Note : Les descriptions sont présentées dans la langue officielle dans laquelle elles ont été soumises.
PR~P~LSIVE P~EL
The ether propulsion app~ratus is a
system of producing propulsion by the use of
electro magnetic energy. It is based upon my
discovery that at the sharp end of any
conducting wire, connected to high voltage
electricity, there exists a propulsive force
which tends to move the wire in space. In a
system where hundreds of millions of sharp
conducting wires, are point in unified
direction, which are connected to an ultra
high voltage source, each point producing a
amall propulsive force, enables this system to
produce a total propulsive force large enough
to move an object in space. This system is
pollution free, noise free, and simultaneously
efficient, economical and dependable.
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The basics oE this invention, long with
typical examples of this invention are
illustr2ted in the accompanying drawings.
Fig. 1 is a side view of suspended wir
connected to a high voltage transformer.
F'ig. 2 i8 the same as figure 1 with the
difference that the end of wire is bent in the
opposite direction.
Fig. 3 is a side view of several indicators
that revolve around high voltage shaft wire.
Fig. 4 is a side view of an indicator.
Fig. 5 is a side elevation of propulsive
system in its, simple form where only -Eew
points have heen shown.
Fig. 6 shows a section line of II II of Fig.
5.
Fig. 7 shows the point and their connecting
link.
Fig. 8 i6 a side view of Fig 7.
F'ig. 9 is a graph showing relation between
voltage and the motive force.
Fig 10 is a side elevation of a suspended
panel with a large number of points connected
to 300,000 volts electricity which causes the
panel to move and rest at an angle.
Fig. 11 is a side view of the panel shown on
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Fig. lOo Here the panel is being weighted at
an angle.
Fig. 12 shows a large number of the points
under a magnifier.
Fig. 13 Shows a section line of II-II of Fig.
12 .
Fig. 14 shows the side view of some examples
of the shape of the insulating material
covering the points.
Fig. 15 shows a side view of some examples of
the shape of the points.
Fig. 16 shows the side view of some examples
of the position of the propulsive points
within insulation.
Fig~ 17 diagrammatically illustra-tes a rever~e
propulsive panel and its connection to the
output of high voltage transformer.
Fig. 18 diagrammatically illustrates a
propulsive panel and its connection to the
output of high voltage transformer.
Fig~ l9 diagrammatically illustrates a
propulsive point with charge collector.
Fig. 20 diagramma-tically illustrates a
propulsive panel with charge collector and it~
connections to independent transformers~
Fig. 2l shows side elevation of a few
propulsive panels being permanently positioned
side by side on the top surface of an object.
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PROPULSIVE P~N~LS
The following experiment illustrates my
discovery of electron-magnetic propulsion that
provides the basi~ upon which the P.P.S. is
designed.
~XPERIMENT NO~ 1
A piece of very fine copper wire 30,
about 1 metre long is suspended in the air,
one end which is connected to one line of a
transformer 31 with an output of about 15,000
volts and a current output capacity of about
30 milliamps, Figure No. 1. Down at the other
end of the wire section about 2 cm. long is
bent toward the left.
When the switch 32 i~ open and there i~
no electricity in the fine wire, the end B
which can swing to the right or left, is at
its rest equllibrium position E. However, the
moment the switch 32 is closed and the fine
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wire is connected to the high voltage
electricity, the end B ~wing~ to the right
rapidly and then rests at a new equilibrium
position N.
If we repeat this experiment, this time
with the difference that the end of the wire
is bent toward the right instead of the left
(see Figure 2). When we close the switch this
time the ed B will move to the left, (exactly
opposite to that of the previous experiment),
and then it rests at a new equilibrium
position of ~ and as long as the switch is
kept closed the end B will remain at that
point until the switch is open then it wi.ll
return to its original position E~
If we repeat the above experiment many
times in which the end oE the fine wire is
bent in different directions, we find that, in
all cases, the movement of the 0nd B is
opposi-te to the direction of the end point o~
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the wire.
The above observations lead us to the
conclusion that at the end point of a fine
conducting wire which is connected to a high
voltage electricity, there exists a propulsive
force which tries to move the wire in space.
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EXPERINENT ~0. 2
A ~traight fine copper wire 35 in Figure
3, is fixed on both ends and serves as a shaft
around which the indicators A to J revolve.
