APPROXIMATION AND NUMERICAL RESULTS FOR PHASE FIELD SYSTEM BY A FRACTIONAL STEP SCHEME
COSTICÃ MOROŞANU
(Iaşi)
(Iaşi)
1. INTRODUCTION
We consider the phase field system
subject to the Dirichlet boundary conditions and initial conditions
where is a bounded domain in with smooth boundary , and and are as in [9], [11].
Setting
system (1.1)-(1.4) takes the form
Let . Then is a real Banach space with respect to the norm defined by
Define the operator by
and the operator
Thus, system (1.6)-(1.7) can be rewritten in the form
For others settings into the abstract framework of the phase-field equations (1.1)-(1.4) see, e.g., [6], [14].
The idea behind the Lie-Trotter scheme (known as the method of fractional step in numerical approximation of PDE's) is to decompose the original problem into several simpler problems.
Here we associate to system ( ) the following approximating scheme
where is a partition of the time-interval is the right limit of at is. We assume the following convention: .
Recall that is the duality mapping of the space (see, for instance, [2]) and that is:
accretive, if for every pair , there exist such that
accretive, if for every pair
or, equivalently,
where
Another convenient way to define the accretiveness is obtained using the directional derivative of the norm
i.e, (ii) can be equivalently written as
(ii')
(ii')
(see also [2], [15], [16]). Recall that if is a real Hilbert space then (see [16], Remark 1.4.1).
It is well known that, under certain hypotheses on , the Cauchy problem
has a generalized solution given by the exponential formula
for every (a classical result of Crandall-Ligget, sec, e.g., [2]).
This is the sense in which we will treat the problems (1.6)-(1.9) and (1.10)-(1.13).
This is the sense in which we will treat the problems (1.6)-(1.9) and (1.10)-(1.13).
2. CONVERGENCE OF THE APPROXIMATE SCHEME
Let us recall the following result due to Barbu and Iannelli ([5]).
THEOREM 2.1. Let be a real Banach space, let be a closed subset of and be a convex subset of such that
(H1) is -accretive and ;
(H2) is a continuous -accretive operator on such that
THEOREM 2.1. Let
(H1)
(H2)
(H3) ;
(H4) For every , there exists such that
(H4) For every
Then, for every , we have
and the limit is uniform on bounded intervals.
Here, by , we have denoted the generalized solution to the Cauchy problem:
Here, by
and by the solution of the corresponding approximative scheme.
This result is not applicable to the problem (1.10)-(1.13) because we cannot find a subset as in (H2) and such that the operator be continuous on .
This result is not applicable to the problem (1.10)-(1.13) because we cannot find a subset
Therefore, we will replace the operator with another one having all the properties required by Theorem 2.1 and we will show that the approximate solution corresponding to this new operator is in fact an approximate solution corresponding to (see Remark 3.1, below). Namely, we consider the operator . defined by (see also Figure 1)
Fig. 1

where
Substituting in and in (2.12) by we obtain:
We associate to system ( ) the approximating scheme (1.10), (1.11), (2.1) and (1.13).
Now we prove
Proposition 2.1. If and then, the operators . and satisfy all the hypotheses of Theorem 2.1.
Proposition 2.1. If
We shall prove first the following lemma.
Lemma 2.1. If and then is 0 -accretive and satisfies the range condition
Lemma 2.1. If
Proof. Using the definition (ii') we must show that, for every is linear and is univalued, i.e.,
Using Green formula and Cauchy-Schwarz's inequality, we get ( is real Hilbert space)
Since then and then
Thus, because ,
i.e.
Hence is -accretive, with .
Other results with respect to the operator , put into other abstract framework , can be found in [14].
Other results with respect to the operator
It is clear that for every the system
has a unique solution for small (see [1], [4], [7]; is supposed to be, as in Theorem 4.1, pp. 131, [4]). Thus (2.2) is true.
The proof of Proposition 2.1. By Proposition 3.9 pp. 110 ([2]), we have that is -accretive and surjective. Taking into account Lemma 2.1 and because is single valued and the semigroup is differentiable on (see [3]), we remark that all the hypotheses of Theorem 2.1 are fulfilled and therefore the proof of Proposition 2.1 is complete.
Remark 2.1. If we can choose such that , a.e. then
and the solution of the approximate problem ( is in fact the solution of the approximate problem .
3. NUMERICAL RESULTS
We consider and . For the space interval we use the grid with equidistant nodes
Denote by the approximated matrix for , where
As well, we denote by the approximative matrix for where
Using a standard implicit scheme, (1.6)-(1.7) are discretized as
and
where
Setting
Setting
(3.1) and (3.2) can be rewritten for the level of time , in matrix form
with , of dimension, given by
and .
Let denote the vector-solution for level of time , i.e.
Let
System (3.3) takes the form
where .
Thus we have to solve the nonlinear system
Thus we have to solve the nonlinear system
Using the Newton iterative method to solve it, we have
where
Using an implicit scheme and the Newton iterative method, we obtain from (2.1)
where
Using the very same way of discretization and implicit scheme, the approximative version of (1.10) is given by
and
with .
For fixed , the computation of the approximate solution by fractional step method can be illustrated as in Figure 2
For fixed

Fig. 2
and, the numerical algorithm to calculate it, can be obtained by the following sequence
next
sol:
sol:
Solve the linear system (3.7)
where itmax is the number of iterations, prescribed, eps is the accuracy desired and (respectively ) denote the approximated solution for (respectively .
For the numerical tests we consider:
The initial value

Fig. 3
and the initial value is the solution of stationary equation , i.e the solution of the following equation (see Figure 4 for )

Fig. 4
(see also [10] or [12]).
We observe that and thereby if we choose
then , and then .
In Table 1 there are given some numerical tests executed on a PC 386SX computer with math coprocessor.
We observe that
then
In Table 1 there are given some numerical tests executed on a PC 386SX computer with math coprocessor.
Table 1
| The CPU-time spent by fractional step method | The CPU-time spent by iterative Newton method (3.5) | M | N | |
| 1 | 83 hund | 1" 10 hund | 17 | 17 |
| 2 | 5" 11 hund | 7" 42 hund | 17 | 37 |
| 3 | 8" 89 hund | 11"26 hund | 27 | 37 |
| 4 | 11" 37 hund | 15" 92 hund | 37 | 37 |
| 5 | 14" 94 hund | 47 | 37 |
For , Figures 3 and 4 show the approximate solution while For , Figures 3 and 4 show the approxim .

Fig. 5
Fig. 5

Remark 3.1. i) Because , then is the approximate solution for the operator .
ii) Let us point out that that the choosing of the value is limited only by the arithmetic of the computer (the epsilon-machine).
ii) Let us point out that that the choosing of the value
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Received 15.09.1995
Department of Mathematics University of Iasi 6000 Iasi Romania
Fig. 6
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