JP5273598B2 - Water electromagnetic field treatment method and electromagnetic field treatment apparatus - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a method and an apparatus for simply treating water in an electromagnetic field with high economic efficiency and general versatility. <P>SOLUTION: For example, a coil 2 is provided outside of a water pipe 1 in a water channel to flow water 3 to be treated therethrough, and the coil 2 is supplied with a specific AC current having a specific frequency or a specific peak current from an AC power supply 4, wherein one resonance frequency is selected as the specific frequency of the AC current from a resonance frequency group including a plurality of resonance frequencies. A resonance magnetic field is thus induced in the water channel by the above specific peak current. By the electromagnetic field treatment imparting to the water 3 to be treated an oscillating electromagnetic field induced by such a specific AC current, activated treated water 5 can be obtained easily with high efficiency. <P>COPYRIGHT: (C)2008,JPO&amp;INPIT

Description

  The present invention relates to an electromagnetic field treatment method and an electromagnetic field treatment apparatus for water that efficiently generate functional water.

  Conventionally, various methods of physicochemical treatment have been studied in order to enhance the function of water. For example, it has been well known that an aqueous solution is subjected to electrolytic treatment to produce acid water having a sterilizing and cleaning function, or electrolytic reduced water containing abundant hydrogen. In addition, by applying electromagnetic field treatment to water, for example, the water cluster is divided into small parts to change the properties of the water (see, for example, Patent Document 1). A technique that does not attach a scale or the like to flowing pipes or toilet facilities, boiler facilities, wastewater treatment facilities, etc. has been put to practical use (see, for example, Patent Document 2). Water that is activated by subjecting such normal water to physicochemical treatment is called functional water.

In the electromagnetic field treatment method for generating the functional water, for example, in Patent Document 1, an electric field based on a pulsed voltage, or an electric field and a magnetic field thereof are applied to the water to be treated. Moreover, in patent document 2, the alternating current from which a frequency changes temporally in the band of 20 Hz-1 MHz is sent, for example to the coil wound around the outer side of piping. Here, the electron energy generated by the frequency modulation control gives electrolytic energy to the fluid flowing in the pipe by using fluid molecules and ions in the fluid as a medium. Then, the surface of the scale and the inner wall of the pipe are strongly negatively charged, the scale and the inner wall of the pipe repel each other, the scale becomes small crystallized, the bond becomes unstable, and the scale is easily detached from the inner wall of the pipe. Alternatively, the generated electrons eventually change the red rust generated on the inner wall of the steel pipe into stable black rust, thereby preventing the progress of the corrosion reaction.
JP 7-68266 A JP 2000-212782 A

  However, in the electromagnetic field treatment method as described above, the effect may not be sufficiently generated depending on the type of the aqueous solution that is the water to be treated. In addition, there are cases where the prevention / removal or rust prevention of scale adhesion by electromagnetic field treatment is almost impossible. Therefore, for example, in Patent Document 2, it is necessary to test the effect of the modulated electric field treatment through a desktop test in advance before performing the electromagnetic field treatment on the water to be treated. For this reason, the electromagnetic field treatment method is extremely complicated and has low operability, and the conditions for the modulated electric field treatment need to be changed depending on the type of water to be treated, so that its versatility is poor. It was.

  The above problems are caused by little physicochemical elucidation regarding the mechanism of functional water generation by electromagnetic field treatment of water. So far, many other proposals have been made on the method of generating functional water by electromagnetic field treatment of water, but it is difficult to analyze the mechanism of functional water generation by experimental science, and the reliability of the electromagnetic field treatment method itself is questioned. There were not a few proposals to see.

  The present invention has been made in view of the above circumstances, and based on experimental scientific grounds, has a simple and highly economical and versatile, electromagnetic field treatment method for water that generates functional water with high efficiency and An object is to provide an electromagnetic field processing apparatus.

  The inventor conducted detailed experiments on the ability to dissolve activated treated water activated by applying an electromagnetic field treatment that vibrates against water. Then, in the activation of water by treatment of an oscillating electromagnetic field induced by an electromagnetic field induced current such as an alternating current flowing in the coil, it is found that there is a resonance frequency in the frequency of the electromagnetic field induced current, and the value of the resonance frequency Measured. Moreover, the experimental new fact was acquired about the peculiarity of the above-mentioned resonance frequency in activation of water. The present invention has been made based on these new findings.

  In order to achieve the above object, an electromagnetic field treatment method for water according to a first aspect of the invention activates the water by passing an electromagnetic field induced current through a coil and applying an oscillating electromagnetic field induced in the coil to the water. In the electromagnetic field treatment method for water, one resonance is selected from the first resonance frequency group of the electromagnetic field induced current that activates the water or the second resonance frequency group of the electromagnetic field induced current that activates the water. A frequency is selected, and an oscillating electromagnetic field is induced in the coil by an electromagnetic field induced current having one selected resonance frequency.

  And the electromagnetic field processing method of the water concerning 2nd invention is the electromagnetic field processing method of the water which sends an electromagnetic field induction current to a coil, gives the vibration electromagnetic field induced to the said coil to water, and activates the said water Selecting one resonance frequency from a first resonance frequency group of the electromagnetic field induced current that activates the water or a second resonance frequency group of the electromagnetic field induced current that activates the water, and The configuration is such that an oscillating electromagnetic field is induced in the coil by an electromagnetic field induced current having a frequency within a half-value width in the resonance characteristic of the selected resonance frequency.

  And the electromagnetic field treatment method for water according to the third aspect of the invention is an electromagnetic field treatment method for water that activates the water by applying an electromagnetic field induced current to the coil and applying an oscillating electromagnetic field induced in the coil to the water. Selecting one resonance frequency from each of the first resonance frequency group of the electromagnetic field induced current that activates the water and the second resonance frequency group of the electromagnetic field induced current that activates the water, An oscillating electromagnetic field is induced in the coil by an electromagnetic field induced current having one resonance frequency selected from the first resonance frequency group and an electromagnetic field induced current having one resonance frequency selected from the second resonance frequency group. It has the structure of

  And the electromagnetic field processing method of the water concerning 4th invention is the electromagnetic field processing method of the water which flows the electromagnetic field induction electric current through a coil, gives the vibration electromagnetic field induced by the said coil to water, and activates the said water Selecting one resonance frequency from each of the first resonance frequency group of the electromagnetic field induced current that activates the water and the second resonance frequency group of the electromagnetic field induced current that activates the water, An electromagnetic field induced current having a frequency within the half-value width in the resonance characteristic of the resonance frequency selected from the first resonance frequency group and a half-value width in the resonance characteristic of the resonance frequency selected from the second resonance frequency group. A vibration electromagnetic field is induced in the coil by an electromagnetic field induced current having a frequency.

In the above invention, the first resonant frequency group, resonant frequency _A -2 of 151.5Hz or near the resonant frequency _A -1 of the 222.5Hz or near the resonant frequency _{A 0} of 345.0Hz or near , 484 Hz or its vicinity resonance frequency A ₁ , 954 Hz or its vicinity resonance frequency A ₂ , 3.5 kHz or its vicinity resonance frequency A ₃ , 7.0 kHz or its vicinity resonance frequency A ₄ , 20.0 kHz or its The resonance frequency A ₅ , 37.3 kHz in the vicinity or the resonance frequency A ₆ , 80.0 kHz in the vicinity thereof, or the resonance frequency A _{7 in the} vicinity thereof, and the second resonance frequency group includes resonances in the vicinity of 205.0 Hz. frequency _B -2, the resonance frequency of the 301.0Hz or near the _B -1, 4 6.0Hz or resonant frequency _B 0 in the vicinity thereof, 655Hz or resonant frequency _B 1 near its resonant frequency _B 2 of 1.29kHz or in the vicinity thereof, 4.73KHz or in the vicinity of the resonance frequency _B 3 thereof, 9.47KHz or Resonance frequencies B ₄ and 27.0 kHz in the vicinity thereof, resonance frequencies B ₅ and 50.4 kHz in the vicinity thereof, resonance frequencies B ₆ and 108.0 kHz in the vicinity thereof, or resonance frequencies B _{7 in the} vicinity thereof are included. The nearby resonance frequency is about ± 1.2% of the numerical value of the resonance frequency.

  In the above invention, in a preferred aspect, the peak of the oscillating magnetic field induced in the coil by the electromagnetic field induced current at the resonance frequency is obtained by setting the peak current of the electromagnetic field induced current at the resonance frequency to a specific current value. The strength is set so that the strength of the resonance magnetic field becomes a specific magnetic field strength, or the strength of the magnetic field within the half-value width in the resonance characteristics of the resonance magnetic field. Here, the intensity of the resonant magnetic field is a positive integer multiple of the magnetic field intensity of the fundamental mode.

In the above preferred embodiment, the magnetic field strength of the resonance mode of the resonance magnetic field in the electromagnetic field induced current of the resonance frequency A _i (i = an integer of −2 to 7) is 5.3 mG or Its vicinity, 7.4 mG or its vicinity, 12.3 mG or its vicinity, 17.3 mG or its vicinity, 31.9 mG or its vicinity, 130.6 mG or its vicinity, 323.0 mG or its vicinity, 1123.5 mG or its Near, 2556.0 mG or the vicinity thereof, 6039.0 mG or the vicinity thereof, and the magnetic field intensity of the resonance magnetic field in the electromagnetic field induced current of the resonance frequency B _j (j = integer of −2 to 7) is In the order of the numbers of j, 7.1 mG or its vicinity, 10.4 mG or its vicinity, 3mG or its vicinity, 23.5mG or its vicinity, 47.1mG or its vicinity, 188.2mG or its vicinity, 463.5mG or its vicinity, 1601.0mG or its vicinity, 3342.5mG or its vicinity, 7302.9mG Or the vicinity. The magnetic field strength in the vicinity thereof is about ± 2% of the numerical value of the magnetic field strength.

  Moreover, in the said invention, in a suitable one aspect | mode, the influence of geomagnetism is removed with respect to the said coil. Here, the axial center of the coil is arranged in a plane orthogonal to the direction of the geomagnetism. Alternatively, the coil is encapsulated by a magnetic shield. Alternatively, the magnetic field strength of the geomagnetism in the axial direction of the coil is detected, and a static magnetic field is applied to the coil so that the magnetic field strength becomes substantially zero.

  Furthermore, in the above-mentioned invention, in a preferred aspect, the water is subjected to an electromagnetic field treatment after degassing the carbon dioxide gas.

  Furthermore, in the above-described invention, in a preferred aspect, an insulator is disposed in a water passage in a region where the coil is wound, and the water is subjected to electromagnetic field treatment by changing the flow of the water.

  Alternatively, the electromagnetic field treatment apparatus for water according to the fifth aspect of the invention is an electromagnetic field treatment apparatus for water that activates the water by applying an electromagnetic field induced current to the coil and applying an oscillating electromagnetic field induced in the coil to the water. And one selected from a coil and a first resonance frequency group of the electromagnetic field induced current that activates the water or a second resonance frequency group of the electromagnetic field induced current that activates the water And a power source for supplying an electromagnetic field induced current having a resonance frequency to the coil.

  A water electromagnetic field treatment apparatus according to a sixth aspect of the present invention is a water electromagnetic field treatment apparatus that activates the water by applying an electromagnetic field induced current to the coil and applying an oscillating electromagnetic field induced in the coil to the water. And one selected from a coil and a first resonance frequency group of the electromagnetic field induced current that activates the water or a second resonance frequency group of the electromagnetic field induced current that activates the water And a power source that supplies an electromagnetic field induced current having a frequency within a half-value width in a resonance characteristic of a resonance frequency to the coil.

  And the electromagnetic field processing apparatus of the water concerning 7th invention is an electromagnetic field processing apparatus of the water which sends an electromagnetic field induction current to a coil, gives the vibration electromagnetic field induced by the said coil to water, and activates the said water A coil, a resonance frequency within a first resonance frequency group of the electromagnetic field induced current that activates the water, and a second resonance frequency of the electromagnetic field induced current that activates the water. An alternating current supply unit that supplies an alternating current amplitude-modulated with one resonance frequency in the group and a drive power supply unit that drives the alternating current supply unit are provided.

  An electromagnetic field treatment apparatus for water according to an eighth aspect of the invention is an electromagnetic field treatment apparatus for water that activates the water by passing an electromagnetic field induced current through the coil and applying an oscillating electromagnetic field induced in the coil to the water. A coil, a frequency within a half-value width in a resonance characteristic of one resonance frequency in a first resonance frequency group of the electromagnetic field induced current that activates the water, and the water that activates the water An alternating current supply unit for supplying an alternating current amplitude-modulated with a frequency within a half-value width in the resonance characteristic of one resonance frequency in the second resonance frequency group of the electromagnetic field induced current; and And a drive power supply unit for driving.

