U.S. patent number 3,921,620 [Application Number 05/323,045] was granted by the patent office on 1975-11-25 for magnetic medical treatment device.
Invention is credited to Takeo Nakayama.
United States Patent |
3,921,620 |
Nakayama |
November 25, 1975 |
Magnetic medical treatment device
Abstract
A magnetic medical treatment device having a plurality of
magnets or magnetic shells so arranged that the same polarity poles
of the magnets or magnetic shells closely contact a selected part
of a human body such that polarization and induced currents are
efficiently generated in the human body. Each of the magnetic
shells of the same polarity is provided with a ferromagnetic metal
plate on the side thereof opposite the body contacting sides of the
magnetic shells.
Inventors: |
Nakayama; Takeo (Arakawa,
Tokyo, JA) |
Family
ID: |
27431619 |
Appl.
No.: |
05/323,045 |
Filed: |
January 12, 1973 |
Current U.S.
Class: |
600/15 |
Current CPC
Class: |
A61N
2/06 (20130101) |
Current International
Class: |
A61N
2/00 (20060101); A61N 2/06 (20060101); A61N
001/42 () |
Field of
Search: |
;128/1R,1.3,24.1,68.1,82.1,379,380,381,382,384,385 |
References Cited
[Referenced By]
U.S. Patent Documents
Foreign Patent Documents
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|
12,847 |
|
1849 |
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UK |
|
259,818 |
|
May 1963 |
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AU |
|
429,079 |
|
May 1935 |
|
UK |
|
259,271 |
|
Oct 1963 |
|
AU |
|
371 |
|
1879 |
|
UK |
|
Primary Examiner: Kamm; William E.
Attorney, Agent or Firm: Weiner; Irving M.
Claims
What is claimed is as follows:
1. A magnetic medical treatment device for a human wherein magnetic
force is utilized to achieve a desired magnetic flux which is cause
to act upon a human body generating polarization and induced
currents within said human body, and comprising:
a supportive apparatus for magnetic means adapted to contact a
portion of the human body;
a plurality of magnetic means arranged in a plurality of rows upon
a first surface of said supportive device, each of the means being
disposed with respect to each other such that one pole of each
magnetic means closely contacts a selected part of the human body
to achieve a desired intensity of magnetic flux; and
at least one ferromagnetic metal plate affixed to a second surface
of said supportive device which is opposite said first surface of
said supportive device;
wherein said supportive device comprises a belly-band having a main
body and said magnetic means secured to said first surface of said
supportive device where said belly-band contacts the waist portion
of said human body.
2. The magnetic medical treatment device according to claim 1,
wherein said magnetic means comprises a first plurality of magnets
positioned in the center of said main body and a second plurality
of magnets positioned in any area adjacent to one end of said main
body where the belly-band contacts the waist portion and belly
portion, respectively, of said human body, and wherein, when said
belly-band is worn by a human body, the poles are the same polarity
of said first plurality of magnets substantially face the poles of
the opposite polarity of said second plurality of magnets.
Description
BACKGROUND OF THE INVENTION
I. Field of the Invention
The present invention relates to a magnetic medical treatment
device for efficiently causing magnetic flux to act on a human
body.
II. Description of the Prior Art
A magnetic medical treatment wrist band which allegedly
magnetically cures an affected part of a human body by the
utilization of the magnetic force of magnets has been known.
However, the conventional magnetic medical treatment wrist band has
been constructed by merely arranging magnets in a particular
pattern.
SUMMARY OF THE INVENTION
This invention, which will be subsequently described in greater
detail, relates to a magnetic medical treatment device for
efficiently causing magnetic flux to act on a human body and
comprises a plurality of magnets so arranged that the same polarity
poles of the magnets contact a selected part of a human body. The
present invention is applicable to magnetic medical treatment
devices such as a wrist band, belly-band, pillow, bed, pad and
plaster which magnetically treat an affected part of a human body.
