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Untitled - Cdm.unimo.it

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Derivative Matrices 129<br />

Similarly, for the Chebyshev and Laguerre cases, we respectively get<br />

(7.1.16) c (1)<br />

i<br />

(7.1.17) c (1)<br />

i<br />

⎧<br />

0 if i = n,<br />

=<br />

⎪⎨ 2ncn<br />

⎪⎩<br />

c (1)<br />

i+2 + 2(i + 1)ci+1 if<br />

if i = n − 1,<br />

1 ≤ i ≤ n − 2,<br />

1<br />

2 c(1)<br />

2 + c1 if i = 0,<br />

=<br />

⎧<br />

⎨ 0 if i = n,<br />

⎩<br />

0 ≤ i ≤ n − 1.<br />

c (1)<br />

i+1 − ci+1 if<br />

The Herm<strong>it</strong>e case has already a simplified form given by (7.1.13).<br />

7.2 Derivative matrices in the physical space<br />

Here we consider Pn−1, n ≥ 2, to be generated by the basis of Lagrange polynomials<br />

{l (n)<br />

j }1≤j≤n introduced in section 3.2. In view of (3.2.2), the derivative of a polynomial<br />

p ∈ Pn is obtained by evaluating<br />

(7.2.1)<br />

In particular, we have<br />

d<br />

p =<br />

dx<br />

(7.2.2) p ′ (ξ (n)<br />

i ) =<br />

n<br />

j=1<br />

n<br />

j=1<br />

p(ξ (n)<br />

j ) d<br />

dx l(n)<br />

j .<br />

d (1)<br />

ij p(ξ(n)<br />

j ), 1 ≤ i ≤ n,

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