New Energy Technologies Magazine nr 3 2005.pdf - Index of

the water heating are evidently insufficient for
producing such a result.
Using a usual and rather plausible
calorimeter procedure, a measured increase
of the quantity of heat produced by the
generator per unit of time can considerably
exceed a measured energy consumed by the
generator during the same period of time.
Efficiency of the heating becomes specially
notable if a temperature of an initial water
subjected to mechanoactivation is (66.5 3.5)C,
[3], [4], [5]. Energy inputs for the water heating
with initial temperature t = 66.5C are minimal
and obviously inequivalent to the heat quantity,
which is required for this.
Such facts require an explanation, therefore,
different, sometimes rather unexoected
hypotheses about “the reasons of the extraproductivity
of hydro-dynamic
heatgenerators” have been suggested.
For example, according to work [49],
production of the excessive heat is connected
with the theory of world aether. It is also
suggested naming the heat production effect
after V.A. Kochetkov, who considers this effect
as a merely aether effect. A supporting data is
provided.
In work [14], on the basis of the the virial law
proven already by R. Klausis, it is affirmed that
any accelerated rotation motion of an actuating
body must be accompanied by a discharge of a
part of its self-energy in the form of heat and,
therefore, by a temperature increase.
In work [50], it is suggested that one of the
reasons of the excessive heat can be chemical
reactions of the actuating body – water and its
solutes – stimulated by an influence of
hypothetical torsion fields.
In article [51], the excessive heat is considered
as an emanation of the energy of physical
vacuum (!); in work [52] it is considered as a
result of cold fusion using exotic anions and
ersions; and in above mentioned work 48, it is
considered as an influence of the “cosmological
vector potential”. However, if we take into
account a possibility to "deceive” a supply
meter by a thyristor transducer, which
increases a frequency of a current supplied to
the pump drive (a know-how of a “pioneer”,
Mr. Potapov), everything becomes more than
simple!
2. Mechanoactivation
Researches of the mechanoactivated water’s
properties have being carried out for quite a
long time [53], [54], [55].
It has been found out that many of liquid’s
physical qualities can reversibly change as a
result of a liquid’s mechanical treatment. For
example, numerical values of relative statistical
dielectric penetrability ε, heat capacity C, light
refraction coefficient n and others of the
mechanoactivated water can considerably
differ from reference values [56], which
characterize usual water.
One of the most important reasons of such
differencies are cavitation effects
accompanying the liquid’s mechanoactivation.
Due to the fact that surfaces of cavitation
cavities are borders of phases’ division, nearsurface
layers of the liquid near the borders of
the division are in a mechanical stress, which
significantly differs from a state of free liquid.
Under a developed cavitation, a relative volume
of near-surface layers of the liquid becomes
rather big: there are from 10 3 to 10 5 of steamgas
pulse cavitation bubbles with an average
diameter of about 10 mkm each in each milliliter
of the cavitating liquid.
Due to this, physical properties of the
mechanoactivated cavitating liquid always
depend on its properties in the near-surface
layers.
According to the dependencies shown on Fig.
4, it is obvious that dielectric penetrability of
water ε in a thin film or a drop, beginning with
thickness of the film d o
or diameter of the drop
D o
, becomes considerably less than a
penetrability of water in a free volume.
In the event of a decrease of water flat layer’s
thickness d from 40 to 10 mkm, its relative
dielectric penetrability permanently diminishes
from nominal value ε = 81 to value ε = 10 3, i.e.
it diminishes up to almost an order of
32 New Energy Technologies #3(22) 2005