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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.

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