Longitudinal electromagnetic waves, visualisation and measurements

Abstract

The invention relates to an electric sensor (10) for a coherent longitudinal electromagnetic wave emitted by a biological object (1), the sensor comprising a tubular casing (11) comprising a barrel (12) having a front end (13) that is open and a rear end (14) that is closed on the upstream pole of a bipolar switch (15), wherein the downstream pole of the bipolar switch (13) is connected to a potential charge collector (16) made of diamagnetic material, preferably copper. The invention also relates to a system comprising an electrometer designed to co-operate with this sensor (10), and to a measurement method implementing the sensor and the electrometer.

Description

[0001] "Longitudinal electromagnetic waves, visualization and measurements"

[0002] This application incorporates by reference the following provisional patent applications: FR2405605 filed on May 30, 2024, FR2405606 filed on May 30, 2024.

[0003] State of the art

[0004] Patent WO2016196231 A1 describes systems and methods for generating and utilizing scalar longitudinal waves (SLWs). This document presents specific antennas, such as linear monopoles and bifilar coils, designed to transmit or receive these waves. The authors state that these waves can pass through Faraday cages, which would distinguish them from transverse waves.

[0005] Patent WO2016196231 A1 - Systems and methods for generating and utilizing scalar longitudinal waves. This patent describes systems and methods for generating and utilizing scalar longitudinal waves (SLW). It presents specific antennas, such as linear monopoles and bifilar coils, designed to transmit or receive these waves. KR20140011732 clock-wise coil on quartz installed pyramid shape for subtle energy.

[0006] KR20130124726 flexible printed circuit board tesla coil installed shoes.

[0007] W02013155580 scalar energy device.

[0008] KR100997951 scalar wave emitted to method manufacture.

[0009] EP 2380628Portable re-balancing unit for stimulating an organism electromagnetically.

[0010] The patents cited above relate to wave generation, but do not address the measurement of potentials and wavelengths, nor their disappearance in the presence of ferromagnetic materials. They present the supposed effects of scalar waves, without proving their existence to be accepted by the scientific community.

[0011] Note on the use of pyrolytic carbon: Pyrolytic carbon is used, among other things, as a heat conductor, in the manufacture of composites, prostheses, and grids for certain high-power tubes. In this patent, pyrolytic carbon is used in the composition of an instrument for measuring an electrical quantity. It is chosen for its high time constant, which corresponds to the change in electron spins, proportional to the length.

[0012] Known methods and apparatus for measuring weak magnetic fields

[0013] Measurement of weak fields by squid

[0014] Currently, only the SQUID, a cryoelectronic component consisting of a superconducting ring with an insulating junction, has the capacity to measure these extremely weak magnetic fields. It is used in laboratory magnetometers.

[0015] The SQUID allows for very precise measurements, with a sensitivity on the order of 1 E-7 emu. It is a laboratory instrument that incorporates a cabinet generating cold close to absolute zero.

[0016] It is much more expensive and bulky.

[0017] The present invention has the advantage of operating at room temperature, in non-laboratory environments.

[0018] Measuring biophotons https: / / www.slate.fr / sciences / lueur-corps-etres-vivants-vegetaux-forets-biophotons-veille-maladie?utm source=firefox-newtab-fr-fr

[0019] It is a method of measuring incoherent photon waves in the near field with a high-gain device, in a spectral band ranging from ultraviolet to infrared, with a conventional method of measuring transverse waves.

[0020] We hypothesize that we are measuring the same waves, which are called "biophotons." These would be photon emissions from living organisms, a quanta of electromagnetic radiation, with whole-energy and periodic jumps. However, the acquisition methods differ; in the present invention, we capture coherent longitudinal wave emissions, independent of distance, without spectral limits.

[0021] Specificity of longitudinal and transverse electromagnetic waves

[0022] Longitudinal waves, also known as Tesla waves, have been little studied to date. They propagate in the direction of their oscillation, unlike electromagnetic waves, which are transverse. Transverse waves are blocked by a Faraday cage, while longitudinal waves pass through them unimpeded.

[0023] We hypothesize that this propagation of the longitudinal wave in matter corresponds to an alignment of electron spins. Once the alignment is complete, there is no longer any obstacle; the material has become transparent to the waves, and they are traversed without attenuation, at incomparable speeds.

[0024] The only known and accepted longitudinal waves are the electrostatic waves of Irving Langmuir (1920), which are longitudinal oscillations of the electric field in an ionized gas, in response to a density perturbation; they are not associated with a magnetic field. In transverse electromagnetism, the principle of image capture is based on the acquisition of photons captured by photoelectric sensors, photodiodes, and matrix sensors, which are limited in spatial response, related to pixel resolution, and in bandwidth. These same sensors capture longitudinal waves without spatial or spectral limitations; the resolution is atomic.

