WO2011055403A1 - Appareil électromagnétique mécaniquement statique pour accélérer des molécules électriquement neutres en utilisant leur moment électrique dipolaire - Google Patents

Appareil électromagnétique mécaniquement statique pour accélérer des molécules électriquement neutres en utilisant leur moment électrique dipolaire Download PDF

Info

Publication number
WO2011055403A1
WO2011055403A1 PCT/IT2010/000446 IT2010000446W WO2011055403A1 WO 2011055403 A1 WO2011055403 A1 WO 2011055403A1 IT 2010000446 W IT2010000446 W IT 2010000446W WO 2011055403 A1 WO2011055403 A1 WO 2011055403A1
Authority
WO
WIPO (PCT)
Prior art keywords
treating
treating chamber
electric field
electric
molecules
Prior art date
Application number
PCT/IT2010/000446
Other languages
English (en)
Inventor
Achille Zanzucchi
Original Assignee
Achille Zanzucchi Editore Di Achille Zanzucchi
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Priority claimed from IT000090A external-priority patent/ITPR20090090A1/it
Priority claimed from IT000082A external-priority patent/ITPR20100082A1/it
Application filed by Achille Zanzucchi Editore Di Achille Zanzucchi filed Critical Achille Zanzucchi Editore Di Achille Zanzucchi
Publication of WO2011055403A1 publication Critical patent/WO2011055403A1/fr

Links

Classifications

    • H—ELECTRICITY
    • H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
    • H05H3/00—Production or acceleration of neutral particle beams, e.g. molecular or atomic beams
    • H05H3/04—Acceleration by electromagnetic wave pressure
    • B—PERFORMING OPERATIONS; TRANSPORTING
    • B03—SEPARATION OF SOLID MATERIALS USING LIQUIDS OR USING PNEUMATIC TABLES OR JIGS; MAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
    • B03C—MAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
    • B03C1/00—Magnetic separation
    • B03C1/02—Magnetic separation acting directly on the substance being separated
    • B03C1/023—Separation using Lorentz force, i.e. deflection of electrically charged particles in a magnetic field
    • B—PERFORMING OPERATIONS; TRANSPORTING
    • B03—SEPARATION OF SOLID MATERIALS USING LIQUIDS OR USING PNEUMATIC TABLES OR JIGS; MAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
    • B03C—MAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
    • B03C1/00—Magnetic separation
    • B03C1/02—Magnetic separation acting directly on the substance being separated
    • B03C1/025—High gradient magnetic separators
    • B03C1/031—Component parts; Auxiliary operations
    • B03C1/033—Component parts; Auxiliary operations characterised by the magnetic circuit
    • B03C1/0335—Component parts; Auxiliary operations characterised by the magnetic circuit using coils
    • B—PERFORMING OPERATIONS; TRANSPORTING
    • B03—SEPARATION OF SOLID MATERIALS USING LIQUIDS OR USING PNEUMATIC TABLES OR JIGS; MAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
    • B03C—MAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
    • B03C1/00—Magnetic separation
    • B03C1/02—Magnetic separation acting directly on the substance being separated
    • B03C1/23—Magnetic separation acting directly on the substance being separated with material carried by oscillating fields; with material carried by travelling fields, e.g. generated by stationary magnetic coils; Eddy-current separators, e.g. sliding ramp
    • B03C1/24—Magnetic separation acting directly on the substance being separated with material carried by oscillating fields; with material carried by travelling fields, e.g. generated by stationary magnetic coils; Eddy-current separators, e.g. sliding ramp with material carried by travelling fields
    • B03C1/253—Magnetic separation acting directly on the substance being separated with material carried by oscillating fields; with material carried by travelling fields, e.g. generated by stationary magnetic coils; Eddy-current separators, e.g. sliding ramp with material carried by travelling fields obtained by a linear motor
    • B—PERFORMING OPERATIONS; TRANSPORTING
    • B03—SEPARATION OF SOLID MATERIALS USING LIQUIDS OR USING PNEUMATIC TABLES OR JIGS; MAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
    • B03C—MAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
    • B03C1/00—Magnetic separation
    • B03C1/32—Magnetic separation acting on the medium containing the substance being separated, e.g. magneto-gravimetric-, magnetohydrostatic-, or magnetohydrodynamic separation

