http://philica.com/display_article.php?article_id=155

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Article body

1. Basics
The existence of the vacuum-energy is nowadays generally accepted. It
is verified by measurements of the expansion of the universe within
physical cosmology [5,6,7,8]. This type of verification of the
vacuum-energy is based on the gravitation caused by the mass connected
with the vacuum-energy, since energy is equivalent to mass.

In the Theory of General Relativity, as the modern theory of the
gravitation, the gravitative effect of vacuum-energy results in the
cosmological constant Λ [9,10,11]. Although the existence of the
vacuum-energy is proven, its energy-density is still unclear today.
The value of the energy-density is regarded as the largest discrepancy
in modern physics. As an average over several literature references of
cosmology, the energy-density can be estimated at about
(9.0±0.27)·10-10J/m3, whereas in Geometrodynamics a value of
h·c·π/Lp4=3.32·10+113J/m3 is suspected [12]. However the latter value
is calculated by an integration over all wavelengths of the quantum
mechanical zero point oscillations within the vacuum (these are
infinitesimally many), whereby divergence problems are suppressed
simply by the means of cut-off radii. Several other approaches to
suppress the divergence problems of these improper integrals (leading
to the energy density) result in further other values for the
energy-density of the vacuum [13,14], but they do not solve the
problem of the ambiguity.

At least the existence of vacuum-energy is beyond dispute, so that it
should be possible to verify this energy in the laboratory. That is
indeed the case. Two possible ways to this proof have been developed,
namely for a metallic rotor in the electrostatic field in [2] and for
a superconducting rotor in the magnetic field in [15]. Since the work
presented here is based on the first mentioned method, this one is
briefly recapitulated in the following lines.

In Fig. 1 a metallic disk (so-called field-source, drawn in red) is
electrically charged and thus it produces an electrostatic field,
which interacts with the rotor (in blue drawn colour), causing an
attractive force, which can be computed with simple elementary methods
of classical electrodynamics, namely with the image-charge-method
[16,17]. This force is well-known, it is the same force, with which an
electrostatically charged plastic ruler attracts paper confetti as
everybody knows from childhood. An other way to understand this
attractive force is, to regard the field-source and the rotor as
opposite plates of a capacitor, which are known to attract each other.
But the crucial point is, that the capacitor plates are not parallel
to each other, so that the force-vectors are somehow diagonal
relatively to the flux-lines of the field. Consequently there is a
component of the force exerting a torque onto the rotor, resulting in
a rotation as soon as the bearing allows the capacitor plates (which
are the rotor blades) to rotate.

The trick is now: During the rotating the distance between the blue
and the red capacitor plate does not change at all, so that the
rotation should be continued endlessly, as long as the capacitor is
electrically charged. In fact this rotation is actually proven
experimentally in [18]. The fact that the experiment of [18] was
carried out in air, led to doubts of physicist colleagues, who
reminded that the rotation could be produced by the recoils of ionized
gas-molecules of the surrounding air [19,20], because the voltage
between the field-source and the rotor can sometimes reach several
10kV. In order to exclude this argument, the experiment was
transferred into the vacuum, in order to avoid gas ions and their
recoils - and the rotor rotated in the vacuum, without being driven by
gas ions [4].

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They go on to describe the experiment performed in a vacuum.  It does
look promising.

Everyone complicates the efficiency calculation by determining power
first.  If you know mechanical torque, the mechanical energy per cycle
is a trivial calculation as is electrical energy per cycle.

Terry

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