[0025] Sounds are captured by microphones; for example, electret microphones or coil microphones with a floating core collect information about the air pressure gradient. These same sensors, incorporating diamagnetic sensors, capture a longitudinal electromagnetic wave without spectral attenuation. When the microphone is positioned in front of the oral cavity, due to the chiral effect, it is the signal emitted by the brain that is captured, which is the direct result of the expression of thought. When this sound has been recorded by engraving on a vinyl record, the transmission of information from the brain at the moment of recording, via the microphone and the vinyl medium, is faithfully reproduced for us today.

[0026] The present patent application presents a method and apparatus for visualizing and measuring waves that cannot be transverse, whose effects are conclusive and which have as a corollary the existence of longitudinal waves.

[0027] Lexicon

[0028] Biological object: This is a set of molecules of a biological object all having the same vibrational period.

[0029] Wave function: This is the set of electromagnetic quantities contained in a diamagnetic body that are transferred to another diamagnetic body through contact between them. This transfer occurs without energy exchange. We propose the hypothesis that it involves an alignment of the electron spins of matter subjected to a longitudinal field.

[0030] Longitudinal wave function [A1 volt ] <=>[A1 cm] A transverse electric potential gradient of 1 volt is correlated with a displacement along the longitudinal axis of a length of 1 cm.

[0031] Entanglement cone: A charged diamagnetic solid is enveloped by a standing wave; as it moves, this solid is detectable at a distance correlated with its potential, according to the law [A1 volt ] <=>[A1 cm]. For example, a 3.3 volt battery is detectable at 3.3 cm.

[0032] Reference potential: This is the zero potential in the longitudinal frame of reference of iron.

[0033] Longitudinal potential: This is the potential of a charged diamagnetic object, for example biological, relative to the reference potential.

[0034] Longitudinal charging time constant of an object: This is the propagation time in this object over a distance of 1 meter to reach the equilibrium potential.

[0035] The potential quantity does not come into play; a rise of A 1 volt or A 10 volts occurs in the same time frame.

[0036] Perimeter of entanglement: this is the spatial limit of equipotentiality of zero potential, between transverse waves of zero electrical potential difference and longitudinal waves.

[0037] Chirable effect: A molecule is chirable when it has no intrinsic symmetry. There is symmetry with respect to a mirror image; the two forms are not superimposable.

[0038] Characteristics of Scalar Longitudinal Waves • Maxwell's equations, which govern classical electromagnetism, predict that in a vacuum (or in a homogeneous and isotropic medium), electromagnetic waves are necessarily transverse. This means that the electric and magnetic fields oscillate perpendicularly to the direction of wave propagation.

[0039] • It is recognized that electromagnetic waves are transverse in a vacuum, it is also accepted that longitudinal components can appear in non-homogeneous media, such as plasmas, and in the vicinity of conductive objects.

[0040] • The present invention specifies that these conductive objects are exclusively those which have diamagnetic properties, which excludes ferromagnetic materials, and defines the specific conditions of this proximity which are described in the paragraph accompanied by the two necessary conditions: the presence of a second object of lower longitudinal potential and that there is a relative displacement between them.

[0041] • We note in scientific articles this statement, the magnetization of diamagnetic materials disappears when the cause that created it ceases (wikipedia Diamagnetism when the field is no longer applied, the magnetization disappears).

[0042] This is contradicted by Lipeo patent FR 2210131, which is based on the magnetic remanence of diamagnetic bodies.

[0043] This disappearance is only apparent. It is revealed during the relative movement between two diamagnetic bodies of different potential, constrained in relative position with respect to each other, which causes a repulsive force which decreases over time according to a linear law depending on the nature of the diamagnetic body with the lower potential.

[0044] These are stationary, vectorial, sinusoidal matter waves, directed from the pole of higher potential to the pole of lower potential. They carry phase information from the higher pole and do not transfer any energy. They are generated by an increment or decrement in distance between the two poles along a straight or curved path. They appear when the distance between the two poles, expressed in centimeters, is less than the longitudinal electrical potential difference, expressed in volts.

[0045] They disappear in the presence of a change of direction, if the radius is less than half the wavelength.

[0046] Every point on the trajectory retains in memory the wave function, which contains the longitudinal quantities of phase and amplitude, regardless of the medium traversed: vacuum, liquid, gas, solid.

[0047] Propagation occurs without distance limitations, without loss of information, along any wire of any type or on the surface of any medium. It occurs in two distinct modes within the material and on the surface. The propagation speeds are very different.

[0048] Longitudinal waves from different sources do not mix; the source with the highest potential propagates, inhibiting the weaker one. These waves, decomposed into a Fourier series, only have the first term.

[0049] Through observation of living organisms, we have found repetitive electrical phenomena that obey intrinsic laws, which we attribute to longitudinal waves. The semi-sinusoidal movements of the moving electrode are the visual evidence that attests to the existence of longitudinal waves.

