06.01.2015 Views

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

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

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.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!