Guide

The FinEtools package is used here to solve heat conduction problems.

Tutorials are provided in the form of Julia scripts and Markdown files in a dedicated folder: index of tutorials.

Modules

The package FinEtoolsHeatDiff has the following structure:

  • Top-level: FinEtoolsHeatDiff is the top-level module.

  • Heat conduction: AlgoHeatDiffModule (algorithms), FEMMHeatDiffModule, FEMMHeatDiffSurfModule (FEM machines to evaluate the matrix and vector quantities), MatHeatDiffModule (heat diffusion material)

Heat conduction FEM machines

There is one for the interior integrals and one for the boundary integrals. The machine for the interior integrals can be used to compute:

  • Conductivity matrix.

  • Load vector corresponding to prescribed temperature.

The machine for the boundary integrals can be used to compute:

  • Surface heat transfer matrix.

  • Heat load vector for surface heat transfer.

Algorithms

Solution procedures and other common operations on FEM models are expressed in algorithms. Anything that algorithms can do, the user of FinEtools can do manually, but to use an algorithm is convenient.

Algorithms typically (not always) accept a single argument, modeldata, a dictionary of data, keyed by Strings. Algorithms also return modeldata, typically including additional key/value pairs that represent the data computed by the algorithm.

Heat diffusion algorithms

There is an implementation of an algorithm for steady-state heat conduction.

Examples

Two-dimensional heat transfer with convection: convergence study.

Consider a plate of uniform thickness, measuring 0.6 m by 1.0 m. On one short edge the temperature is fixed at 100 °C, and on one long edge the plate is perfectly insulated so that the heat flux is zero through that edge. The other two edges are losing heat via convection to an ambient temperature of 0 °C. The thermal conductivity of the plate is 52.0 W/(m .°K), and the convective heat transfer coefficient is 750 W/(m^2.°K). There is no internal generation of heat. Calculate the temperature 0.2 m along the un-insulated long side, measured from the intersection with the fixed temperature side. The reference result is 18.25 °C.

The reference temperature at the point A is 18.25 °C according to the NAFEMS publication (which cites the book Carslaw, H.S. and J.C. Jaeger, Conduction of Heat in Solids. 1959: Oxford University Press).

The present tutorial will investigate the reference temperature and it will attempt to estimate the limit value more precisely using a sequence of meshes and Richardson's extrapolation.

We begin by defining a few geometric parameters.

using FinEtools
# Geometrical dimensions
Width = 0.6 * phun("M")
Height = 1.0 * phun("M")
HeightA = 0.2 * phun("M")
Thickness = 0.1 * phun("M")
tolerance = Width / 1000

And now we are ready to define the conductivity of the material.

using FinEtoolsHeatDiff
# Conductivity matrix
kappa = [52.0 0; 0 52.0] * phun("W/(M*K)") 
m = MatHeatDiff(kappa)

The surface heat transfer coefficient (film coefficient) is also defined,

# Surface heat transfer coefficient
h = 750 * phun("W/(M^2*K)")

as is the temperature along one edge.

# Prescribed temperature.
T1 = 100 * phun("K")

Now we are ready to round the simulation five times, for progressively increasing refinement levels, and collect the computed value of the reference quantity.

# Five progressively refined models will be created and solved. 
modeldata = nothing
resultsTempA = Float64[]
params = Float64[]
for nref in 2:6
    # The mesh is created from two rectangular blocks to begin with.
    fens, fes = T3blockx([0.0, Width], [0.0, HeightA])
    fens2, fes2 = T3blockx([0.0, Width], [HeightA, Height])
    # The meshes are then glued into a single entity.
    fens, newfes1, fes2 = mergemeshes(fens, fes, fens2, fes2, tolerance)
    fes = cat(newfes1, fes2)
    # Refine the mesh desired number of times.
    for ref in 1:nref
        fens, fes = T3refine(fens, fes)
    end
    # The boundary is extracted.
    bfes = meshboundary(fes)
    # The prescribed temperature is applied along edge 1 (the bottom
    # edge in Figure 1).
    list1 = selectnode(fens; box = [0.0 Width 0.0 0.0], inflate = tolerance)
    essential1 = FDataDict("node_list" => list1, "temperature" => T1)
    # The convection (surface heat transfer) boundary condition is applied
    # along the edges 2,3,4. 
    list2 = selectelem(fens, bfes; box = [Width Width 0.0 Height], inflate = tolerance)
    list3 = selectelem(fens, bfes; box = [0.0 Width Height Height], inflate = tolerance)
    # The boundary integrals are evaluated using a surface FEMM.
    cfemm = FEMMHeatDiffSurf(
        IntegDomain(subset(bfes, vcat(list2, list3)), GaussRule(1, 3), Thickness),
        h,
    )
    convection1 = FDataDict("femm" => cfemm, "ambient_temperature" => 0.0)
    # The interior integrals are evaluated using a volume FEMM.
    femm = FEMMHeatDiff(IntegDomain(fes, TriRule(3), Thickness), m)
    region1 = FDataDict("femm" => femm)
    # Make the model data
    modeldata = FDataDict(
        "fens" => fens,
        "regions" => [region1],
        "essential_bcs" => [essential1],
        "convection_bcs" => [convection1],
    )
    # Call the solver
    modeldata = AlgoHeatDiffModule.steadystate(modeldata)
    # Locate the node at the point A  [coordinates (Width,HeightA)].
    list4 = selectnode(fens; box=[Width Width HeightA HeightA], inflate=tolerance)
    # Collect the temperature  at the point A.
    Temp = modeldata["temp"]
    println("$(Temp.values[list4][1])")
    push!(resultsTempA, Temp.values[list4][1])
    push!(params, 1.0 / 2^nref)
end

The computed results can be processed with Richardson extrapolation to arrive at an estimate of the true solution.

# These are the computed results for the temperature at point A:
println("$( resultsTempA  )")
# Richardson extrapolation can be used to estimate the limit.
solnestim, beta, c, residual = richextrapol(resultsTempA[(end-2):end], params[(end-2):end])
println("Solution estimate = $(solnestim)")
println("Convergence rate estimate  = $(beta)")

In order to visualize the results, we export to Paraview. The geometry is two-dimensional: this means we can visualize the temperature as a three dimensional surface raised above the mesh.

# Postprocessing
geom = modeldata["geom"]
Temp = modeldata["temp"]
regions = modeldata["regions"]
vtkexportmesh(
    "T4NAFEMS--T3-solution.vtk",
    connasarray(regions[1]["femm"].integdomain.fes),
    [geom.values (Temp.values / 100)],
    FinEtools.MeshExportModule.VTK.T3;
    scalars = [("Temperature", Temp.values)],
)
vtkexportmesh(
    "T4NAFEMS--T3-mesh.vtk",
    connasarray(regions[1]["femm"].integdomain.fes),
    geom.values,
    FinEtools.MeshExportModule.VTK.T3,
)

Alt Visualization of the temperature field