TW201338821A - Molecules-magnetization generator - Google Patents

Abstract

The present invention provides a molecules-magnetization generator comprising a main structure, a magnetic material and a magnetic generating coil. The main structure has a hollow area. The magnetic material is configured on the inner side of the main structure. The magnetic generating coil is configured on the outer side of the main structure for promoting magnetic field intensity inside the hollow area.

Description

Molecular magnetization generator

The present invention relates to magnetic field generators, and more particularly to a molecular high magnetization generator.

A magnetic field that changes over time or does not change over time has a certain size and a certain direction, which may be different at any two points in space. Magnetic fields that change over time may also have different directions and sizes at different points in the same time; magnetic fields that do not change over time remain constant at the same point. The two most common giant magnet sources are permanent magnets and conductors with current. At present, both experimental and theoretical proofs indicate that there is no substantial difference in the fields produced by the two magnetic sources. In fact, the main mechanism of magnetic field generation is the same for both types of magnetic sources.

The uniform magnetic field space plays an important role in physical experiments, materials science, and medical applications. The uniformity of the magnetic field space is the difference between the maximum and minimum values of the magnetic field in the magnetic field space divided by the average. Conventional techniques for generating a uniform magnetic field space are achieved by a solenoid coil magnetic field generator or a Helmholtz coil magnetic field generator.

It is well known that magnetic fields and electric fields affect biological tissues. Magnetic fields and electric fields have been used to fight disease and the body parts of wounds, and they also hope that they can do their best. An example of such treatment is disclosed in U.S. Patent No. 3,915,151, which is primarily directed to the treatment of ruptured bones and uses a preferred flat coil to create a magnetic field that is oriented longitudinally to the treatment object, i.e., parallel to the foot or hand. In one embodiment, an electrostatic field is introduced in addition to the magnetic field. This is accomplished by two oppositely opposed electrodes applied to the electrode at a relatively high potential difference voltage. The electric field provided herein flows through the treatment object at a right angle to the magnetic field flow. The charged particles in the treatment zone are brought to an oscillating state of motion by supplying a voltage that varies in amplitude. Due to the magnetic field and the direction of flow of an electric field, the charged particles will only oscillate at a right angle to the skeletal structure and thus perpendicular to the direction of flow of the main blood of the treatment object. The venous blood flow, that is, the blood flow to the heart, is not affected by this treatment.

The function of electromagnetic therapy equipment is based on generally accepted laws of physics and chemistry and findings within the scope of medical research. This theoretical basis is especially the result of a combination of magnetohydrodynamics and protomorphology, which is revealed in Jackson's "Classical Electrodynamics" by Princeton University and "Vacuum Gas Electro-Physics" by Lyman Spitzer.

Based on the magnetic field generator described above and its use, the present invention further provides a novel molecular high magnetization generator.

In view of the above disadvantages, it is an object of the present invention to provide a molecular high magnetization generator which can generate a high efficiency spiral magnetic field.

It is still another object of the present invention to provide a molecular high magnetization generator whereby magnetic field resonance effects can be produced.

An embodiment of the present invention provides a molecular high magnetization generator, comprising: a structure, a magnetic material, and a magnetic field generating coil, the structure having a hollow portion, the magnetic material being disposed inside the structure The magnetic field generating coil is disposed on an outer surface of the structure to increase the magnetic field strength of the hollow portion.

The structure is a hollow cylinder, and the inner layer is a hollow cylinder type magnetostatic.

In one embodiment, the molecular high magnetization generator of the present invention can be used in the treatment of biological tissues.

The invention will be described in conjunction with the embodiments and the accompanying drawings. It is to be understood that all of the embodiments of the invention are illustrative and not intended to be limiting. Therefore, the invention may be applied to other embodiments in addition to the embodiments described herein. The invention is not limited to any embodiment, but should be determined by the scope of the appended claims and their equivalents.

