6-node displacement and pore pressure cohesive element with the transition from
Darcy flow to Poiseuille flow
COHAX4P(S)
6-node displacement and pore pressure cohesive element
Active Degrees of Freedom
1, 2, 8
Additional Solution Variables
None.
Coupled Temperature-Displacement Element
COHAX4T(S)
4-node displacement and temperature cohesive element
Active Degrees of Freedom
1, 2, 11
Additional Solution Variables
None.
Coupled Temperature-Pore Pressure Element
CODAX4PT(S)
6-node temperature and pore pressure cohesive element
Active Degrees of Freedom
1, 2, 8,11 (1 and 2 on the middle face are constrained by corresponding values on the
top and bottom faces)
Additional Solution Variables
None.
Coupled Slurry Concentration-Pore Pressure Element
CODAX4C(S)
6-node displacement, pore pressure, and slurry concentration cohesive element
Active Degrees of Freedom
1, 2, 8 at nodes on the top and bottom faces; 1, 2, 8, 31 at nodes on the middle face
(1 and 2 on the middle face are constrained by corresponding values on the top and
bottom faces)
Additional Solution Variables
None.
Coupled Temperature-Slurry Concentration-Pore Pressure Element
CODAX4Q(S)
6-node temperature and slurry cohesive element
Active Degrees of Freedom
1, 2, 8, 11 at nodes on the top and bottom faces; 1, 2, 8, 11, 31 at nodes on the
middle face (1 and 2 on the middle face are constrained by corresponding values on the
top and bottom faces)
Additional Solution Variables
None.
Nodal Coordinates Required
Element Property Definition
You can define the element's initial constitutive thickness. The default initial
constitutive thickness of cohesive elements depends on the response of these elements. For
continuum response, the default initial constitutive thickness is computed based on the
nodal coordinates. For traction-separation response, the default initial constitutive
thickness is assumed to be 1.0. For response based on a uniaxial stress state, there is no
default; you must indicate your choice of the method for computing the initial
constitutive thickness. See Specifying the Constitutive Thickness for details.
Abaqus calculates the thickness direction automatically based on the midsurface of the
element.
Nonuniform body force in radial direction with magnitude supplied via user
subroutine DLOAD in Abaqus/Standard and VDLOAD in Abaqus/Explicit.
Load ID (*DLOAD): BZNU
Body force
FL−3
Nonuniform body force in axial direction with magnitude supplied via user
subroutine DLOAD in Abaqus/Standard and VDLOAD in Abaqus/Explicit.
Load ID (*DLOAD): CENT(S)
Not supported
FL−4(ML−3T−2)
Centrifugal load (magnitude is input as , where is the mass density per unit volume, is the angular velocity).
Load ID (*DLOAD): CENTRIF(S)
Rotational body force
T−2
Centrifugal load (magnitude is input as , where is the angular velocity).
Load ID (*DLOAD): GRAV
Gravity
LT−2
Gravity loading in a specified direction (magnitude is input as acceleration).
Load ID (*DLOAD): Pn
Pressure
FL−2
Pressure on face n.
Load ID (*DLOAD): PnNU
Not supported
FL−2
Nonuniform pressure on face n with magnitude supplied
via user subroutine DLOAD in Abaqus/Standard and VDLOAD in Abaqus/Explicit.
Load ID (*DLOAD): SBF(E)
Not supported
FL−5T2
Stagnation body force in radial and axial directions.
Load ID (*DLOAD): SPn(E)
Not supported
FL−4T2
Stagnation pressure on face n.
Load ID (*DLOAD): VBF(E)
Not supported
FL−4T
Viscous body force in radial and axial directions.
Load ID (*DLOAD): VPn(E)
Not supported
FL−3T
Viscous pressure on face n, applying a pressure
proportional to the velocity normal to the face and opposing the motion.
Distributed Heat Fluxes
Distributed heat fluxes are available for all elements with temperature degrees of
freedom. They are specified as described in Thermal Loads. Distributed
heat flux magnitudes are per unit area or per unit volume. They do not need to be
multiplied by .
*dflux
Load ID (*DFLUX): BF
Body heat flux
JL−3T−1
Heat body flux per unit volume.
Load ID (*DFLUX): BFNU
Body heat flux
JL−3T−1
Nonuniform heat body flux per unit volume with magnitude supplied via user
subroutine DFLUX in Abaqus/Standard.
Load ID (*DFLUX): Sn
Surface heat flux
JL−2T−1
Heat surface flux per unit area into face n.
Load ID (*DFLUX): SnNU
Not supported
JL−2T−1
Nonuniform heat surface flux per unit area into face n
with magnitude supplied via user subroutine DFLUX in Abaqus/Standard.
Film Conditions
Film conditions are available for all elements with temperature degrees of freedom.
They are specified as described in Thermal Loads.
*film
Load ID (*FILM): Fn
Surface film condition
JL−2T−1−1
Film coefficient and sink temperature (units of ) provided on face n.
Load ID (*FILM): FnNU(S)
Not supported
JL−2T−1−1
Nonuniform film coefficient and sink temperature (units of ) provided on face n with magnitude
supplied via user subroutine FILM.
Radiation Types
Radiation conditions are available for all elements with temperature degrees of
freedom. They are specified as described in Thermal Loads.
*radiate
Load ID (*RADIATE): Rn
Surface radiation
Dimensionless
Emissivity and sink temperature provided for face n.
Surface-Based Loading
Distributed Loads
Surface-based distributed loads are specified as described in Distributed Loads.
*dsload
Load ID (*DSLOAD): P
Pressure
FL−2
Pressure on the element surface.
Load ID (*DSLOAD): PNU
Pressure
FL−2
Nonuniform pressure on the element surface with magnitude supplied via user
subroutine DLOAD in Abaqus/Standard and VDLOAD in Abaqus/Explicit.
Load ID (*DSLOAD): SP(E)
Pressure
FL−4T2
Stagnation pressure on the element surface.
Load ID (*DSLOAD): VP(E)
Pressure
FL−3T
Viscous pressure applied on the element surface. The viscous pressure is
proportional to the velocity normal to the element face and opposing the motion.
Stress and other tensors (including strain tensors) are available for elements with
continuum response. Both the stress tensor and the strain tensor contain true values.
For the constitutive calculations using a continuum response, only the direct
through-thickness and the transverse shear strains are assumed to be nonzero. All the
other strain components (that is, the membrane strains) are assumed to be zero (see
Modeling of an Adhesive Layer of Finite Thickness
for details). All tensors have the same number of components. For example, the stress
components are as follows:
S11
Direct membrane stress.
S22
Direct through-thickness stress.
S33
Direct membrane stress.
S12
Transverse shear stress.
Cohesive Elements Using a Uniaxial Stress State
Stress and other tensors (including strain tensors) are available for cohesive
elements with uniaxial stress response. Both the stress tensor and the strain tensor
contain true values. For the constitutive calculations using a uniaxial stress response,
only the direct through-thickness stress is assumed to be nonzero. All the other stress
components (that is, the membrane and transverse shear stresses) are assumed to be zero
(see Modeling of Gaskets and/or Small Adhesive Patches for details). All tensors have the same number of components. For example, the stress
components are as follows:
S22
Direct through-thickness stress.
Cohesive Elements Using a Traction-Separation Response
Stress and other tensors (including strain tensors) are available for elements with
traction-separation response. Both the stress tensor and the strain tensor contain
nominal values. The output variables
E,
LE, and
NE all contain the nominal strain when
the response of cohesive elements is defined in terms of traction versus separation. All
tensors have the same number of components. For example, the stress components are as
follows: