the new fuels with magnecular structure - Institute for Basic Research

102 RUGGERO MARIA SANTILLI
as partially illustrated in Figs. 22 and 29, as well as for all additional MS scans
not reported here for brevity.
III) The above MS peaks characterizing magnecules admit no IR signature,
thus confirming that they do not have a valence bond. In fact, none of the peaks
here considered had any IR signature as partially illustrated in Figs. 23 and 30,
thus confirming the achievement of an essentially pure population of magnecules.
IV) The IR signature of the only molecule detected in macroscopic percentage,
that of the CO 2 , is mutated precisely with the appearance of two additional peaks,
as shown in Fig. 24 and independently confirmed in Fig. 31. Since any peak in the
IR signature represents an internal bond, the mutation here considered confirms
the creation by the PlasmaArcFlow technology of new internal magnetic bonds
within conventional molecules, as per Fig. 11.
V) The anomalous adhesion of magnecules is confirmed in both tests from the
evidence that the background (blank) at the end of the tests following conventional
flushing continued to show the presence of essentially the same magnecules
detected during the tests, as illustrated in Figs. 26 and 32.
VI) The atomic weight of magnecules mutates in time because magnecules can
break down into fragments due to collisions, and then form new magnecules with
other fragments. This feature is clearly illustrated by the macroscopic differences
of the two scans of Figs. 27 and 28 via the same instrument on the same gas
under the same conditions, only taken 30 minutes apart.
VII) Magnecules can accrue or lose individual atoms, dimers or molecules. This
additional feature is proved in the scans of Figs. 27 and 28 in which one can see
that: the peak at 286 a.m.u. of the former becoming 287 a.m.u. in the latter,
thus establishing the accretion of one hydrogen atom; the peak at 302 a.m.u. in
the former becomes 319 a.m.u. in the latter, thus establishing the accretion of
the H–O dimer; the peak at 328 a.m.u. in the former becomes 334 a.m.u. in the
latter, thus establishing the accretion of one O 2 molecule; the peak at 299 a.m.u.
in the former become 297 a.m.u. in the latter, thus exhibiting the loss of one H 2
molecule; etc. It should be indicated that these features have been confirmed by
all subsequent GC-MS/IRD scans not reported here for brevity.
The other features of Definition require measurements other than those via
GC-MS/IRD and, as such, they will be discussed in the next section.
A most forceful implication of the experimental evidence presented in this
section is that it excludes valence as the credible origin of the attractive force
characterizing the detected clusters. This feature is forcefully established by the