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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

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