the new fuels with magnecular structure - Institute for Basic Research

50 RUGGERO MARIA SANTILLI
in commercial or academic laboratories. Therefore, the great majority of analytic
laboratories lack the very instrument necessary for a final and unequivocal
identification of a conventional molecules, let alone that of magnecules.
3.3 Unambiguous Detection of Magnecules
Since magnecules have properties very different from those of conventional
molecules, the experimental detection of magnecules requires a special care. In
particular, methods which have been conceived and developed for the detection of
molecules are not necessarily effective for the detection of the different chemical
species of magnecules precisely in view of the indicated differences.
The first indication of a possible gas magnecule is given by MS peaks with large
atomic weight which cannot be explained via conventional molecular hypotheses.
The second indication of a gas magnecule is given by the lack of identification
of said heavy peaks in the MS following a search among all known molecules. A
third indication of a gas magnecule then occurs when said unknown MS peak has
no IR signature, except those of its constituents with much smaller atomic weight,
which occurrence establishes the lack of a valence bond. Final identification of a
gas magnecule requires the knowledge of the method used in the production of
the gas and other evidence.
As it is the case also for molecules, a serious spectrographic analysis of magnecules
requires GC-MS detectors necessarily equipped with IRD, because only
such an instrument permits the direct test of the same peaks under both the
MS and IR scan. Again, if the IRD operates separately from the GC-MS, the
indicated joint inspection is not possible; the IRD can only detect ordinary molecular
dimers; the experimental belief that the MS peak must be a molecule is then
consequential.
As a concrete example verified later on with actual tests, consider the spectrographic
analysis of magnegas. This is a light gas whose heaviest molecule in
macroscopic percentages should be the CO 2 at 44 a.m.u. Consider now an MS
peak of magnegas at 481 a.m.u. It is evident that, while small deviations could
be adapted to quantum chemistry, large deviations of such an order of magnitude
cannot be reconciled with established knowledge in a credible way, thus permitting
the hypothesis that the MS peak in a light gas with 481 a.m.u. can be a
magnecule. The MS scan of the peak soon establishes the impossibility for the
computer to identify the peak among all existing molecules. When the GC-MS is
equipped with IRD, the analyst can scan the same peak with 481 a.m.u. under