Z. Bilicki et J. Kestin, REASONS FOR THE OCCURRENCE OF SPURIOUS SOLUTIONS IN 2-PHASE FLOW CODES, Nuclear Engineering and Design, 149(1-3), 1994, pp. 11-15
This paper discusses the mathematical models used as a basis for the c
alculation of critical conditions in two-phase flow. In practice, solu
tions are obtained with the aid of discretized versions of such models
. It has now been established that the portrait of solutions in the ph
ase space of any analytic model does not stand in a one-to-one relatio
n to the map of solutions of any discretized version of such a model.
As a result, computer outputs may develop spurious solutions. Branches
of such spurious solutions often depart from the correct analytic sol
ution in a haphazard manner, and bear no relation to the correct solut
ion. Such degenerate solutions do not differ from their correct counte
rparts by merely containing acceptable numerical or truncation errors,
but fail to fit the correct solutions even approximately. In the case
of the most common analytic models used in two-phase flows through ch
annels of varying cross-sectional areas, spurious solutions develop wh
en the correct solution passes through or close to the saddle point in
phase space. The paper examines two modes of obtaining critical-flow
solutions. In some cases, a steady-state version (partial derivative p
artial derivative t = 0) of the more general model is used. In other c
ases, the full equation (partial derivative/partial derivative t not e
qual 0) is used, and the solution contains a transient but converges t
o the steady-state mode. This paper shows that the implied critical cr
oss-section locations are identical in either mode of operation. The r
eason for the occurrence of spurious solutions is found in a term whic
h assumes the indeterminate singular form 0/0 in the steady-state vers
ion of the model. By a suitable transformation, it is shown that this
term is also present in the factor of partial derivative sigma/partial
derivative t in the time-dependent version. It has been shown earlier
that solutions passing through the singular point can be obtained wit
h the aid of the theory of dynamical systems. In order to exclude the
possibility of the appearance of spurious solutions, the numerical cod
e, in either version, must be so arranged as to start the integration
with the singular point.