[0050] Ferromagnetic materials obey the conventional laws of transverse electromagnetism. Living cells are composed of water and carbon, which are diamagnetic. Diamagnetic materials react to longitudinal waves and are only slightly affected by transverse waves. Their magnetic susceptibility is on the order of ten thousand times weaker than that of ferromagnetic materials. This difference is explained by the fact that the vectors of ferromagnetic waves, on the one hand, and diamagnetic and paramagnetic waves, on the other, are in quadrature. Consequently, a change in the ferromagnetic field has very little effect (one ten-thousandth) on diamagnetic and paramagnetic materials.

[0051] As observations progressed, leading to the present invention, we noted repetitive phenomena, which are linked to two laws:

[0052] - The wave function [1 volt] <=> [1 cm],

[0053] - The selection of the highest potential along an axis.

[0054] When a charged diamagnetic element is brought near a battery, a repulsion occurs, which is strongest when they are in contact. The repulsive force of a DC battery does not depend on its current. The force is independent of the current and is proportional to its voltage, which is the potential difference between its two terminals.

[0055] This invention aims to validate the existence of longitudinal waves through reproducible measurements obtained from repeatable experiments. In classical physics (Maxwell), free scalar waves do not exist. All physical fields are described as vector or tensor (like the electromagnetic or gravitational field).

[0056] The present invention presents a reproducible means of demonstrating the memory of water, which is diamagnetic. The repulsive force is independent of polarity. It is identical with respect to the positive pole or the negative pole.

[0057] - The distance at which the repulsive force is established corresponds to a strict law of 1 volt per cm. For example, a 3.3 volt lithium battery produces a repulsive effect when a threshold of less than 3.3 cm is crossed, corresponding to the onset of wave compression.

[0058] After crossing the compression threshold of 3.3 cm, a phase unwinding over 1 cm produces a potential difference of 1 volt - o [V = nv] = is a linear function of [L = nd], where n is the number of stacked cells at rest, polarities being irrelevant. o L is the resulting entanglement distance. Table 1: Comparison of transverse and longitudinal waves The capture of coherent longitudinal waves

[0059] The LIPEO FR3140443 A1 patent relates to a charge absorber of electromagnetic radiation.

[0060] This is not a charge absorption of a transverse wave, which implies a transfer of energy, but the capture of a longitudinal wave without acquisition of electrical charge, the memorization of a state materialized by spin orientations.

[0061] What is new and inventive in the present invention is the capture of a coherent wave obtained by adding a gun (figures 1A, 1B).

[0062] The electrical sensor (10) comprises a tubular casing (11) a straight barrel (12) whose inlet end (13) is open and whose outlet end 14 is connected to a switch (15), which is connected to a diamagnetic copper wave collector (16).

[0063] The coherence of the longitudinal wave is inversely proportional to the solid angle defined by the ratio between the section of the opening diameter in (13) and the length of the barrel.

[0064] Example provided for illustrative purposes

[0065] Dimensions: 12 mm diameter, 60 mm length

[0066] Resin casing (11),

[0067] Inner diameter of the tube (12): (p = 1 mm

[0068] SPST SMD touch switch (15)

[0069] Straight barrel length h = 30 mm

[0070] Copper collector, 4 mm diameter, 6 mm length

[0071] Solid angle Q = S / h 2 = 0.026 sr

[0072] Figure 2 illustrates in particular such a solid angle.

[0073] Scalar operators

[0074] Scalar potential addition operators

[0075] Three variants are presented below

[0076] 1-battery variant and switch

[0077] Variant 1 is illustrated in Figure 3. Three elements in series: A battery, an SMD switch and a copper wave collector.

[0078] Each press of the push button produces an accumulation of longitudinal potential.

[0079] The body is at zero potential.

[0080] Example: CR 2032 battery, 3.33 volts - 3 presses Vs = 9.99 volts

[0081] Variant 2 stacks and alternating stacks of insulating and copper surface

[0082] Variant 2 is illustrated in Figure 4.

[0083] The insulating operator (50) is a stack of n copper clinquants separated by insulators.

[0084] The addition factor is a = n+1

[0085] Example of a static addition operator with a factor of 3 performed by 2 copper surfaces.

[0086] With a 3.3-volt battery, Vs = 2 + 1 Vbattery = 9.9 volts

[0087] Variant 3: Battery and winding

[0088] Variant 3 is illustrated in Figure 5.

[0089] The addition factor is a = (n-1), where n is the number of turns. Example with a 34-turn winding.

[0090] With a 3.33 volt battery, Vs = (34-1) x 3.33 = 99 volts

[0091] The scalar multiplication operator

[0092] First option: series windings

[0093] This is a combination of at least two adders in series, where the output of the first is offset relative to the input of the second. This first option is illustrated in Figure 6.

[0094] Let a first adder have gain n and a second adder have gain m.

[0095] The multiplication factor is a = nm.

[0096] Second option

[0097] Example of a 50% gain operator

[0098] This second option is illustrated in figure 7.

[0099] 3.33 battery + 3 gain adder + 5 push button presses, the resulting potential is 50 volts.