The first figure shows a schematic diagram of the direction of magnetic lines of force in a current. When a current is passed through a carrier, the magnetic field generated around the carrier can be determined according to Biot-Savart Law. With a magnetostatic approximation, when the current slowly changes with time (for example, when the current-carrying wire moves slowly), the magnitude, direction, and distance of the magnitude of the magnetic field can be approximated by using the Biu-Salvar law. In addition, in a current-carrying wire, the direction of the magnetic field lines and the direction of the current in the circuit can be determined according to the right hand of Ampere. For example, in a vertical downward current, the direction of the magnetic flux generated by the current is a clockwise direction; and in a solenoid coil that inputs a current from the bottom to the top, the magnetic flux direction generated by the current coil It is from left to right.

The second figure shows a schematic structural view of a molecular high magnetization generator of the present invention. As shown in the second figure, in the present embodiment, the molecular high magnetization generator 100 includes a structure 100a, a magnetostatic magnetic material 101, and a moving magnetic field generating coil 103. The structure 100a is a hollow cylinder having a hollow portion 105. The magnetic material 101 is placed on the inner layer 102 of the structure 100a, and the magnetic field generating coil 103 is disposed on the outer surface 104 of the structure 100a. In one embodiment, the inner layer 102 is a hollow cylinder type magnetostatic, the magnetic material 101 of the inner layer 102 may be included in the inner ring (surrounding) portion of the structure 100a, or the magnetic body 101 is external. The independent magnetic body of the structure 100a is embedded in the inner space. In one embodiment, the magnetic field generating coil 103 is a solenoid coil disposed on the outer surface 104 of the structure 100a. In one embodiment, in order to keep the coils of the solenoids in place, two sides of the insulating material may be disposed on the surface of each side of the solenoid.

In some substances, the magnetic moments generated by the orbiting and rotating electrons do not completely cancel each other, so the atoms and molecules in these substances contain the average magnetic moment of the net value. The applied magnetic field causes the magnetic moments of the molecules to line up in the direction of the applied magnetic field, thus increasing the magnetic flux density. However, when the magnetic moments of the molecules are arranged, they are hindered by the force of random thermal vibration. This effect produces a slight amount of bonding, while the amount of flux density that can be increased is relatively small. The substance having the above characteristics is a weak magnetic material. Weak magnetic materials usually have very small positive magnetic susceptibility, such as aluminum, magnesium, titanium, tungsten, etc., with a magnetization constant of about 10 ^-5 orders.

The weak magnetic of weak magnetic materials is mainly due to the magnetic bipolar distance of the electrons that rotate. The driving force is generated by an applied magnetic field to align the molecular magnetic dipole moments. However, this driving force is resisted by the interference effect caused by thermal vibration. The effect of weak magnetic is closely related to temperature. When the temperature is low and there is a small amount of thermal collision, the strength of the weak magnetic field is strong.

The magnetization constant of a ferromagnetic material is several orders of magnitude larger than the magnetization constant of a weakly magnetic material. Strong magnetic materials, such as iron, cobalt, nickel, etc., are composed of many small magnetic domains. These small magnetic domains can range in size from a few micron to about 1 centimeter (mm), each small magnetic domain. It contains about 10 ¹⁵ or 10 ¹⁶ atoms. These small magnetic domains are affected by the electrons of rotation, even in the absence of an external magnetic field, so that the magnetic poles within them are aligned. In this case, these small magnetic domains are completely magnetized. When a magnetic field is applied to the ferromagnetic material, the boundaries of those magnetic domains (including the magnetic moments lined up with the applied magnetic field) move to increase the volume of the magnetic domains containing the magnetic moments, making the volume of other magnetic domains cut back. Finally, the magnetic flux density will increase. In other words, the strong magnetic properties of ferromagnetic materials are caused by the strong coupling effect between the magnetic bipolar moments of atoms within the magnetic domain.

The magnetostatic magnetic material (magnetic body) 101 of the present invention can be made of a weak magnetic material or a strong magnetic material, and the weak magnetic material or the ferromagnetic material is determined depending on the actual application.