In the fifth to eighth inventions, the first resonance frequency group is 151.5 Hz or a resonance frequency A- ₂ , 222.5 Hz in the vicinity thereof, or a resonance frequency A- ₁ , 345.0 Hz in the vicinity thereof, or the same. Resonance frequencies A ₀ and 484 Hz in the vicinity or resonance frequencies A ₁ and 954 Hz in the vicinity thereof, resonance frequencies A ₂ and 3.5 kHz in the vicinity thereof, resonance frequencies A ₃ and 7.0 kHz in the vicinity thereof, or resonance frequencies A _{4 in the} vicinity thereof Resonance frequency A ₅ at or near 20.0 kHz, resonance frequency A ₆ at or near 37.3 kHz, resonance frequency A ₇ at or near 80.0 kHz, and the second resonance frequency group includes 205. 0Hz or in the vicinity of the resonance frequency _B -2 that, 301.0Hz or resonant periphery of the vicinity thereof Number _B -1, 466.0Hz or resonant frequency _B 0 in the vicinity thereof, 655Hz or resonant frequency _B 1 near its resonant frequency _B 2 of 1.29kHz or near, resonance of 4.73kHz or near the frequency _{B 3} , 9.47 kHz or a resonance frequency B ₄ in the vicinity thereof, 27.0 kHz or a resonance frequency B ₅ in the vicinity thereof, 50.4 kHz or a resonance frequency B ₆ in the vicinity thereof, 108.0 kHz or a resonance frequency B _{7 in the} vicinity thereof . The nearby resonance frequency is about ± 1.2% of the numerical value of the resonance frequency.

  In the fifth to eighth aspects of the present invention, in a preferred aspect, the peak current of the electromagnetic field induced current at the resonance frequency is set to a specific current value, so that the coil is induced by the electromagnetic field induced current at the resonance frequency. The peak intensity of the generated oscillating magnetic field is set to be the intensity of the resonant magnetic field that has a specific magnetic field intensity, or the magnetic field intensity that is within the half value width in the resonance characteristics of the resonant magnetic field. Here, the intensity of the resonant magnetic field is a positive integer multiple of the magnetic field intensity of the fundamental mode.

In the above preferred embodiment, the magnetic field strength of the resonance mode of the resonance magnetic field in the electromagnetic field induced current of the resonance frequency A _i (i = an integer of −2 to 7) is 5.3 mG or Its vicinity, 7.4 mG or its vicinity, 12.3 mG or its vicinity, 17.3 mG or its vicinity, 31.9 mG or its vicinity, 130.6 mG or its vicinity, 323.0 mG or its vicinity, 1123.5 mG or its Near, 2556.0 mG or the vicinity thereof, 6039.0 mG or the vicinity thereof, and the magnetic field intensity of the resonance magnetic field in the electromagnetic field induced current of the resonance frequency B _j (j = integer of −2 to 7) is In the order of the numbers of j, 7.1 mG or its vicinity, 10.4 mG or its vicinity, 3mG or its vicinity, 23.5mG or its vicinity, 47.1mG or its vicinity, 188.2mG or its vicinity, 463.5mG or its vicinity, 1601.0mG or its vicinity, 3342.5mG or its vicinity, 7302.9mG Or the vicinity. The magnetic field strength in the vicinity thereof is about ± 2% of the numerical value of the magnetic field strength.

  In the fifth to eighth inventions, in a preferred aspect, means for removing the influence of geomagnetism is attached to the coil.

  According to the configuration of the present invention, it is possible to provide a highly efficient electromagnetic field treatment method for water and an electromagnetic field treatment apparatus that are simple and have high economic efficiency, versatility, and stability.

Several preferred embodiments of the present invention will be described below with reference to the drawings. Here, the same code | symbol is attached | subjected to the mutually same or similar part.
[Embodiment 1]
FIG. 1 is an explanatory diagram of an example of a method for treating water with an electromagnetic field in this embodiment. FIG. 2 is a current waveform diagram showing an example of an alternating current that is an electromagnetic field induced current. As shown in FIG. 1, for example, a coil 2 is provided on the outside of a water pipe 1 made of vinyl chloride, and water to be treated 3 such as tap water and drainage is allowed to flow through the water pipe 1 and will be described later through an AC power source 4. An alternating current having a resonance frequency that is a specific frequency is supplied to the coil 2. Here, it is preferable that the waveform of the alternating current has a sharp temporal change such as a square waveform as shown in FIG.

  Furthermore, although the details will be described later, the AC peak current is set to a specific current value at the resonance frequency. Hereinafter, the induced magnetic field induced in the coil 2 by this specific current value is referred to as a resonant magnetic field. In this way, by applying the oscillating electromagnetic field induced by the alternating current of the specific frequency to the water 3 to be treated, the activated treated water 5 activated with high efficiency by the oscillating electromagnetic field as shown in FIG. Get.

  Alternatively, as shown in FIG. 3, the electromagnetic field applying unit 7 having a coil connected to the AC power source 4 is immersed in the stored water 9 of the tank 8. In this state, an alternating current having a resonance frequency as described above is supplied to the electromagnetic field applying unit 7 through the alternating current power source 4. Alternatively, the AC peak current is set to a specific current value at the resonance frequency. In this way, by applying the oscillating electromagnetic field induced by the alternating current of the specific frequency to the stored water 9, the stored water 9 is activated by the oscillating electromagnetic field to be activated treatment water.

Hereinafter, the above-described resonance frequency and resonance magnetic field will be described in detail. The present inventor supplies alternating currents of various frequencies to a coil having known electromagnetic characteristics, and dissolves calcium phosphate (Ca ₃ (PO ₄ ) ₂ ) in active treated water generated by subjecting tap water to electromagnetic field treatment. Detailed experiments were conducted on the characteristics. Specifically, in this experiment, an experimental apparatus for electromagnetic field treatment as schematically shown in FIG. 4 was used.

In this experimental apparatus, the inside of the experimental tank 10 is divided into three storage chambers 12, 13, and 14 by a partition plate 11. Here, as water to be treated, tap water having a pH value of about 7 and having a pH value of about 7 is used as the water to be treated, and this ion-exchanged water is pump 15 provided in the middle of the water pipe 1. Accordingly, the storage chambers 12, 13, and 14 are circulated in this order. Here, the coil 2 is wound around the outside of the water flow pipe 1 on the downstream side of the pump 15 and connected to the AC power source 4. The coil 2 is formed by uniformly winding a copper wire coil into a cylindrical shape having a winding diameter of 3.5 cmφ over a pipe length of 14.4 cm. In addition, calcium phosphate (Ca ₃ (PO ₄ ) ₂ ) 16, which is hardly soluble in normal water, is placed in powder form at the bottom of the storage chamber 12, and a water collection pipe 17 communicates with the storage chamber 14.

  In the above experiment, since the influence of geomagnetism appears in the experimental result as will be described later, the axis of the coil 2 is set in the east-west direction. In addition, since the influence of ions such as calcium and magnesium in tap water also appears in the above results, the water to be treated was tap water in which an ion exchange resin was passed.

In such an experimental apparatus, the AC power supply 4 has a variable frequency and current of a square-wave AC current. Therefore, under the conditions of various alternating current frequencies and peak currents, the tap water is subjected to electromagnetic field treatment to obtain activated treated water, and calcium hydrogen phosphate ions (Ca) in the activated treated water in the storage chamber 14 are obtained. (HPO ₄ )) The concentration of ^2- was measured. Here, the calcium phosphate 16 is dissolved according to the chemical formula (1) by the active treated water.

  In this way, the solubility of calcium phosphate 16 in the active treated water, that is, the ability to dissolve the active treated water was examined in detail. Moreover, the pH value of the active treated water was also measured. Here, the frequency of the alternating current is examined in the range of 140 Hz to 115 kHz.

The concentration of the first hydrogen phosphate calcium ion is measured by performing an electromagnetic field treatment for a certain period of time (about 10 hours), and then opening the valve of the water collection pipe 17 to collect the active treated water in the storage chamber 14 and using it as a standard solution. It was carried out by a known precipitation titration method using silver nitrate (AgNO ₃ ) and a potassium chromate (K ₂ CrO ₄ ) solution as an indicator.

  As a result, it was found that the solubility of the calcium phosphate 16 increases specifically in a specific frequency band of alternating current as described above. It was also found that the solubility of calcium phosphate 16 increased specifically even at a specific current value of alternating current. A specific frequency and a specific current value in such an alternating current will be collectively described below as a resonance frequency and a resonance magnetic field, respectively.

{Resonance frequency}
In the specific frequency, there are a plurality of two types of resonance frequencies having different properties, which will become apparent from the following description. Therefore, these resonance frequencies are classified into a first resonance frequency group and a second resonance frequency group.
(First resonance frequency group)
As shown in FIGS. 5 to 10, the first resonance frequency group includes at least a plurality of resonance frequencies A _i (i = 1 to 6). Here, FIG. 5 to FIG. 10 show the resonance characteristics of the resonance frequency in the oscillating electromagnetic field processing, and in the frequency band where the solubility of the calcium phosphate 16 shows the specificity, the horizontal axis represents the frequency of the alternating current flowing through the coil 2, The vertical axis represents the solubility of calcium phosphate 16.

From FIG. 5, the resonance frequency A ₁ is 484 Hz or the vicinity thereof, and the range of the half width (Δf) is 462 to 504 Hz. Here, the full width at half maximum (Δf) is a frequency at which the solubility of the calcium phosphate 16 becomes 1/2 or more of the difference between the maximum solubility value and the solubility of untreated water in the resonance frequency band having this specificity. It is a band. Hereinafter, from FIG. 6, the resonance frequency A ₂ is 954 Hz or the vicinity thereof, and the range of the full width at half maximum (Δf) is 915 to 995 Hz. From Figure 7, the resonant frequency _{A 3} is 3.5kHz or in the vicinity thereof, the scope of its half-value width (Delta] f) is 3.25～3.72KHz. From Figure 8, the resonant frequency _{A 4} is a 7.0kHz or in the vicinity thereof, the scope of its half-value width (Delta] f) is 6.46～7.54KHz. 9, the resonant frequency _{A 5} represents a 20.0kHz or in the vicinity thereof, the scope of its half-value width (Delta] f) is 17.3～22.4KHz. Then, from FIG. 10, the resonant frequency _{A 6} is 37.3kHz or in the vicinity thereof, the scope of its half-value width (Delta] f) is 34.9～40.3KHz.

Further, as shown in FIGS. 11 to 13, a resonance frequency A _i (i = integer of −2 to 0) exists in the first resonance frequency group. That is, from FIG. 11, the resonance frequency A- ₂ is 151.5 Hz or the vicinity thereof, and the range of the full width at half maximum (Δf) is 147.5 to 154.7 Hz. From FIG. 12, the resonance frequency A ₋₁ is 222.5 Hz or the vicinity thereof, and the range of the half width (Δf) is 217.2 to 228.1 Hz. From FIG. 13, the resonance frequency A ₀ is 345.0 Hz or the vicinity thereof, and the range of the half width (Δf) is 338.5 to 351.0 Hz.

(Second resonance frequency group)
As shown in FIGS. 14 to 19 and the like, the second resonance frequency group includes at least a plurality of resonance frequencies B _i (i = 1 to an integer of 1 to 6). In these figures, as in the case of FIGS. 5 to 13, the horizontal axis represents the frequency of the alternating current and the vertical axis represents the solubility in the frequency band where the solubility is specific.

From FIG. 14, the resonance frequency B ₁ is 655 Hz or the vicinity thereof, and the range of the half width (Δf) is 606 to 722 Hz. Hereinafter, from Fig. 15, the resonant frequency _{B 2} is 1.29kHz or in the vicinity thereof, the scope of its half-value width (Delta] f) is 1.19～1.38KHz. From Figure 16, the resonant frequency _{B 3} is 4.73kHz or in the vicinity thereof, the scope of its half-value width (Delta] f) is 4.59～4.93KHz. From Figure 17, the resonant frequency _{B 4} is 9.47kHz or in the vicinity thereof, the scope of its half-value width (Delta] f) is 9.06～9.98KHz. From Figure 18, the resonant frequency _{B 5} is 27.0kHz or in the vicinity thereof, the scope of its half-value width (Delta] f) is 25.0～28.9KHz. Then, from FIG. 19, the resonant frequency _{B 6} is 50.4kHz or in the vicinity thereof, the scope of its half-value width (Delta] f) is 49.1～51.8KHz.

Further, in this second resonance frequency group, as shown in FIGS. 20 to 22, a resonance frequency B _i (i = an integer of −2 to 0) exists. That is, from FIG. 20, the resonance frequency B- ₂ is 205.0 Hz or the vicinity thereof, and the range of the half width (Δf) is 201.5 to 208.5 Hz. From FIG. 21, the resonance frequency B- ₁ is 301.0 Hz or the vicinity thereof, and the range of the half width (Δf) is 293.0 to 310.5 Hz. From FIG. 22, the resonance frequency B ₀ is 466.0 Hz or the vicinity thereof, and the range of the half width (Δf) is 457.2 to 474.6 Hz.

Here, the vicinity of the resonance frequency A _i and the resonance frequency B _i (i = integer of −2 to 6) is preferably about ± 1.2% of the numerical value of each of the resonance frequencies. Within this range, a solubility of 80% or more of the solubility at the resonance frequency can be obtained, and there is no problem in practical use of functional water generation.

