Heat Transfer
Welcome to the Heat Transfer toolbox.
1. Heat Toolbox
1.1. Models
The model used by default with the heat toolbox is represented by this equation
with the following properties :
-
\(q=-k \nabla T\) is the conductive heat flux,
-
\(Q=0\) is heat source by default equal to 0,
-
\(\Omega\) the domain where the model is applied (.i.e. the materials).
For a steady-state problem, the temperature does not change with time, and the first term disappears.
1.1.1. Heat sources
The source term \(Q\) in the heat equation is used to model internal heat generation and absorption with positive and negative values respectively.
For adding a heat source term in the model, a JSON key called heat-sources
must be added and the JSON value associated can be
-
a string: explicit expression of \(Q\),
-
a JSON object: setup one heat source,
-
an array of JSON object : \(Q\) is composed of several heat sources.
We also consider two ways for defined a heat source :
-
from an explicit expression of the heat source
-
from an expression of the heat rate \(P\). In this case, \(Q = P/V\), where \(V\) is the volume of the material belongs to this model.
The setup of a heat source is defined from the properties listed in the next table.
Keyword | Description | Value Type | Default Value |
---|---|---|---|
|
possible values : |
string |
|
|
expression with respect to the type used |
string |
The term \(Q\) can be also split into \(N\) terms (for example due to the multiple physics). The term \(Q\) can be written as \(Q=\sum_{i=1}^N Q_i\).
This setup can be done by using an array of JSON objects for the heat-sources
entry. And each JSON object corresponds to the previous description of one heat source.
{
"Models": {
"heat": [
{ (1)
"name": "heat1",
"materials": [
"mymatA",
"mymatB"
],
"setup": {
"heat-sources": [ (2)
{ (3)
"type": "heat-source",
"expr": "3"
},
{ (4)
"type": "heat-rate",
"expr": "2*exp(t):t"
}
]
}
},
{ (5)
"name": "heat2",
"materials": [
"mymatC"
],
"setup": {
"heat-sources": { (6)
"expr": "30"
}
}
}
]
}
}
1 | setup of first model called heat1 on materials mymatA and mymatB |
2 | heat sources will be composed of 2 terms that we will call \(Q_1\) and \(Q_2\) (with \(Q=Q_1+Q_2\)) |
3 | we define \(Q_1=3\) |
4 | we define \(Q_2=2*exp(t)/V\) with \(V\) the measure of materials mymatA and mymatB |
5 | setup of second model called heat2 on materials mymatC |
6 | we define one heat source with \(Q=30\) |
1.1.2. Convective heat transfert
Modeling heat transfer in fluid requires taking into account the convective effect in the heat equation. The heat equation is written as :
with \(\boldsymbol{u}\) the fluid velocity.
For adding this feature to the model, a convection
section should be added.
The value can be a string corresponding to velocity expression.
{
"Models": {
"heat": {
"setup": {
"convection": "{-30*(y+-0.7)*(y-0.5)*(y>0.5)*(y<0.7),0}:y"
}
}
}
}
1.2. Materials
Name | Symbol | Shape | Description |
---|---|---|---|
thermal-conductivity |
k |
scalar or matrix |
thermal conductivity |
density |
rho |
scalar |
density |
thermal-expansion |
beta |
scalar |
thermal expansion |
specific-heat-capacity |
Cp |
scalar |
specific heat capacity |
1.3. Fields and symbols expressions
Name | Description | Shape |
---|---|---|
temperature |
the temperature field |
scalar |
Symbol | Expression | Description |
---|---|---|
heat_T |
\(T\) |
evaluate the temperature |
heat_grad_T_0 |
\(\frac{\partial T}{\partial x}\) |
evaluate the first component of gradient of temperature |
heat_grad_T_1 |
\(\frac{\partial T}{\partial y}\) |
evaluate the second component of gradient of temperature |
heat_grad_T_2 |
\(\frac{\partial T}{\partial z}\) |
evaluate the third component of gradient of temperature |
heat_dn_T |
\(\nabla T \cdot \boldsymbol{n}\) |
evaluate the normal derivative of temperature |
heat_nflux |
\(-k \nabla T \cdot \boldsymbol{n}\) |
evaluate the normal flux |
1.4. Boundary Conditions
1.4.1. Temperature imposed
JSON keywords : temperature
, temperature_imposed
Property | Description | Value Type | Is Optional | Default Value |
---|---|---|---|---|
|
mesh marker where the BC is applied |
|
yes |
name given to the BC |
|
expression of |
|
false |
{
"BoundaryConditions": {
"heat": { (1)
"temperature": { (2)
"bc1": { (3)
"markers": "gamma1", (4)
"expr": "293-10*(y-1)*(y+1):y" (5)
},
"bc2": { (6)
"expr": "293+0.38*t:t"
}
}
}
}
}
1 | the toolbox identity |
2 | JSON keyword for defining this kind of boundary condition |
3 | name given to a boundary condition of type temperature imposed |
4 | marker names where the boundary condition is applied |
5 | the expression of the temperature imposed |
6 | another boundary condition of type temperature imposed where the marker used will be the name (i.e. bc2 ) |
The temperature imposed can be applied on all kind of marked entities (elements,faces,edges,points) |
1.4.2. Heat flux
JSON keywords : heat_flux
, flux
Property | Description | Value Type | Is Optional | Default Value |
---|---|---|---|---|
|
mesh marker where the BC is applied |
|
yes |
name given to the BC |
|
expression of |
|
false |
{
"BoundaryConditions": {
"heat": {
"flux": {
"bc1": {
"markers": [
"MarkerNeumann_1",
"MarkerNeumann_2"
],
"expr": "34*t:t"
}
}
}
}
}
The expression given to the heat flux boundary condition can depend on the unknown (i.e. any symbols depending on the temperature). |
1.4.3. Convective heat flux
JSON keywords : convective_heat_flux
Property | Description | Value Type | Is Optional | Default Value |
---|---|---|---|---|
|
mesh marker where the BC is applied |
|
yes |
name given to the BC |
|
expression of |
|
false |
|
|
expression of |
|
false |
{
"BoundaryConditions": {
"heat": {
"convective_heat_flux": {
"bc1": {
"h": "16",
"Text": "287"
}
}
}
}
}
The expressions given to the convective heat flux boundary condition can depend on the unknown but the automatic differentiation is not implemented here, so the jacobian will be inexact if a Newton solver is used. |
1.4.4. Radiative heat flux
Radiative heat transfer is not yet available in the toolboxes. An application implementing radiative heat is currently available in feelpp/doc/manual/heat. |
New sections in the JSON configuration file are necessary. Firstly, the "Coating" section, which contains information about the radiative properties of the emitting surfaces, especially the value of the emissivity constant \(\epsilon\).