Definitions

  • the present invention has as object a mechanically static electromagnetic apparatus for accelerating electrically neutral molecules utilizing their weak dipolar electric moment and the Lorentz force of electrology.
  • the apparatus finds employment as:
  • the electromagnetic device object of the present patent has two groups of main applications:
  • GROUP B For the APPLICATIONS GROUP B the separation of components with physical methods (excluding that with chemical methods) is made, in the present technique, mainly through the complex and sometimes very expensive process of fractional destination of chemical-physical components in liquid phase, with previous liquefaction of the start mixture, if in gas form.
  • the destination is made in columns, generally at trays, utilizing the difference between the boiling points of the components.
  • the separation by means of centrifuges is employed only in some cases, as for the isotopes of uranium. Let's take into consideration, for example, the separation by destination of a mixture of the two hydrocarbons propane and propylene in a tray column. In corrispondence of an intermediate tray the feed is introduced.
  • a tray is an "enrichment element" in the more volatile component. This enrichment is obtained by creating in the tray a chemical-physical equilibrium between a liquid phase and a gas one, in which the concentration of the more volatile component in the vapour is higher than that in the liquid.
  • the aim of the present invention is that of proposing a very innovative electromagnetic device that can allow for the above applications great simplifications and savings in costs.
  • the device in question comprising the characteristics shown in one or more of the attached Claims, allows to obtain good results in attaining such aim, above all for the presence exclusively of static parts and for the direct linear acceleration of the substances to be treated without the necessity of transforming a rotatory motion into a linear one or vice-versa.
  • Fig. 1 shows a propeller (pump for liquids);
  • Fig. 1a shows section A-A of Fig. 1;
  • Fig. 2 shows a separator of chemical components
  • Fig. 2a shows section A-A of Fig. 2;
  • Fig. 3-A shows wave forms of the vectors electric field strength E and magnetic induction B in a first chemical-physical case
  • Fig. 3-B shows wave forms of the vectors electric field strength E and magnetic induction B in a second chemical-physical case
  • Fig. 4 shows a propeller as that of Fig. 1 realized by replacing the electric field strength E with Hertz waves;
  • Fig. 4a shows section A-A of Fig. 4.
  • electric polarization As is known, the phenomenon of the production, in an atom or a molecule, of a dipolar electric moment is called electric polarization. Such polarization can be spontaneous (caused by internal interactions in a multiatomic molecule between the positive electric charges and the negative ones), induced (by external electromagnetic fields), or combined between the two previous types.
  • the center-of-mass of the positive electric charges (atom nuclei) and that of the negative ones (peripheral orbital electrons of the atoms) can be non-coincident, due to phenomenon either intrinsic relating to the structure of a multiatomic molecule or induced by an external electric field.
  • the product of the value of the total positive charge of the molecule by the distance between the centers-of-mass of the positive and negative charges forms a dipolar electric moment.
  • the dipolar electric moment is given by the product [e- ⁇ ] and can be measured in the unit [e m] (electron-meter).
  • the unit [e m] electron-meter
  • the literature it is, generally, measured in the unit [C m] (Coulomb-meter) or in the unit [D] (Debye), being 1 D equivalent to
  • a substance under treatment liquid, in gas form or solid
  • a Treating Chamber 1 consisting, as real single constructive element, in a stretch of suitable length of a Treating Tube 14, in non-conductive material and internally empty, to the action of an alternating magnetic field at waves generally sinusoidal (but that can be also rectangular or rectangular with rounded- off corners), with vector "magnetic induction" B perpendicular to the direction of the thrust to be obtained and, simultaneously, to an alternating electric field, isofrequential and with the same characteristics in regard to the form of the wave, with vector "electric field strength" E perpendicular to both B and to the direction of the thrust.
  • CASE 1 occurs when the stretching is partial and takes for its development, from the stretching angles [-a] to [+a], a full half-period of oscillation of the waves of the two fields. This same CASE 1 occurs for total stretching too, on condition that it still take, for its development, a half-period of oscllation of the waves.
  • the above situation with partial stretching occurs, for example, with liquid water as substance to be treated, even with very high voltages of the electric field, for the strong resistance of the molecule, due mainly to its high dipolar electric moment, to the alignment of its electric axis.
  • CASE 2 is represented in Fig. 3-B, where B is shifted in advance by an angle sensibly ⁇ 90° (for example, 20°) with respect to E.