The reason is currently unknown between the first resonance frequency group and the second resonance frequency group, but it seems to have a certain regularity. For example, the ratio (B _i / A _i ) between the resonance frequency B _i and the resonance frequency A _i is a constant value of approximately 1.35 in an integer i = −2 to 6. This value is expressed as the mass ratio of the hydrogen hydrate ion to the hydroxide hydrate ion, but its truth is unknown at present. Considering these regularities, it is estimated that 80 kHz exists as the resonance frequency A _{7 in} the first resonance frequency group and 108 kHz exists as B _{7 in} the second resonance frequency group. However, in these cases, the alternating current becomes too high and transmission is likely to occur and measurement is not possible.

However, as will be described later, when a positive square pulse waveform current is used instead of the square waveform alternating current shown in FIG. 2, the resonance frequency A ₇ of 80.0 kHz and the resonance frequency B ₇ of 108 are used. 0.0 kHz is measured.

  In the first embodiment, an alternating current of any one frequency selected from the first resonance frequency group or the second resonance frequency group described above is supplied from the AC power source 4 to the coil 2, and the water channel 1 An oscillating electromagnetic field is applied to the water 3 to be treated. By doing in this way, the to-be-processed water 3 is activated simply and efficiently.

{Resonant magnetic field}
At the above-described resonance frequency, as shown in FIGS. 23 to 40, the solubility of calcium phosphate is specifically increased by a specific current value. Here, FIGS. 23 to 40 show the resonance characteristics of the resonance magnetic field at the resonance frequency. At a specific current value in which the solubility of the calcium phosphate 16 shows specificity, the horizontal axis shows the AC peak current flowing through the coil 2 at that time. The induced magnetic field strength is taken, and the solubility of calcium phosphate 16 is plotted on the vertical axis. Here, the induced magnetic field strength is the peak strength of the magnetic field 6 that is induced and vibrates along the direction in which the water 3 to be treated in the coil 2 flows, corresponding to the current peak current.

From Figure 23, the resonant frequency _{A 1,} alternating peak current induced magnetic field intensity at that time is 23.5MA (amps) is the solubility specifically increases at 69.1MG (gauss) or in the vicinity thereof. The induced magnetic field at this time is a resonant magnetic field, and the range of the half width (Δb) is 64.1 to 72.8 mG. Here, the half width (Δb) is such that the solubility of the calcium phosphate 16 is ½ or more of the difference between the maximum value of the solubility and the solubility in the case of untreated water in the resonance magnetic field region having this specificity. This is a region of induced magnetic field strength.

Such resonance magnetic field, there are many in the resonant frequency A _1. This will be described with reference to FIGS. 41 and 42 show an example of the distribution of resonant magnetic fields, in which the induced magnetic field strength is taken on the horizontal axis, the solubility of calcium phosphate 16 is taken on the vertical axis, and there are many resonant magnetic fields that specifically increase the solubility. It is. Here, broken lines in FIG. 41 shows the two resonant magnetic field in the case of the resonant frequency A _1, the solid line in the figure shows three resonant magnetic field in the case of a resonant frequency A _2. The broken line (4) is the same as that shown in FIG. 23, and the details are a 4-fold mode resonance magnetic field, as will be described later. A broken line (3) is a similar triple-mode resonance magnetic field. Similarly, the solid line in FIG. (1), (2), has a (3), each base mode when the resonant frequency A _2, 2-times mode, a resonant magnetic field of 3-fold mode.
The solid line in FIG. 42 shows three resonant magnetic field in the case of a resonant frequency A _3, the broken line in the figure shows the two resonant magnetic field in the case of a resonant frequency B _3. The solid line in FIG. (1), (2), has a (3), each base mode when the resonant frequency _{A 3,} 2-times mode, 3-times mode. Similarly, the broken line (1) and (2) are the fundamental mode and the double mode, respectively, when the resonance frequency is B ₃ .
From the above, at the resonance frequency A ₁ , the current electromagnetic field processing experimental apparatus could not be measured because the AC peak current was too small, but it was 17.4 which is 1/4 of the induced magnetic field strength in the resonance field of the quadruple mode. There is a fundamental mode resonant magnetic field at 3 mG or in the vicinity thereof, and there are many resonant magnetic fields of n times the fundamental mode. Here, n is a positive integer.

The presence of a large number of resonant magnetic field thus n times mode shown at the resonance frequency A _1, as shown in FIG. 43 and 44, common to all of the first and second resonant frequency group described above doing. 43 and 44 are correlation diagrams of the resonance frequency and the resonance magnetic field, in which the horizontal axis indicates the AC frequency, and the vertical axis indicates the induced magnetic field strength in the resonance magnetic field. In the figure, the ◯ marks are measured with the above experimental apparatus. In the figure, up to 4 times mode is shown and there is no more, but at resonance frequencies A ₃ and B ₃ that are easy to measure with this experimental apparatus, a resonance magnetic field of n times mode that is 5 times or more of the fundamental mode is confirmed. Yes. Incidentally, the place where the AC peak current is too small to be measured around the fundamental mode is indicated by a broken circle.

Hereinafter, the resonant magnetic field at the first resonant frequency group explained are summarized in Figure 43 and 44, from FIG. 24, the resonant frequency _{A 2,} when the 2-times mode, alternating peak current is 22.7mA at that time The resonant magnetic field is 63.8 mG or its vicinity. And the range of the half value width ((DELTA) b) is 60.5-66.4 mG. Here, the induced magnetic field strength of the resonance magnetic field of the fundamental mode in this case is 31.9 mG or the vicinity thereof.
Similarly, from FIG. 25, the resonant frequency _{A 3,} the case of the base mode, a resonant magnetic field at that time alternating peak current is 46.5mA is 130.6mG or in the vicinity thereof. And the range of the half value width ((DELTA) b) is 102.5-156.7mG. Further, from FIG. 26, the resonant frequency _{A 4,} when the base mode, a resonant magnetic field at that time alternating peak current is 115.0mA is 323.0mG or in the vicinity thereof. The range of the half width (Δb) is 298.1 to 351.8 mG.

Similarly, from FIG. 27, the resonant frequency _{A 5,} when the base mode, a resonant magnetic field at that time alternating peak current is 400.0mA is 1123.5mG or in the vicinity thereof. And the range of the half width (Δb) is 989.3 to 1234.4 mG. Further, from FIG. 28, the resonant frequency _{A 6,} the case of the base mode, a resonant magnetic field at that time alternating peak current is 910.0mA is 2556.0mG or in the vicinity thereof. And the range of the half width (Δb) is 2328.1 to 2752.7 mG.

Furthermore, from FIG. 29, in the 5 times mode of the resonance frequency A- ₂ , the resonance magnetic field is 26.4 mG or the vicinity thereof. And the range of the half width (Δb) is 25.2 to 27.5 mG. Here, the induced magnetic field strength of the resonance magnetic field of the fundamental mode in this case is 5.3 mG or the vicinity thereof. Similarly, from FIG. 30, the resonance magnetic field is 36.8 mG or the vicinity thereof in the 5-fold mode of the resonance frequency A- ₁ . And the range of the half width (Δb) is 29.5 to 40.4 mG. In this case, the induced magnetic field strength of the resonance magnetic field in the fundamental mode is 7.4 mG or the vicinity thereof. From FIG. 31, in the 5 times mode of the resonance frequency A ₀ , the resonance magnetic field is 61.7 mG or the vicinity thereof. And the range of the half width (Δb) is 59.4 to 64.1 mG. In this case, the induced magnetic field strength of the resonance magnetic field in the fundamental mode is 12.3 mG or the vicinity thereof.

Then, at the resonant magnetic field in the second resonant frequency group, from Fig. 32, the resonant frequency _{B 1,} when the 4-times mode, alternating peak current is 33.5mA 94.1mG or near the resonant magnetic field at that time become. And the range of the half value width ((DELTA) b) is 90.1-99.2 mG. Here, the induced magnetic field strength of the resonance magnetic field in the fundamental mode in this case is 23.5 mG or the vicinity thereof.
Similarly, from FIG. 33, the resonant frequency _{B 2,} when the 2-times mode, a resonant magnetic field at that time alternating peak current is 33.5mA is 94.1mG or in the vicinity thereof. And the range of the half value width ((DELTA) b) is 85.7-102.1mG. Here, the induced magnetic field strength of the resonance magnetic field of the fundamental mode in this case is 47.1 mG or the vicinity thereof. Further, from FIG. 34, the resonant frequency _{B 3,} when the base mode, a resonant magnetic field at that time alternating peak current is 67.0mA is 188.2mG or in the vicinity thereof. And the range of the half value width ((DELTA) b) is 171.9-201.7mG.

Similarly, from FIG. 35, the resonant frequency _{B 4,} the case of the base mode, a resonant magnetic field at that time alternating peak current is 165.0mA is 463.5mG or in the vicinity thereof. The range of the half width (Δb) is 368.0 to 547.7 mG. Further, from FIG. 36, the resonant frequency _{B 5,} when the base mode, a resonant magnetic field at that time alternating peak current is 570.0mA is 1601.0mG or in the vicinity thereof. The range of the half width (Δb) is 1235.9 to 1938.1 mG. Further, from FIG. 37, the resonant frequency _{B 6,} the case of the base mode, a resonant magnetic field at that time alternating peak current is 1.19A is 3342.5mG or in the vicinity thereof. The range of the half width (Δb) is 3145.9 to 3623.4 mG.

Furthermore, from FIG. 38, in the 5 times mode of the resonance frequency B- ₂ , the resonance magnetic field is 35.3 mG or in the vicinity thereof. And the range of the half value width (Δb) is 34.1 to 36.4 mG. In this case, the induced magnetic field strength of the resonance magnetic field in the fundamental mode is 7.1 mG or the vicinity thereof. Similarly, from FIG. 39, the resonance magnetic field is 52.1 mG or the vicinity thereof in the 5-fold mode of the resonance frequency B- ₁ . The range of the half width (Δb) is 49.9 to 54.4 mG. In this case, the induced magnetic field strength of the resonance magnetic field in the fundamental mode is 10.4 mG or the vicinity thereof. From FIG. 40, the resonance magnetic field is 81.6 mG or in the vicinity thereof in the 5 times mode of the resonance frequency B ₀ . The range of the half width (Δb) is 75.2 to 87.6 mG. In this case, the induced magnetic field strength of the resonance magnetic field in the fundamental mode is 16.3 mG or the vicinity thereof.

Here, the vicinity of the resonance magnetic field of the fundamental mode at the resonance frequency A _i and the resonance frequency B _i (i = an integer of −2 to 6) is a magnetic field that is about ± 2% of the intensity value of each of the resonance fields. A region is preferred.

  In the first embodiment, at any one frequency selected from the first resonance frequency group or the second resonance frequency group described above, the resonance magnetic field in the n-fold mode of each of the above-described resonance magnetic fields in the base mode is obtained. An alternating current to be induced is supplied from the AC power source 4 to the coil 2, and an oscillating electromagnetic field is applied to the water to be treated 3 in the water passage 1. In this way, the water to be treated 3 is made into the activated treated water 5 that has been activated to a high level easily and efficiently.

In the electromagnetic field treatment using the resonance frequency described in the first embodiment or the resonance magnetic field at that frequency, the specific increase in the solubility of the calcium phosphate 16 is caused by the active treated water 5 obtained by subjecting the water to be treated 3 to the electromagnetic field treatment. It shows that hydrogen ions increase. When hydrogen ions (H ⁺ ; actually hydrated ions) in tap water increase, the reaction from the left to the right proceeds in chemical formula (1), and calcium phosphate 16 dissolves as the above-described first hydrogen phosphate calcium ions. This is because it becomes soluble in the activated water. In addition, in the pH measurement of the said to-be-processed water 3, the fall of the value was seen and the increase in the hydrogen ion was confirmed.

Here, as the amount of hydrogen ions increases, the amount of hydroxide ions (OH ⁻ ; actually hydrated ions) also increases to the same extent as hydrogen ions. When the specifically increased solubility of calcium phosphate shown in FIGS. 5 to 40 is, for example, about 4 × 10 ⁻⁵ mol (mol) / liter, the active treated water 5 has a dissociation constant Kw of tap water of Kw = It is the same as reaching 1.6 × 10 ⁻¹³ , and corresponds to the case where the temperature of tap water rises to 70 ° C. or higher.

  In this way, by supplying an alternating current having a specific frequency (resonance frequency) or a specific current value (resonance magnetic field) as described above to the coil, and applying a vibrating electromagnetic field treatment to tap water, the treatment was performed at room temperature. In the tap water, hydrogen ions and hydroxide ions that are four times or more that of untreated tap water are generated.

Here, it is preferable to deaerate carbon dioxide gas (CO ₂ ) in water as a pretreatment for performing an electromagnetic field treatment of water. By this deaeration, a large amount of hydrogen ions and hydroxide ions can be stably present in the activated treated water 5. For example, if a large amount of carbon dioxide is dissolved in the water, such as groundwater or well water, the carbon dioxide reacts with hydrogen ions and hydroxide ions in the water as shown in chemical formula (2), and from right to left or from left to right Reaction to occur. And it becomes unstable because the amount of hydroxide ions decreases or the amount of hydrogen ions increases conversely. It has been confirmed that when the amount of dissolved carbon dioxide increases, the measured value becomes unstable even in the measurement of the pH meter of the treatment liquid.

  Thus, in the case of water such as ground water or well water having high solubility of carbon gas, removal of carbon gas is extremely effective in order to stably treat them.

