1. Reference problem#

1.1. Geometry#

_images/Object_1.svg
Hauteur:

\(h=\mathrm{1,00}[m]\)

Width:

\(l=\mathrm{1,00}[m]\)

Thickness:

\(e=\mathrm{1,00}[m]\)

1.2. Material properties#

_images/Object_2.svg

\([\mathrm{GPa}]\)

Modulus of elasticity

_images/Object_3.svg

Poisson’s ratio

_images/Object_4.svg

\([\mathrm{\mu m}/m]\)

endogenous shrinkage coefficient

_images/Object_5.svg

\([\mathrm{\mu m}/{\mathrm{m.m}}^{3}/l]\)

desiccation shrinkage coefficient

_images/Object_6.svg

\([\mathrm{\mu m}/m/°C]\)

coefficient of thermal expansion

Here we also enter the sorption-desorption curve that relates the water content

_images/Object_7.svg

To hygrometry

_images/Object_8.svg

.

In this case it was assumed that the two quantities were linked by the following linear relationship:

_images/Object_9.svg

[l/m3] =

_images/Object_10.svg

[%].

Settings specific to BETON_UMLV:

_images/Object_11.svg

\([\mathrm{MPa}]\)

spherical part: apparent stiffness associated with the skeleton formed by hydrate blocks at the mesoscopic scale

_images/Object_13.svg

\([\mathrm{MPa}]\)

spherical part: apparent stiffness intrinsically associated with hydrates at the microscopic scale

_images/Object_15.svg

\([\mathrm{MPa}]\)

deviatoric part: stiffness associated with the capacity of adsorbed water to transmit charges (load bearing water)

_images/Object_17.svg

\([\mathrm{MPa.s}]\)

spherical part: apparent viscosity associated with the diffusion mechanism within the capillary porosity

_images/Object_80.svg

\([\mathrm{MPa.s}]\)

spherical part: apparent viscosity associated with the mechanism of interlamellar diffusion

_images/Object_82.svg

\([\mathrm{MPa.s}]\)

deviatory part: viscosity associated with water adsorbed by hydrate sheets

_images/Object_84.svg

\([\mathrm{MPa.s}]\)

deviatoric part: viscosity of free water.

Settings specific to BETON_BURGER:

_images/Object_93.svg

\([\mathrm{MPa}]\)

spherical part: apparent stiffness associated with the reversible domain of delayed deformations

_images/Object_97.svg

\([\mathrm{MPa}]\)

deviatoric part: associated stiffness associated with the reversible domain of delayed deformations

_images/Object_99.svg

\([\mathrm{MPa.s}]\)

spherical part: apparent viscosity associated with the reversible range of delayed deformations

_images/Object_101.svg

\([\mathrm{MPa.s}]\)

spherical part: apparent viscosity associated with the irreversible diffusion mechanism

_images/Object_103.svg

\([\mathrm{MPa.s}]\)

deviatory part: viscosity associated with the reversible domain of delayed deformations

_images/Object_105.svg

\([\mathrm{MPa.s}]\)

deviatoric part: apparent viscosity associated with the irreversible diffusion mechanism

\(\kappa =3.0\times {10}^{-3}\)

Irreversible deformation standard controlling the nonlinearity applied to the long-term deformation module

1.3. Boundary conditions and loads#

In this test, a homogeneous drying field is created in the structure varying linearly over a period of 750 days, the initial humidity is \(100\text{\%}\) (condition of a sealed test piece) and decreases progressively to \(50\text{\%}\) on the 750th day.

The degree of hydration varies linearly from 0 to 1 between the initial moment and the 28th day.

Mechanical loading corresponds to unidirectional compression in the vertical direction (\(z\) in \(\mathrm{3D}\)); its intensity is \(12[\mathrm{MPa}]\). The load is applied in \(\mathrm{1s}\) and is kept constant for 100 days.

1.4. Initial conditions#

The start of the calculation is assumed at time \(–1\). At this moment there is no drying field or mechanical stress.

At instant 0, a drying field corresponding to \(100\text{\%}\) humidity is applied, a hydration field corresponding to zero progress and a thermal field at the reference temperature are applied.