  • THis case is taken into consideration when, for scarce resistance of the molecules of the substance to be treated to the alignment of their electric axes, there is a "total stretching” in a “stretching interval” very short with respect to the quarter of wavelength (interval t2-t2' of the axis of the abscissae of the figure). Such a situation can occur, for example, with gases at not very high pressures.
  • the path of the equivalent electron, as component in the y-direction with respect to the antagonist equivalent positron in a half-period is equal to [2 ⁇ ] in the case of total stretching, and is set, in the case of partial stretching, equal to a product [26-R], where R is a dimensionless constant which will be called "stretching factor".
  • the average velocity [v] will be, in the following, called “velocity of the schematic equivalent electron”, or simply, “equivalent velocity”.
  • the relaxation times in the molecular polarization are relatively long, because of which, for most polar molecules, such polarization can be, practically, utilized only up to a maximum of 100 MHz. In the electronic and atomic polarizations the relaxation times are much shorter, allowing the employment of higher frequencies.
  • a second critical factor is the phase relation between the magnetic and electric fields.
  • phase shifting between the vectors E and B can be predicted in some cases approximately, while in other can be established, practically, only experimentally. In any case it is needed that the regulation of the phase shifting be made, for each Treating Chamber, with great precision, between 0° and 90°. A not optimal phase shifting can lead to sensible reductions of the thrusts obtainable, or also to their zeroing.
  • a third critical factor is represented by the sizes of the Treating Chambers.
  • each Treating Chamber along y and z must not exceed a small fraction of the wavelength of the vectors E and B equal to few degrees of the oscillation. This in order to make possible, at all points of the Chamber, the interaction provided between the two sinusoids of the same vectors E and B. For example, with frequencies of 100 MHz, to which a wavelength of about 3 m corresponds, it is possible to utilize Treating Chambers with sizes along y and z up to 6 cm, corresponding to (7.2)°.
  • a fourth critical factor is the counter-polarization of the molecules of a substance under treatment.
  • This counter-polarization is responsible for the fact that only partial stretching occur, even for high voltages of the electric field.
  • a voltage of the electric field 100000 V/cm (which is technically realizable because the resistivity of water increases by much at the very high frequencies).
  • This counter-polarization is less critical in gases, especially if at not very high pressures.
  • the electronic polarization is the only choice for the apolar molecules. It requires, however, very high voltages for the electric field, due to the scarce deformability of the atoms. Advantages of the electronic polarization are to be present for all species of monoatomic or multiatomic molecules and to have, as already said, "relaxation times" (in the order of 10 ⁇ 16 s) by far shorter than those of the molecular polarization, which allows the utilization of high frequencies.
  • the waves of the electric field can be replaced by Hertz waves obtained, for example, from a magnetron. They, in fact, cause stretchings of the molecules, due to the effect of their dipolar electric moment, identical to those produced by waves of electric voltage. It is necessary that the oscillations of the Hertz waves be in the direction of the vector E of the electric field, which they replace.
  • Base Project A BASE PROJECT A and BASE PROJECT B
  • Such projects regard the calculation of the thrusts obtainable on a substance within a propeller, formed by a rectilinear Treating Tube of the internal section of [2 x 1.5] cm, in which there are obtained 15 Treating Chambers each 4 cm long, spaced 4 cm from each other, with length of the Tube of about 130 cm.
  • the substance under treatment is liquid water in which the thrust is to be determined
  • Base Project B is dry air at 4 Kg/cm 2 eff. for which it is to be calculated the possible separation grade between nitrogen and oxygen.
  • a Frequency Converter 2 at two outlets 2a and 2b (First and Second HF - High Frequency - Line) connected at its inlet 2c to a Power Net at 50 Hz, supplies to all the apparatus:
  • the alternating voltage of the First HF Line 2a must be such as to make circulate in the turns 7 the intensity provided for the current.
  • the Propeller 4 consists of the following elements, or comprises the following elements.
  • a Treating Tube 14 in non-conducting material, internally empty, lying along x, in which the water flows, from an inlet 11 and an outlet 12.
  • At least one Treating Chamber 1 defined as stretch of a certain length of the Treating Tube 14, said Treating Chamber representing a real physical unit, in that it could be realized also as a separate cylindrical container open at both ends and connected in correspondence of these to other Treating Chambers with suitable transmission elements (small tubes).
  • the two plates of each Process Condenser are placed outside the Treating Tube, at the minimum possible distance from the walls of this, securing anyway the insulation from the ferrite. In general it is possible also, for certain fluids, to place the two plates inside the Treating Tube, at direct contact with the fluid.