Conversely, by subjecting the water to the vibrating electromagnetic field treatment, a gas such as carbon dioxide dissolved in the water can be degassed very efficiently. Although the mechanism of this degassing has not yet been clarified, it has been dissolved in water and dissociated as ions as the reaction progressed from right to left in the chemical formula (2) together with the stirring effect of water clusters as described later. It seems that it is easy to deaerate by returning to carbon dioxide.
The effect of water degassing by such electromagnetic field treatment is, for example, the generation of functional water in which effective gas such as hydrogen-dissolved water or ozone-dissolved water is dissolved by dissolving, for example, hydrogen or ozone in pure water or ultrapure water. Can be used very effectively. This is because it is essential to degas carbon dioxide dissolved in water in order to increase the dissolution efficiency in dissolving the effective gas in water.

  Further, by applying the vibrating electromagnetic field treatment to the tap water, the generated activated treated water 5 is very easily mixed with oil such as gasoline at room temperature. In the mixing of gasoline and activated treated water 5, a W / O type emulsion in which water droplets are dispersed in oil can be easily produced simply by injecting activated treated water 5 into gasoline at room temperature. In addition, an O / W emulsion in which oil droplets are dispersed in water can be easily produced as well. It was confirmed that the W / O emulsion can be used as a fuel for automobiles.

In the activated treated water 5 generated in the above embodiment, the increase in hydrogen ions and hydroxide ions as described above makes it possible to prevent the scale adhesion on the inner wall of the pipe or to remove the adhesion scale, for example. Usually, water and tap water contains a certain amount of ions of mineral components such as calcium, magnesium or potassium. And these are easy to form a crystal in water. However, due to the increase in the amount of hydrogen ions, for example, calcium oxalate (Ca (COOH) ₂ ), which is a crystalline substance that is hardly soluble in tap water, is easily dissolved in tap water without being crystallized. Further, insoluble urea nitrate (CO (NH) ₂ · HNO ₃ ) in which urea and nitrate ions in tap water are combined is easily dissolved by an increase in the amount of hydroxide ions in tap water. Similarly, uric acid (R (OH) ₂ ; R is a hydrocarbon) that is hardly soluble in tap water is easily dissolved by an increase in the amount of hydroxide ions. Further, for example, fats and oils such as fatty acid esters (R ₁ —COO—R ₂ ; R ₁ and R ₂ are hydrocarbons) are hydrolyzed by hydrogen ions and hydroxide ions to be converted into fatty acids and easily dissolved in water. . In this way, scale adhesion on the inner wall of the pipe is greatly reduced.

Also, an increase in the hydrogen ions and hydroxide ions allows for rust prevention liable iron pipe inner wall instead of the iron (Fe) to black rust (Fe 3 _{O 4).}

Also, an increase in hydrogen ions and hydroxyl ions in the treatment liquid is more soluble in tap water ammonia (NH ₃₎ as ammonium ions. For this reason, when the said process liquid is used for a toilet, it becomes possible to make it odorless.

  Further, the activated treated water 5 in the present embodiment makes it possible to reform heavy oil or light oil by the increased hydrogen ions and hydroxide ions. This is because the carbon (C) -carbon (C) bond of these oils is dissociated by hydrogen ions and hydroxide ions and decomposed into alcohols or alkenes. These modified oils are easily dissolved in tap water, and the adhesion of oil in the piping is greatly reduced.

  In the present embodiment, various effects as described above are generated by the electromagnetic field processing using the specific alternating current. And it is not necessary to test the effect of the modulation electric field processing through a desktop test in advance as in the prior art. Moreover, this electromagnetic field processing method is very simple, and power consumption in the electromagnetic field processing is extremely small. Thus, the electromagnetic field process of this embodiment has high economic efficiency. And since an effect arises irrespective of the kind of to-be-processed liquid, the versatility is also high.

[Embodiment 2]
Next, a preferred second embodiment of the present invention will be described. The feature of this embodiment is that one resonance frequency selected from the first resonance frequency group and the second resonance frequency group of the alternating current described in the first embodiment is used, and these two resonance frequencies simultaneously. It is where water is activated. By doing so, water is efficiently subjected to electromagnetic field treatment, and the active treated water is extended as a functional water. FIG. 45 is a waveform diagram showing an example of an alternating current that induces an oscillating electromagnetic field by mixing these two resonance frequencies.

  In this embodiment, as shown in FIG. 45, the alternating current is composed of two resonance frequencies, and the first frequency current 21 and the second frequency current 22 are amplitude-modulated so that, for example, the AC peak current is different. 1 is supplied to the coil 2 shown in FIG. 1 or the electromagnetic field applying unit 7 shown in FIG. Here, the waveform in the first frequency current 21 is a square waveform as shown in FIG. 2, and the frequency is selected from the first resonance frequency group described in the first embodiment. Similarly, the waveform in the second frequency current 22 is also a square waveform, and the frequency is selected from the second resonance frequency group.

  Here, the amplitude of the first frequency current 21, that is, the AC peak current, is preferably set so that the resonance magnetic field described in the first embodiment is generated at the resonance frequency selected from the first resonance frequency group. The amplitude of the second frequency current 22, that is, the AC peak current is preferably set so that the resonance magnetic field described in the first embodiment is generated at the resonance frequency selected from the second resonance frequency group. The amplitudes of the first frequency current 21 and the second frequency current 22 are larger in the case of the first frequency current 21 than in the case of the second frequency current 22, unlike the case shown in FIG. It doesn't matter. Alternatively, both amplitudes may be the same.

  Such an alternating current is obtained by adding amplitude modulation to frequency modulation by so-called two frequencies. Here, the repetition of the first frequency current 21 and the second frequency current 22 is set to an alternating frequency of 50 to 150 times / second (Hz). Then, the duty cycles of the first frequency current 21 and the second frequency current 22 are arbitrarily adjusted. Here, in a preferred embodiment, the alternating frequency is 100 Hz. Further, the duty cycles of the first frequency current 21 and the second frequency current 22 at the alternating frequency are set to 50%, respectively.

There are various other methods for selecting one resonance frequency from each of the first resonance frequency group and the second resonance frequency group and simultaneously activating water by the two selected resonance frequencies. For example, as shown in FIG. 46, as described with reference to FIG. 1, an alternating current having a resonance frequency f _A selected from the first resonance frequency group through the first AC power supply 23 is passed through the outer coil of the water pipe 1. Shed. At the same time, an AC current having a resonance frequency f _B selected from the second resonance frequency group is passed through the second AC power supply 24 to the coil outside the water pipe 1. Here, the winding direction of both coils may be the same or reverse. Thus, if the to-be-processed water 3 of the tap water is flowed through the water pipe 1, for example, the activated treated water 5a is generated.

Or as shown in FIG. 47, the 1st electromagnetic field provision part 25 provided with the coil connected to the 1st alternating current power supply 23, and the 2nd electromagnetic field provision part provided with the coil connected to the 2nd alternating current power supply 24 26 is immersed in the stored water 9 of the tank 8. In this state, the AC current having the resonance frequency f _A described above is supplied to the first electromagnetic field applying unit 25 through the first AC power source 23. At the same time, the AC current having the resonance frequency f _B described above is supplied to the second electromagnetic field applying unit 26 through the second AC power supply 24. In this way, by applying alternating currents of two resonance frequencies to the stored water 9, the stored water 9 is activated by the oscillating electromagnetic field to be activated treatment water.

Here, the two types of alternating current waveforms are preferably square waveforms as shown in FIG. 2, for example. The amplitude of the alternating current at the resonance frequency f _A may be set so that the resonance magnetic field described in the first embodiment is generated at the resonance frequency selected from the first resonance frequency group. Then, the amplitude of the alternating current at the resonance frequency f _B may be set so that the resonance magnetic field described in the first embodiment is generated at the resonance frequency selected from the second resonance frequency group.

  In the present embodiment, as described above, the time during which the water activation effect lasts becomes longer, and the life of the functional water becomes longer. This will be described with reference to FIG.

  In FIG. 48, the horizontal axis represents the preservation period of the activated water after the electromagnetic field treatment, and the vertical axis represents the solubility of the calcium phosphate 16 by the activated water. Here, the electromagnetic field treatment was performed for a certain time (about 10 hours) by removing the powder of calcium phosphate 16 in the storage chamber 12 in the experimental apparatus shown in FIG. Then, the activated treated water was stored at room temperature, and the ability of the preserved activated treated water to dissolve calcium phosphate after a predetermined storage period was examined.

In the figure, a solid line shows a case where an electromagnetic field process is performed using an alternating current using the two resonance frequencies described with reference to FIG. Here, the frequency of the first frequency current 21 is one resonance frequency of the first resonance frequency group, and the frequency of the second frequency current 22 is one resonance frequency of the second resonance frequency group. The amplitudes of these frequency currents are set so that a resonant magnetic field is generated. The alternating frequency is 100 Hz, and the duty cycle of the first frequency current 21 and the second frequency current 22 at the alternating frequency is 50%.
The broken line in the figure is the same as that of the first embodiment, and is the case of one resonance frequency of the first resonance frequency group or the second resonance frequency group. The electromagnetic field processing is performed by an alternating current using a single frequency. This is an example result. Here, the amplitude of the one frequency current is set so that a resonant magnetic field is generated.
The dotted line in the figure shows the result of an example of the AA (or BB) homogeneous mixed frequency, when the electromagnetic field processing is performed by the alternating current using the two resonance frequencies described in FIG. Here, the frequencies of the first frequency current 21 and the second frequency current 22 are resonance frequencies selected from the same first resonance frequency group. Alternatively, both resonance frequencies are selected from the same second resonance frequency group. The amplitudes of these frequency currents are set so that a resonant magnetic field is generated. The alternating frequency is 100 Hz, and the duty cycle of the first frequency current 21 and the second frequency current 22 at the alternating frequency is 50%.
Specifically, as the result of the example shown in FIG. 48, the results obtained using the resonance frequency A _i (i = 3,4) and the resonance frequency B _j (j = 3,4) are listed. It has been.

As shown in FIG. 48, the activated treated water dissolves the calcium phosphate 16 in the case of the solid line AB heterogeneous mixed frequency, the broken line single frequency, and the dotted line AA (BB) homogeneous mixed frequency. The ability to do lasts. And it decays with its storage period, but with the solid line the decay is much smaller than with the dashed line and the duration of water activation increases. For example, in the broken line, the solubility of untreated water returns to 2.65 × 10 ⁻⁵ mol / liter in a storage period of 12 to 13 hours, but in the solid line, the solubility is 3 even in the storage period of 12 to 13 hours. .About.13 × 10 ⁻⁵ mol / liter and does not decrease much thereafter. In addition, in the case of the solid line, as shown in the storage period 0 hour, the degree of initial activation increases.
On the other hand, in the dotted line, the attenuation is greater than in the broken line, and the duration of water activation is reduced. For example, it returns to the same level as untreated water in a storage period of about 6 to 7 hours. In addition, in the case of the dotted line, as shown in the storage period of 0 hour, the initial degree of activation is reduced compared to the case of the single frequency of the broken line.

  Thus, in this embodiment, the electromagnetic field treatment is performed by alternating alternating current using two different resonance frequencies, so that the degree of activation is increased and the lifetime of the effect of the activated water is further prolonged. That is, the state in which the amount of hydrogen ions and the amount of hydroxide ions during treatment are larger than in the case of untreated water continues for a long time. Conversely, when the same kind of resonance frequency is used, the degree of activation is reduced and the sustained life of the effect of the activated treated water is shortened.

  Such a prolonged life of the active treated water indicates that the active treated water generated in this embodiment can be used effectively as a cleaning agent or the like. It can be used as various detergents or functional water such as the functions exhibited by water having a large amount of hydrogen ions or hydroxide ions described in the first embodiment, for example, dissolution of fatty acids, deodorization, modification of oils, and the like.

Next, the electromagnetic field processing mechanism using an alternating current having a specific frequency in the first embodiment or the second embodiment will be described. The power consumed in the water of about 100 cc through the coil 2 by the alternating current of the specific frequency is, for example, 0 at most at the resonance frequency A _i (i = 3,4) and the resonance frequency B _j (j = 3,4). 0.5 mW (watt) to 10 mW. Such extremely small power energy generates activated treated water having the above-described effects. Moreover, the frequency of such a specific alternating current belongs to the low frequency band. For example, compared to the case where plasma is excited by ionizing a gas as in the case of plasma generation using an AC frequency of 100 kHz to several tens of MHz, the frequency of 10 kHz or less is small and the power energy is extremely small. In the electric field treatment in the embodiment, generation of free electrons through water ionization and electron energy cannot be imparted thereto.

Certainly, a substance such as a salt (NaCl) in water is easily ionized (hydrated ion) and dissolved by breaking its strong ionic bond and dissociating. However, this is caused by the extremely high dipole efficiency (relative dielectric constant of about 80) of water, and the energy generated in the process of hydration (becomes hydrated ions) breaks the bond. Here, hydrogen ions (H ⁺ ) are certainly hydrated ions. However, the hydroxide ion (OH ⁻ ) hardly hydrates and the dissociation of water molecules is small. For this reason, the pH value of ordinary neutral water is 7, and the dissociation is about 1 × 10 ⁻⁷ mol / l together with hydrogen ions.