Each indicator is made of fine metal
wire about 10 cm. long and the centre of which
is wound up just few turns around a pin or
needle and then carefully the pin or needle is
removed and both ends are bent 90 degrees in
such a way that both ends are in opposite
directions (Figure No. 4). In Figure 3 these
indicators re positioned at an increased
distance from each other. For example B = 1
cm. C = 1.5 cm. CD - 2 cm. DE = 2.5 cm. EF
= 3 cm. FG = 3.5 cm. CH = 4 cm. HI = 4.5
cm. and IJ = 5 cm. I~ we connect one end o F
the wire 35 to one line of a tran~former 36
with an output of 15,000 volts and a current
output of 30 milliamps and khe ~witch 37 is
closed, the indicators E to J immediately
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begin revolving around the shaft wire rapidly,
the indicators E, F and H in one direction and
the indicators G, I and J in another
direction.
The reason they revolve in different
directions is because the pointed ends of
indicators E, F, H are in opposite direction
to the pointed ends of indicators G, I, U.
The indicators A to E, unlike the others, do
not revolve at all. The reason being, these
indicators are too close to each other and
cancel each other's propulsive force. To
illustrate this, the distances are increased
to 3 cm. and after closing the switch all the
indicators A to J 6tart revolving rapidly;
A C D E F H in one direction, and the
indicators B G I J in another direction.
Repeating the experiment using a 300,000
volt transformer. This time the indicator6
are po~itioned in very close proximity to each
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other. For example As = 2 mm. BC = 2 mm. CD
= 2 mm. EF = 2 mm. FG - 2 mm. GH = 2 mm.
HE = 2 mm. IJ = 2 mm. (Figure 3).
When the switch 37 is closed, all the
indicators begin revolving very rapidly. A~
the indicators turn the distances between them
gradually increases. This shows that beside
the existence of propulsive force described
before there exists another force which tends
to repel the points from each other. Probably
this force was responsible by not letting the
indicator revolved when the voltage was very
low.
T~ EFFECT OF VOLTAOE INCREASE ON T~E AMOUN
OF PROPULSION
If we, again, repeat the experiments with
the difference that we increase the voltage,
we find that by observing the movement of the
end B, its speed and measuring the distance of
displacement, the amount of propulsion
produced at the end of the wire is also
increased. After repeating the experimen~
with different voltages I have found that the
amount of propulsion produced is directly
proportional to the voltage supplied. See
figure 9.
For example, in previous experiments, the
voltage of 15,000 volts produced a propulsion
of .005 gram and a voltage of 30,000 volts
produced .01 gram lift and a voltage of
300,000 volts produced a propulsive force of
.1 gram lift.
At the above voltages the variation of
propulsion with the voltage appears to be a
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straight line.
Assuming the variation of propulsion with
much high voltages continues to be a ~traight
line then the voltage needed to produce a .4
gram lift would be 1,200,000 volts. Looking
at the graph (Figure 9~ we see that there is
the po6sibility that the relation between
propulsion and relatively much higher voltages
could be exponential. In ~uch a case, the
voltage needed to produce a.4 gram lift will
be much lower than 1,200,000 volts.
Furthermore, choosing the right shape of the
points and the right mixture of metals and
oxides and radioactive material will
definitely increase the propulsion.
In order to increase propul~ion at lower
voltages, we may be able to use a charge pump.
A charge pump basically i~ a capacitor with
the difference that each of it~ conducting
plates have, at least, two or more connecting
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lines. It is being charged as capacitor but
discharge by the changed of the polarity of
only one of the conducting plates. Doing so,
creating a sudden charge pressure which is the
result of the presence of charges of the same
sign ~polarity) on all the plates and causing
the excess charges to escape from the
propulsion causing points which are connected
to one of the plates by a connecting line.
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FORCE PER U~IT AREA
On a square wooden panel 20, (Fig. 10) b
cm x 6 cm, total of 750 steel pins 21 were
positioned as in Fig. 10, each point 2 mm.
apart. All the pin~ were connected to each
other by copper wires 40. The said panel was
suspended by two steel piano wires 23 about 9~
long. The piano wires were also connected to
the pins by copper wire~. The ends of the
said piano wires were looped 24. A small
piece of piano wire 25 about 12" long, was
pa~sed through the holes 24 and was made to
serve as a shaft which wires 23 can swing.
The steel wire 25 i6 suspended in the air by
two supporting long cotton strings 26 which
were about 3.7 metres long and the end6 of the
strings were attached to the ceiling 27 which
was about 8 metres high. The shaft 25 was
then connected to only one terminal 28 of a
300,000 volt transformer 31 which was located
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outside of the building and only one terminal
of the high voltage output of the transformer
which was heavily insulated passed through the
centre of the wall. The other terminal of the
high voltage output was not connected to
anything. The distance between the ~uspended
panel and all the surrounding walls, ceiling
or floor were measured to be over 3.8 metre~.