[0100] The scalar division operator

[0101] Variant 1 stacking

[0102] Variant 1 is illustrated in Figure 8.

[0103] 2-winding variant

[0104] Variant 2 is illustrated in Figure 9.

[0105] The last element is connected to a ferromagnetic mass

[0106] The ratio is n / p

[0107] The reset operator

[0108] This operator is illustrated in Figure 10.

[0109] When the copper cylinder is brought into contact with a ferromagnetic mass, the potential drops to zero. Iron constitutes a magnetic zero.

[0110] Example application: scalar analog calculator

[0111] This example is illustrated in Figure 11.

[0112] Each switch can be replaced by a VMOS component whose gate is biased.

[0113] Repeated contact n times by pressing K3 produces m increments of potential V1 = (n+1-s) v. The final result is V2 = (n+1-s)( m+1)v.

[0114] Reset by pressing K4 which clears the wave information in the ferromagnetic mass.

[0115] The Longitudinal Wave Electromagnetometer

[0116] Principle

[0117] As illustrated in Figures 12A, 12B, 12C, the electrometer (20) is a potential comparator, comparing the potential of a biological object (1) with the potential of a continuous reference source (2). The potential of the object (1), which is acquired beforehand by a sensor (10), is compared to that of the reference source, which is transferred to a movable electrode (22) rotating around a vertical axis (23). A fixed electrode (21) divides the space into an object semi-space (3) in which the sensor (10) moves along a linear axis x, guided on a V-shaped track (26), and an image semi-space (4) in which the movable electrode (23) moves.When the sensor (10) is at a distance d in cm < V in volts according to the fundamental law of longitudinal waves [ 1 volt ] <=> [ 1 cm ], the plasma (24 ) between the sensor (10) and the moving electrode (24) acquires a potential Vi = V- d, which is transmitted by entanglement to the plasma (25) between the two electrodes (23 and (24) which creates a force on the moving electrode (24) in the clockwise direction, when this potential reaches the potential of the reference source (2) the moving electrode initiates a movement: Vi = V s + d.

[0118] Example of measurement: reading d = 37 mm compared to a source VS = 10 volts.

[0119] Vi = Vs + d, i.e., 10 volts + 3.7 volts = 13.7 volts.

[0120] Description of the basic electrometer

[0121] It is a basic instrument intended for outdoor measurements, hand-portable with reading on a graduated scale (27).

[0122] Example provided:

[0123] Fixed electrode made of copper strip.

[0124] Mobile electrode made of pyrolytic carbon, 1 mm thick.

[0125] X-axis travel: 180 mm.

[0126] The advantages of this basic device are the speed of measurement, its low cost, and its suitability for measuring plants outdoors.

[0127] The basic version of the device can be tricky for a novice looking for the critical tilt angle. The automatic version described below solves this problem. It eliminates the operator's need for dexterity in adjusting the tilt angles.

[0128] Description of the stand-mounted electrometer

[0129] It is a laboratory instrument for live processing or processing of photographs. It delivers potential and wavelength measurements.

[0130] The device (40) described above incorporates:

[0131] - A basic magnetometer (20).

[0132] - A subset of the magnetometer plate tilt (50).

[0133] - A scalar operator.

[0134] - A servo subset (60).

[0135] - A display of the quantities (70) potential and wavelength.

[0136] The tilt subset

[0137] The tilt subset (50) is illustrated in figure 13.

[0138] It ensures the angular positioning and immobilization of the magnetometer according to angles of inclination a and b.

[0139] It comprises a base (51) which supports a steel sheet cradle (54) that pivots through an angle α about an axis oriented 0X, held in position by a lateral magnet (52). This cradle supports the magnetometer which pivots through an angle β about an axis (57) oriented along the OY axis, held in position by a magnet (58).

[0140] The magnetometer (20) is held in its critical tilting position when the moving electrode is in position C1. The operator maintains this critical positioning by holding the magnetometer (20) in its tilt with their right hand and slowly advancing the sensor with their left hand. The servo subassembly

[0141] The servo subset is illustrated in Figure 14.

[0142] The deflection angle of the moving electrode is measured using an optoelectronic device consisting of a screen attached to the electrode that blocks a photoelectric cell in barrier mode. The signal received by the receiver is proportional to the deflection angle c of the electrode. A setpoint value for the deflection C1 is defined, which corresponds to a critical equilibrium point before tipping.

[0143] During sensor movement, the moving electrode rotates via the plasma. When the setpoint value is reached, feedback is applied by polarizing the inner face of the stationary electrode by driving a voltage generator, thus creating potential equilibrium in the plasma.

[0144] As the sensor advances, the transverse voltage of the generator follows the longitudinal potential of the sensor.

[0145] When the sensor reaches the origin Xo, the potential across the generator terminals is recorded. This method is illustrated in Figure 15A.

[0146] Measuring the potential of the biological object

[0147] The sensor is connected to the diode. The plasma and the moving electrode acquire the potential of the biological object.