The electromagnetic field treatment using an alternating current of a specific frequency in the present embodiment gives energy to the rotation of the water cluster existing in the water, and the rotation energy of the water cluster gradually increases, and the water molecule ( It is thought that it collides with H ₂ O) and dissociates water molecules into hydrogen ions and hydroxide ions.

  That is, by supplying an alternating current having the specific resonance frequency to the coil 2, a magnetic field is generated, for example, in tap water in the water pipe 1. Assuming that the magnetic flux density is a B vector, the B vector also changes with time at the same frequency along with the current of the above frequency. This time change generates an E vector of an electric field that changes at the same frequency according to Equation (1). The electromagnetic field energy of the same frequency as the frequency of the alternating current resonates with the gap of rotation specific energy quantized by regarding the water cluster as a rigid body of the moment of inertia I, and the water cluster starts rotating. Here, it is uncertain whether the excitation of the rotation of the water cluster by the resonance is caused by photons emitted from the oscillating electromagnetic field or by photons emitted by hydrogen ions or hydroxide ions that are accelerated by the oscillating electromagnetic field according to Equation (2).

  Here, q is the charge amount, V vector is the thermal motion velocity of hydrogen ions or hydroxide ions, B vector is the magnetic flux density, and E vector is the electric field.

  In the above embodiment, there is a resonant magnetic field in the induced magnetic field strength applied to the tap water through the coil 2. This induced magnetic field strength is considered to be related to the rotation start of the water cluster. Lorentz force according to Equation (2) acting on charges such as hydrogen ions or hydroxide ions adhering to the surface of the water cluster regarded as a rigid body, if it matches these thermal motion speeds, the charge is attracted to the magnetic flux to rotate. Trigger. A suitable range of the magnetic field is considered to be a condition that facilitates the rotation start of the water cluster.

  As described above, hydrogen ions or hydroxide ions adhere to the surface of the water cluster regarded as a rigid body. The direction of rotation start of the water cluster is completely reversed by this positive charge or negative charge. When each of these water clusters starts to rotate, the attached charge receives an extremely large electric field generated by Equation (1), and the rotational energy of the water cluster increases to the extent that it dissociates water molecules. I think that the. Here, in order to dissociate water molecules, the rotation of the water cluster has a rotation speed of about GHz.

The dissociation model of water hydrogen ion and hydroxide ion due to the rotation of the water cluster is theoretical and has not been proved yet. Thus, if the rotation of the water cluster is related, the number of water-bonded water molecules contained in the water cluster is, for example, about 1.2 × 10 ⁴ in the case of the resonance frequency A ₃ , and the resonance In the case of the frequency B _3, the number is about 1 × 10 ⁴ . The number of water-bonded water molecules contained in the water cluster decreases as the resonance frequency increases. Here, the rotation specific energy obtained by quantizing the water cluster as a rigid body having the moment of inertia I is calculated, and the rotation specific energy gap resonates with the electromagnetic field energy generated in the water by the alternating current of the specific resonance frequency. As an example, the number of water molecules in the water cluster is calculated by obtaining the moment of inertia I.

  The rotation of the water cluster efficiently stirs the water and effectively degass the water, as described in the effect of the first embodiment. And it is thought that the effect increases as the resonance frequency increases.

  Considering the rotation of the water cluster, in the second embodiment, it is very easy to understand the high sustainability of the treated water subjected to the electromagnetic field treatment by alternating alternating current using two kinds of resonance frequencies. That is, it is thought that it is caused by the following mechanism. This will be described with reference to FIG. 49 based on the model described above. Here, FIG. 49 schematically shows the rotation of the water cluster. FIG. 49A shows a case where there is a rotation of a water cluster to which hydrogen ions are attached (hereinafter referred to as a hydrogen ion attachment cluster) and a rotation of a water cluster to which hydroxide ions are attached (hereinafter referred to as a hydroxide ion attachment cluster). It is. FIG. 49B shows the case where only the rotation of the water cluster to which hydrogen ions or hydroxide ions are attached. In FIG. 49, an electric field E and a magnetic field (magnetic flux density) B are shown, but these vibrate with time.

  As shown in FIG. 49A, if the hydrogen ion attachment cluster 27 rotates clockwise, the hydroxide ion attachment cluster 28 rotates counterclockwise. Here, even if a contact occurs between these clusters (27, 28), there is no effect that their rotations decelerate mutually. For this reason, rotation of a water cluster becomes easy to continue. Such a mechanism seems to work in the case of the solid line shown in FIG. Here, the hydrogen ion attachment cluster 27 absorbs rotational energy in the alternating current of the first resonance frequency group described above, and the hydroxide ion attachment cluster 28 rotates in the alternating current of the second resonance frequency group. It is absorbed by energy.

  On the other hand, as shown in FIG. 49 (b), when only the hydrogen ion attachment clusters 27 exist, they rotate together in the clockwise direction. Since they are reversed, they slow down each other. For this reason, the rotation of the water cluster is difficult to be sustained. Such a mechanism seems to work in the case of the dotted line shown in FIG. This also occurs in the case of only the hydroxide ion adhesion cluster 28.

  In the second embodiment, various methods other than the method described with reference to FIGS. 45 to 47 can be considered. For example, in the AC power source 4 described with reference to FIG. 1 or FIG. 3, an AC current consisting of one resonance frequency selected from the first resonance frequency group and an AC current consisting of one resonance frequency selected from the second resonance frequency group. A combined current is formed by combining the currents. Then, this combined current is supplied to the coil or the electromagnetic field applying unit 7. Even if it does in this way, water will be activated simultaneously by these two resonance frequencies, and the same effect as mentioned above will arise.

[Embodiment 3]
Next, a third embodiment of the present invention will be described. The feature of this embodiment resides in effectively removing the influence of geomagnetism described in the first embodiment from the electromagnetic field processing. By doing in this way, the stable electromagnetic field processing of water becomes easy, without depending on the place where the coil which generates an oscillating electromagnetic field is arranged, or how to attach it.

For example, in the vicinity of Tokyo, as schematically shown in FIG. 50, geomagnetism Be having a horizontal component force of about 310 mG and a vertical component force of about 340 mG exists from the south side to the north side. In addition, the magnetic field strength of this geomagnetism changes with the season or time. In the experimental apparatus shown in FIG. 4 described in the first embodiment, it has been confirmed that the influence of geomagnetism on the electromagnetic field processing can be eliminated if the geomagnetic component disappears in the direction of the axis of the coil 2. In particular, when an alternating current having a resonance frequency A _i (i = an integer of −2 to 4) and an resonance frequency B _j (an integer of j = −2 to 4) is used, the resonance magnetic field of the fundamental mode is the same as that of the geomagnetism or Since it becomes less than that, it is important to remove the influence of this geomagnetism.

  As a preferred first method, as shown in FIG. 50, the coil to which the alternating current is supplied is arranged so that the axial center of the coil is on a vertical plane 32 orthogonal to the geomagnetic (Be) direction 31. That is. Here, the target coil is, for example, the coil 2 attached to the outside of the water conduit 1 described in the first and second embodiments, the coil with a built-in electromagnetic field providing unit (7, 25, 26), or the like. .

And the suitable 2nd method is to enclose the outer side of the said coil with a magnetic shield, as shown in FIG. 51 (a) and 51 (b), the coil 2 is formed outside the water pipe 33 made of a material having a relative magnetic permeability of about 1 such as a polymer material or a resin material. Further, the magnetic shield 34 is encapsulated and arranged on the outer side. Here, in FIG.51 (b), the magnetic shield 34 encloses the outer side of the coil 2, and the outer side of the water flow pipe 33 extended on the both sides of the coil 2 and over the length. Further, the magnetic shield 34 is made of a magnetic material having a large relative permeability. For example, a sheet-like cobalt-based amorphous sheet is preferably used.
By doing so, the geomagnetism Be is shielded by the magnetic shield 34 and the intrusion into the water conduit 33 is greatly reduced. In the structure shown in FIG. 51B, the geomagnetism Be that enters from the inlet side or the outlet side of the water conduit 33 is shielded.

  Similarly, as shown in FIG. 51 (c), the coil 2 is wound outside the central region of a water pipe 33a made of a material having a relative permeability of about 1, for example, U-shaped, The magnetic shield 34 is encapsulated beyond the region where the coil 2 is encapsulated and further bent into a U-shape of the water pipe 33a. In this case, for example, in FIG. 51 (a), the geomagnetism Be that enters from the inlet side or the outlet side of the water conduit 33 cannot be sufficiently shielded. However, in FIG. Can be completely prevented.

  51 may be applied to the coil of the water conduit 1 shown in FIG. 1 or 46, or the electromagnetic field applying unit shown in FIG. 3 or 47. You may apply to the coil with which (7, 25, 26) was equipped.

And in the suitable 3rd method, as shown in FIG. 52, the coil 2 is wound by the outer side of the center area | region of the U-shaped water pipe 1a, and the coil 2a is wound by the magnetic body core 35. Both ends thereof are arranged so as to substantially contact a U-shaped bent region. The U-shaped water conduit 1 a and the magnetic core 35 are accommodated in a magnetic shielding container 36. Here, the coil 2 and the coil 2a have the same winding direction and are connected to the AC power source 4 in series, and are formed in a magnetic field direction formed at the end of the magnetic core 35 and a U-shaped bending region. The direction of the formed magnetic field is made the same.
By doing in this way, the induced magnetic field strength in the central region of the U-shaped water conduit 1a becomes uniform in the two-axis center of the coil. The geomagnetism Be is shielded by the magnetic shielding container 36. For this reason, the magnetic flux density in the water flow pipe 1a becomes uniform in the axial direction of the coil 2, and the water to be treated flowing in the water flow pipe 1 can be activated with high efficiency.

The preferred fourth method is a method of demagnetizing by compensating the geomagnetism, which is a static magnetic field, as shown in FIG. As shown in FIG. 53, a part of the water pipe 1 is bent in an L-order shape, and the coil 2 is wound outside the line-shaped region of the water pipe 1. And the magnetic sensor 37 is arrange | positioned in the L-shaped bending part, and the static magnetic field of the axial center direction of the coil 2 is detected. The constant current source 38 is controlled based on the detected value of the static magnetic field, and a reverse static magnetic field generated by the degaussing coil 39 is generated in the water pipe 1 so as to compensate for the geomagnetic static magnetic field. In this way, control is always performed so that the static magnetic field in the axial direction of the magnetic sensor 37 becomes zero. Here, in FIG. 53, the AC power supply 4 connected to the coil 2 is omitted for the sake of simplicity.
By doing in this way, the influence of the geomagnetism in the water flow pipe 1 is completely eliminated, and it becomes possible to activate the treated water with high efficiency without being influenced by the environmental change at all.

[Embodiment 4]
Next, a fourth embodiment of the present invention will be described. In the present embodiment, an electromagnetic field processing apparatus that is preferably used in the electromagnetic field processing described in the first, second, or third embodiment will be described.

  As shown in FIG. 54, the electromagnetic field treatment device 41 includes a coil 2 attached to the outside of the water flow pipe 1 serving as a flow path of water to be treated, and an alternating power supply for supplying alternating currents of two different resonance frequencies to the coil 2. The power supply unit 43 that drives the current supply unit 42 and the alternating current supply unit 42 is provided.

  As shown in FIG. 55, the alternating current supply unit 42 has, as its main configuration, a crystal resonator 44, for example, a frequency dividing circuit 45 that generates three frequency signals, and frequency modulation that modulates two of the frequencies. A circuit 46 and an amplitude modulation circuit 47 are included. Here, these circuits are digital circuits, and semiconductor integrated circuits are preferably used. This semiconductor integrated circuit is composed of a semiconductor element such as a MOSFET or a BiP transistor, and its drive voltage is a plurality of voltages of 20 V or less and is supplied from a drive power supply 43. In this way, the alternating current supply unit 42 is extremely compact and lightweight.

Here, the inductance of the coil 2 may be set to about 10 ⁻⁵ H. This reactance is 5Ω or less when the resonance frequency of the alternating current is, for example, 1 kHz to 50 kHz. Therefore, a resistance of about 100Ω connected in series with the coil 2 is provided so that the peak current flowing through the coil 2 is substantially constant.

  In the frequency divider 45, a first frequency signal in the first resonance frequency group, a second frequency signal in the second resonance frequency group, and an alternating frequency signal in the range of 50 to 150 Hz are generated. . Then, in the frequency modulation circuit 46, a signal having a modulation frequency modulated by the alternating frequency is generated by the first frequency signal and the second frequency signal. Then, in the amplitude modulation circuit 47, the modulation frequency signal is subjected to amplitude modulation of the voltage at the alternating frequency, and the alternating current whose current is amplitude-modulated is supplied to the coil 2 through the resistor of about 100Ω.

  In this way, the alternating current supply unit 42 supplies the alternating current as shown in FIG. That is, currents having two frequencies, the first frequency current 21 and the second frequency current 22, are supplied with amplitude modulation so that the peak currents are different from each other. Here, the first frequency current 21 is a frequency band in the first resonance frequency group, and it is preferable that the peak current is set to a current value that induces the resonance magnetic field. The second frequency current is a frequency band in the second resonance frequency group, and it is preferable that the peak current is set to a current value that induces the resonance magnetic field.