  • the Process Condensers are connected with one another in parallel. The voltage to be applied to the plates is that coming from the Voltage Transformer 9 through Phase Regulator (following point).
  • a Primary Phase Regulator 10 placed downstream the Voltage Transformer 9 with the function of regulating the phase relation between the electric field strength E of the electric field and the vector B of the magnetic field for the only Treating Chamber or for the complex in parallel of the Treating Chambers.
  • the phase of the vector E from 0° to 90°, in such a way as to have in the same Treating Chamber the optimal phase relation between the vectors E and B, it is to be acted on the Phase Regulators 10 and 10a.
  • phase regulation can be obtained with very simple devices, because of the very short wavelengths.
  • the quarter of wavelength is about 75 cm, and to such length it corresponds the phase variation from 0° to 90° which occurs in the current along a conductor.
  • the Phase Regulator 10 can be realized as a device which can vary, in non-inductive way, from 0 to 75 cm the length of an additional stretch of conductor to be inserted into the circuit.
  • Each Regulator 10a can be realized as the Regulator 10 with a stretch of additional conductor of length shorter than that of the same Regulator 10. While for the Regulators 10a it can be sufficient, generally, the setting at the manufacturing, the Regulator 10 can be positioned at the installation and in subsequent times.
  • the sizing has been chosen trying to obtain that the flux lines of the vector B do not run out, as possible, from the "nucleus" of the magnetic field.
  • the induction B can be calculated as follows.
  • the current to the turns is chosen at the maximum value compatible with a reactive voltage in the turns constructively acceptable and with a value of the magnetic induction in the ferrites of about 0.1 T (Tesla, V-s/m 2 ), at which it is thought that the ferrite chosen can work at the very high frequency of 100 MHz and at the ordinary temperatures.
  • some pairs of contiguous turns can be connected in parallel, with one only resonance condenser at the oulet from the same parallel. It is possible also to provide a resonance condenser downstream a complex of any number of contiguous turns in series connected.
  • the circuit of the vector B in space is better utilized. Sill better it is utilized if the propellers are disposed along the generatrices of a cylinder. In such case the first pile considered would be closed at ring along a circle having axis paralle to x.
  • the arrangement of more Treating Chambers along a Treating Tube, rectilinear or not, as in the propeller here considered, will be called “distribution at aligned Treating Chambers”.
  • the arrangement at more Treating Tubes superimposed or side by side above described, intended to optimize the distribution of the magnetic fields outside the Treating Chambers, will be called “disposition at Treating Tubes side bv side”.
  • a problem can be represented by the tolerability, by the ferrite at ordinary temperatures, of an induction B of 100 mT at the frequency of 100 MHz. Such tolerability is to be experimentally verified.
  • the main can be the following.
  • the consequent increase of the inductive voltage at the turns is technicaly acceptable till, for example, 250000 V.
  • a further increase of the induction with respect to point 3A) can be made possible by inserting a Resonance Condenser at each turn, instead of at each pair of turns. Because of the very high frequency such Resonance Condensers result of very reduced sizes..
  • the scheme of the apparatus is identical to that of BASE PROJECT A. Identical are also the values of frequency (100 MHz) and voltage of the electric field
  • the force acting on a single molecule [F N2 , F 02 ] is calculated, on the basis of the Lorentz formula on a single electron, as product [e-B-v] in absolute value.
  • the waves of the electric field can be replaced by Hertz waves obtained, for example, from a magnetron. Such waves must produce oscillations in the direction of the vector E of the electric field that they replace.
  • a "launcher" 15 of Fig. 4 is of the type of those employed in the microwave ovens.
  • the launcher is to be oriented in such a way as to launch the waves towards the opposite side of the Treating Chamber (in y-direction).
  • Treating Tube for any form of the Treating Tube (rectilinear, circular, helicoidal, etc.),
  • the present invention finds a first application as motor in a pump for liquids.
  • the advantages presented by this technology with respect to the traditional groups [electric motor / centrifugal pump] result considerable, for the following facts:
  • propellers for solid substances in pieces, or in powder, or in suspension in liquids as, for example, wheat in corns, milk in powder, coal powder suspended in water, etc.
  • the present invention has application also as generator of electricity fed by liguids, for which, in general, the same considerations made for the pumping of liquids are valid.
  • the present invention has application also as generator of electricity fed by gases, for which the same considerations made for the compression of gases are valid.
