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JuliaApproximation / ApproxFun.jl


Julia package for function approximation



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ApproxFun is a package for approximating functions. It is in a similar vein to the Matlab package Chebfun and the Mathematica package RHPackage.

The ApproxFun Documentation contains detailed information, or read on for a brief overview of the package.


Take your two favourite functions on an interval and create approximations to them as simply as:

using ApproxFun
x = Fun(identity,0..10)
f = sin(x^2)
g = cos(x)

Evaluating f(.1) will return a high accuracy approximation to sin(0.01). All the algebraic manipulations of functions are supported and more. For example, we can add f and g^2 together and compute the roots and extrema:

h = f + g^2
r = roots(h)
rp = roots(h')

using Plots

Differentiation and integration

Notice from above that to find the extrema, we used ' overridden for the differentiate function. Several other Julia base functions are overridden for the purposes of calculus. Because the exponential is its own derivative, the norm is small:

f = Fun(x->exp(x),-1..1)

Similarly, cumsum defines an indefinite integration operator:

g = cumsum(f)
g = g + f(-1)

Algebraic and differential operations are also implemented where possible, and most of Julia's built-in functions are overridden to accept Funs:

x = Fun()
f = erf(x)
g = besselj(3,exp(f))
h = airyai(10asin(f)+2g)

Solving ordinary differential equations

Solve the Airy ODE u'' - x u = 0 as a BVP on [-1000,200]:

x = Fun(identity,-1000..200)
d = domain(x)
D = Derivative(d)
B = dirichlet(d)
L = D^2 - x
u = [B;L] \ [airyai(d.a);airyai(d.b);0]

Nonlinear Boundary Value problems

Solve a nonlinear boundary value problem satisfying the ODE 0.001u'' + 6*(1-x^2)*u' + u^2 = 1 with boundary conditions u(-1)==1, u(1)==-0.5 on [-1,1]:



Periodic functions

There is also support for Fourier representations of functions on periodic intervals. Specify the space Fourier to ensure that the representation is periodic:

f = Fun(cos,Fourier(-π..π))
norm(f' + Fun(sin,Fourier(-π..π))

Due to the periodicity, Fourier representations allow for the asymptotic savings of 2/π in the number of coefficients that need to be stored compared with a Chebyshev representation. ODEs can also be solved when the solution is periodic:

s = Chebyshev(-π..π)
a = Fun(t-> 1+sin(cos(2t)),s)
L = Derivative() + a
f = Fun(t->exp(sin(10t)),s)
B = periodic(s,0)
uChebyshev = [B;L]\[0.;f]

s = Fourier(-π..π)
a = Fun(t-> 1+sin(cos(2t)),s)
L = Derivative() + a
f = Fun(t->exp(sin(10t)),s)
uFourier = L\f



Other operations including random number sampling using [Olver & Townsend 2013]. The following code samples 10,000 from a PDF given as the absolute value of the sine function on [-5,5]:

f = abs(Fun(sin,-5..5))
x = ApproxFun.sample(f,10000)

Solving partial differential equations

We can solve PDEs, the following solves Helmholtz Δu + 100u=0 with u(±1,y)=u(x,±1)=1 on a square. This function has weak singularities at the corner, so we specify a lower tolerance to avoid resolving these singularities completely.

d = Interval()^2                            # Defines a rectangle
Δ = Laplacian(d)                            # Represent the Laplacian
f = ones(∂(d))                              # one at the boundary
u = \([Dirichlet(d);Δ+100I],[f;0.];         # Solve the PDE
surface(u)                                  # Surface plot

High precision

Solving differential equations with high precision types is available. The following calculates e to 300 digits by solving the ODE u' = u:

setprecision(1000) do
    @test u(1) ≈ exp(BigFloat(1))


S. Olver & A. Townsend (2014), A practical framework for infinite-dimensional linear algebra, Proceedings of the 1st First Workshop for High Performance Technical Computing in Dynamic Languages, 57–62

A. Townsend & S. Olver (2014), The automatic solution of partial differential equations using a global spectral method, J. Comp. Phys., 299: 106–123

S. Olver & A. Townsend (2013), Fast inverse transform sampling in one and two dimensions, arXiv:1307.1223

S. Olver & A. Townsend (2013), A fast and well-conditioned spectral method, SIAM Review, 55:462–489