Property | Description | Value Type | Is Optional |
---|---|---|---|
|
list of mesh markers associated to a radiative surface |
|
no |
|
value of the emissivity of the radiative surface |
|
no |
{
"Coating":{
"materialName": {
"markers": [
"markerName"
],
"epsilon": "0.5"
}
}
}
Secondly, the "radiative_enclosure_heat_flux" and "radiative_blackbody_heat_flux" sections, inside the "BoundaryConditions" section, which specify the decomposition of the radiating boundaries into cavities, independent of each other, open or closed, where the radiative boundary conditions are imposed.
Property | Description | Value Type | Values | Is Optional |
---|---|---|---|---|
|
Specifies if the cavity is isolated (closed) or if it communicates with a black body (open) |
|
|
no |
|
list of mesh markers associated to a radiative surface |
|
no |
|
|
Stefan-Boltzmann constant |
|
no |
|
|
Reference temperature of the black body (only for open enclosures) |
|
yes |
|
|
Information for the computation/loading of view factors of the cavity |
JSON |
no |
Property | Description | Value Type | Values | Is Optional |
---|---|---|---|---|
|
Specifies if view factors have to be computed or loaded from file |
|
|
no |
|
File name for the computation of view factors (JSON format) or loading (CSV) |
|
no |
Property | Description | Value Type | Values | Is Optional |
---|---|---|---|---|
|
list of mesh markers associated to a radiative surface |
|
no |
|
|
Stefan-Boltzmann constant |
|
no |
|
|
Reference temperature of the black body (only for open enclosures) |
|
yes |
{
"BoundaryConditions": {
"heat": {
"radiative_enclosure_heat_flux": {
"Cavity": {
"enclosure": "closed",
"markers": ["InnerTop", "LowerTop","LeftTop","RightTop"],
"sigma": "sigma:sigma",
"Tref": "Tref_C+273.15:Tref_C",
"viewfactors": {
"status":"load",
"filename":"$cfgdir/VF_Matrix_Cavity_1.csv"
// "status":"compute",
// "filename":"$cfgdir/rectangular_cavity_vf.json"
}
}
},
"radiative_blackbody_heat_flux": {
"Gamma_BBC_1": {
"markers": ["Gamma_B_11","Gamma_B_12"],
"Tref": "Tref_C+273.15:Tref_C",
"sigma": "sigma:sigma"
}
}
}
}
}
Finally, an additional JSON file per cavity is necessary if the view factor matrix needs to be computed. This file will specify the algorithm to be use in order to compute the view factors, and the markers forming the cavity.
Property | Description | Value Type | Values | Is Optional |
---|---|---|---|---|
|
Choose between raytracing (obstructed and non-obstructed cavities) and quadrature (only non-obstructed cavities) |
|
|
no |
|
Choose the algorithm (only for UnobstructedPlanar) between DoubleAreaIntegration (2D) and SingleAreaIntegration (3D) |
|
|
yes |
|
Quadrature order (only for UnobstructedPlanar) |
|
yes |
|
|
list of mesh markers associated to the cavity |
|
no |
{
"viewfactor": {
"type": "UnobstructedPlanar",
"algorithm":"DoubleAreaIntegration",
"quadrature_order":2,
"markers":["RadiativeSurface1", "RadiativeSurface2","RadiativeSurface3"],
"description": "The viewfactor of a closed triangular cavity."
}
}
1.6. Post Processing
1.6.1. Exports
Name | Description |
---|---|
temperature |
the temperature field |
velocity-convection |
evaluate the gradient of temperature |
pid |
the mesh partitioning |
all |
all fields available |
All materials properties given in the section Materials can be also exported by specifying the name in the fields entry.
|
1.6.2. Measures
Normal-Heat-Flux
Parameters
section{
"Normal-Heat-Flux": { (1)
"bottom": { (2)
"markers": [ (3)
"bottom1",
"bottom2"
],
"direction": "inward" (4)
},
"top": { (5)
"direction": "inward"
}
}
}
1 | kind of measure |
2 | name of measure |
3 | surface markers where the measure is computed |
4 | direction : inward or outward |
5 | another measure applied on surface marker called top (because when markers is no present, the name is used as marker name) |