skade eaction ffusion ne-dimensional System - ZIB
skade eaction ffusion ne-dimensional System - ZIB
skade eaction ffusion ne-dimensional System - ZIB
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haper<br />
ntroduction<br />
Usng the program KARDOS, sysems of semli<strong>ne</strong>ar parabolic initial boundary<br />
value problems of the for<br />
{x)ut ~ {D{X)U) F(u X G 0 C R\ t G [t t<br />
Ci(, ^GTiCön<br />
un + a(x)u £2(^ x x £ T2 C df<br />
u(tx) = u0(x<br />
are solvable. Here, u = (u u2,... ur) is a vector function The matrix<br />
function P(x) may vanish on subset of ft. The discretizaton is do<strong>ne</strong> by<br />
the Rothe method. In contrast to he widespread method of li<strong>ne</strong>s, time is<br />
discretized first than space. The main advantage of this sequence is the<br />
possibility o compute the pace discretizaton optimal during the time integration<br />
b an adaptiv multileve finite element method. Therefore the<br />
KASKADE toolbox is modified to handle o<strong>ne</strong>-<strong>dimensional</strong> problems. In<br />
KARDOS a special embedded Runge-Kutta method of order 32) has bee<br />
implemented. This method keeps its accuracy even in the case of ifferenial<br />
algebraic equations (P(x) = 0 somewhere).<br />
The above differetial equations can be reformulated into an abstract Cauchy<br />
problem poibl of differenal-algebraic type in an appropriate Hilbrt<br />
pace H<br />
Pu f(u u G H ,t e[tt<br />
u(0) = u0<br />
Now, a three-stage embedded Rosenbroc ethod for his pure tim problem<br />
looks as follows:<br />
{P ~ 7" r /«(«o))A;8 = r/(u0 + Yl a<br />
1.<br />
) + T f{uo Y l i = 1 3<br />
3=1 J=<br />
Uo +<br />
u0 + Y<br />
3 =<br />
1.3)