vedo/examples/other/dolfin/heatconv.py

"""Heat equation in moving media."""
# Credits: Jan Blechta
# https://github.com/blechta/fenics-handson/blob/master/heatconv
from dolfin import *
set_log_level(30)


# Create mesh and build function space
mesh = UnitSquareMesh(30, 30, "crossed")
V = FunctionSpace(mesh, "Lagrange", 1)

# Create boundary markers
tdim = mesh.topology().dim()
boundary_parts = MeshFunction("size_t", mesh, tdim - 1)
left = AutoSubDomain(lambda x: near(x[0], 0.0))
right = AutoSubDomain(lambda x: near(x[0], 1.0))
bottom = AutoSubDomain(lambda x: near(x[1], 0.0))
left.mark(boundary_parts, 1)
right.mark(boundary_parts, 2)
bottom.mark(boundary_parts, 2)

# Initial condition and right-hand side
ic = Expression("""pow(x[0] - 0.25, 2) + pow(x[1] - 0.25, 2) < 0.2*0.2
                   ? -25.0 * ((pow(x[0] - 0.25, 2) + pow(x[1] - 0.25, 2)) - 0.2*0.2)
                   : 0.0""", degree=1,
)
f = Expression("""pow(x[0] - 0.75, 2) + pow(x[1] - 0.75, 2) < 0.2*0.2
                  ? 1.0
                  : 0.0""", degree=1,
)

# Equation coefficients
K = Constant(1e-2)  # thermal conductivity
g = Constant(0.01)  # Neumann heat flux
b = Expression(("-(x[1] - 0.5)", "x[0] - 0.5"), degree=1)  # convecting velocity

# Define boundary measure on Neumann part of boundary
dsN = Measure("ds", subdomain_id=1, subdomain_data=boundary_parts)

# Define steady part of the equation
def operator(u, v):
    return (K * inner(grad(u), grad(v)) - f * v + dot(b, grad(u)) * v
    ) * dx - K * g * v * dsN

# Define trial and test function and solution at previous time-step
u = TrialFunction(V)
v = TestFunction(V)
u0 = Function(V)

# Time-stepping parameters
dt = 0.02
theta = Constant(0.5)  # Crank-Nicolson scheme

# Define time discretized equation
F = ((1.0 / dt) * inner(u - u0, v) * dx
    + theta * operator(u, v)
    + (1.0 - theta) * operator(u0, v)
)

# Define boundary condition
bc = DirichletBC(V, Constant(0.0), boundary_parts, 2)

# Prepare solution function and solver
u = Function(V)
problem = LinearVariationalProblem(lhs(F), rhs(F), u, bc)
solver = LinearVariationalSolver(problem)

# Prepare initial condition
u0.interpolate(ic)
u.interpolate(ic)


######################################################Time-stepping
from vedo.dolfin import plot

t = 0.0
while t < 3:
    solver.solve()

    plot(u,
        text=__doc__+"\nTemperature at t = %g" % t,
        style=2,
        axes=3,
        lw=0, # no mesh edge lines
        warp_zfactor=0.1,
        isolines={"n": 12, "lw":1, "c":'black', "alpha":0.1},
        scalarbar=False,
        interactive=False,
    ).clear()

    # Move to next time step
    u0.assign(u)
    t += dt