The magnetic medical treatment device of the present invention
greatly enhances treating effects by effectively utilizing magnetic
force to increase flux density. For this purpose, according to the
present invention, the magnetic treatment device comprises a
plurality of magnets so arranged that the magnets of the same
polarity closely contact a selected part of a human body or
alternatively, the magnets are applied with ferromagnetic metal
plates to the sides thereof oppoiste to the sides where the magnets
contact the human body, whereby flux density can be greatly
increased to enhance curing effects.
It is therefore a principal object of the present invention to
provide a magnetic medical treatment device which can treat an
affected part of a human body.
It is another object of the present invention to provide a magnetic
medical treatment device which treats an affected part of a human
body by arranging a plurality of magnets in a unique way.
It is still another object of the present invention to provide a
magnetic medical treatment device which treats an affected part of
a human body by arranging a plurality of magnetic shells in a
unique way.
It is a further object of the present invention to provide a
magnetic medical treatment device which comprises a plurality of
magnets so arranged that the same polarity poles of the magnets
closely contact an affected part of a human body.
It is a further object of the present invention to provide a
magnetic medical treatment device which comprises a plurality of
magnetic shells so arranged that the same polarity poles of the
magnetic shells closely contact the body while the magnetic shells
are provided with ferromagnetic metal plates on the sides opposite
to the sides where the shells contact the human body.
It is a further object of the present invention to provide a
magnetic medical treatment device in the form of a belly-band
comprising a plurality of magnets so arranged that the same
polarity poles of the magnets closely contact an affected part of a
human body.
It is still a further object of the present invention to provide a
magnetic medical treatment device in the form of a belly-band which
comprises a plurality of magnetic shells so arranged that the same
polarity of the magnetic shells closely contact an affected part of
a human body, and the magnetic shells are provided with
ferromagnetic metal plates on the sides thereof opposite to the
sides where the magnetic shells contact the human body.
According to the present invention, there has been provided a
magnetic medical treatment belly-band comprising a main body, a
plurality of magnets secured to one side of the main body where the
band contacts a selected part of a human body, the magnets being so
arranged that the poles of the same polarity are disposed in one
and the same direction. Cloth pieces cover the magnets.
Other objects, advantages and applications of the present invention
will be more apparent to those skilled in the art of magnetic
medical treatment devices when the following detailed description
of some examples of the best modes contemplated for practicing the
invention is read in conjunction with the accompanying drawings
which show specific embodiments of the invention for illustration
purposes only, but not for limiting the scope of the appended
claims.
BRIEF DESCRIPTION OF THE DRAWINGS
The description herein makes reference to the accompanying drawings
wherein like reference characters refer to like or equivalent
components throughout the several views, and in which:
FIG. 1 is a magnetic figure of one embodiment of a magnetic medical
treatment device constructed in accordance with the principles of
the present invention and in which the same polarity poles of
magnets are arranged in the same direction;
FIG. 2 is a magnetic figure of a second embodiment of a magnetic
medical treatment device constructed in accordance with the
principles of the present invention and in which the opposite
polarity poles of magnets are alternately arranged;
FIG. 3 is a view showing the principle on the basis of which a
polarizing current is generated;
FIG. 4 is a view showing the principle on the basis of which an
induced current is generated;
FIG. 5 is a reverse side view of a belly-band in which the present
invention is embodied;
FIG. 6 is a perspective view of a belly-band in which a different
type of magnetic medical treatment device embodying the present
invention is employed; and
FIG. 7 is a perspective view of a belly-band in which a further
different type of magnetic medical treatment device embodying the
present invention is employed.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
When the same polarity poles of several magnets are arranged in one
and the same direction as shown in FIG. 1 and applied against a
selected part of a human body, the magnetic lines of force
surrounding the magnets to the extent that the driven magnetic
lines of force may permeate deep into the human body whereby a high
polarization current is generated in the human body. The curve of
the magnetic field outside of each of the outermost magnets will be
greater than those around the remaining magnets, thereby generating
an induced current. Therefore, the arrangement of magnets as shown
in FIG. 1 is most effective to generate polarization current and
induced current.