[0148] The operator adjusts the platform's angle to bring the electrode to the reference point at angle C1, by playing through successive iterations on the angles a and b.

[0149] The potential of the stationary electrode is compared with the potential of the diode wall, which is at the same potential as the living organism. The moving electrode begins to rotate, and the photoelectric cell is covered. The potential of the biological organism is then recorded on the voltmeter.

[0150] Measurement of the wavelength of the biological object

[0151] After reaching and exceeding the sensor potential, the moving electrode is subjected to the vector potential resulting from the reference potential and the sensor.

[0152] V = V ref - V sensor sin a.

[0153] We initiate a decrease in the potential V of the reference electrode, the blade performs a semi-sinusoidal movement in the trigonometric direction each reversal point corresponds to half a wavelength (see figure 15B).

[0154] The visualization of sinusoidal waves is proof that the waves are not transverse.

[0155] The magnetometer described in patent FR 22 10131 is based on transverse wave theory. It features a charge-sensing electrode and measures the deflection of an electrode caused by manual or motorized movement of the sensor along a linear axis; the measured magnetic field strength is proportional to the measured deflection.

[0156] We observe an alternating motion of the electrode, which cannot be explained by the laws of conventional electromagnetism based on transverse waves governed by Maxwell's laws. The observation of this sinusoidal motion constitutes proof of the existence of longitudinal waves.

[0157] Principle of longitudinal wave dynamics

[0158] The movement of the electrode results from the transmission of diamagnetic potential gradient information in a chain (illustrated in Figure 16) alternating copper and air, which are diamagnetic solid and gaseous media.

[0159] The last link is an air cavity whose rear wall is free. The distance between the two walls, through a chirable entanglement phenomenon, is proportional to the potential gradient produced by the displacement of the sensor.

[0160] The semi-sinusoidal movement illustrates the vibratory and stationary phenomenon of longitudinal waves.

[0161] Realization

[0162] Provided as an example

[0163] Amplitude angle at 10 degrees

[0164] Amplitude angle b 2 degrees

[0165] Positioning angle c1 25° electrode (29) pyrolytic carbon plate 25 X 10 mm thickness 2 mm

[0166] Features

[0167] Measurement time 10 seconds.

[0168] Measurement uncertainty of potentials 0.1 volt at 1 standard deviation.

[0169] Uncertainty in measurement of wavelengths: 1 mm to 1 standard deviation.

[0170] Photograph of longitudinal wave emissions

[0171] The camera is a scalar imager.

[0172] Principle of the scalar imager (illustrated in figure 17).

[0173] The camera performs a scalar projection onto the image plane of objects along each axis. It is the potential of the level 5 strawberry object, although masked by the level 3 apple object, that is projected onto the image plane. The scalar wave of the strawberry has passed through the apple. The boundary depends on the coherence created by the aperture. Thus, the longer the focal length of the lens, the greater the depth of scalar coherence.

[0174] Features

[0175] • The image is the scalar replication in a 2D image plane of scalar information of scalar information in a 3D object half-space.

[0176] • Zero attenuation as a function of distance.

[0177] • Atomic spatial resolution.

[0178] • Pixel resolution is not a factor, since the information is fixed beneath the photosensitive layer to visible radiation: o Measurements are independent of position on the X-axis. o The depth of measurement is related to the focal length. o Measurements can be taken along curved surface trajectories. o For example, along an optical fiber or a copper conductor. The speed of movement of the biological object

[0179] The approach movement must be slow, preferably axial and less than 3mm / s. We observe that a rapid movement does not produce any repulsive force on the moving electrode; the standing wave could not be established in the object semi-space.

[0180] Boundaries

[0181] There is no limit to spatial resolution. Thus, in the case of a digital camera, pixel resolution does not matter, and similarly, in the case of a film photograph, grain is irrelevant.

[0182] The wave, upon passing through the diaphragm, changes direction, which has the effect of a diopter. The angle α of the vector with respect to the axis of the diaphragm upon exiting is symmetrical and equal to that upon entering α.

[0183] First application example: tumor measurements

[0184] Pathogenic zones are biological objects detected by biological overactivity.

[0185] A brain tumor will thus be measured in potential and amplitude, without spatial resolution limits.

[0186] Second example of application: recording the emission profile of human beings

[0187] Figure 18 illustrates the axial profile of a 50-year-old man: Potential curve in blue in volts, and wavelength curve in brown in cm.

[0188] Figure 19 illustrates, on the left, the potential profile of a person considered positive max +30 volts; on the right, the potential profile of a person considered negative or masking a perverse spirit min -80 volts.

[0189] Third example: Acquisition of longitudinal magnetic quantities related to thought

[0190] It can be acquired from a photograph, for example from anthropometric frontal and profile photographs.

[0191] This signal is vectorial and is directed by thought towards a sensory terminal. When it is a speech, the wave is directed towards the mouth.

[0192] The spaces between the incisor teeth act as a diaphragm, and through the chirable effect, the brainwave is deflected at a symmetrical angle. The brainwaves are stored on a diamagnetic support positioned on this axis (see Figure 20).

