Paper 4 , Section II, 40E

Numerical Analysis | Part II, 2020

(a) For a function f=f(x,y)f=f(x, y) which is real analytic in R2\mathbb{R}^{2} and 2-periodic in each variable, its Fourier expansion is given by the formula

f(x,y)=m,nZf^m,neiπmx+iπny,f^m,n=141111f(t,θ)eiπmtiπnθdtdθf(x, y)=\sum_{m, n \in \mathbb{Z}} \widehat{f}_{m, n} e^{i \pi m x+i \pi n y}, \quad \widehat{f}_{m, n}=\frac{1}{4} \int_{-1}^{1} \int_{-1}^{1} f(t, \theta) e^{-i \pi m t-i \pi n \theta} d t d \theta

Derive expressions for the Fourier coefficients of partial derivatives fx,fyf_{x}, f_{y} and those of the product h(x,y)=f(x,y)g(x,y)h(x, y)=f(x, y) g(x, y) in terms of f^m,n\widehat{f}_{m, n} and g^m,n\widehat{g}_{m, n}.

(b) Let u(x,y)u(x, y) be the 2-periodic solution in R2\mathbb{R}^{2} of the general second-order elliptic PDE

(aux)x+(auy)y=f\left(a u_{x}\right)_{x}+\left(a u_{y}\right)_{y}=f

where aa and ff are both real analytic and 2-periodic, and a(x,y)>0a(x, y)>0. We impose the normalisation condition 1111udxdy=0\int_{-1}^{1} \int_{-1}^{1} u d x d y=0 and note from the PDE 1111fdxdy=0\int_{-1}^{1} \int_{-1}^{1} f d x d y=0.

Construct explicitly the infinite-dimensional linear algebraic system that arises from the application of the Fourier spectral method to the above equation, and explain how to truncate this system to a finite-dimensional one.

(c) Specify the truncated system for the unknowns {u^m,n}\left\{\widehat{u}_{m, n}\right\} for the case

a(x,y)=5+2cosπx+2cosπya(x, y)=5+2 \cos \pi x+2 \cos \pi y

and prove that, for any ordering of the Fourier coefficients {u^m,n}\left\{\widehat{u}_{m, n}\right\} into one-dimensional array, the resulting system is symmetric and positive definite. [You may use the Gershgorin theorem without proof.]

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