The
Electrostatic Pressure in action Experiment by
Jean-Louis Naudin created on
February 18th, 2003 - JLN Labs
- February 20th, 2003 All
informations in this page are published free and are intended for
private/educational purposes and not for commercial applications
This experiment is well known in high
schools ( i.e : See " Electrostatique, Electrocinétique
" by Maurice Ravaille - Collection de Sciences Physiques
dirigée par Marcel Peschard Edition Baillère, page 125
). The basic principle of the Lafforgue's device is to use an
asymmetrical electrostatic pressure for producing a thrust Vs
external referential ( the Universe ), this is fully explained in
his patent. Lafforgue has called this the " Action Force
" or the " Expansion Force ".
The electrostatic pressure is independant of the voltage polarity,
perpendicular to the conductive armature surface
and always towards the
outside of the shape
P = dF / dS = s2/2eo
This experiment shows the electrostatic
pressure in action on a soap bubble.
Experiment description
:
This experiment is very
simple and can be replicated by anyone. You only need to have :
a small
cylindrical container filled with liquid soap ( a bubble
kit for children )
a High Voltage
generator which is able to give about 25 KV DC.
Experiment : The HV output of your power supply is
connected as shown in the diagram above. Then, with the ring,
blow a big bubble, drop it on top of the container and switch on
the HV power supply...
TESTS
RESULTS :
When High Voltage ( +25 KV DC ) is
switched on the soap bubble inflates and leaves the device
upwards only by the electrostatic pressure ( see the photos below
) :
See
the video of the Electrostatic Pressure in action on a soap
bubble
The electrostatic forces
are "generated" by the interaction of
polarised atoms (q) on an electric vector field
(E), i.e. F=q.E, positive or negative according
to the sign of (q). By suitable geometry of the
polarised armatures, and/or by the use of
electric charges induced by induction effect,
and/or by the use of suitably arranged
dielectrics, it becomes possible to break the
symmetry of the expansion forces on one of the
axes of the three-axis reference system and thus
to obtain a non-zero resultant force (Fn). The
isolated system is then propelled, and it draws
the charges (q) and (E) along with it, thus F=q.E
remains constant. This force can be used as a
means of propulsion for any vehicle or even as
motive force for producing energy.
Systèmes
isolés auto-propulsés par des forces
électrostatiques
Les
forces électrostatiques sont " engendrées
" par interaction d'atomes polarisés (q)
sur un champ vectoriel électrique (E), soit F =
q. E positive ou négative selon le signe de (q).
Par une géométrie adaptée des armatures
polarisées, et / ou par l'utilisation de charges
électriques induites par effet d'influence, et /
ou par l'utilisation de diélectriques
convenablement disposés, il devient possible de
rompre la symétrie des forces d'expansion sur
l'un des axes du trièdre de référence et
obtenir ainsi une force résultante ( F n )
non nulle. Le système isolé est alors propulsé
et il entraîne avec lui les charges (q) et (E),
donc F = q. E reste constant. Cette force peut
être utilisée comme moyen de propulsion de tout
engin ou bien comme force motrice pour produire
de l'énergie.
Un très court
extrait de ce brevet ( 55 pages ) : "
Cette disposition permet à tout engin ainsi
équipé, et surtout aéronautique et spatial, de
pouvoir changer de direction extrêmement
rapidement, voire de s'immobiliser, puis de
repartir en sens inverse promptement "