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0.8
0.6
0.4
0.2
0
−0.2
−0.4
−0.6
−0.8
−1
0
1
2
3
4
5
6
t
Fig. 4.8 The analytical solution . u D cos.t /; v D sin.t // and the numerical solution . u n ; v n /,in
dashed lines , produced by the implicit Euler scheme ( 4.130 )
An implicit Euler scheme for this system reads
u nC1 u n
t
v nC1 v n
t
D v nC1
D u nC1
;
;
(4.142)
which can be rewritten in the form
u nC1 C t v nC1
u n D 0;
(4.143)
v nC1 t u nC1
v n D 0:
Observe that in order to compute . u nC1 ; v nC1 / based on . u n ; v n /, we need to solve a
nonlinear system of equations. To clarify matters, we study ( 4.143 ) for a fixed value
of n.Let˛ D u n and ˇ D v n . We want to compute x D u nC1 and y D v nC1 .Let
f.x;y/ D x C t y 3 ˛;
g.x; y/ D y t x 3 ˇ:
(4.144)
Then system ( 4.143 ) can be written on the generic form
f.x;y/ D 0;
g.x; y/ D 0:
(4.145)
 
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