  Here, the frequency of the first frequency current 21 is set to the resonance frequency of the first resonance frequency group or the frequency within the half width (Δf) thereof, and the peak current is within the half width (Δb) of the resonance magnetic field. You may do it. Similarly, the frequency of the second frequency current 22 is set to the resonance frequency of the second resonance frequency group or the frequency within the half width (Δf) thereof, and the peak current is within the half width (Δb) of the resonance magnetic field. It may be made to become. Here, the duty cycles of the first frequency current 21 and the second frequency current 22 at the alternating frequency are arbitrarily variable.

  The effect described in the second embodiment is produced by subjecting the liquid to be processed to an electromagnetic field treatment using such an electromagnetic field treatment apparatus. In addition, this apparatus is very compact and lightweight, and can be installed in various places, and is excellent in convenience.

  Next, a preferred aspect of the present embodiment will be described with reference to FIG. FIG. 56 is a schematic enlarged view of the water pipe 1 for explaining this embodiment. In this embodiment, a flow path changing mechanism for changing the flow path of the liquid to be processed in the water conduit 1 is provided.

  As shown in FIG. 56 (a), a number of baffle plates 48 are arranged in the water conduit 1 in which the coil 2 is installed. The baffle plate 48 meanders the flow path of the water to be treated 3 and flows in the water pipe 1. Here, the baffle plate 48 is preferably an insulator, and is formed by molding a polymer material or a resin material such as vinyl chloride or polystyrene.

  In the case of FIG. 56 (b), for example, a plurality of cylindrical rods 49 are connected to each other by thin connecting members 50 in the water pipe 1 where the coil 2 is installed. By this cylindrical rod 49, the flow path of the water to be treated 3 is unevenly distributed on the side wall side of the water flow pipe 1. Even in this case, the cylindrical rod 49 and the connecting member 50 are preferably insulators, and are made of a polymer material or a resin material like the baffle plate 48.

  The polymer material or resin material has a relative magnetic permeability of about 1 like water, and has a relative dielectric constant of 10 or less. By providing such a flow path changing mechanism in the water pipe 1, the intensity of the electric field E received by the water to be treated 3 according to the formula (1) is increased on average, and the effect of the electromagnetic field treatment is increased. This is because the electric field is the largest in the vicinity of the inner wall of the water conduit 1 and in the vicinity of the baffle plate 48 or the cylindrical rod 49, and a strong electric field is generated by making such a large number of such neighborhoods the flow path of the water 3 to be treated. This is because it takes longer.

  Furthermore, another preferred aspect of the present embodiment will be described with reference to FIG. FIG. 57 is a block diagram showing this embodiment. This embodiment is suitable when the liquid to be treated described in the first embodiment is groundwater or well water containing a relatively large amount of carbon dioxide.

  As shown in FIG. 57, a carbon dioxide degassing device 51 is disposed in the front stage of the electromagnetic field processing device 41. Here, the carbon dioxide deaeration device 51 releases carbon dioxide from the raw water containing a relatively large amount of the carbon dioxide. As this discharge method, for example, there are various methods such as a method of applying ultrasonic waves to raw water to degas carbon dioxide, an aeration method of raw water, and a heating / cooling method of raw water.

  By using the electromagnetic field treatment system including the carbon dioxide gas degassing device 51, stable electromagnetic field treatment of water to be treated according to the first embodiment, the second embodiment, or the third embodiment can be performed.

  Furthermore, in still another preferred aspect of the present embodiment, various geomagnetism removing means for removing the influence of geomagnetism as described in the third embodiment are incorporated in the electromagnetic field processing apparatus. Among the above-mentioned geomagnetism removing means, especially the means using the geomagnetism demagnetization method described in FIG. 53 eliminates the influence of geomagnetism inside the water pipe 1 and can be freely adapted to environmental changes and is stable and highly efficient. This is very suitable because it facilitates the activation of water.

  Next, some modified examples of this embodiment will be described. The electromagnetic field processing device 41 supplies alternating currents having two different resonance frequencies to one coil. However, as described in the second embodiment, the alternating currents having two different resonance frequencies are different from each other. The structure supplied to a coil may be sufficient. Further, these coils may have a structure built in the electromagnetic field supply unit (7, 25, 26).

  Further, as a modification of the electromagnetic field processing apparatus of the present embodiment, as described in the first embodiment, an electromagnetic field processing apparatus having a structure in which an alternating current having a single frequency among the resonance frequencies is supplied to the coil may be used. .

  Furthermore, as a modification of the electromagnetic field processing apparatus of the present embodiment, a structure in which a positive or negative polarity pulse waveform current such as a signal clock is used may be used. Such a unipolar waveform current is also an electromagnetic field induced current. This will be described with reference to FIG. Here, FIG. 58A is a schematic configuration diagram of an electromagnetic field processing apparatus that supplies a current having a unipolar pulse waveform. FIG. 58B is a current waveform diagram in this case, and shows a square pulse waveform of the positive electrode.

  As shown in FIG. 58 (a), the electromagnetic field treatment apparatus in this case is wound in the reverse direction of the normal winding coil 53 indicated by white circles attached to the outside of the water flow pipe 52 and the normal winding coil 53. The reverse winding coil 54 includes a unipolar current supply unit 55 that alternately supplies a current having a unipolar pulse waveform to the normal winding coil 53 and the reverse winding coil 54.

  As shown in FIG. 58 (b), the currents of the same square pulse whose phases are shifted from each other by half a cycle are alternately supplied to the normal winding coil 53 and the reverse winding coil. As shown in FIG. 58 (a), both ends of the forward winding coil 53 and the reverse winding coil 54 are fixed to the ground potential. Here, the circuit of the unipolar current supply unit 55 for generating the square pulse current is a digital circuit, and the semiconductor integrated circuit as described above is preferably used.

  In this way, in the water conduit 52, an oscillating electromagnetic field similar to the case where the alternating current having the waveform shown in FIG. 2 is supplied to one coil is generated, and the activation of water is the case of the first embodiment. You can do the same. In this modified example, since the current of the pulse waveform can be generated by a single power source, an electromagnetic field processing device having high stability at low cost is realized.

  Further, as a modification of the present embodiment, in the electromagnetic field processing apparatus as shown in FIG. 58, for example, only the normal winding coil 53 or the reverse winding coil 54 is used, and a current having a unipolar pulse waveform is used as the electromagnetic field induced current. Even if it is the electromagnetic field processing method which supplies to one of the said coils, the solubility of the calcium phosphate mentioned above increases compared with untreated water, and activation of water is possible.

As described above, when a unipolar pulse waveform current is used instead of the square waveform AC current shown in FIG. 2, it belongs to the first resonance frequency group as shown in FIG. 59 and FIG. The resonance frequency A ₇ of 80.0 kHz and the resonance frequency B ₇ of 108.0 kHz belonging to the second resonance frequency group are measured. Here, FIGS. 59 and 60 show the resonance characteristics of the resonance frequency in the electromagnetic field processing in which the current of the positive rectangular pulse is supplied to, for example, the positive winding coil 53 and vibrates. In the frequency band in which the solubility of the calcium phosphate 16 exhibits specificity, the horizontal axis represents the frequency of the positive current flowing through the positive winding coil 53 and the vertical axis represents the solubility of the calcium phosphate 16.

From Figure 59, the resonant frequency _{A 7} is 80.0kHz or in the vicinity thereof, the scope of its half-value width (Delta] f) is 76.5～83.1KHz. Here, the full width at half maximum (Δf) is a frequency at which the solubility of the calcium phosphate 16 becomes 1/2 or more of the difference between the maximum solubility value and the solubility of untreated water in the resonance frequency band having this specificity. It is a band. Further, from FIG. 60, the resonance frequency B ₇ is 108.0 kHz or the vicinity thereof, and the range of the half width (Δf) is 104.8 to 111.1 kHz.

  Even in these cases, the above-described resonant magnetic field is measured as shown in FIGS. 61 and 62 show the resonance characteristics of the resonance magnetic field at the resonance frequency. The horizontal axis represents the induced magnetic field intensity at the peak current of the positive current flowing through the positive winding coil 53, and the vertical axis represents the calcium phosphate 16. The solubility is taken.

From Figure 61, the resonant frequency _{A 7,} the case of the base mode, a resonant magnetic field is induced field strength 6039.0mG or near. And the range of the half value width ((DELTA) b) is 5027.8-6797.4mG. Also, the resonant frequency _{B 7,} when the base mode, a resonant magnetic field is induced field strength 7302.9mG or near. And the range of the half value width ((DELTA) b) is 6618.8-8033.2mG.

  Although the preferred embodiments of the present invention have been described above, the above-described embodiments do not limit the present invention. Those skilled in the art can make various modifications and changes in specific embodiments without departing from the technical idea and technical scope of the present invention.

  In the above embodiment, it is preferable that the alternating current, alternating current, or unipolar waveform current has a current value that changes rapidly in time, such as a pulse waveform other than a square waveform, a sawtooth waveform, or the like. In addition, a sinusoidal waveform can be used although its effect is reduced.

  Further, the coil to which the alternating current, alternating current or unipolar waveform current is supplied may be attached to the outside of the water to be treated, and the oscillating electromagnetic field generated in the coil may irradiate the water to be treated from the outside.

  Moreover, the coil shape wound around a water pipe should just be a thing which can produce | generate the magnetic field which changes temporally, and various ways of winding other than the said spiral shape can be considered. And the activated water produced | generated by the electromagnetic field process of this embodiment can be applied to various uses as functional water in which hydrogen ions and hydroxide ions are dissolved abundantly.

