WO1991004102A1 - Procede et dispositif d'extraction d'ions par action a distance - Google Patents

Procede et dispositif d'extraction d'ions par action a distance Download PDF

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Publication number
WO1991004102A1
WO1991004102A1 PCT/US1990/005342 US9005342W WO9104102A1 WO 1991004102 A1 WO1991004102 A1 WO 1991004102A1 US 9005342 W US9005342 W US 9005342W WO 9104102 A1 WO9104102 A1 WO 9104102A1
Authority
WO
WIPO (PCT)
Prior art keywords
coil
ions
magnetic flux
diode
electrical charges
Prior art date
Application number
PCT/US1990/005342
Other languages
English (en)
Inventor
Harry Eichler
Panagiotis T. Pappas
Jorge C. Cure
Original Assignee
Harry Eichler
Pappas Panagiotis T
Cure Jorge C
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 US07/446,984 external-priority patent/US5068039A/en
Application filed by Harry Eichler, Pappas Panagiotis T, Cure Jorge C filed Critical Harry Eichler
Publication of WO1991004102A1 publication Critical patent/WO1991004102A1/fr

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Classifications

    • A—HUMAN NECESSITIES
    • A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61N—ELECTROTHERAPY; MAGNETOTHERAPY; RADIATION THERAPY; ULTRASOUND THERAPY
    • A61N2/00—Magnetotherapy
    • A61N2/02—Magnetotherapy using magnetic fields produced by coils, including single turn loops or electromagnets
    • 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

