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the new fuels with magnecular structure - Institute for Basic Research

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140 RUGGERO MARIA SANTILLI<br />

Figure 57. A conceptual rendering of a perspective view of <strong>the</strong> central hypo<strong>the</strong>sis submitted<br />

<strong>for</strong> <strong>the</strong> first time in this section via Fig. 55, better illustrating <strong>the</strong> bond via opposing magnetic<br />

polarities of <strong>the</strong> two H-atoms, as well as <strong>the</strong> unstable character of <strong>the</strong> configuration due to<br />

collision <strong>with</strong> o<strong>the</strong>r species and intrinsic instabilities to be studied in a <strong>for</strong>thcoming section.<br />

The plausibility of <strong>the</strong> <strong>new</strong> <strong>for</strong>m of water is supported by <strong>the</strong> fact that, when<br />

H − O − H is liquid, <strong>the</strong> <strong>new</strong> species (H × H) − O is expected to be gaseous. This<br />

is due to various reasons, such as <strong>the</strong> fact that <strong>the</strong> hydrogen is much lighter than<br />

<strong>the</strong> oxygen in <strong>the</strong> ratio 1 to 16 amu. As a result, <strong>the</strong> <strong>new</strong> species (H × H) − O is<br />

essentially equivalent to ordinary gaseous oxygen in con<strong>for</strong>mity <strong>with</strong> conventional<br />

<strong>the</strong>rmodynamical laws, since <strong>the</strong> transition from <strong>the</strong> liquid to <strong>the</strong> gas state implies<br />

<strong>the</strong> increase of <strong>the</strong> entropy, as well known.<br />

Alternatively, <strong>the</strong> loss of electric polarization in <strong>the</strong> transition from H − O − H<br />

to (H × H) − O is expected to cause <strong>the</strong> loss of <strong>the</strong> processes permitting <strong>the</strong> very<br />

existence of <strong>the</strong> water molecule, such as <strong>the</strong> hydrogen bridges between dimers<br />

O − H of different molecules. Transition to a gaseous <strong>for</strong>m is <strong>the</strong>n consequential,<br />

thus confirm <strong>the</strong> plausibility of <strong>the</strong> <strong>new</strong> <strong>for</strong>m of water (H × H) − O proposed in<br />

this section.<br />

However, it can also be seen that <strong>the</strong> <strong>new</strong> <strong>for</strong>m of water (H × H) = O is<br />

unstable, and decomposes in H × H and O. This decomposition is supported by

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