It is explanatory drawing which shows an example of the method of performing the electromagnetic field process concerning the 1st Embodiment of this invention. It is a wave form diagram of an example of an alternating current concerning a 1st embodiment of the present invention. It is explanatory drawing which shows the method of carrying out another electromagnetic field process concerning the 1st Embodiment of this invention. It is a block diagram of the experimental apparatus of the electromagnetic field process used in the 1st Embodiment of this invention. It is a graph showing a resonance characteristic of the resonance frequency A ₁ in the alternating current of the first embodiment of the present invention. It is a graph showing a resonance characteristic of the resonance frequency A ₂ at alternating current of the first embodiment of the present invention. It is a graph showing a resonance characteristic of the resonance frequency A ₃ at alternating current of the first embodiment of the present invention. It is a graph showing a resonance characteristic of the resonant frequency A ₄ at alternating current of the first embodiment of the present invention. It is a graph showing a resonance characteristic of the resonance frequency A ₅ at alternating current of the first embodiment of the present invention. It is a graph showing a resonance characteristic of the resonance frequency A ₆ at an alternating current of a first embodiment of the present invention. It is a graph which shows the resonance characteristic of resonance frequency A- ₂ in the alternating current of the 1st Embodiment of this invention. It is a graph which shows the resonance characteristic of resonance frequency A- ₁ in the alternating current of the 1st Embodiment of this invention. It is a graph showing a resonance characteristic of the resonance frequency A ₀ at alternating current of the first embodiment of the present invention. It is a graph showing a resonance characteristic of the resonance frequency B ₁ at alternating current of the first embodiment of the present invention. It is a graph showing a resonance characteristic of the resonance frequency B ₂ at alternating current of the first embodiment of the present invention. It is a graph showing a resonance characteristic of the resonance frequency B ₃ at alternating current of the first embodiment of the present invention. It is a graph showing a resonance characteristic of the resonant frequency B ₄ at the alternating current of the first embodiment of the present invention. It is a graph showing a resonance characteristic of the resonance frequency B ₅ at alternating current of the first embodiment of the present invention. It is a graph showing a resonance characteristic of the resonance frequency B ₆ at alternating current of the first embodiment of the present invention. It is a graph which shows the resonance characteristic of resonance frequency B- ₂ in the alternating current of the 1st Embodiment of this invention. It is a graph which shows the resonance characteristic of resonance frequency B- ₁ in the alternating current of the 1st Embodiment of this invention. It is a graph showing a resonance characteristic of the resonance frequency B ₀ at the alternating current of the first embodiment of the present invention. It is a graph which shows the resonance characteristic of the resonant magnetic field in resonance frequency A1 of the _1st Embodiment of this invention. Is a graph showing a resonance characteristic of a resonant magnetic field at the resonant frequency A ₂ of the first embodiment of the present invention. Is a graph showing a resonance characteristic of a resonant magnetic field at the resonant frequency A ₃ of the first embodiment of the present invention. Is a graph showing a resonance characteristic of a resonant magnetic field at the resonant frequency A ₄ of the first embodiment of the present invention. Is a graph showing a resonance characteristic of a resonant magnetic field at the resonant frequency A ₅ of the first embodiment of the present invention. Is a graph showing a resonance characteristic of a resonant magnetic field at the resonant frequency A ₆ of the first embodiment of the present invention. It is a graph which shows the resonance characteristic of the resonant magnetic field in resonance frequency A- ₂ of the 1st Embodiment of this invention. It is a graph which shows the resonance characteristic of the resonant magnetic field in resonance frequency A- ₁ of the 1st Embodiment of this invention. Is a graph showing a resonance characteristic of a resonant magnetic field at the resonant frequency A ₀ of the first embodiment of the present invention. It is a graph which shows the resonance characteristic of the resonant magnetic field in resonance frequency B1 of the _1st Embodiment of this invention. It is a graph showing a resonance characteristic of a resonant magnetic field at the resonant frequency B ₂ of the first embodiment of the present invention. It is a graph showing a resonance characteristic of a resonant magnetic field at the resonant frequency B ₃ of the first embodiment. It is a graph showing a resonance characteristic of a resonant magnetic field at the resonant frequency B ₄ of the first embodiment of the present invention. It is a graph showing a resonance characteristic of a resonant magnetic field at the resonant frequency B ₅ of the first embodiment of the present invention. It is a graph showing a resonance characteristic of a resonant magnetic field at the resonant frequency B ₆ of the first embodiment of the present invention. It is a graph which shows the resonance characteristic of the resonant magnetic field in resonance frequency B- ₂ of the 1st Embodiment of this invention. It is a graph which shows the resonance characteristic of the resonant magnetic field in resonance frequency B- ₁ of the 1st Embodiment of this invention. It is a graph showing a resonance characteristic of a resonant magnetic field at the resonant frequency B ₀ of the first embodiment of the present invention. It is a graph which shows an example of distribution of the resonance magnetic field in a 1st embodiment of the present invention. It is a graph which shows another example of distribution of the resonant magnetic field in the 1st Embodiment of this invention. It is a correlation diagram of the resonant frequency and resonant magnetic field in the 1st Embodiment of this invention. It is another correlation figure of the resonant frequency and resonant magnetic field in the 1st Embodiment of this invention. It is a wave form diagram which shows an example of the alternating current used for the electromagnetic field process concerning the 2nd Embodiment of this invention. It is explanatory drawing which shows the method of carrying out another electromagnetic field process concerning the 2nd Embodiment of this invention. It is explanatory drawing which shows another method of processing an electromagnetic field concerning the 2nd Embodiment of this invention. It is a graph which shows the sustainability of the effect of the active treated water which carried out the electromagnetic field process concerning the 2nd Embodiment of this invention. It is a schematic diagram for demonstrating the effect of the electromagnetic field process concerning the 2nd Embodiment of this invention. It is a schematic diagram which shows the method of removing the influence of the geomagnetism concerning the 3rd Embodiment of this invention. It is sectional drawing which shows the method of magnetically shielding the geomagnetism concerning the 3rd Embodiment of this invention. It is sectional drawing which shows another method of magnetically shielding the geomagnetism concerning the 3rd Embodiment of this invention. It is sectional drawing which shows the method of the geomagnetic demagnetization concerning the 3rd Embodiment of this invention. It is a schematic block diagram of the electromagnetic field processing apparatus of the 4th Embodiment of this invention. It is a circuit block diagram of the specific alternating current generation in the electromagnetic field processing apparatus of the 4th Embodiment of this invention. It is a block diagram of the flow-path change mechanism of the to-be-processed water in the suitable aspect of the 4th Embodiment of this invention. It is a layout block diagram of the electromagnetic field processing apparatus in the suitable aspect of the 4th Embodiment of this invention. It is a figure which shows schematic structure of the electromagnetic field processing apparatus of the modification of the 4th Embodiment of this invention. It is a graph showing a resonance characteristic of the resonance frequency A ₇ in unipolar current according to a fourth embodiment of the present invention. It is a graph showing a resonance characteristic of the resonance frequency B ₇ in unipolar current according to a fourth embodiment of the present invention. It is a graph showing a resonance characteristic of a resonant magnetic field at the resonant frequency A ₇ in the fourth embodiment of the present invention. It is a graph showing a resonance characteristic of a resonant magnetic field at the resonant frequency B ₇ of the fourth embodiment of the present invention.

Explanation of symbols

1, 1a, 33, 33a, 52 Water pipe 2, 2a Coil 3 Water to be treated 4 AC power supply 5, 5a Activated water 6 Magnetic field 7, 25, 26 Electromagnetic field applying part 8 Tank 9 Reservoir 10 Experiment tank 11 Partition plate 12 , 13, 14 Reservoir 15 Pump 16 Calcium phosphate 17 Sampling tube 21 First frequency current 22 Second frequency current 23 First AC power supply 24 Second AC power supply 27 Hydrogen ion adhesion cluster 28 Hydroxide ion adhesion cluster 31 Geomagnetism Direction 32 Vertical plane 34 Magnetic shield 35 Magnetic core 36 Magnetic shielding container 37 Magnetic sensor 38 Constant current source 39 Degaussing coil 41 Electromagnetic field processing device 42 Alternating current supply unit 43 Drive power supply unit 44 Crystal oscillator 45 Frequency dividing circuit 46 Frequency Modulation circuit 47 Amplitude modulation circuit 48 Baffle plate 49 Cylindrical bar 50 Connecting material Coil Kai wound opposite the coil 54 1 carbon dioxide degassing apparatus 53 positive wound 55 one polarity current supply unit

Claims (22)

