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Untitled - Cdm.unimo.it

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118 Polynomial Approximation of Differential Equations<br />

Proof - Expand all the squared norms in (6.6.10) (or (6.6.11)) in terms of the inner<br />

product in L 2 w(I) and recall (6.2.5).<br />

Another characterization of the aliasing error is given by (see (3.3.1) and (6.2.11))<br />

<br />

∞<br />

<br />

∞<br />

=<br />

(6.6.12) Aw,nf = Iw,n(f − Πw,n−1f) = Iw,n<br />

k=n<br />

ckuk<br />

k=n+1<br />

ck(Iw,nuk),<br />

where ck, k ∈ N, are the Fourier coefficients of f and uk = P (α,β)<br />

k , k ∈ N. The<br />

last equal<strong>it</strong>y in (6.6.12) follows by observing that, for any n ≥ 1, Iw,n is a continuous<br />

operator in C 0 ( Ī) (see section 6.8). A similar relation holds for Ãw,nf. In the Chebyshev<br />

case, the formula (6.6.12) takes a simplified form, thanks to the periodic<strong>it</strong>y of the cosine<br />

function, i.e.<br />

(6.6.13) Aw,nf =<br />

n−1 <br />

∞<br />

m=1 j=1<br />

(c2jn+m − c2jn−m)Tm.<br />

Moreover, we note that Aw,nTjn ≡ 0, ∀j ≥ 1. A discussion of the effects of the aliasing<br />

error in the computation of solutions of boundary value problems are given in canuto,<br />

hussaini, quarteroni and zang(1988).<br />

We analyse now the case when I is not bounded. Let us start w<strong>it</strong>h the Laguerre<br />

approximations (w(x) = x α e −x , α > −1, x ∈ I =]0,+∞[).<br />

Theorem 6.6.3 - Let δ ∈]0,1[ and let f ∈ C 0 ( Ī) satisfy limx→+∞ f(x)e −δx = 0.<br />

Then we have<br />

(6.6.14) lim<br />

n→+∞ f − Iw,nf L 2 w (I) = 0.<br />

The same relation holds for the error f − Ĩw,nf, relative to the Gauss-Radau interpo-<br />

lation operator.<br />

Proof - For any pn ∈ Pn−1, we have (compare w<strong>it</strong>h (6.6.2))<br />

(6.6.15) f − Iw,nf L 2 w (I) ≤ f − pn L 2 w (I) +<br />

⎛<br />

⎝<br />

n<br />

(pn − f)<br />

j=1<br />

2 (ξ (n)<br />

j ) w (n)<br />

j<br />

⎞<br />

⎠<br />

1<br />

2<br />

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