In FIG. 2, the opposite polarity poles of magnets are alternately
arranged. Although the magnetic field outside of each of the
outermost magnets may have a greater curve than those around the
remaining magnets and an induced current will be generated as in
the arrangement of FIG. 1, the magnetic lines of force pass around
only the surface of the human body and consequently, only a low
polarization current is generated.
The greater the number of magnets in an array, the more effective
is the generation of polarization and induced currents. In such a
case, the magnetic lines of force between adjacent magnets are
expelled far away from the associated magnets by the magnetic lines
of force surrounding the magnets to permeate deep into the human
body and the curve of the magnetic fields around the outermost
magnets is greater than those of the magnetic fields around the
intermediate magnets.
It is generally preferable to arrange magnets in a number of n (n
being greater than 2) along an axis of ordinate and an axis of
abscissa and at a slanted angle thereto. The greater the value of
n, the more effective is the generation of polarization and induced
currents. When the same polarity poles of the magnets are arranged
in one and the same direction, it has been experimentally found
that the magnetic lines of force are driven far away from the
magnets due to the repulsion force between the same polarity poles
of magnets so that the magnetic line of force can permeate deep
into the human body. It has been also found that the magnetic lines
of force outside the outermost magnets in the array pass by nearer
to the associated magnets than the magnetic lines of force for the
intermediate magnets pass by the associated magnets and the
magnetic lines of force for the outermost magnets will have a curve
greater than that of those for the intermediate magnets. However,
when the opposite polarity poles of the magnets are alternately
arranged, most of the magnetic lines of force will pass along only
the surface of the human body and only a small portion of the
magnetic lines of force will permeate deep into the human body.
When the magnets are arranged in a ring with the same polarity
poles of the magnets directed inwardly, the magnetic lines of force
will extend to the center of the ring without attenuation. On the
other hand, when the opposite polarity poles of the magnets are
alternately arranged in a ring, the magnetic lines of force having
the opposite polarities will attract toward each other and in
consequence, the magnetic lines of force will pass along only the
surface of the human body.
A ring of magnets which is called a magnetic band in the art is
generally worn on an arm or leg. In the limbs of a human, blood and
body fluid flow in the longitudinal direction thereof in both the
hypodermal and deep areas in the human body. Therefore, it is
preferable that the magnetic lines of force pass at right angles to
the longitudinal direction of the limbs and will not attenuate in
the deep area of the human body. In other words, since a
polarization current is more effective than an induced current for
medical treatment, it is preferable that the magnets be arranged to
increase the polarization current as much as possible or the
magnets be arranged with the same polarity poles of the magnets
disposed on the inner side.
The effects of a magnetic field upon a living body are due to the
fact that the electrolyte within the living body is dissociated by
polarization and induced currents and the dissociation of
electrolyte is effective in controlling the sympathetic nerve
system among autonomic nervous systems.
Effects of polarization and induced currents on a human body are as
follows:
1. Polarization current:
As shown in FIG. 3, when it is assumed that a component of force
having the flux density of 2 which acts on a blood vessel 1, at
right angles thereto is B gauss, the electromotive force generated
thereby is E volt. The polarization current (the principle of an
electromagnetic flow meter) is a current which is generated at
electromotive force E. The polarization current generates an ionic
polarization in the blood vessel which in turn causes electrolyte
dissociation in the human body.
2. Induced current:
As shown in FIG. 4, when a magnet 3 is applied against a human body
4, only a non-uniform magnetic field acts on the human body 4.
Therefore, when some systems of the human body having a curvature
(blood, intracelluar liquid, lymph and the like) move in the
direction of the curvature or in a direction at right angles to the
plane of the magnetic pole, the electromotive force is in
proportion to variation in the magnetic lines of force across which
such systems move for a unit time. The relationship between the
electromotive force E and variation in the magnetic lines of force
may be expressed by the equation E = Kd.phi./dt wherein K is a
proportional constant and d.phi./dt is the flux density across
which a particular system of the human body moves for a unit time.