In an electromagnetic field treatment method for water, an electromagnetic field induced current is passed through a coil, and an oscillating electromagnetic field induced in the coil is applied to water to activate the water.
One resonance frequency is selected from the first resonance frequency group of the electromagnetic field induced current that activates the water or the second resonance frequency group of the electromagnetic field induced current that activates the water,
Inducing an oscillating electromagnetic field in the coil by an electromagnetic field induced current of the selected one resonance frequency,
The first resonant frequency group, resonant frequency _A -2 of 151.5Hz or near the resonant frequency _A -1 of the 222.5Hz or near the resonant frequency _A 0 of 345.0Hz or in the vicinity thereof, 484Hz or its Resonance frequency A ₁ , 954 Hz in the vicinity or resonance frequency A ₂ in the vicinity thereof, 3.5 kHz or resonance frequency A ₃ in the vicinity thereof, 7.0 kHz or resonance frequency A ₄ in the vicinity thereof, 20.0 kHz or resonance frequency in the vicinity thereof A ₅ , resonance frequency A ₆ at or near 37.3 kHz, or resonance frequency A ₇ at or near 80.0 kHz,
The second resonance frequency group is 205.0 Hz or a resonance frequency B ₋₂ , 301.0 Hz in the vicinity thereof, or a resonance frequency B ₋₁ , 466.0 Hz in the vicinity thereof, or a resonance frequency B ₀ , 655 Hz or in the vicinity thereof. Resonance frequency B ₁ , 1.29 kHz in the vicinity or resonance frequency B ₂ in the vicinity thereof, 4.73 kHz or resonance frequency B ₃ in the vicinity thereof, 9.47 kHz or resonance frequencies B ₄ in the vicinity thereof, 27.0 kHz or in the vicinity thereof Resonance frequency B ₅ , resonance frequency B ₆ at or near 50.4 kHz, resonance frequency B ₇ at or around 108.0 kHz,
The method for treating an electromagnetic field of water, wherein the resonance frequency in the vicinity thereof is about ± 1.2% of the numerical value of the resonance frequency. In an electromagnetic field treatment method for water, an electromagnetic field induced current is passed through a coil, and an oscillating electromagnetic field induced in the coil is applied to water to activate the water.
One resonance frequency is selected from the first resonance frequency group of the electromagnetic field induced current that activates the water or the second resonance frequency group of the electromagnetic field induced current that activates the water,
Inducing an oscillating electromagnetic field in the coil by an electromagnetic field induced current having a frequency within a half-value width in the resonance characteristic of the selected resonant frequency,
The first resonant frequency group, resonant frequency _A -2 of 151.5Hz or near the resonant frequency _A -1 of the 222.5Hz or near the resonant frequency _A 0 of 345.0Hz or in the vicinity thereof, 484Hz or its Resonance frequency A ₁ , 954 Hz in the vicinity or resonance frequency A ₂ in the vicinity thereof, 3.5 kHz or resonance frequency A ₃ in the vicinity thereof, 7.0 kHz or resonance frequency A ₄ in the vicinity thereof, 20.0 kHz or resonance frequency in the vicinity thereof A ₅ , resonance frequency A ₆ at or near 37.3 kHz, or resonance frequency A ₇ at or near 80.0 kHz,
The second resonance frequency group is 205.0 Hz or a resonance frequency B ₋₂ , 301.0 Hz in the vicinity thereof, or a resonance frequency B ₋₁ , 466.0 Hz in the vicinity thereof, or a resonance frequency B ₀ , 655 Hz or in the vicinity thereof. Resonance frequency B ₁ , 1.29 kHz in the vicinity or resonance frequency B ₂ in the vicinity thereof, 4.73 kHz or resonance frequency B ₃ in the vicinity thereof, 9.47 kHz or resonance frequencies B ₄ in the vicinity thereof, 27.0 kHz or in the vicinity thereof Resonance frequency B ₅ , resonance frequency B ₆ at or near 50.4 kHz, resonance frequency B ₇ at or around 108.0 kHz,
The method for treating an electromagnetic field of water, wherein the resonance frequency in the vicinity thereof is about ± 1.2% of the numerical value of the resonance frequency. In an electromagnetic field treatment method for water, an electromagnetic field induced current is passed through a coil, and an oscillating electromagnetic field induced in the coil is applied to water to activate the water.
Selecting one resonance frequency from each of a first resonance frequency group of the electromagnetic field induced current that activates the water and a second resonance frequency group of the electromagnetic field induced current that activates the water;
An oscillating electromagnetic field is induced in the coil by an electromagnetic field induced current of one resonance frequency selected from the first resonance frequency group and an electromagnetic field induced current of one resonance frequency selected from the second resonance frequency group. ,
The first resonant frequency group, resonant frequency _A -2 of 151.5Hz or near the resonant frequency _A -1 of the 222.5Hz or near the resonant frequency _A 0 of 345.0Hz or in the vicinity thereof, 484Hz or its Resonance frequency A ₁ , 954 Hz in the vicinity or resonance frequency A ₂ in the vicinity thereof, 3.5 kHz or resonance frequency A ₃ in the vicinity thereof, 7.0 kHz or resonance frequency A ₄ in the vicinity thereof, 20.0 kHz or resonance frequency in the vicinity thereof A ₅ , resonance frequency A ₆ at or near 37.3 kHz, or resonance frequency A ₇ at or near 80.0 kHz,
The second resonance frequency group is 205.0 Hz or a resonance frequency B ₋₂ , 301.0 Hz in the vicinity thereof, or a resonance frequency B ₋₁ , 466.0 Hz in the vicinity thereof, or a resonance frequency B ₀ , 655 Hz or in the vicinity thereof. Resonance frequency B ₁ , 1.29 kHz in the vicinity or resonance frequency B ₂ in the vicinity thereof, 4.73 kHz or resonance frequency B ₃ in the vicinity thereof, 9.47 kHz or resonance frequencies B ₄ in the vicinity thereof, 27.0 kHz or in the vicinity thereof Resonance frequency B ₅ , resonance frequency B ₆ at or near 50.4 kHz, resonance frequency B ₇ at or around 108.0 kHz,
The method for treating an electromagnetic field of water, wherein the resonance frequency in the vicinity thereof is about ± 1.2% of the numerical value of the resonance frequency. In an electromagnetic field treatment method for water, an electromagnetic field induced current is passed through a coil, and an oscillating electromagnetic field induced in the coil is applied to water to activate the water.
Selecting one resonance frequency from each of a first resonance frequency group of the electromagnetic field induced current that activates the water and a second resonance frequency group of the electromagnetic field induced current that activates the water;
An electromagnetic field induced current having a frequency within the half-value width in the resonance characteristic of the resonance frequency selected from the first resonance frequency group and a half-value width in the resonance characteristic of the resonance frequency selected from the second resonance frequency group. By inducing an oscillating electromagnetic field in the coil with an electromagnetic field induced current of frequency,
The first resonant frequency group, resonant frequency _A -2 of 151.5Hz or near the resonant frequency _A -1 of the 222.5Hz or near the resonant frequency _A 0 of 345.0Hz or in the vicinity thereof, 484Hz or its Resonance frequency A ₁ , 954 Hz in the vicinity or resonance frequency A ₂ in the vicinity thereof, 3.5 kHz or resonance frequency A ₃ in the vicinity thereof, 7.0 kHz or resonance frequency A ₄ in the vicinity thereof, 20.0 kHz or resonance frequency in the vicinity thereof A ₅ , resonance frequency A ₆ at or near 37.3 kHz, or resonance frequency A ₇ at or near 80.0 kHz,
The second resonance frequency group is 205.0 Hz or a resonance frequency B ₋₂ , 301.0 Hz in the vicinity thereof, or a resonance frequency B ₋₁ , 466.0 Hz in the vicinity thereof, or a resonance frequency B ₀ , 655 Hz or in the vicinity thereof. Resonance frequency B ₁ , 1.29 kHz in the vicinity or resonance frequency B ₂ in the vicinity thereof, 4.73 kHz or resonance frequency B ₃ in the vicinity thereof, 9.47 kHz or resonance frequencies B ₄ in the vicinity thereof, 27.0 kHz or in the vicinity thereof Resonance frequency B ₅ , resonance frequency B ₆ at or near 50.4 kHz, resonance frequency B ₇ at or around 108.0 kHz,
The method for treating an electromagnetic field of water, wherein the resonance frequency in the vicinity thereof is about ± 1.2% of the numerical value of the resonance frequency. By setting the peak current of the electromagnetic field induced current at the resonance frequency to a specific current value, the peak intensity of the oscillating magnetic field induced in the coil by the electromagnetic field induced current at the resonance frequency becomes a specific magnetic field strength. 5. The electromagnetic field treatment method for water according to claim 1, wherein the strength of the magnetic field or the magnetic field strength within a half-value width in the resonance characteristics of the resonant magnetic field is set. 6. The electromagnetic field treatment method for water according to claim 5, wherein the intensity of the resonance magnetic field is a positive integer multiple of the magnetic field intensity of the fundamental mode. The magnetic field strength of the resonance mode of the resonance magnetic field in the electromagnetic field induced current of the resonance frequency A _i (i = an integer of −2 to 7) is 5.3 mG or the vicinity thereof, 7.4 mG Its vicinity, 12.3 mG or its vicinity, 17.3 mG or its vicinity, 31.9 mG or its vicinity, 130.6 mG or its vicinity, 323.0 mG or its vicinity, 1123.5 mG or its vicinity, 2556.0 mG or its Neighborhood, 6039.0 mG or its neighborhood,
The magnetic field strength of the resonance mode of the resonance magnetic field in the electromagnetic field induced current of the resonance frequency B _j (j = −2 to 7) is 7.1 mG or its vicinity, 10.4 mG Its vicinity, 16.3 mG or its vicinity, 23.5 mG or its vicinity, 47.1 mG or its vicinity, 188.2 mG or its vicinity, 463.5 mG or its vicinity, 1601.0 mG or its vicinity, 3342.5 mG or its Neighborhood, 7302.9 mG or its neighborhood,
7. The electromagnetic field treatment method for water according to claim 6, wherein the magnetic field strength in the vicinity thereof is about ± 2% of the numerical value of the magnetic field strength. The electromagnetic field treatment method for water according to any one of claims 1 to 7, wherein an influence of geomagnetism is removed from the coil. The water electromagnetic field treatment method according to claim 8, wherein an axis of the coil is disposed in a plane orthogonal to the direction of the geomagnetism. 9. The electromagnetic field treatment method for water according to claim 8, wherein the coil is encapsulated by a magnetic shield. 9. The electromagnetic field treatment method for water according to claim 8, wherein a magnetic field strength of the geomagnetism in the axial direction of the coil is detected, and a static magnetic field is applied to the coil so that the magnetic field strength becomes substantially zero. . The electromagnetic field treatment method according to any one of claims 1 to 11, wherein the water is subjected to an electromagnetic field treatment after degassing the carbon dioxide gas. The electromagnetic field processing method according to any one of claims 1 to 12, wherein an insulator is disposed in a water passage in a region where the coil is wound, and the water is subjected to electromagnetic field treatment by changing the flow of the water. . An electromagnetic field treatment apparatus for water that activates the water by applying an electromagnetic field induced current to the coil and applying an oscillating electromagnetic field induced in the coil to the water,
Coils,
Electromagnetic field induction at one resonance frequency selected from the first resonance frequency group of the electromagnetic field induced current that activates the water or the second resonance frequency group of the electromagnetic field induced current that activates the water. A power supply for supplying current to the coil;
Have
The first resonant frequency group, resonant frequency _A -2 of 151.5Hz or near the resonant frequency _A -1 of the 222.5Hz or near the resonant frequency _A 0 of 345.0Hz or in the vicinity thereof, 484Hz or its Resonance frequency A ₁ , 954 Hz in the vicinity or resonance frequency A ₂ in the vicinity thereof, 3.5 kHz or resonance frequency A ₃ in the vicinity thereof, 7.0 kHz or resonance frequency A ₄ in the vicinity thereof, 20.0 kHz or resonance frequency in the vicinity thereof A ₅ , resonance frequency A ₆ at or near 37.3 kHz, or resonance frequency A ₇ at or near 80.0 kHz,
The second resonance frequency group is 205.0 Hz or a resonance frequency B ₋₂ , 301.0 Hz in the vicinity thereof, or a resonance frequency B ₋₁ , 466.0 Hz in the vicinity thereof, or a resonance frequency B ₀ , 655 Hz or in the vicinity thereof. Resonance frequency B ₁ , 1.29 kHz in the vicinity or resonance frequency B ₂ in the vicinity thereof, 4.73 kHz or resonance frequency B ₃ in the vicinity thereof, 9.47 kHz or resonance frequencies B ₄ in the vicinity thereof, 27.0 kHz or in the vicinity thereof Resonance frequency B ₅ , resonance frequency B ₆ at or near 50.4 kHz, resonance frequency B ₇ at or around 108.0 kHz,
The electromagnetic field processing apparatus characterized in that the resonance frequency in the vicinity thereof is about ± 1.2% of the numerical value of the resonance frequency. An electromagnetic field treatment apparatus for water that activates the water by applying an electromagnetic field induced current to the coil and applying an oscillating electromagnetic field induced in the coil to the water,
Coils,
In the resonance characteristic of one resonance frequency selected from the first resonance frequency group of the electromagnetic field induced current that activates the water or the second resonance frequency group of the electromagnetic field induced current that activates the water A power supply for supplying an electromagnetic field-induced current having a frequency within a half-value width to the coil;
Have
The first resonant frequency group, resonant frequency _A -2 of 151.5Hz or near the resonant frequency _A -1 of the 222.5Hz or near the resonant frequency _A 0 of 345.0Hz or in the vicinity thereof, 484Hz or its Resonance frequency A ₁ , 954 Hz in the vicinity or resonance frequency A ₂ in the vicinity thereof, 3.5 kHz or resonance frequency A ₃ in the vicinity thereof, 7.0 kHz or resonance frequency A ₄ in the vicinity thereof, 20.0 kHz or resonance frequency in the vicinity thereof A ₅ , resonance frequency A ₆ at or near 37.3 kHz, or resonance frequency A ₇ at or near 80.0 kHz,
The second resonance frequency group is 205.0 Hz or a resonance frequency B ₋₂ , 301.0 Hz in the vicinity thereof, or a resonance frequency B ₋₁ , 466.0 Hz in the vicinity thereof, or a resonance frequency B ₀ , 655 Hz or in the vicinity thereof. Resonance frequency B ₁ , 1.29 kHz in the vicinity or resonance frequency B ₂ in the vicinity thereof, 4.73 kHz or resonance frequency B ₃ in the vicinity thereof, 9.47 kHz or resonance frequencies B ₄ in the vicinity thereof, 27.0 kHz or in the vicinity thereof Resonance frequency B ₅ , resonance frequency B ₆ at or near 50.4 kHz, resonance frequency B ₇ at or around 108.0 kHz,
The electromagnetic field processing apparatus characterized in that the resonance frequency in the vicinity thereof is about ± 1.2% of the numerical value of the resonance frequency. An electromagnetic field treatment apparatus for water that activates the water by applying an electromagnetic field induced current to the coil and applying an oscillating electromagnetic field induced in the coil to the water,
Coils,
One resonance frequency in the first resonance frequency group of the electromagnetic field induced current that activates the water and one of the second resonance frequency group of the electromagnetic field induction current that activates the water An alternating current supply unit for supplying an alternating current amplitude-modulated with a resonance frequency;
A drive power supply unit for driving the alternating current supply unit;
Have
The first resonant frequency group, resonant frequency _A -2 of 151.5Hz or near the resonant frequency _A -1 of the 222.5Hz or near the resonant frequency _A 0 of 345.0Hz or in the vicinity thereof, 484Hz or its Resonance frequency A ₁ , 954 Hz in the vicinity or resonance frequency A ₂ in the vicinity thereof, 3.5 kHz or resonance frequency A ₃ in the vicinity thereof, 7.0 kHz or resonance frequency A ₄ in the vicinity thereof, 20.0 kHz or resonance frequency in the vicinity thereof A ₅ , resonance frequency A ₆ at or near 37.3 kHz, or resonance frequency A ₇ at or near 80.0 kHz,
The second resonance frequency group is 205.0 Hz or a resonance frequency B ₋₂ , 301.0 Hz in the vicinity thereof, or a resonance frequency B ₋₁ , 466.0 Hz in the vicinity thereof, or a resonance frequency B ₀ , 655 Hz or in the vicinity thereof. Resonance frequency B ₁ , 1.29 kHz in the vicinity or resonance frequency B ₂ in the vicinity thereof, 4.73 kHz or resonance frequency B ₃ in the vicinity thereof, 9.47 kHz or resonance frequencies B ₄ in the vicinity thereof, 27.0 kHz or in the vicinity thereof Resonance frequency B ₅ , resonance frequency B ₆ at or near 50.4 kHz, resonance frequency B ₇ at or around 108.0 kHz,
The electromagnetic field processing apparatus characterized in that the resonance frequency in the vicinity thereof is about ± 1.2% of the numerical value of the resonance frequency. An electromagnetic field treatment apparatus for water that activates the water by applying an electromagnetic field induced current to the coil and applying an oscillating electromagnetic field induced in the coil to the water,
Coils,
A frequency within a half-value width in a resonance characteristic of one resonance frequency in a first resonance frequency group of the electromagnetic field induced current that activates the water, and a first frequency of the electromagnetic field induced current that activates the water. An alternating current supply unit for supplying an alternating current amplitude-modulated with a frequency within a half-value width in the resonance characteristic of one resonance frequency in the two resonance frequency groups;
A drive power supply unit for driving the alternating current supply unit;
Have
The first resonant frequency group, resonant frequency _A -2 of 151.5Hz or near the resonant frequency _A -1 of the 222.5Hz or near the resonant frequency _A 0 of 345.0Hz or in the vicinity thereof, 484Hz or its Resonance frequency A ₁ , 954 Hz in the vicinity or resonance frequency A ₂ in the vicinity thereof, 3.5 kHz or resonance frequency A ₃ in the vicinity thereof, 7.0 kHz or resonance frequency A ₄ in the vicinity thereof, 20.0 kHz or resonance frequency in the vicinity thereof A ₅ , resonance frequency A ₆ at or near 37.3 kHz, or resonance frequency A ₇ at or near 80.0 kHz,
The second resonance frequency group is 205.0 Hz or a resonance frequency B ₋₂ , 301.0 Hz in the vicinity thereof, or a resonance frequency B ₋₁ , 466.0 Hz in the vicinity thereof, or a resonance frequency B ₀ , 655 Hz or in the vicinity thereof. Resonance frequency B ₁ , 1.29 kHz in the vicinity or resonance frequency B ₂ in the vicinity thereof, 4.73 kHz or resonance frequency B ₃ in the vicinity thereof, 9.47 kHz or resonance frequencies B ₄ in the vicinity thereof, 27.0 kHz or in the vicinity thereof Resonance frequency B ₅ , resonance frequency B ₆ at or near 50.4 kHz, resonance frequency B ₇ at or around 108.0 kHz,
The electromagnetic field processing apparatus characterized in that the resonance frequency in the vicinity thereof is about ± 1.2% of the numerical value of the resonance frequency. The power supply or the alternating current supply unit sets the peak current of the electromagnetic field induced current at the resonance frequency to a specific current value, and specifies the peak intensity of the oscillating magnetic field induced in the coil by the electromagnetic field induced current at the resonance frequency. 18. The water according to claim 14, wherein the intensity of the resonant magnetic field becomes a magnetic field intensity within a half-value width in a resonance characteristic of the resonant magnetic field. Electromagnetic field processing device. The electromagnetic field treatment apparatus for water according to claim 18, wherein the intensity of the resonance magnetic field is a positive integer multiple of the magnetic field intensity of the fundamental mode. The magnetic field strength of the resonance mode of the resonance magnetic field in the electromagnetic field induced current of the resonance frequency A _i (i = an integer of −2 to 7) is 5.3 mG or the vicinity thereof, 7.4 mG Its vicinity, 12.3 mG or its vicinity, 17.3 mG or its vicinity, 31.9 mG or its vicinity, 130.6 mG or its vicinity, 323.0 mG or its vicinity, 1123.5 mG or its vicinity, 2556.0 mG or its Neighborhood, 6039.0 mG or its neighborhood,
The magnetic field strength of the resonance mode of the resonance magnetic field in the electromagnetic field induced current of the resonance frequency B _j (j = −2 to 7) is 7.1 mG or its vicinity, 10.4 mG Its vicinity, 16.3 mG or its vicinity, 23.5 mG or its vicinity, 47.1 mG or its vicinity, 188.2 mG or its vicinity, 463.5 mG or its vicinity, 1601.0 mG or its vicinity, 3342.5 mG or its Neighborhood, 7302.9 mG or its neighborhood,
20. The electromagnetic field treatment apparatus for water according to claim 19, wherein the magnetic field strength in the vicinity thereof is about ± 2% of the numerical value of the magnetic field strength. 21. The electromagnetic field treatment apparatus for water according to claim 14, wherein means for removing the influence of geomagnetism is attached to the coil. The electromagnetic field treatment apparatus according to any one of claims 14 to 21, wherein the water is subjected to the electromagnetic field treatment after the water is degassed with carbon dioxide.

Images