[0193] A basic way to collect the information is to place a horizontal piece of paper measuring 40 x 40 mm in contact with the nose for a few seconds.

[0194] In most people undergoing the test, a very positive thought is measured between 15 and 25 volts, and a very negative thought is measured between -15 and -25 volts.

[0195] This process is envisaged for continuous recordings during sleep with accelerated processing, in a manner analogous to the accelerated acquisition and reading of cardiological signals by a Holter process.

[0196] On each axis, the highest potential is detected and stored. This allows for the detection of hyperactive cancer cells, without spatial resolution limitations.

[0197] Fourth example: recording the waves of manuscripts, signatures, drawings, painting

[0198] The brain's vector signal is directed to the hand and imprinted on the ink and paper, the painter's canvas via the brush. Through this process, we obtain information from the moment of thought that presides over the creation of a manuscript: will, musical score, poem.

[0199] As a corollary, we can detect forgeries in writing.

[0200] Wavelength is a marker of stability and serenity. It is particularly high in mystics. Conversely, a liar, with a destabilized metabolism, will have a low wavelength, possibly as low as 15 or even 10 mm.

[0201] Examples are illustrated in Figure 21. In the last case, the very low potential reveals a suspicious indifference on the part of the writer which cannot be explained in this tragic moment.

[0202] Recording of longitudinal signals

[0203] The wave is not limited by the bandwidth capacity of the medium; a bandwidth of, for example, 1 kHz is sufficient. It is thus recorded continuously in a conventional magnetic memory such as an EPROM or magnetic tape intended for sound recordings.

[0204] Teleportation

[0205] Principle

[0206] A charged object, as it moves, ionizes a gaseous medium, which retains a standing wave trace at every point along its path.

[0207] The acquisition of this signal at a point X of the trajectory is carried out in a direction normal to the YZ plane at point X.

[0208] Let two diamagnetic objects, for example credit cards M1 and M2 of identical format in a place A, M1 carries information Fi located at X1, Y1.

[0209] As illustrated in Figure 22, M2 is placed in contact with M1. It acquires the information Xi. Then it is moved away from M1 to be placed at a location B.

[0210] Along path AB, the gaseous medium has been ionized, the stationary magnetic wave relative to Xi is present along the entire path.

[0211] This initial transmission defines a carrier wavelength. The molecules will then align themselves with each other along the entire path.

[0212] A reset of the Fi information on M1 by a ferromagnetic object produces the reset of Xi on the M2 card.

[0213] From point B, the M2 card in turn sends information, which is captured at A.

[0214] We have established a full duplex link between two points.

[0215] By respecting the conditions of straight or curvilinear trajectories, whose radius is greater than their common wavelength, the information remains common to M1 and M2. Map M2 is moved to a location B.

[0216] Any positive gradient of potential AV from one of the points of M1 is replicated identically on M2, regardless of the distance and medium traversed.

[0217] After each transmission of information, one of the two terminals M1 or M2 performs a magnetic reset in order to send new information.

[0218] The transmission of negative potential information is achieved by introducing a potential offset, so that the message is positive. The card description is given as an example.

[0219] Credit card format

[0220] It consists of a front side: a sheet of diamagnetic material, for example cellulose pulp paper or a polymer, and a back side of aluminum foil with a thickness of 0.1 or 0.25 mm.

[0221] This aluminum shielding prevents information loss upon contact or in an area of ​​higher potential.

[0222] It contains one or more memory ranges referenced in XY position.

[0223] Transmission rules

[0224] This is a transmission in the plasma generated by the movement of a charged object. The transmission occurs exclusively via a positive potential gradient. The first passage defines a diamagnetic wave carrier.

[0225] • Reset after each transmission. This reset does not affect the carrier in any way.

[0226] Information entered is only taken into account if it is increasing.

[0227] • Multiplexing o The waves do not mix, only the base of the highest potential is transferred.

[0228] Interception along the route

[0229] As illustrated in Figures 23A and 23B, at every point along the trajectory AB, ionization of the medium through which the object passes occurs, and the information remains stationary. A card M3, inserted between A and B at point C, intercepts the information. It is spatially referenced by a stop along the Y and Z axes. When it comes to rest, card M3 acquires the information.

[0230] It is removed by a movement normal to the curved trajectory, to reach a place D, where it retains the information Fi.

[0231] The information is now shared between objects M1, M2, and M3 located in 3 places.

[0232] Thus, information is exchanged between n cards arranged in n different locations.

[0233] Information circulating

[0234] The information contained on the map can be a set, for example a number in x1y1, an image referenced by an origin in X2, y2, a biological sequence.

[0235] Transmission time is independent of the amount of information to be transmitted.

[0236] There are no spatial or frequency limits in image transmission.

[0237] Network

[0238] It consists of servers, hubs, and channels

[0239] In summary:

[0240] Information exchange system using a longitudinal wave network to connect servers distributed in space without physical support or radio relays.