Current generated by the electromotive force is called an induced
current. The induced current also causes electrolyte dissociation.
When the magnetic poles are arranged so that the magnetic field
induced by the magnetic poles effectively generates polarization
and induced currents in a human body in the manner as mentioned
hereinabove, there is provided a most effective magnetic medical
device.
FIG. 5 shows one embodiment of the magnetic medical treatment
device of the invention which is in the form of a belly-band
comprising a main body 5 having a center portion (the center
portion is applied against the waist of a human body when the
device is worn by a human) which is provided with magnets 6 in a
plurality of rows with the same polarity poles of the magnets
directing in the same direction on the side which contacts the
belly of a human body when the belly-band is applied against the
belly. Numeral 7 denotes a cloth piece which covers the
magnets.
With the arrangement and construction of the magnetic medical
treatment device of the invention, when the belly-band is applied
against the human body, the magnetic lines of force induced by the
magnets can permeate deeper into the human body than the magnetic
lines of force induced by the magnets in the corresponding
conventional magnetic medical treatment devices can permeate into
the human body.
FIG. 6 and FIG. 7 show modified embodiments of a belly-band of the
invention. In the embodiments of FIG. 6, a plurality of magnetic
shells 6 are arranged in a plurality of rows in the center or waist
portion in the body 5 of the belly-band and the magnetic shells are
provided with ferromagnetic metal plates 8 on the side thereof
opposite to the side where the shells contact the haman body. In
the embodiment of FIG. 7, the belly-band is provided with a group
of magnetic shells 6 in a plurality of rows in the center or waist
portion and belly portion, respectively, and each of the groups of
magnetic shells are also provided with the ferro-magnetic plate 8
as mentioned in connection with the embodiment of FIG. 6. Although
not shown, the magnetic shells may be secured to any desired other
position of the belly-band then the waist and belly portion as
mentioned above, i.e., to an area in the belly-band which
corresponds to the side of a human body. In such a case, the
magnetic shells may be arranged with the poles having the same
polarity (N pole or S pole) directing in one and the same direction
or the poles having the opposite polarities may be alternately
arranged.
When a plurality of magnetic shells are, respectively, provided in
the waist portion and belly portion of the belly-band in such an
arrangement that one or more magnets in the waist portion face one
or more magnets in the belly portion, the magnet or magnets in the
waist portion and the magnet or magnets in the belly portion should
be so arranged that when the belly-band is worn by a human body,
the magnets of the opposite polarities face toward each other and
in some cases, all the poles of N polarity are provided in the
waist portion and all the poles of S polarity are provided in the
belly portion.
The magnetic medical treatment devices of the invention are
characterized in that in any of the above-mentioned embodiments of
FIGS. 6 and 7, the side of the belly-band opposite to the side
where the belly-band contacts any part of the human body is
provided with a plate of ferromagnetic material so that the
magnetic field which acts upon the human body is intensified.
Experiments were conducted for determining flux densities in the
direction of a magnetic axis at various points along the magnetic
axis for an instance in which a single magnetic shell was placed on
a wooden plate and for the other case in which the same magnetic
shell was placed on an iron plate. In conducting the experiments,
in order to maintain the probe of a gauss meter at a precisely
predetermined distance from the magnetic axis, acryl resin sheets
of different thicknesses were placed over selected points of the
magnetic axis and the probe was moved along the magnetic axis
maintaining the probe in contact with the resin sheets by pressing
the probe against the resin sheets with a slight force. the
particular gauss meter employed was a model GX-09 made by the
Nippon Denji Sokki K.K. (Japan Electro Magnetic Measuring
Instrument Co., Ltd.) and the results of the measuring experiments
will be given in the following Table 1.
