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Examples 275<br />

cond<strong>it</strong>ions U(±1,t) = 0, t ∈ [0,T]. Finally, an in<strong>it</strong>ial cond<strong>it</strong>ion U(x,t) = U0(x), x ∈ Ī,<br />

is provided. A conservation property is immediately obtained by noting that<br />

(12.3.2)<br />

<br />

d<br />

|U|<br />

dt I<br />

2 (x,t) dx =<br />

<br />

= i ζ U<br />

I<br />

∂2Ū ∂x2 + ǫ |U|4 − ζ Ū ∂2U ∂x<br />

<br />

I<br />

<br />

U ∂Ū<br />

∂t<br />

2 − ǫ |U|4<br />

<br />

∂U<br />

+ Ū (x,t) dx<br />

∂t<br />

<br />

(x,t) dx = 0, ∀t ∈]0,T],<br />

where the upper bar denotes the complex conjugate and we used integration by parts.<br />

This means that the quant<strong>it</strong>y <br />

I |U|2 (x,t)dx is constant w<strong>it</strong>h respect to t. Another<br />

quant<strong>it</strong>y which does not vary w<strong>it</strong>h respect to t is <br />

ζ <br />

∂U <br />

∂x<br />

2 − ǫ<br />

2 |U|4<br />

<br />

(x,t)dx.<br />

We denote by V and W the real and imaginary parts of U respectively, hence<br />

U = V + iW. Thus, we rewr<strong>it</strong>e (12.3.1) as a system<br />

(12.3.3)<br />

w<strong>it</strong>h<br />

⎧<br />

⎪⎨<br />

⎪⎩<br />

− ∂W<br />

∂t (x,t) = −ζ ∂2 V<br />

∂x 2 (x,t) − ǫ |U(x,t)|2 V (x,t)<br />

∂V<br />

∂t (x,t) = −ζ ∂2 W<br />

∂x 2 (x,t) − ǫ |U(x,t)|2 W(x,t)<br />

(12.3.4) V (±1,t) = W(±1,t) = 0, t ∈ [0,T].<br />

I<br />

x ∈ I, t ∈]0,T],<br />

The in<strong>it</strong>ial cond<strong>it</strong>ions are V (x,0) = V0(x), W(x,0) = W0(x), x ∈ Ī, U0 = V0 + iW0.<br />

For the approximation we use the collocation method based on the Legendre Gauss-<br />

Lobatto points for the variable x, and an implic<strong>it</strong> fin<strong>it</strong>e-difference scheme for the variable<br />

t (see section 10.6). The in<strong>it</strong>ial polynomials in P 0 n, n ≥ 2 (see (6.4.11)) are such that<br />

p (0)<br />

n := Ĩw,nV0 and q (0)<br />

n := Ĩw,nW0 , where the interpolation operator is defined in<br />

section 3.3 (w ≡ 1). We subdivide the interval [0,T] in m ≥ 1 equal parts of size<br />

h := T/m. The successive polynomials p (k)<br />

n , q (k)<br />

n ∈ P 0 n, 1 ≤ k ≤ m, are determined at<br />

the nodes η (n)<br />

i , 1 ≤ i ≤ n − 1, by the formulas

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