[0241] The hub is a node where things pass through.

[0242] If two waves are present simultaneously in a hub, the resulting interference causes data loss. Therefore, the information must be multiplexed to pass through the hub sequentially. Mixed network: longitudinal waves and the internet

[0243] Longitudinal information can also be transmitted via the internet. Therefore, it can be transmitted interchangeably via the longitudinal wave network or the internet.

[0244] Therapy

[0245] Existing patent on wave therapy US6845270 apparatus for destroying pathogen molecules using frequencies.

[0246] Pathogenic cells have greater potential than healthy cells. Their danger lies in their ability to spread progressively over time.

[0247] The therapeutic principle consists of disrupting the vibrational pattern of pathogenic cells by targeting them with a wave acquired from a healthy cell, which is amplified by a scalar amplification operator. The healthy wave will then dominate the dissonant pathogenic wave. During the transient phase, which can last several hours or even several days, a zero potential is observed, signifying the absence of vibration. Then, the former pathogenic zone attunes itself to the wavelength of the healthy zone.

[0248] The therapeutic medical device, in its basic design, is a longitudinal wave sensor to which a scalar amplification operator has been added.

[0249] Description (with reference to figures 24A, 24B)

[0250] Body 86 of the device

[0251] Acquisition via the front end by pressing the push button switch K1 (81). The Ve wave information is stored in the copper collector (82) and is presented at the output Vs for a measurement prior to therapy.

[0252] This information is amplified by means of a scalar amplifier consisting of two coils (83) and (84) in series with offset axes. By pressing the push-button switch K2 (85), the wave Ve is amplified and stored in the collector (85), its forward potential from Ve = Vs to aVe, where a is the amplification factor, which is the product of the number of turns in the coils (83) and (84).

[0253] Example implementation

[0254] Windings (83) and (84) in enamelled or unenameled copper wire diameter 0.2 mm.

[0255] Gain 100 product of the number of turns n1 = 10 of the winding (83) by the number of turns n2 = 10 of the winding (84).

[0256] K1 (81) and K2 (82) SMD pushbuttons.

[0257] Copper collector (85) diameter 4 mm length 10 mm.

[0258] Body (86) 86 in resin diameter 12 mm length 100 mm.

[0259] Operating procedure

[0260] The acquisition is made via photograph

[0261] 1. Target a healthy area close to the unhealthy area,

[0262] 2. Acquisition of sound information by relying on K1,

[0263] 3. Target the unhealthy area,

[0264] 4. Support on K2,

[0265] An intertwining occurs between the photograph and the organ in the healthy area.

[0266] 5. taking a picture of the treated area, 6. measuring the potential, after treatment, we verify that we obtain a zero potential signifying a disorganization of the unhealthy cells.

[0267] Applications

[0268] - Dermatology

[0269] - Oncology

[0270] Teletherapy

[0271] Principle

[0272] The acquisition is performed on a photograph of the organ containing the pathogenic area. The outline of the pathogenic area is visually identified.

[0273] The procedure is similar to that described live. Information from the healthy area is extracted from this image, amplified, and then applied to the pathogenic area of ​​the photo.

[0274] Then the processed image is teleported. A disorganization of the pathogenic molecules occurs remotely.

[0275] Scalar processing of images of the cosmos

[0276] The question arises as to what is being measured: is it dark matter?

[0277] By enlarging the image, as illustrated in Figure 25, the spatial resolution is increased by a factor equal to the product of the gains. The theoretical limit is that of the atom.

[0278] Voyage vers l'infini by Christophe GALFARD, detail from page 107.

[0279] The amplification by a factor of 100 obtained by two successive magnifications of gain 10, reveals on the third image a dark object with a potential of 234 volts, clearly higher than all terrestrial biological objects.

[0280] APPLICATIONS

[0281] Some examples of applications are summarized below.

[0282] - Measurement of longitudinal electromagnetic waves (oel) positive and negative potentials, and wavelength of biological objects: animals, plants, bacteria, viruses, fungi, water, homeopathic medicines based on sucrose, stars live, or recorded on any diamagnetic medium, without spatial or spectral resolution limit.

[0283] - Measurement of positive and negative emitted waves and wavelength at any point in the brain of a human being directly in front of the oral cavity by chirable projection, via a screen with an opening onto a diamagnetic support placed at the level of the nose, the support being for example a paper.

[0284] - Vector measurement of the waves of the different biological organs composing the brain, live or on photo, by three sensors arranged along three axes: front, profile and inclined oral cavity, along an axis of symmetry, application to monitoring during sleep and detection of cancer cells, detection of forgeries in writing and painting.

[0285] - Medical device for reducing the biological activity of dissonant unhealthy cells of wavelength A2 and potential V2, live or on photograph by capturing the healthy longitudinal wave, of wavelength A1 and potential V1 by amplifying it by a scalar factor a, followed by a back-emission in front of the unhealthy cells by this amplified wave aV1, which produces an immediate destabilization of the wavelength A2 of the unhealthy cells, lowering V2 below a measurable threshold.