  • the present invention has application also as flow indicator for fluids.
  • An apparatus for the flow measurement of fluids with the technology at dipolar electric moment is constructed as a generator of electricity.
  • Converter that can be, anyway, shared among several indicators and, eventually, with pumps or compressors.
  • the present invention finds utilization also as separator of chemical components from a mixture.
  • Examplex can be for the mixable liquids the stratification of heavy water in the ocean depths (in which the percentage of D 2 0 is higher even by 30% than that existing at the surface), and for gases the stratification of carbon dioxide in the grounds adjacent to the perforations of the geothermal plants.
  • the separation oc components in gas phase is relatively simple, in that in them there can be considered as absent the interactions which are exerted among the molecules of liquids.
  • the determining factor is the differential volumetric thrusts between the two pure components (Archimedes' thrust).
  • the same separation requires absolute absence of turbolence in the mixture and occurs generally very slowly, since the gravity imposes to molecules of different species equal accelerations.
  • the differential volumetric thrust theoretically calculated is contrasted by the interactions among the molecules of the liquid. These interactions have no effect in the total propulsion, while in the differential propulsion they reduce the differential acceleration impressed to two heterolog molecules, in certain cases making very difficult their separation, or even blocking it.
  • the equivalent of a destination tray is a stretch of a Treating Chamber within the Treating Tube into which the mixture of the components to be separated is introduced.
  • the inside of the tube is empty, and this involves enormous simplification and reduction of construction costs with respect to the system at destination columns.
  • the savings in the construction and operation costs are, in the new system, particularly great in the case of gas start mixtures (as nitrogen and oxygen from air), in that it is avoided the process, very expensive, of their preliminary liquefaction. Also for liquid start mixtures the savings in the operating costs are, in the new system with respect to that of the destination, very high, above all for the fact that it is avoided the vaporization of liquids in quantities that can be a multiple even high of that of the liquid of the feed.
  • Another application is the separation of electrolytes from liquids, as is the case, for example, of the desalting of sea watter.
  • the interfacial (or ionic) polarization is utilized. Introducing into a Treating Tube, at an intermediate point, sea water, there are obtained from an end of the Tube a concentrated salt solution, and from the other desalted water.
  • This type of separation would have the advantage represented by arms of dipolar electric moment much greater than those utilizable in the non-ionic polarizations.
  • the migrations of the ions due to an inversion of the electric field are of an order of magnitude higher than that of the displacements considered for the schematic equivalent electron in the other types of polarization.
  • the propeller finds application also for the purification of chemical substances for the purpose of eliminating, up to high grade, impurities from substances for which it is needed to reach an extreme purity, as reagents for analyses.
  • Another industrial application can be that of the separation of the isotopes of atoms, in particular the separation of the isotopes of hydrogen and uranium.
  • the separation of the isotopes of hydrogen would be made on hydrogen in the combined state, as water (mixture of H 2 0, D 2 0 e T 2 0) in liquid phase.
  • the separation of the isotopes of uranium can be executed on uranium in form of hexafluoride in gas phase.
  • the separation is to be made as in Base Project B, with the following particularities.
  • the Treating Tube very long, as in the case of the isotopes of hydrogen, it is introduced, at an intermediate point, the crude uranium hexafluoride in gas form at the pressure, for example, of 10 Kg/cm 2 eff. Once filled the tube, all its openings are closed and the gas in the inside is left in absolute stillness for a time, for example, of 10'. Then the two ends of the tube are opened obtaining from one of them hexafluoride of U235 enriched at 99%.
  • the process can be made continuous by introducingh the mixture of the feed and extracting the two components at extremely low velocities.
  • the Lorentz forces on the molecules of the substance under treatment are produced by subjecting the same molecules to a combination of a magnetic field and one electric alternating and isofrequential.
  • the velocity necessary for the production of the Lorentz force on a molecule is obtained by displacing, at each inversion of the electric field, the positive and negative electric charges of the same molecule utilizing its dipolar electric moment. The motion of these electric charges can be seen as an intra-atomic motion of electrons.
  • the combination magnetic field/electric field can be replaced by another [magnetic field - Hertz waves].

