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 39<br />
By denoting <strong>with</strong> <strong>the</strong> arrow ↑ <strong>the</strong> vertical magnetic polarity North-South and<br />
<strong>with</strong> <strong>the</strong> arrow ↓ <strong>the</strong> vertical polarity South-North, and by keeping <strong>the</strong> study<br />
at <strong>the</strong> absolute zero degree temperature, when exposed to <strong>the</strong> above indicated<br />
extreme magnetic fields, <strong>the</strong> hydrogen molecule H–H can be polarized into such<br />
a <strong>for</strong>m that <strong>the</strong> orbit of <strong>the</strong> isoelectronium is in a plane <strong>with</strong> resulting <strong>structure</strong><br />
H ↑ −H ↓ (Fig. 7).<br />
The elementary hydrogen magnecule can <strong>the</strong>n be written<br />
{H a ↑ −Hb ↓ } × {Hc ↑ −Hd ↓ }, (2.15)<br />
where: a, b, c, d denote different atoms; <strong>the</strong> polarized hydrogen atom H a ↑ is<br />
bonded magnetically to <strong>the</strong> polarized atom H c ↑ <strong>with</strong> <strong>the</strong> South magnetic pole of<br />
atom a bonded to <strong>the</strong> North pole of atom c; and <strong>the</strong> North polarity of atom b<br />
is bonded to <strong>the</strong> South polarity of atom d (see, again, Fig. 11.A). This results<br />
in a strong bond due to <strong>the</strong> flat nature of <strong>the</strong> atoms, <strong>the</strong> corresponding mutual<br />
distance being very small and <strong>the</strong> magnetic <strong>for</strong>ce being consequently very large.<br />
Moreover, unlike <strong>the</strong> case of <strong>the</strong> unstable clusters due to electric polarization<br />
discussed in Sect. 2.1, <strong>the</strong> above magnetic bonds are very stable because motions<br />
due to temperature apply to <strong>the</strong> bonded couple (2.15) as a whole.<br />
For o<strong>the</strong>r magnecules we can <strong>the</strong>n write<br />
or, more generally<br />
{H ↑ −H ↓ } × {C ↑ −O ↓ }; (2.16)<br />
{H ↑ −H ↓ } × H ↓ × {C ↑ −O ↓ } × {H ↑ −O ↓ } × {H ↑ −C ↓ −A−B−C . . . }×. . . , (2.17)<br />
where A, B, and C are generic atoms in a conventional molecular chain and <strong>the</strong><br />
atoms <strong>with</strong>out an indicated magnetic polarity may indeed be polarized but are<br />
not necessarily bonded depending on <strong>the</strong> geometric distribution in space.<br />
Magnecules can also be <strong>for</strong>med by means o<strong>the</strong>r than <strong>the</strong> use of external magnetic<br />
fields. For instance, magnecules can be produced by electromagnetic fields<br />
<strong>with</strong> a distribution having a cylindrical symmetry; or by microwaves capable of<br />
removing <strong>the</strong> rotational degrees of freedom of molecules and atoms, resulting<br />
in magnetic polarizations. Similarly, magnecules can be <strong>for</strong>med by subjecting a<br />
material to a pressure that is sufficiently high to remove <strong>the</strong> orbital rotations.<br />
Magnecules can also be <strong>for</strong>med by friction or by any o<strong>the</strong>r means not necessarily<br />
possessing magnetic or electric fields, yet capable of removing <strong>the</strong> rotational degrees<br />
of freedom <strong>with</strong>in individual atomic <strong>structure</strong>s, resulting in consequential<br />
magnetic polarizations.