationSource> </InlineEquation>. The volumetric input <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10659_2025_10122_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="35" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>W</mi> <mrow> <mi>v</mi> <mi>o</mi> <mi>l</mi> </mrow> </msub> </math></EquationSource> <EquationSource Format="TEX">$W_{vol}$</EquationSource> </InlineEquation> is considred as an additive part. Each model is then simultaneously fitted to extant multi-axial experimental datasets, and the favourable correlation between the models’ predictions and the experimental data is demonstrated. Exemplar challenging individual datasets including a shear-softening behaviour exhibited by an elastomeric foam are also considered, whereby the excellent predictions of the said behaviours by the models will be illustrated. The compatibility of both models with the kinematics of slight compressibility will also be discussed and presented.</p>

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Large Isotropic Elastic Deformations: On a Comprehensive Model to Correlate the Theory and Experiments for Compressible Rubber-Like Materials

  • Afshin Anssari-Benam,
  • Giuseppe Saccomandi

摘要

The comprehensive incompressible strain energy function devised in a preceding contribution (J. Elast. 153:219–244, 2023) is extended in this work for application to the finite deformation of isotropic compressible rubber-like materials. Based on the two established approaches in the literature for constructing a compressible strain energy function W $W$ from the incompressible counterpart, two models are developed and presented: one model is developed on using a J ( = λ 1 λ 2 λ 3 ) $J\left (= \lambda _{1} \thinspace \lambda _{2} \thinspace \lambda _{3} \right )$ term added to the general functional form of the incompressible model; and the second model on using the isochoric, or modified, principal stretches ( λ ¯ a ) $\left (\bar{\lambda }_{a}\right )$ , a = 1 , 2 , 3 $a = 1,2,3$ , in the functional form of the incompressible model, to account for the deviatoric contribution W d e v $W_{dev}$ . The volumetric input W v o l $W_{vol}$ is considred as an additive part. Each model is then simultaneously fitted to extant multi-axial experimental datasets, and the favourable correlation between the models’ predictions and the experimental data is demonstrated. Exemplar challenging individual datasets including a shear-softening behaviour exhibited by an elastomeric foam are also considered, whereby the excellent predictions of the said behaviours by the models will be illustrated. The compatibility of both models with the kinematics of slight compressibility will also be discussed and presented.