better heat example

This commit is contained in:
Jukka Aho
2016-06-09 23:17:57 +03:00
parent 06a4623acc
commit 74ed32a96c
2 changed files with 49 additions and 24 deletions
+8
View File
@@ -312,14 +312,22 @@ function call(solver::Solver)
info("Starting nonlinear iteration #$(solver.iteration)")
# 2.1 update linearized assemblies (if needed)
info("Assembling problems ...")
tic()
for problem in solver.problems
problem.assembly.changed = true # force reassembly
assemble!(problem, solver.time)
end
t1 = round(toq(), 2)
info("Assembled in $t1 seconds.")
# 2.2 call solver for linearized system (default: direct lu factorization)
info("Solve linear system ...")
tic()
u, la = solve_linear_system(solver, Val{solver.linear_system_solver})
push!(solver.norms, (norm(u), norm(la)))
t1 = round(toq(), 2)
info("Solved Ax = b in $t1 seconds.")
# 2.3 update solution back to elements
for problem in solver.problems
+41 -24
View File
@@ -13,48 +13,65 @@ using JuliaFEM.Test
3 => [1.0,1.0],
4 => [0.0,1.0])
# volume element
element = Element(Quad4, [1, 2, 3, 4])
# define volume element
el1 = Element(Quad4, [1, 2, 3, 4])
update!(element, "geometry", X)
update!(element, "temperature thermal conductivity", 6.0)
update!(element, "temperature load", [12.0, 12.0, 12.0, 12.0])
update!(element, "density", 36.0)
update!(el1, "geometry", X)
update!(el1, "temperature thermal conductivity", 6.0)
update!(el1, "temperature load", 12.0)
update!(el1, "density", 36.0)
# boundary element
boundary_element = Element(Seg2, [1, 2])
update!(boundary_element, "geometry", X)
# linear ramp from 0 to 6 in time 0 to 1
update!(boundary_element, "temperature flux", 0.0 => 0.0, 1.0 => 6.0)
# define boundary element for flux
el2 = Element(Seg2, [1, 2])
update!(el2, "geometry", X)
# linear ramp from 0 -> 6 in time 0 -> 1
update!(el2, "temperature flux", 0.0 => 0.0, 1.0 => 6.0)
# define heat problem and push elements to problem
problem = Problem(Heat, "one element heat problem", 1)
push!(problem, element, boundary_element)
push!(problem, el1, el2)
# Set constant source f=12 with k=6. Accurate solution is
# T=1 on free boundary, u(x,y) = -1/6*(1/2*f*x^2 - f*x)
# define boundary element for dirichlet boundary condition
el3 = Element(Seg2, [3, 4])
update!(el3, "geometry", X)
update!(el3, "temperature 1", 0.0)
boundary_condition = Problem(Dirichlet, "T=0 on top", 1, "temperature")
push!(boundary_condition, el3)
# manual assembling of problem + solution:
assemble!(problem, 0.0)
A = full(problem.assembly.K)
b = full(problem.assembly.f)
A_expected = [
4.0 -1.0 -2.0 -1.0
-1.0 4.0 -1.0 -2.0
-2.0 -1.0 4.0 -1.0
-1.0 -2.0 -1.0 4.0]
@test isapprox(A, A_expected)
free_dofs = [1, 2]
@test isapprox(A, A_expected)
@test isapprox(A[free_dofs, free_dofs] \ b[free_dofs], [1.0, 1.0])
# using Solver
solver = Solver("solve heat problem")
solver.is_linear_system = true
push!(solver, problem, boundary_condition)
# Set constant source f=12 with k=6. Accurate solution is
# T=1 on free boundary, u(x,y) = -1/6*(1/2*f*x^2 - f*x)
# when boundary flux not active (at t=0)
solver.time = 0.0
call(solver)
# interpolate temperature at middle of element 2 (flux boundary) at time t=0:
T = el2("temperature", [0.0], 0.0)
@test isapprox(T[1], 1.0)
# Set constant flux g=6 on boundary. Accurate solution is
# u(x,y) = x which equals T=1 on boundary.
# at time t=1.0 all loads should be on.
empty!(problem.assembly)
assemble!(problem, 1.0)
A = full(problem.assembly.K)
b = full(problem.assembly.f)
T = A[free_dofs, free_dofs] \ b[free_dofs]
@test isapprox(T, [2.0, 2.0])
solver.time = 1.0
call(solver)
T = el2("temperature", [0.0], 1.0)
@test isapprox(T[1], 2.0)
end