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Chapter 8. Chebyshev spectral methods

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<strong>8.</strong>2. CHEBYSHEV DIFFERENTIATION MATRICES TREFETHEN 1994 269<br />

<strong>8.</strong>2. <strong>Chebyshev</strong> di erentiation matrices<br />

[Just a sketch]<br />

From now on \<strong>Chebyshev</strong> points" means <strong>Chebyshev</strong> extreme points.<br />

Multiplication by the rst-order <strong>Chebyshev</strong> di erentiation matrix DN transforms a vector of data at the <strong>Chebyshev</strong> points into approximate derivatives<br />

at those points:<br />

2 3 2 3<br />

v0 w0 D N<br />

6<br />

4<br />

.<br />

v N<br />

7<br />

5 =<br />

6<br />

4<br />

.<br />

w N<br />

As usual, the implicit de nition of D N is as follows:<br />

CHEBYSHEV SPECTRAL DIFFERENTIATION BY POLYNOMIAL INTERPOLA-<br />

TION.<br />

(1) Interpolate v by a polynomial q(x)=q N (x)<br />

(2) Di erentiate the interpolant atthe grid points x j :<br />

7<br />

5 :<br />

w j =(D Nv) j = q 0 (x j): (8:2:1)<br />

Higher-order di erentiation matrices are de ned analogously. From this<br />

de nition it is easy to work out the entries of D N in special cases. For N =1:<br />

For N =2:<br />

x =<br />

2<br />

3<br />

7<br />

x =<br />

6<br />

4 1<br />

5 D1 =<br />

;1<br />

2<br />

6<br />

4<br />

1<br />

3<br />

7<br />

0<br />

7<br />

5<br />

;1<br />

D2 =<br />

2<br />

6<br />

4<br />

2 1<br />

6 2 ;<br />

4<br />

1 2<br />

1<br />

2 ; 1 3<br />

7<br />

5:<br />

2<br />

3 2 ;2 1 2<br />

3<br />

7<br />

1<br />

2 0 ; 1 2<br />

; 1 2 2 ; 3 7<br />

5<br />

2<br />

:

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