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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88 RUGGERO MARIA SANTILLI<br />
thus being able at that time to <strong>for</strong>m molecules <strong>with</strong> exo<strong>the</strong>rmic reactions of type<br />
(2.5). In <strong>the</strong> event magnecules would not contain dimers and atoms, <strong>the</strong>ir only<br />
possible constituents are conventional molecules, in which case no excess energy<br />
is possible during combustion.<br />
The large differences of MS peaks in <strong>the</strong> two tests at NTS and at PCFL of<br />
exactly <strong>the</strong> same gas in exactly <strong>the</strong> same range from 40 to 500 a.m.u., even though<br />
done <strong>with</strong> different GC-MS/IRD equipment, illustrates <strong>the</strong> importance of having<br />
a ramp time of <strong>the</strong> order of 26 minutes. In fact, sixteen different peaks appear in<br />
<strong>the</strong> MS scan following a ramp time of 26 minutes, as illustrated by Fig. 21, while<br />
all <strong>the</strong>se peaks collapsed into one single peak in <strong>the</strong> MS scan of Figs. 27 and 28,<br />
because <strong>the</strong> latter were done <strong>with</strong> a ramp time of about 1 minute. There<strong>for</strong>e, <strong>the</strong><br />
collapse of <strong>the</strong> sixteen peaks of Fig. 21 into <strong>the</strong> single large peak of Figs. 27 and<br />
28 is not a feature of magnecules, but ra<strong>the</strong>r it is due to <strong>the</strong> insufficient ramp<br />
time of <strong>the</strong> instrument.<br />
4.7 Anomalous Energy Balance of Hadronic Molecular<br />
Reactors<br />
As is well known, <strong>the</strong> scientific efficiency of any equipment is under-unity in <strong>the</strong><br />
sense that, from <strong>the</strong> principle of conservation of <strong>the</strong> energy and <strong>the</strong> unavoidable<br />
energy losses, <strong>the</strong> ratio between <strong>the</strong> total energy produced and <strong>the</strong> total energy<br />
used <strong>for</strong> its production is smaller than one.<br />
For <strong>the</strong> case of magnegas production, <strong>the</strong> total energy produced is <strong>the</strong> sum of<br />
<strong>the</strong> energy contained in magnegas plus <strong>the</strong> heat acquired by <strong>the</strong> liquid, while <strong>the</strong><br />
total energy available is <strong>the</strong> sum of <strong>the</strong> electric energy used <strong>for</strong> <strong>the</strong> production of<br />
magnegas plus <strong>the</strong> energy contained in <strong>the</strong> liquid recycled. There<strong>for</strong>e, from <strong>the</strong><br />
principle of conservation of <strong>the</strong> energy we have <strong>the</strong> scientific energy balance<br />
Total energy produced<br />
Total energy available = E mg + E heat<br />
E electr + E liq<br />
< 1. (4.13)<br />
An important feature of hadronic reactors is that <strong>the</strong>y are commercially overunity,<br />
namely, <strong>the</strong> ratio between <strong>the</strong> total energy produced and only <strong>the</strong> electric<br />
energy used <strong>for</strong> its production, is bigger than one,<br />
E mg + E heat<br />
E electr<br />
> 1. (4.14)<br />
In this commercial calculation <strong>the</strong> energy contained in <strong>the</strong> liquid is not considered<br />
because liquid wastes imply an income, ra<strong>the</strong>r than costing money.