International audienceSecond gradient theories have to be used to capture how local micro heterogeneities macroscopically affect the behavior of a continuum. In this paper a configurational space for a solid matrix filled by an unknown amount of fluid is introduced. The Euler–Lagrange equations valid for second gradient poromechanics, generalizing those due to Biot, are deduced by means of a Lagrangian variational formulation. Starting from a generalized Clausius–Duhem inequality, valid in the framework of second gradient theories, the existence of a macroscopic solid skeleton Lagrangian deformation energy, depending on the solid strain and the Lagrangian fluid mass density as well as on their Lagrangian gradients, is proven
International audienceThe second gradient model of poromechanics, introduced in Part I, is here line...
AbstractSecond gradient theories have been developed in mechanics for treating different phenomena a...
The second gradient model of poromechanics, introduced in Part I, is here linearized in the neighbor...
International audienceSecond gradient theories have to be used to capture how local micro heterogene...
Second gradient theories have to be used to capture how local micro heterogeneities macroscopically ...
Second gradient theories have to be used to capture how local micro heterogeneities macroscopically ...
Local dilatancy and solid-fluid surface tension are two of the driving micro-phenomena which charact...
Second gradient theories have been developed in mechanics for treating different phenomena as capill...
International audienceSecond gradient theories have been developed in mechanics for treating differe...
AbstractSecond gradient theories have been developed in mechanics for treating different phenomena a...
International audienceIn this paper a general set of equations of motion and duality conditions to b...
International audienceThe principle of virtual power is used to derive the equilibrium field equatio...
International audienceThe principle of virtual power is used to derive the equilibrium field equatio...
The principle of virtual power is used to derive the equilibrium field equations of a porous solid s...
In this paper a general set of equations of motion and duality conditions to be imposed at macroscop...
International audienceThe second gradient model of poromechanics, introduced in Part I, is here line...
AbstractSecond gradient theories have been developed in mechanics for treating different phenomena a...
The second gradient model of poromechanics, introduced in Part I, is here linearized in the neighbor...
International audienceSecond gradient theories have to be used to capture how local micro heterogene...
Second gradient theories have to be used to capture how local micro heterogeneities macroscopically ...
Second gradient theories have to be used to capture how local micro heterogeneities macroscopically ...
Local dilatancy and solid-fluid surface tension are two of the driving micro-phenomena which charact...
Second gradient theories have been developed in mechanics for treating different phenomena as capill...
International audienceSecond gradient theories have been developed in mechanics for treating differe...
AbstractSecond gradient theories have been developed in mechanics for treating different phenomena a...
International audienceIn this paper a general set of equations of motion and duality conditions to b...
International audienceThe principle of virtual power is used to derive the equilibrium field equatio...
International audienceThe principle of virtual power is used to derive the equilibrium field equatio...
The principle of virtual power is used to derive the equilibrium field equations of a porous solid s...
In this paper a general set of equations of motion and duality conditions to be imposed at macroscop...
International audienceThe second gradient model of poromechanics, introduced in Part I, is here line...
AbstractSecond gradient theories have been developed in mechanics for treating different phenomena a...
The second gradient model of poromechanics, introduced in Part I, is here linearized in the neighbor...