Definitions

  • the invention relates to a method and device for dispersing ions by remote action.
  • Szent-Gyorgyi observed the importance of the ratio D/A in the cells, wherein D stands for substanc ⁇ es that donate electrons, while A stands for substances that accept electrons. This is seen, for example, from the three publications by Szent-Gyorgyi mentioned above. He observed that when D/A «l, the cells remain in the resting phase. On the other hand when D/A>1, the cells go into the miotic phase. Szent-Gyorgyi also observed experimentally that the introdction of acceptors in the blood stream of mice with a particular type of cancerous tumors, arrested the growth of the same. The introduction of donors in the body of the affected organism do not produce any significant effect because the cells are rich in donors.
  • a device for removing ions and/or electrical charges inside materials by remote action comprising first means for producing magnetic flux being spaced from a material from which ions and/or electri ⁇ cal charges are to be removed, second means surrounding the material for eliminating and/or smoothing the negative (decreasing) phase of the magnetic flux, and means for short circuiting the second means.
  • the first means may be a first electrically powered coil
  • the second means may be a second coil
  • the short circuiting means may be a diode short circuiting the second coil.
  • the coils are connected together or the coils form one coil or one of the coils is part of the other of the coils.
  • the diode is a rectifying diode.
  • a first movable arm on which the first coil is disposed, a second arm on which the second coil is disposed, a surface below the second coil for supporting the material, and means for supplying electrical power to the first coil.
  • a capacitor filter connected to the electrical power supplying means, a rheostat connected to the capacitor filter, a capacitor bank connected to the rheostat, and a spark gap disposed between the capacitor bank and the first coil.
  • a method for removing ions and/or electrical charges inside materials by remote action which comprises producing magnetic flux with a first electrically powered coil spaced from a material from which ions and/or electrical charges are to be removed, surrounding the material with a second coil spaced from said first coil and short circuited by a diode, and eliminating and/or smoothing the negative (decreasing) phase of the magnetic flux with the second coil.
  • An advantage of the invention proposed herein is that of being non-invasive, making its application ideal to disperse ions in biological matter.
  • Fig. 1 is a fragmentary, diagrammatic, perspective view of the remote action ion dispersing device according to the invention
  • Fig. 2 is a perspective view of part of the device of Fig. 1 showing the magnetic lines;
  • Fig. 3 is an equivalent schematic circuit diagram of the device
  • Fig. 4 is a cross-sectional view of the coil of the device with an equivalent schematic circuit diagram
  • Fig. 5 is a graph of the potential induced by the device.
  • a first main coil 1 which is mounted on an arm that is movable in the direction of the arrows and to which an intermittent current is supplied with a fast rise time, i.e., a square or triangu ⁇ lar pulse, from an electrical source 8 or from the discharge current of a charged capacitor.
  • a movable table 7 made of insulating material is disposed above or below the coil 1.
  • a material or the object containing a region 2 in which ions are to be dispersed is disposed on top of the table 7. As seen in Figs.
  • the coil 1 is accordingly located in such a way that its magnetic lines B, which have been given reference numeral 3, pass through the region 2, or in other words the region 2 is placed close to the perimeter of a concentric magnetic potential A of the coil 1, which has been given reference numeral 4.
  • the coil 5 is short circuited with a fast recovery, high tension and high power diode 6.
  • the polarity of the diode 6 depends on the direction of the current which is desired to be induced in the region 2.
  • the current in the region 2 is opposite to the current in the coil 5, which corresponds to the conducting current in the diode 6.
  • the polarity of the coil 1 is chosen in such a way as to have the initial current thereof opposite to the desired induced current in the region 2.
  • the function of the device is as follows: When a high surge voltage is supplied to the coil, then a rapidly rising current flows. At the same time an induced current appears on every conducting surface, or in every conducting volume, that opposes the increase of the magnetic flux in the coil l, according to The Lenz Rule of Electromagnetism. During this phase, the coil 5 remains inactive, because the diode 6 connected thereto is polarized not to conduct. However, ions are displaced towards a particular direction in the region 2 from which they are desired to be dispersed. Immediately after this, and as a rule, the current in the coil 1 will be set into oscillations that will depend on the frequency of the natural resonance thereof. During those periods, the current in the coil 1 will be decreasing.
  • the coil 5 will start conducting a current again to maintain the existing magnetic flux, according to The Lenz Rule. In this way, the coil 5 considerably delays the fall of the initial flux through the region 2 while the coil 1 continues to execute damping oscillations. Finally, the magnetic flux through the region 2 will fall to zero, after a time which will mainly depend on the self inductance and resistance of the coil 5: t « L/R.
  • the device is expected to operate effectively as a "DC inductor” or “DC transformer”, so to speak, with respect to any non-1inearly conducting medium, (or medium with non-constant ohmic resistance) , by appropriately choos ⁇ ing the parameters of the coils 1 and 5, as well as the voltage and internal resistance of the power supply.
  • the amount of transported charges increases with the repetition of the function cycle of the device, i.e. by repeating the voltage surges in the coil 1.
  • the transported or dispersed charge is a function of the time of operation of the device.
  • the electrical diagram of the working model of the device is given in the Fig. 3.
  • the electrical source or power supply 8 is formed of an adjustable source of voltage supplying 500 to 16,000 volts and a capacitor filter of luF, 20 kv.
  • the power supply is connected through a rheostat 9, to the main device which is formed of a specially constructed capacitor bank 10, which has the following characteristics: very fast discharge time, very high power, very low internal resistance and parasitic self inductance, and is made of two cooper sheets which are 0.3 mm thick, 1 m 2 in area and are separated by a sheet of glass which is 3 mm thick and has the same area, as well as a spark gap 11 with an adjustable gap distance, that are connected as shown in the diagram of Fig. 3.
  • the coil l is formed of several turns which are 40 cm in diameter of insulated copper wire being 4 mm in diameter.
  • the coil 5 is formed of about 1000 turns of 80 cm in diameter of enamel copper wire being 2 mm in diameter.
  • a sample object used in one of the examples or trials for dispersing the ions thereof is formed two small uncharged capacitors A and B of luF given reference numeral 12, which are connected through a non-linear resistor or varistor 13 as shown in Fig. 4 and placed inside the coil 5 at a distance of 50 cm from the coil 1.
  • the power supply was adjusted to charge the capacitor 10 causing arc discharge in the spark gap 11 approximately every 0.3 seconds.
  • the capacitors A and B given reference numeral 12 were immediate ⁇ ly measured with a volt meter.
  • the capacitor A was found charged in the forward direction by several tenths of a volt and the capacitor B in the reverse direction by several hundredths of a volt.
  • the difference in the charges is explained by the expected dielectric leakage of the capacitor B, charged in the reverse direction.
  • no systematic charge was found in the capacitors A and B, contrary to what was observed before. The difference was distinct and considerable.
  • the advantages of the device are the following:
  • the basis of the operation thereof is the production of the waveform of the induced potential in the diagram of Fig. 5. It appears as though the production of such a waveform with another electronic device is not possible or easy, because a consid ⁇ erably large power of several K watts is required for sub ⁇ stantial results in practice. In such a case, any coil which would have the power to produce a predetermined form of magnetic flux, would carry parasitic oscillations or would have produced unwanted components of tension in the induced potential.
  • the effec ⁇ tiveness of the coil 5 and the diode 6 is so great that regardless of the form of magnetic flux which the coil 1 is producing, the induced potential in the region 2 is almost always of the desired form in the diagram of Fig. 5.
  • the coil 1 may even be powered by a perfect sinusoidal tension of a definite frequency (i.e. it may be powered with the mains frequency, or by a power of a much higher frequency) , for avoiding nearby unwanted interference, with satisfactory results for the induced tension in the region 2.
  • the induced tension of the diagram of Fig. 5 appears only near the region 2 and not all over the effective space surrounding the coil 1, where it would cause unwanted induced induction to the operators of the device or to other objects outside the region 2.
  • the power which the coil 5 and the diode 6 absorb, is a small fraction of the power of the coil 1 (of several Kwatts) . In this way, the coil 5 and the diode 6 with the high requirements thereof may easily cope with the stress of a much lower power.
  • the field of the coil 1 is modified to the minimum required degree, which will cause minimum interfer ⁇ ence in the case of a sinusoidal power supply.
  • the device according to the invention is clearly superior for it requires no invasion or entry into the region 2, such through the use of electrodes or chemical substances, for example.
  • the expected applications extend to a large spectrum of technology and science, where charge or ion transport is required to occur in regions which are not easily accessible, in biology, medicine, the chemical industry, Electrolysis, electrolytic metal plating, electrolytic casting, direct current power supply and energy, without using direct con ⁇ tacts, or in general, where a DC transformer, or a DC induc ⁇ tor, is required.