When the switch 32 was closed, the pan~l moved
to the left and rested ~t an angle. This
angle was recordedO The switch was then
opened and at the same recorded angle ~ ) the
panel, from its centre, was positioned on a
scale 30, Fig. 11. The scale showed 78 grams.
Therefore the total orce equivalent to the
measured weight was measured to be 78 grams.
Since 750 pins were used, the average force of
each point was measured to be .104 grams.
If we had used a larger panel, ~or
exampl~, 1 m x 1 m and positioned the points
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every 2 mm apart then we would have a total of
250,000 points covered the surface of the
panel. The force created would have been 26
Kg/m2. Furthermore, if we had increased the
voltage from 300,000 volts to 1,200,000 volts
then the force would have increased to 104
Kg/m2. It is important to note at 1,200,000
volts, the di6tance needed between points
could be reduced to 1 mm. Then in an area of
1 m2 we could have as many as 1,000,000
points and the force created would be 416
Kg/m2 .
In an area 20 metres radius we can have
as many as 1,256,000,000 points, each point 1
mm apar-t and at the voltage of 1,200,000 volts
each point produces .4 gram lift. The total
force created by all the points w.ill be 502.4
ton lift.
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REVERSE PROPUI SIVE PANE:L
I have found that by covering the sharp
section of each point with sufficient
electrical insulating material, the force
created by the points are rever6ed. For
example if we repeat the experiment No.
Figure No. 1, with the difference that the
sharp end of the wire at B i6 covered with
sufficient insulating material. After closing
the switch 32, we find that the end B, instead
of moving to the right, it moves to the left,
which is exactly opposite of the previous
experiment. The same will be true in
experiment shown in Fig. 2, thi6 time the en~
B moves to the right. 1'his shows that the
pre6ence o~ sufficient electrical insulating
material at the tip of the po.int reverses the
direction of the force.
If we repeat the experiment described in
Fig. 9, 10 and 11 with the dif~erence that the
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points are covered by sufficient amount of
insulation, we find that in all cases similar
results are obtained.
Fig. 17 shows a reverse propulsive panel
made of dielectrics 43, within the dielectrics
there embedded in large number of points 41.
These points are directed iIl generally
parallel direction to each other by number of
conducting lines 40 or a metal sheet~ The
sharp end of the points are covered by
sufficient amount of insulation. Fig. 14
shows some examples of the positions of a
point 41 within insulation 43 and at the same
time it shows some examples of the shape of
the insulation covering the points.
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PROP~LSIVE PANEL
I have found also that if we position the
points inside dielectrics in a way that only
a very thin layer of insulation, or nothing at
all, covers ~he sharp end of the points,
neither the amount of the force nor the
direction of the force is affected. ~hi~
shows that the dielectrics can be used to
support and protect the points. The
dielectrics also allows the points to be
closer to each other.
Fig. 16 shows few examples of how the
points could be positioned inside the
electrical insulating material.
Please note tha-t the difference between
propulsive and reverse propulsive points are
the amount of insulation covering the point.
Fig. 18 shows a propulsive panel made of
dielectrics within the dielectric~ there are
embedded in large number of points.
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The panels can have different sizes and
can ~e constructed in a way that its
electrical conducting lines can easily
connected with other panel~.
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PROPULSIVE P~EL WIT~ OEIARGE COLL~.CTOR
Fig. 19 shows a propulsive point with a
charge collector. Here the point is al80
connected to a secondary output of a D.C.
power supply with relatively low output
voltage. The sharp end of the point is
located in close proximity to a conducting
loop which is connected to the secondary power
supply. The loop serves as a charge collector
and thus prevents the build up of any unwanted
negative charge around the points.
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Fig 21 shows a typical example of this
invention, a propulsive panel that can be used
to power an object. The propulsive panel may
have different shapes designing or æizes.
Here only as an example, to illustrate the
invention, the panels are flat and rectangular
with dimensions 30 cm. x 20 cm. x 8 mm. The
panel iæ laid on the surface of the skin of an
object and secured permanently by a number of
screws or nails, or rivet by glue or any other
known method on the surface of the object. If
the objec-t is larye there may be a very large
number of the panels used side by side as in
Fig. 21/ and all the panelæ being connected
together electrically by known techniques and
the said panels permanently posi.tioned by
already known techniques. The panels being
connected to power supplies.