TABLE 1
__________________________________________________________________________
Distance of probe from 0 4 9 15 21 pole face (mm)
__________________________________________________________________________
Density When one magnetic shell 620 400 145 68 32 of mag- was
placed on a wooden netic plate of 5 mm. thick field (gauss) When
one magnetic shell 850 510 195 94 43 was placed on an iron (137)
(128) (135) (138) (134) plate of 0.3 mm. thick
__________________________________________________________________________
(The parenthesized figures represent the determined values of flux
densities at selected points on a magnetic shell placed on the iron
plate on the basis of the flux densities at the corresponding
points on a magnetic shell placed on the wooden plate which are
assumed as 100. In an case, the figures less than three places of
decimals are ignored.)
From the above Table 1, it will be seen that the flux density in
the magnetic axis direction is greater in the case wherein a
magnetic shell is placed on the iron plate than the flux density in
the magnetic axis direction in the case wherein the same magnetic
shell is placed on the wooden plate which is non-magnetic both at
the pole face and each of the selected points.
A second series of experiments where conducted for determining flux
densities in the direction of the magnetic axis of a magnetic shell
in the space above the magnetic shell for a case in which an
elongated glass sheet having magnetic shells arranged thereon with
the same polarity directed in one and the same direction was placed
on a wooden plate and for the case the same glass sheet was placed
on an iron plate and the results of the measuring experiments will
be given in the following Table 2.
TABLE 2 ______________________________________ Distance of probe
from Glass pole face (mm) sheet 3 mm 6 mm 9 mm 13 mm
______________________________________ Flux Magnetic 340 200 134 78
density shells (gauss) placed on a wooden plate Magnetic 450 290
200 120 shells placed on an (115) (145) L140) (154) iron plate
______________________________________ (The parenthisized figures
represent the determined values of flux densities at selected
points on magnetic shells placed on the iron plate on the basis of
the flux densities at the corresponding points on magneti shells
placed on the wooden plate which are assumed as 100. In any case,
the figures less than three places of decimals are ignored.)
A third series of experiments were conducted for determining flux
densities in the magnetic axis direction for an instance in which
the opposite polarity poles of magnetic shells were alternately
arranged on a wooden plate and for the other case in which the same
magnetic shells were placed in the same alternate arrangement on an
iron plate and the results of measuring experiments will be given
in the following Table 3.
TABLE 3 ______________________________________ Glass Distance of
probe sheet from pole face 3 mm 6 mm 9 mm 13 mm
______________________________________ Flux Magnetic density shells
(gauss) placed on a 420 222 156 78 wooden plate Magnetic shells 450
290 200 120 placed on an iron (115) (145) (140) (154) plate
______________________________________ (The parenthesized figures
represent the determined values of flux densities at selected
points on magnetic shells placed on the iron plate on the basis of
the flux densities at the corresponding points on magneti shells
placed on the wooden plate which are assumed as 100. In any case,
the figures less than three places of decimals are ignored.)
It is clear from the experimental results shown in Tables 2 and 3
that whether the magnetic shells are arranged so that the poles of
the same polarity mat direct in the same direction or the poles of
the opposite polarities are alternately arranged, the flux
densities in the magnetic axis when the magnetic shells are placed
on the iron plate (ferromagnetic material) are greater than those
when the magnetic shells are placed on the wooden plate
(non-magnetic material) at different points along the magnetic
axis.
A fourth series of experiments were conducted for determining the
flux densities at different points in the magnetic axis of the
center magnetic shell in an array of magnetic shells secured to the
surface of a glass sheet. In one case, the magnetic shell-carrying
glass sheet was placed on a wooden plate and for the other case,
the same glass sheet was placed on an iron plate. The results of
the measuring experiments will be given in the following Table
4.
TABLE 4 ______________________________________ Glass Distance from
pole sheet face (mm) 3 mm 6 mm 9 mm 13 mm
______________________________________ Flux Magnetic density shells
(gauss) placed on a 330 201 104 64 wooden plate Magnetic 420 221
142 91 shells placed on an (132) (110) (136) (144) iron plate
______________________________________ (The parenthesized figures
represent the determined values of the flux densities at selected
points on the iron plate on the basis of the flux densities at the
corresponding points on the wooden plate which are assumed at 100.
