Chebyshev polynomial approximation to approximate partial differential equations



and has been shown to perform well empirically (Rivlin, 1990). Chebyshev nodes are
also known to possess a further convenient property, i.e. equi-oscillation 3(Judd, 1998).

As important as the choice of the nodes interpolants is that of a family of functions from
which the approximant
P will be drawn. We suggest using a Chebyshev polynomial. This
is defined as4:

Γi(s) = cos(ia cos(s)) i = 0,1,..., n

with Γ0(s)=1,Γ1(s)=s,and Γn+1(s) =2sΓn - Γn-1 (s)

Therefore:

n
V(s)=ciΓi(s)
i=0

(6)


where c0 =


1

n+1


n

V(sk) and
i=0


ci


2n

—∑Vv(sk)cos(iacos(sk)), i = 1,.∙∙,n
n
+ 1 i=0


A Chebyshev basis polynomial, in conjunction with Chebyshev interpolation nodes,
produces an efficient interpolation equation which is very accurate and stable over
n .
However, in our case, to solve the problem in (3), the polynomial we choose should be
able to replicate, not just the function
V at s1,s2,...,sn , but also its derivatives
s1',s2' ,...,sn' . Therefore the approximant that solves our problem can be defined as
follows5:

n

ciΓi(s) =V  (si),i = 1,..., n1

i=1
n

ciΓ'i(s')=V  '(si),i=1,...,n2

i =1

3 This property states that the maximum error of a cubic function, for example, shall be reached at least five
times, and the sign of this error should alternate between the interpolation points.

4 Note that in this application we use the general formula for the Chebyshev basis, however there exists also
a recursive formula.

5 Note that, although one can also use Hermite polynomials to approximate the functional and the slopes,
the latter are inefficient (Judd, 1998).



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