Nano dust fusion

http://greentechinfo.eu/wp-content/uploads/2012/01/George_Egely_-_Nano_Dust_Fusion_v7.pdf

Dr. George Egely has developed a form of LENR that is uncommon but may not
be too far off the mark.

His process is an unusual one. The essential ingredients are dusty plasma
made from nano‐size carbon particles and air and some water vapor. In its
simplest version the process works at atmospheric pressure, and at modest
temperatures at 1000 – 3000 º C.

I would like to offer some suggestions for improvement that are inspired by
the work of Rossi, DGT, and Chan et al.

First, lose those hollow quarts balls and the microwave in preference to a
spark plug. The plug is more robust and reliable. It will pump many more
electrons into the plasma due to its high operational voltage then will a
microwave.

Second, add zirconium carbide nano-powder to the dust; the use of this
metal will provide more charge concentration potential to the plasma. The
use of zirconium carbide with a work function of 3.38  and a very high
melting temperature of 3532 °C will thermalize the gamma radiation
associated with the nuclear reactions of LENR by using a coherent proton
surface charge.

I love carbide of a transition metals because of their high melting
temperature and their compatibity with carbon powder. Together with carbon,
a very hot plasma temperature will increase operational reactor hydrogen
envelope temperatures to the highest turbo generation efficiencies possible.

Third, replace the air with a high pressure hydrogen envelope with the
highest pressure possible.

Some of my reactions to important parts of Dr. George Egely narrative:

On page 6:

*My theory of cold fusion centers on charge concentration as the primary
mechanism for shilding the coulumb barrier.*

*In support of this concept from Dr, Egely’s text as follows:*

*Here the more or less familiar rules of quantum mechanics or Q.E.D. rule.
In our opinion, strong interaction and “classical” fusion start to dominate
the process above a certain power density in the middle layer. Sparking is
visible on slow motion films. Obviously, the amplitude of oscillation also
depends on the plasma radius, pressure, and temperature. At the center of
the plasma, the amplitudes should be much higher than those at the outer
wall of the acoustic resonator. (There can be the highest amplitude of a
spherical standing wave). See Fig. 5 for the three layers.*

*Near the center of the plasma sphere (middle layer), charge shielding can
dominate nuclear processes due to the enormous surface charge density of
the dust. Then repulsing charges of like protons can be overcome by the
huge negative charge density of the carbon particles.*

*On the slow motion video records, one can clearly see the appearance of
sudden small sparks en mass. Then the Geiger counter starts to click,
though at moderate levels. At present no one knows what goes on in the
center of the acoustic resonator.*

*In Fig. 6 these simultaneous mechanisms are shown as field amplification
by resonant surface polaritons (Fig. 6/a), direct volumetric polarization
by electron and ion impact (Fig. 6/b), and charge shielding (Fig. 6/c) is
shown, where strong interaction rules (again at a different size level) at
the characteristic size of a nucleon. Obviously these are all hypothetical
mechanisms, as they cannot be observed directly.*

On page 23 (b)

*At higher input energy, the sparking region appears, along a mild degree
of radiation – both x rays and particles. (There is a slight radioactivity
in the exhausted dust and the quartz sphere after the power is switched
off, for a couple of days).*

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