DiffEqApproxFun.jl is a component package in the DifferentialEquations ecosystem. It holds the components for solving differential equations using spectral methods defined by types from ApproxFun.jl. Users interested in using this functionality should check out DifferentialEquations.jl.
The indirect ApproxFun interface allows one to define an
ODEProblem directly from ApproxFun expressions. It will automatically convert this into a spectral ODE problem where the vector is the spectral coefficients. The pro for this method is that it can be used with any ODE solver on the common interface such as Sundials. However, this method uses a constant number of coefficients and truncates the expansions given by ApproxFun to always match this size and so it's a little bit wasteful. But this presents itself as one of the easiest ways to solve a spectral discretization of a PDE.
To define such a problem, we first need to define our inital condition as a
using DiffEqApproxFun S=Fourier() u0=Fun(θ->cos(cos(θ-0.1))-cos(cos(0-0.1)),S)
Now let's define our ODE which takes in
Fun types and spits out new
c=Fun(cos,S) ode_prob = ODEProblem((u,p,t)->u''+(c+1)*u',u0,(0.,1.))
To turn this into an indirect ApproxFun problem, we use the
prob = ApproxFunProblem(ode_prob)
We can now solve this using any solver:
using OrdinaryDiffEq sol=solve(prob,Tsit5()) # OrdinaryDiffEq.jl using Sundials sol=solve(prob,CVODE_BDF()) # Sundials.jl using ODEInterfaceDiffEq sol=solve(prob,radau()) # ODEInterfaceDiffEq.jl
The solution interface works on this output, so to grab the solution at the 5th timepoint we do
sol.t. Each solution is a
Fun type, which we can evaluate. Thus we can get the value at
x=0.2 at time
sol(0.2). The interpolations generate their own Fun types, so the value of
x=0.2 at time
t=0.5 is calculated via
Normally you will want to solve a PDE with non-trivial boundary conditions. If possible you should make your
Fun discretization match the BCs. For example, this is done automatically when the BCs are periodic and the discretization is periodic. But this isn't always possible, in which case you will need to define a
bc function which projects the solution at each step to satisfy the boundary conditions. For example, we can have Dirichlet conditions s.t. the solution must be zero at the endpoints of our interval in the problem above via:
function bc(t,u) C=eye(S)[3:end,:] tmp = [Evaluation(0); Evaluation(2π); C]\[0.;0.;u] end
Then we can generate a callback via
BoundaryCallback and have the solver utilize this callback. This requires a common interface solver which is compatible with the callback interface.
boundary_projection = BoundaryCallback(bc) sol=solve(prob,Tsit5(),callback=boundary_projection)
The resulting solution satisfies the boundary conditions.
sol(0.5) returns the interpolated
Fun type at time
Fun types have their own plotting recipes. Thus you can plot the solution at snippets of time directly like
plot(sol,labels="t=0.0") plot!(sol(0.5),labels="t=0.5") plot!(sol[end],labels="t=1.0")
The direct ApproxFun interface is simply using a
Fun as an initial condition and a function on
Fun types as the function in a standard
*DiffEq solvers like OrdinaryDiffEq.jl will directly handle this as an adaptive-space spectral discretization of the PDE. However, care has to be taken since this can cause the number of coefficients to grow rapidly. One may need to use an L-stable integrator and change the linear solver which is used. This is still in development.
about 2 months ago