Landscapes

  • Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Fluid Mechanics (AREA)
  • Physical Or Chemical Processes And Apparatus (AREA)

Abstract

L'invention porte sur un dispositif électromagnétique pour accélérer des molécules électriquement neutres d'une substance, lequel dispositif est caractérisé par le fait qu'il comprend : - un tube de traitement (14) en un matériau non conducteur, dans lequel la substance devant être traitée est introduite ; - des circuits électromagnétiques statiques qui entourent le tube de traitement ci-dessus, exerçant sur la substance devant être traitée des actions électromagnétiques qui poussent celle-ci axialement, par l'utilisation du moment électrique dipolaire des molécules. Le procédé de traitement de molécules accélère lesdites molécules en utilisant leur moment électrique dipolaire faible, les soumettant à une combinaison d'un champ magnétique et d'un champ électrique, ou, en variante, d'un champ magnétique et de l'une parmi des ondes de hertz, alternatives et isofréquentielles, en utilisant la force d'électrologie de Lorentz.
PCT/IT2010/000446 2009-11-09 2010-11-09 Appareil électromagnétique mécaniquement statique pour accélérer des molécules électriquement neutres en utilisant leur moment électrique dipolaire WO2011055403A1 (fr)

Applications Claiming Priority (4)

Application Number Priority Date Filing Date Title
IT000090A ITPR20090090A1 (it) 2009-11-09 2009-11-09 Dispositivo elettromagnetico statico per accelerare molecole elettricamente neutre utilizzando il loro momento dipolare
ITPR2009A000090 2009-11-09
ITPR2010A000082 2010-11-04
IT000082A ITPR20100082A1 (it) 2010-11-04 2010-11-04 Dispositivo elettromagnetico meccanicamente statico per accelerare molecole elettricamente neutre utilizzando il loro momento elettrico dipolare

Publications (1)

Publication Number Publication Date
WO2011055403A1 true WO2011055403A1 (fr) 2011-05-12

Family

ID=43805730

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/IT2010/000446 WO2011055403A1 (fr) 2009-11-09 2010-11-09 Appareil électromagnétique mécaniquement statique pour accélérer des molécules électriquement neutres en utilisant leur moment électrique dipolaire

Country Status (1)

Country Link
WO (1) WO2011055403A1 (fr)

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4663932A (en) * 1982-07-26 1987-05-12 Cox James E Dipolar force field propulsion system
DE4114772A1 (de) * 1991-05-06 1992-11-12 Kaufmann Klaus Verfahren und einrichtung zum foerdern eines elektrisch polarisierte molekuele zumindest enthaltenden mediums
US20080142729A1 (en) * 2006-12-15 2008-06-19 Mks Instruments, Inc. Inductively-coupled plasma source