In any case, the figures less than three places of decimals are
ignored.)
From the results given in Table 4, it will be seen that the flux
densities when the glass-sheet supported magnetic shells are placed
on the iron plate are greater than those when the same magnetic
shells are placed on the wooden plate. The results of experiments
measured when the magnetic shells of the opposite polarities were
alternately arranged are given in the following Table 5.
TABLE 5 ______________________________________ Glass Distance of
probe from sheet pole face (mm) 3 mm 6 mm 9 mm 13 mm
______________________________________ Flux Magnetic 425 275 162 81
density shells gauss placed on a unit wooden plate Magnetic 410 332
209 108 shells placed on an (120) (117) (128) (133) iron plate
______________________________________ (The parenthesized figures
represent the determined values of flux densities at selected
points on the iron plate on the basis of the flux densities at the
corresponding points of the wooden plate which are assumed as 100.
In any case, the figures less than three places of decimals are
ignored.)
In any case, it has been found that the flux densities when the
magnetic shells are placed on the iron plate (ferro-electro metal
material) are greater than those when the magnetic shells are
placed on the wooden plate (non-magnetic material). And it has been
found that the flux densities when the poles of the magnetic shells
which have the same polarity are arranged in the same direction are
greater than those when the poles having the opposite polarities
are alternately arranged. However, since the same magnets were not
employed in the experiments, the results of which were given in the
above Tables 2 and 3, the absolute values are different.
From the experimental results given hereinabove, the following
conclusions can be made:
1. It is preferable to position a magnet on one side of a
substrate, which side has applied thereto a ferromagnetic metal
sheet rather than positioning the magnet on a non-magnetic
substrate because the space on the other side of the ferromagnetic
metal-applied substrate has a greater flux density.
2. The flux density when the poles of magnets which have the same
polarity are arranged in the same direction is greater than that
when the poles having different polarities are alternately
arranged.
3. When a ferromagnetic metal plate is applied to the outer side or
the side of a magnet which is opposite to the side which contacts
the human body, the flux density which acts on the human body will
be greater than otherwise, regardless of whether the magnet is
disposed in any way.
Therefore, when a predetermined flux density is desired, if a
ferromagnetic metal plate is applied to the side of a magnet
opposite to the side where the magnet contacts the human body, such
a magnet may be of a low magnetic force. The use of the low
magnetic force magnet having the ferromagnetic metal plate applied
to one side thereof will have a high efficiency.
4. In order that a magnetic flux can induce a moderate degree of
magnetic field to act on a human body to efficiently generate
polarization and induced currents in the human body, it is
preferable to apply a ferromagnetic metal plate to the outer side
or the side of the magnet opposite to the side where the magnet
contacts the human body. In a magnetic medical treatment
belly-band, the deeper the magnetic flux permeates the human body,
the better the treatment. Therefore, the belly-band embodying the
present invention is particularly suitable for magnetic medical
treatment purposes.
Since it does not constitute any part of the present invention to
theoretically consider the phenomena which provide such effects,
details of the phenomena will not be disclosed herein. To state
briefly, it is believed that the flux density increases in the
space on the inner side or the side of the magnet where the magnet
contacts a human body because the magnetic reluctance is present on
the other side or the side of the magnet where the magnet does not
contact the human body.
Furthermore, the increase rate of flux density varies depending
upon the arrangement of magnets, the space between magnets and the
material, size, shape and thickness of the ferromagnetic metal
plates. Thus, when the present invention is applied to a magnetic
medical treatment belly-band, it is necessary to select suitable
magnets and ferromagnetic metal plates suitable for particular
applications taking the above factors into consideration.
Although the best modes contemplated for carrying out the present
invention have been shown and described, it will be apparent to
those skilled in the art that other modifications and variations
may be made without departing from the spirit of the present
invention or the scope of the appended claims.
* * * * *