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  • Health & Medical Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Biomedical Technology (AREA)
  • Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
  • Radiology & Medical Imaging (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Animal Behavior & Ethology (AREA)
  • General Health & Medical Sciences (AREA)
  • Public Health (AREA)
  • Veterinary Medicine (AREA)
  • Physical Or Chemical Processes And Apparatus (AREA)

Abstract

Procédé et appareil d'extraction d'ions et/ou de charges électriques de l'intérieur de matériaux par une action à distance. Le procédé et l'appareil consistent à utiliser une première bobine (1) espacée d'un matériau (2) duquel on veut extraire des ions et/ou des charges électriques, la première bobine produisant un flux magnétique, ainsi qu'une seconde bobine (5) entourant le matériau et étant espacée de la première bobine pour éliminer et/ou lisser la phase négative du flux magnétique, et une diode court-circuitant la seconde bobine.
PCT/US1990/005342 1989-09-20 1990-09-19 Procede et dispositif d'extraction d'ions par action a distance WO1991004102A1 (fr)

Applications Claiming Priority (4)

Application Number Priority Date Filing Date Title
GR890100595 1989-09-20
GR89100595 1989-09-20
US446,984 1989-12-06
US07/446,984 US5068039A (en) 1989-09-20 1989-12-06 Method and device for dispersing ions by remote action

Publications (1)

Publication Number Publication Date
WO1991004102A1 true WO1991004102A1 (fr) 1991-04-04

Family

ID=26316658

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/US1990/005342 WO1991004102A1 (fr) 1989-09-20 1990-09-19 Procede et dispositif d'extraction d'ions par action a distance

Country Status (2)

Country Link
AU (1) AU6421390A (fr)
WO (1) WO1991004102A1 (fr)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1995019217A1 (fr) * 1994-01-17 1995-07-20 Martin Koch Processus sans contact de transport d'ions et d'humidite dans des materiaux poreux et appareil realisant ce processus
WO2002026322A1 (fr) * 2000-09-29 2002-04-04 Delisle Clarence A Appareil de traitement des malaises corporels
US7963904B2 (en) 2000-09-29 2011-06-21 Delisle Clarence A Method and device for treating body ailments

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2736843A (en) * 1952-07-25 1956-02-28 Cutler Hammer Inc Alternating current electromagnets
US3337776A (en) * 1964-06-10 1967-08-22 Guidoni Biomedical apparatus for generating controllable magnetic fields
US3703958A (en) * 1969-08-11 1972-11-28 Massachusetts Inst Technology Eddy current apparatus and method of application to a conductive material
US4369345A (en) * 1977-11-11 1983-01-18 Czerlinski George H Method of and apparatus for selective localized differential hyperthermia of a medium
US4458153A (en) * 1982-09-13 1984-07-03 Wesley Richard H Organism destruction by electrohydraulic discharge within a pulsed magnetic field envelope
WO1988005763A1 (fr) * 1987-01-28 1988-08-11 Philippe Niessen Traitement de liquides et de tissus biologiques par induction magnetique
US4818697A (en) * 1986-10-27 1989-04-04 Life Resonances, Inc. Techniques for enhancing the permeability of ions through membranes

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2736843A (en) * 1952-07-25 1956-02-28 Cutler Hammer Inc Alternating current electromagnets
US3337776A (en) * 1964-06-10 1967-08-22 Guidoni Biomedical apparatus for generating controllable magnetic fields
US3703958A (en) * 1969-08-11 1972-11-28 Massachusetts Inst Technology Eddy current apparatus and method of application to a conductive material
US4369345A (en) * 1977-11-11 1983-01-18 Czerlinski George H Method of and apparatus for selective localized differential hyperthermia of a medium
US4458153A (en) * 1982-09-13 1984-07-03 Wesley Richard H Organism destruction by electrohydraulic discharge within a pulsed magnetic field envelope
US4818697A (en) * 1986-10-27 1989-04-04 Life Resonances, Inc. Techniques for enhancing the permeability of ions through membranes
WO1988005763A1 (fr) * 1987-01-28 1988-08-11 Philippe Niessen Traitement de liquides et de tissus biologiques par induction magnetique
US4938875A (en) * 1987-01-28 1990-07-03 Philippe Niessen Method and apparatus for magnetically treating a liquid

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1995019217A1 (fr) * 1994-01-17 1995-07-20 Martin Koch Processus sans contact de transport d'ions et d'humidite dans des materiaux poreux et appareil realisant ce processus
WO2002026322A1 (fr) * 2000-09-29 2002-04-04 Delisle Clarence A Appareil de traitement des malaises corporels
US7963904B2 (en) 2000-09-29 2011-06-21 Delisle Clarence A Method and device for treating body ailments

Also Published As

Publication number Publication date
AU6421390A (en) 1991-04-18

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