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4663932A (en) * 1982-07-26 1987-05-12 Cox James E Dipolar force field propulsion system
DE4114772A1 (de) * 1991-05-06 1992-11-12 Kaufmann Klaus Verfahren und einrichtung zum foerdern eines elektrisch polarisierte molekuele zumindest enthaltenden mediums
US20080142729A1 (en) * 2006-12-15 2008-06-19 Mks Instruments, Inc. Inductively-coupled plasma source

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
L.T. WOOD: "Electromagnetic acceleration of neutral molecules", AMERICAN JOURNAL OF PHYSICS, vol. 42, no. 11, 1 November 1974 (1974-11-01), USA, pages 1020, XP008121290 *
R.W. SCHMIEDER: "An electromagnetic acceleration correction to the Debye relaxation time in a polar liquid", AMERICAN JOURNAL OF PHYSICS, vol. 31, no. 11, 1 November 1963 (1963-11-01), USA, pages 885 - 886, XP008121334 *

Similar Documents

Publication Publication Date Title
Yamada et al. Isotope effect on energy confinement time and thermal transport in neutral-beam-heated stellarator-heliotron plasmas
EP3127233A1 (fr) Système de stockage d'énergie inertielle et schéma de transformateur de puissance hydro-fluoro-éther pour des systèmes de puissance radar et chargement de grand pfn
US11642645B2 (en) Conversion of natural gas to liquid form using a rotation/separation system in a chemical reactor
CA1059946A (fr) Procede de conversion de carburants naturels en produits gazeux, sous l'action d'un rechauffeur a arc
US9462669B2 (en) Plasma confinement device
CN101553973A (zh) 电磁推进力系统
AU2003236884A1 (en) Particle separation
US20110253542A1 (en) Static electromagnetic apparatus for accelerating electrically neutral molecules utilizing their dipolar electric moment
WO2011055403A1 (fr) Appareil électromagnétique mécaniquement statique pour accélérer des molécules électriquement neutres en utilisant leur moment électrique dipolaire
US9125288B2 (en) Ion-mode plasma containment
Kawahira et al. The effect of an electric field on boiling heat transfer of refrigerant-11-boiling on a single tube
US3310689A (en) Production of electrical energy
WO2010055540A1 (fr) Appareil electromagnetique statique concu pour accelerer des molecules electriquement neutres a l'aide de leur moment electrique dipolaire
US4305783A (en) Tokamak with liquid metal toroidal field coil
ITPR20100082A1 (it) Dispositivo elettromagnetico meccanicamente statico per accelerare molecole elettricamente neutre utilizzando il loro momento elettrico dipolare
KR20060105402A (ko) 핵융합 촉진 방법 및 이를 이용한 핵융합 장치
CN201860504U (zh) 粒子感应加速器
ITPR20090090A1 (it) Dispositivo elettromagnetico statico per accelerare molecole elettricamente neutre utilizzando il loro momento dipolare
Ruan et al. A novel natural circulation evaporative cooling system for super-high power intensity ECR ion sources
CA1185020A (fr) Reacteur thermonucleaire et procede d'exploitation
Mailfert et al. Magnetic compensation of gravity in fluids: performance and constraints
Ryzhov et al. The model of plasma-electronic technology of producing electricity from electron beams
Borisevich et al. Calcium Isotope Separation in a Hot-Wall Plasma Centrifuge
Ropoša et al. Application of voltage stabilizer in Slovenian low voltage grid
US20190043632A1 (en) Light-Nuclei Element Synthesis

Legal Events

Date Code Title Description
121 Ep: the epo has been informed by wipo that ep was designated in this application

Ref document number: 10805514

Country of ref document: EP

Kind code of ref document: A1

NENP Non-entry into the national phase

Ref country code: DE

122 Ep: pct application non-entry in european phase

Ref document number: 10805514

Country of ref document: EP

Kind code of ref document: A1