Issue 17 - Free-Energy Devices
Issue 17 - Free-Energy Devices
Issue 17 - Free-Energy Devices
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Chemo-electrical gravitational electrolysis by<br />
V. Studennikov<br />
A possibility of a straight transformation of the heat energy to electricity<br />
Makarov Andrei Fadeevich<br />
The senior science associate of the laboratory of safe explosive works at NC VostNII.<br />
Phone: (384-2) – 64-25-85, vostnii@kemnet.ru<br />
Phone: (384-2) -64-05-45.<br />
Russia, 650000002, Kemerovo, 2nd Tulskii per., 5-5.<br />
The article was prepared with the information support of engineer V.P. Lesov.<br />
Saint-Petersburg, valery.lesov@petroscan.ru<br />
Annotation: ideas on possibility of creating a thermal<br />
electronic pump for the straight transformation of the<br />
low potential heat and spreaded energy to the electric<br />
power are being observed here.<br />
Is a utilization of free energy of the environment,<br />
the absolute temperature of which is about 300K<br />
(0C=273K), possible? In thermodynamics, there<br />
is no prohibition on “eternal engines”, working on<br />
the environment’s account. For example, thermal<br />
EDS appears in transistors’ thermal pairs only at<br />
the natural gradient of temperatures in the<br />
environment. In thermal pumps’ work cycles the<br />
“spreaded” low potential heat energy is used. The<br />
photo electronic emission happens at the<br />
electromagnetic radiation of the visible and IRspecters<br />
expense. The photosinsesys process,<br />
happening even in the dark, is natural too. Finally,<br />
the electric hydrogen generator (EHG) of<br />
Studennikov, transforming “free” energy of heat<br />
to the water (H O) dialysis process on hydrogen<br />
2<br />
H , oxygen O and electric power, is known [1].<br />
2 2<br />
The cycle of heat transformation to electric<br />
chemical energy forms is based on gravitational<br />
separation of heavy and light ions in the fast<br />
spinning dilution of electrolyte. For example, in<br />
the water dilution of bromious acid HBrO ) the 3<br />
formatting ions’ H + /BrO - mass proportion is 1/<br />
3<br />
128 (not counting the solvation skins). At a high<br />
enough informational “overload” in the spinning<br />
reactor-centrifuge the heavy negative ions BrO 3<br />
will be throwing away (“drown”) to periphery, and<br />
light protons H + will be pushed out (“float up”)<br />
to the rotation’s axle. Furthermore, when reaching<br />
- + the reactor’s walls (BrO ) or its central axis (H ),<br />
3<br />
the corresponding ions discharge, giving away to<br />
the corresponding electrodes its load, which is<br />
going further to the external chain, and extracting<br />
-<br />
“electrolysis” gases – H and O at the central and<br />
2 2<br />
peripheral electrodes by a scheme: H + +H + = H - 2<br />
2e- - - ; and BrO +BrO3 =Br2O +(1/2)O +2e 3<br />
3 2 - ;<br />
Br O +H O=2HBrO . The transferred<br />
2 3 2 3<br />
environment heat compensates the electric<br />
chemical work of the water gravitolisys reactorcentrifuge.<br />
So, in the EHG cycle the watersolvent,<br />
and hydrogen, oxygen and electric power<br />
are extracted. – only at the heat spreading account.<br />
Only a small part of the generated energy is spend<br />
on the reactor centrifuge’s rotation drive, mostly<br />
on compensation of the friction forces in the<br />
bearings. The water’s presence in the electric<br />
transfer leads to its electrochemical disintegration,<br />
which requires not less than 3200 kkal/kg of the<br />
supplied heat, limits the working diapason of<br />
negative temperatures, it is necessary to dilute the<br />
electrolyte, “electrolysis” gases’ separation and<br />
extortion from the reactor (2H +O ). But let’s look<br />
2 2<br />
at the closed scheme of electric transfer innon-water<br />
self ionized electrolytes. Let the ions’ discharge<br />
happens with a transformation of the charge carriers<br />
into original substances and a full cycle reconnection<br />
in reactor’s volume. Theoretically, gravitolisys is<br />
possible in the condensed, gaseous or plasma phases.<br />
However, the ionization in gaseous and plasma<br />
phases, usually, is possible only at a high enough<br />
temperature (from approximately 10000K, which is<br />
much higher than of the heat equilibrium of the<br />
environment (about 300K). At the same time<br />
some of the metal dilutions in liquid ammonium<br />
are known, with almost cryogenic temperature of<br />
the ionization and freezing of metal-ammonium<br />
eutectics (approximately 90-160K) – at the<br />
expense of the metals and free electrons’ ions<br />
solvation with the solvent-ammonium<br />
molecules(some of the atoms stay in a dissociated<br />
condition) according the schemes [2]:<br />
26 New <strong>Energy</strong> Technologies, <strong>Issue</strong> #3(18) 2004