The molecular high magnetization generator 100 of the present invention is formed or disposed on the inner circumference of the structural body 100a using the magnetostatic magnetic material 101, and the magnetic magnetic field generating coil 103 is used as the outer circumference, as shown in the second figure. As described above, in a solenoid coil 103 that inputs a current from the left (right) to the right (left), the direction of the magnetic field lines generated by the solenoid coil 103 is from the lower (upper) to the upper (lower). direction. Under the magnetic field generated by the solenoid coil 103 and the magnetic field generated by the magnetic material 101, a magnetic field resonance effect is generated under the interaction of the two magnetic fields; therefore, an appropriate current is applied to the solenoid coil 103 to be hollow ( The heart portion 105 produces a high efficiency helical magnetic field. Therefore, in order to generate a high-efficiency spiral magnetic field, it is necessary to feed a voltage into the solenoid coil 103 of the molecular high magnetization generator 100. For example, using an input power on average of about 100 w/s (Joules) applied to the solenoid coil 103, a magnetic field strength of about 1 T (10,000 Gauss) is generated in the hollow portion 105.

In the physical environment, any substance can be molecularized under the action of a high-surge spiral magnetic field. For example, a non-ferrous metal causes magnetization, that is, the medium has a relative permeability. ). The permeability of most materials is very close to the permeability coefficient μ _{0 of the} vacuum. However, for magnetic substances containing iron (for example, iron, cobalt, nickel, etc.), the relative magnetic permeability μ _{r is} quite large (for example, 50 to 5000, and even higher than 10 ⁶ for special alloys). Therefore, in the present invention, an object (mass) is placed in the molecular high magnetization generator 100 to cause molecularization to cause magnetization. In an atom or molecule 300, each orbital electron 301 is subjected to an external force to detach (jump off) the original orbital domain, as shown in the third b diagram; when the electron 301 returns to the original orbital domain, the electron is applied. The electromagnetic wave is as shown in the third diagram a; in other words, the molecular bond is subjected to an external force (for example, a magnetic field generated by the molecular high magnetization generator 100), and the bonded molecules are dissociated. Therefore, with the molecular high magnetization generator 100 of the present invention, this effect can be applied to (treating) biological tissues.

The present invention has been described above by way of example, and is not intended to limit the scope of the invention. Modifications and similar configurations made within the spirit and scope of the invention are intended to be included within the scope of the appended claims.

100. . . Molecular high magnetization generator

100a. . . Structure

101. . . Magnetic material

102. . . Inner layer

103. . . Magnetic field generating coil

104. . . External surface

105. . . Hollow part

300. . . Atom or molecule

301. . . Electronic domain

The first figure shows a schematic diagram of the direction of magnetic lines of force in a current.

The second figure shows a schematic diagram of a molecular high magnetization generator in accordance with the present invention.

The third figure a shows a schematic diagram of the electrons in each orbital domain being separated from the original orbit by external forces.

The third figure b shows a schematic diagram of each track domain electronically returning to the original track domain.

100. . . Molecular high magnetization generator

100a. . . Structure

101. . . Magnetic material

102. . . Inner layer

103. . . Magnetic field generating coil

104. . . External surface

105. . . Hollow part

Claims (10)

A molecular magnetization generator, comprising: a structure, a magnetic material, and a magnetic field generating coil, the structure having a hollow portion, the magnetic material being disposed in an inner layer of the structure, the magnetic field generating coil being disposed on the The outer surface of the structure to increase the magnetic field strength of the hollow portion. The molecular magnetization generator of claim 1, wherein the structure is a hollow cylinder. The molecular magnetization generator of claim 2, wherein the inner layer is a hollow cylinder type magnetostatic. The molecular magnetization generator of claim 2 or 3, wherein the magnetic material comprises aluminum, magnesium, titanium, tungsten. The molecular magnetization generator of claim 2 or 3, wherein the magnetic material comprises iron, cobalt, nickel. A molecular magnetization generator for use in a biological tissue, comprising: a structure, a magnetic material, and a magnetic field generating coil, the structure having a hollow portion, the magnetic material being disposed in an inner layer of the structure, the magnetic field The generating coil is disposed on an outer surface of the structure to increase the magnetic field strength of the hollow portion. A molecular magnetization generator for use in a biological tissue according to claim 6, wherein the structure is a hollow cylinder. A molecular magnetization generator for use in a biological tissue according to claim 7, wherein the inner layer is a hollow cylinder type magnetostatic. A molecular magnetization generator for use in a biological tissue according to claim 7 or 8, wherein the magnetic material comprises aluminum, magnesium, titanium, tungsten. A molecular magnetization generator for use in a biological tissue according to claim 7 or 8, wherein the magnetic material comprises iron, cobalt, nickel.