[0286] - Voltmeter at a distance from the electrical potentials of electrical generators, -example continuous electric battery - without or with flow of an electric current.

[0287] - Acquisition of a longitudinal wave by conventional commercial sound sensors, without spectral limit: example electrets, and of images by digital cameras, without spatial limit related to pixel resolution, of the highest potential along each axis.

[0288] - Recording of a variable longitudinal wave signal on any diamagnetic medium, for example paper, semiconductor memory without bandwidth limit with atomic resolution.

[0289] - Teleportation of scalar information between two objects, by initialization of the objects by entanglement, having in common an entanglement perimeter, then separation by following curvilinear trajectories of radius greater than the radius of the entanglement perimeter solids and gases; Duplex transmission of positive gradients which accumulate.

[0290] - Full duplex teleportation by longitudinal information waves between two points A and B in wireless space, without radio link, in all gaseous or liquid media, by entanglement of a messenger card in A moved to B, this information being numbers, images reset to zero by contact with a ferromagnetic mass after each information.

[0291] - Acquisition of information at every point of the route located between A and B by a card C.

[0292] - Longitudinal wave telecommunication network consisting of a set of interconnected servers.

Claims

Demands 1. An electrical sensor (10) of coherent longitudinal electromagnetic waves emitted by a biological object (1), comprising a tubular envelope (11), including a barrel (12) whose front end (13) is open and the rear end (14) is closed on the upstream pole of a bipolar switch (15), and in which the downstream pole of said bipolar switch (13) is connected to a potential charge collector (16) of diamagnetic material, preferably copper.

2. A system comprising an electrometer for cooperating with the sensor (10) according to the preceding claim, said electrometer being configured to compare the potential of a biological object (1) with the potential of a continuous reference source (2), said electrometer comprising: • a sensor guide V (10), • a mobile electrode (22) rotating around a vertical axis (23), • a fixed electrode (21) dividing the space into: • a semi-object space (3) in which the sensor (10) moves along a linear axis x, guided by the guide V, and • a semi-image space (4) in which the mobile electrode (22) evolves, in which the potential of the biological object (1) is acquired beforehand by the sensor (10), and the potential of the reference source is transferred to the mobile electrode (22).

3. System according to the preceding claim in which the electrometer comprises at least one scalar operating device, referred to as the scalar operator, said scalar operator being configured to perform scalar operations from a potential measured by the sensor (10), said scalar operator being, for example: • a scalar addition operator implemented during a displacement of the sensor (10), said scalar addition operator being realizable by one of the following three wave perturbation methods: an interruption, and / or a gap between two diamagnetic faces, and / or a double turn, • a scalar multiplication operator, consisting of two distinct addition operators of n and m turns, arranged together so that the output of the first is shifted relative to the input of the second, said scalar multiplication operator having a multiplying factor a = nm.

4. A system according to any one of claims 2 and 3, further comprising a tilting sub-assembly configured to ensure angular positioning and immobilization of the electrometer, said tilting sub-assembly comprising: • a base (51), • a steel sheet cradle (54) configured to support the electrometer, said cradle being arranged on the base (51) and free to pivot by an angle α around an axis oriented 0X, said cradle being configured to be held in position by a lateral magnet (52).

5. System according to the preceding claim in which the electrometer is free to pivot by an angle b about an axis (57) oriented along the OY axis, the electrometer being configured to be held in position by a magnet (58).

6. A system according to any one of claims 2 and 3, further comprising a servo control sub-assembly configured to follow a potential variation of the moving electrode during the movement of the sensor on the guide V, said servo control sub-assembly comprising: • a photoelectric cell partially screened by the moving electrode, delivering a signal proportional to the angle of deflection of the moving electrode, • a voltage generator configured to bias the fixed electrode when a setpoint value of the signal delivered by the photoelectric cell is reached.

7. A method for measuring a coherent longitudinal electromagnetic wave emitted by a biological object, implementing the sensor (10) according to claim (1) and / or the system according to any one of claims 2 to 6, said method comprising: • Aim the sensor at the biological object or a support attached to the biological object, • Place the sensor on the electrometer's guide V, at one distal end, • Move the sensor along the guide V, towards a proximal end, • Measure the potential induced by the rotation of the moving electrode during the movement of the sensor, • Deduce the potential of the biological object (1) by comparison with the potential of the reference source.

8. Method according to the preceding claim wherein the potential measurement is carried out when the electrometer is immobilized in the critical tipping position.

9. Method according to claim 7 further comprising a decreasing polarization of the fixed electrode causing an oscillation of the moving electrode, the oscillation period of the moving electrode corresponding to half a wavelength of the coherent longitudinal electromagnetic wave emitted by the biological object.

10. A method according to any one of claims 7 to 9 wherein the support attached to the biological object is a diamagnetic support, for example paper-based.

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