To be realistic, a model of explosion must reproduce a certain number of observational characteristics:
The composition of ejecta and the particular speeds observed in
the spectra and the lightcurves. In particular, the explosion must
be sufficiently powerful (it must produce Ni sufficient)
and produce sufficient elements of intermediate mass high speed in the
external layers. Moreover, isotopic abundances should not be very
different from those observed in the solar system.
The process of explosion must be robust in order to reproduce the homogeneity of the supernovæ Ia communes; the models should not be very dependent on the parameters of the explosion or the initial conditions.
The power of the explosion must be dependent causalement with the state in which was the dwarf white one before the explosion in order to account for the variations observed according to the stellar population of the galaxy host.