diff --git a/doc/Eqs/otherForceModels_gravityEff_pic1.jpg b/doc/Eqs/otherForceModels_gravityEff_pic1.jpg new file mode 100644 index 00000000..f15ed5b7 Binary files /dev/null and b/doc/Eqs/otherForceModels_gravityEff_pic1.jpg differ diff --git a/doc/Eqs/otherForceModels_gravityEff_pic2.jpg b/doc/Eqs/otherForceModels_gravityEff_pic2.jpg new file mode 100644 index 00000000..bef6f73a Binary files /dev/null and b/doc/Eqs/otherForceModels_gravityEff_pic2.jpg differ diff --git a/doc/Eqs/otherForceModels_gravityEff_pic3.jpg b/doc/Eqs/otherForceModels_gravityEff_pic3.jpg new file mode 100644 index 00000000..f4fdbcb5 Binary files /dev/null and b/doc/Eqs/otherForceModels_gravityEff_pic3.jpg differ diff --git a/doc/Eqs/otherForceModels_gravityEff_pic4.jpg b/doc/Eqs/otherForceModels_gravityEff_pic4.jpg new file mode 100644 index 00000000..89364bff Binary files /dev/null and b/doc/Eqs/otherForceModels_gravityEff_pic4.jpg differ diff --git a/doc/otherForceModel_gravityEff.txt b/doc/otherForceModel_gravityEff.txt new file mode 100644 index 00000000..136a888d --- /dev/null +++ b/doc/otherForceModel_gravityEff.txt @@ -0,0 +1,75 @@ +"CFDEMproject Website"_lws - "Main Page"_main :c + +:link(lws,http://www.cfdem.com) +:link(main,CFDEMcoupling_Manual.html) + +:line + +otherForceModel gravityEff command :h3 + +[Syntax:] + +Defined in "couplingProperties"_CFDEMcoupling_dicts.html#couplingProperties +dictionary. + +otherForceModels +( + gravityEff +); +gravityEffProps +{ + voidfractionFieldName "voidfraction"; + rhoPart number1; +} :pre + +{voidfraction} = name of the finite volume void fraction field :l +{number1} = particle density :l + +:ule + +[Examples:] + +otherForceModels +( + gravityEff +); +gravityEffProps +{ + voidfractionFieldName "voidfraction"; + rhoPart 1500; +} :pre + +[Description:] + +An effective gravitational source term, {gravityEff}, that is necessery to drive the flow only in +case of periodic box simulations. This source term is added to the momentum equation. In case of +simulating periodic boxes with assuming "Homogenous no flow condition" we will have: + +:c,image(Eqs/otherForceModels_gravityEff_pic1.jpg) + +This equation depicts that in "no flow consition" static pressure gradient balances the mixture weight. +Therefore, to derive the flow in the periodic box simulations, a dynamic pressure gradien is defined as, + +:c,image(Eqs/otherForceModels_gravityEff_pic2.jpg) + +If one replaces the static pressure gradient of the fluid momentum equation with, + +:c,image(Eqs/otherForceModels_gravityEff_pic3.jpg) + +The fluid momentum equation solved in case of periodic box simulations will be, + +:c,image(Eqs/otherForceModels_gravityEff_pic4.jpg) + +The {gravityEff} source term is the third term in the RHS of the momentum equation. Note that +the gravitational body force of the fluid momentum equation is considered with this source term. + +In the basic implementation of {gravityEff}, first we calculate the density of the mixture and then +the source term is calculated based on the third term in the RHS of the momentum equation. +[Restrictions:] + +none + +[Related commands:] + +"otherForceModels"_otherForceModels.html +