the new fuels with magnecular structure - Institute for Basic Research
the new fuels with magnecular structure - Institute for Basic Research
the new fuels with magnecular structure - Institute for Basic Research
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THE NEW FUELS WITH MAGNECULAR STRUCTURE 43<br />
The infrared signatures of conventional molecules constituting magnecules are<br />
expected to be mutated, in <strong>the</strong> sense that <strong>the</strong> shape of <strong>the</strong>ir peaks is not <strong>the</strong><br />
conventional one. As indicated in <strong>the</strong> preceding section, <strong>the</strong> mutations most important<br />
<strong>for</strong> industrial applications are those due to <strong>the</strong> presence of <strong>new</strong> IR peaks<br />
representing <strong>new</strong> internal bonds. Never<strong>the</strong>less, various o<strong>the</strong>r <strong>for</strong>ms of IR mutations<br />
are possible.<br />
Feature 5: Mutation of <strong>magnecular</strong> weights.<br />
While molecules preserve <strong>the</strong>ir <strong>structure</strong> and related atomic weight at conventional<br />
temperatures and pressures, this is not <strong>the</strong> case <strong>for</strong> gas magnecules,<br />
which can mutate in time, that is, change <strong>the</strong>ir atomic weight <strong>with</strong> consequential<br />
change of <strong>the</strong> shape and location of <strong>the</strong>ir MS peaks. Since we are referring<br />
to gases whose constituents notoriously collide <strong>with</strong> each o<strong>the</strong>r, magnecules can<br />
break-down during collisions into fragments which can <strong>the</strong>n recombine <strong>with</strong> o<strong>the</strong>r<br />
fragments or o<strong>the</strong>r magnecules to <strong>for</strong>m <strong>new</strong> clusters.<br />
Feature 6: Accretion or emission of individual atoms, dimers or<br />
molecules.<br />
Magnecules are expected to experience accretion or emission of individual<br />
atoms, dimer or molecules <strong>with</strong>out necessarily breaking down into parts. It follows<br />
that <strong>the</strong> peaks of Feature 1 are not expected to remain <strong>the</strong> same over a<br />
sufficient period of time <strong>for</strong> <strong>the</strong> same gas under <strong>the</strong> same conditions.<br />
Feature 7: Anomalous adhesion.<br />
Magnetically polarized gases have anomalous adhesion to walls of disparate<br />
nature, not necessarily of paramagnetic character, as compared to <strong>the</strong> same unpolarized<br />
gas. This is due to <strong>the</strong> well-known property that magnetism can be<br />
propagated by induction, according to which a magnetically polarized molecule<br />
<strong>with</strong> a sufficiently intense magnetic moment can induce a corresponding polarization<br />
of valence and/or o<strong>the</strong>r electrons in <strong>the</strong> atoms constituting <strong>the</strong> wall surface.<br />
Once such a polarization is created by induction, magnecules can have strong<br />
magnetic bonds to <strong>the</strong> indicated walls. In turn, this implies that <strong>the</strong> background<br />
of GC-MS following scans and conventional flushing are often similar to <strong>the</strong> scan<br />
<strong>the</strong>mselves. As a matter of fact, backgrounds following routine flushing are often<br />
used to identify <strong>the</strong> most dominant magnecules. Notice that <strong>the</strong> magnetic polarization<br />
here considered does not require that <strong>the</strong> walls of <strong>the</strong> instrument are of