FIELD RADIATOR FOR CURING CANCER AND OTHER AILMENTS

Abstract: Ailments occur by inoperative states of the molecular mechanisms in the tissue matter. There are functional electrons in the molecular mechanisms, which rotate back and forth angularly within an arc of45 degrees in normal operation. When these electrons rotate more than 45 degrees, they keep on rotating toward 90 degrees, and 180 degrees. Because of operational interrelationship between molecules, adjacent molecules also become inoperative step by step, and lose their normal magnetic rejection to foreign molecules, and growth starts by invasion, as cancer. These depolarized electrons cannot return to their normal polar orientations, and therefore, artificial polar control is required. These mechanisms, however, are arrayed in the tissue three dimensionally, and the invention provides radiation of magnetic field that rotates in the tissue in at least three mutually perpendicular planes, for normalizing the depolarized electrons, as cure of cancer.

Description: Description Field radiator for curing cancer & other ailme s This invention relates to apparatus for treating biolo¬ gical ailments, for example cancer, in tissue matter. More > specifically, the invention relates to apparatus for trea¬ ting ailing tissue matter through the application of magnetic field to the affected re of the tissue matter. Background The r of magnetic application for medical and biolo- 0 gical treatment dates back several thousand years, as far as records indicate, due to observed beneficial effects that have been obtained under some methods of magnetic application. But the actual biological mechanism that responds to magnetic application has never been understood, and the experimentally 5 skilled in this particular art have been trying all possible methods and systems of magnetic application with the hope of finding a way of ensuring that the magnetic field would strike the ailing area from the correct direction to effect the desired treatment. 0 The types of magnetic application that have been used so far, are: steady state magnetic application for a length of time from a singular direction; pulsed application from a sin¬ gular direction for a length of time; and rotary application in a singular plane. The main issue at this point is that these experiments Have indicated that magnetic application can result in some beneficial effects, although so far, only partial improvement of any ailment has been achieved. However, no matter how insignificant the beneficial effec s achieved have been, 30 it must be concluded that the observed effects can result only if the mechanisms in the tissue matter are responsive to magnetic field. The present invention proceeds from the basis that all matters are constructed with atoms and electrons, and therefore, these are the component part3 of the mechanisms of the living molecules that functionally respond to applied magnetism. This electron response represents a change in polar orientation and that the ailment which responds to applied field has been the result of pole disorientati n of some of the active electrons from their normal polar orientations, rendering them inactive. The beneficial effects of well being, 0 resulting from the magnetic application, is due to those pole-disoriented electrons in the molecular mechanisms being reoriented to their normal polar orientations for regaining their active functions, as a representation of well being. The problem is, however, in normal tissue matter the olecu- 5 lar mβchs isos containing these functional electrons are arrayed three dimensionally in t_he tissue, and polar reori¬ entation of only those electrons that happen to be located within a single plane can be achieved and, accordingly, effect only partial well being, which is what has been 0 observed and claimed by the previous experimenters. Brief embodiment of the invention The present invention provides apparatus for treating biological ailments in tissue matter, the apparatus being adaptable for radiating three separate pole-controllable ^ magnetic fields from directions that cross transversely perpendicular one another at a segment of the body under treatment. The poles and radiations of these three fields are then controlled in a sequence and combinations, such that, the magnetic field at the segment of the body lies successi- 0 vely, and with 180 degree polar reversals along a plurality of lines of orientation, nήiic occur in at least three mutually perpendicular planes, for rotating the depolarized electrons in the tissue to their normal polar orientations, a s cure of the ailment, -gU K if oypi Scientific understanding of the art For simple understanding of how electron depolarization occurs injthe tissue matter, the following brief analytical explanation describes how the molecular mechanism in the tis- sue operates in normal healthy state - how it is transformed into an a ili n δ (more specifically, a cancerous) state - and how the ailing state c be reversed into normal operating state. Atomic arrangement of the molecule 10 A living molecule consists of a series of interleaved generators which operate in a specific sequence for genera¬ ting specifically oriented mgnetic fields at the periphery of the molecule. These complex magnetic fields are so timed and oriented that adjacent molecules control each other's trig- lj? gering actions of generation alternately, so that a opera¬ tional interrelationship is created between adjacent mole¬ cules for binding only similar operating molecules in the tissue structure, and rejecting alien molecules. Each generator consists of a air of atoms and a func- 20 tional electron entrapped between the two atoms. This elec¬ tron rotates back and forth within a limited arc of I. degrees under the* control of RNA (ribonucleic acid) and DNA (deoxyri- bonucleic acid) for generation of the required magnetic field. In operation, the electrons from the RNA source are released 25'and drawn toward the functioning electron, by the initial force of the pair of atoms, and regenerated by processional (wobble) feed-back of the functioning electron. This electron rotates up to \ S degrees while precessing from the lowest processional resonance of abou 12 centimeter wavelength, up 30 to 3 centimeter at \ S degree rotation. At 15 degree rotation, a storage mechanism responsively resonant to 3 centimeter wavelength, stores and produces a pulsed voltage to trigger the DNA source for release of DNA atoms. A single DNA atom and a single positive RNA atom are released simultaneously, which travel toward each other to the center of released string of RNA electrons. The travel motion of the DNA and RNA atoms toward each other causes sufficient magnetic flux for a single released electron to travel to the positive RNA atom, and the ywo atoms move away for elimination, or reuse. From the above explanation, it is seen that the trig- gering action of the RNA source represents start of regene- ration in a backw a rd process, and this process continues until all of the released RNA electrons are eliminated for a new start of cyclic generation. This generates the specific field that binds similar molecules together in normal operating state. One important aspect of such operation is that, both the RNA and DNA sources to the generator are attached to respective RNA and DNA supply atoms, so that when one of these sources releases an atom it must be replenished by an atom from its string at the same time, because when this string is broken the source will not release an atom, no matter how much it may be stimulated to do so. Similarly, the RNA source will release electrons without being replenished by electrons, but when the magnetic tie of the string is broken, it becomes incapable of releasing electrons. Transformation into cancerous state , The above given conditions relate to the normal opera¬ tion of a molecule. Supposing now that during release of RNA electrons the RNA source is stimulated unnaturally (for exam¬ ple, by cancer causing agent) for releasing far greater number of electrons than required for normal operation. In this case, the charge of the storage mechanism cannot start triggering action of the DNA source for reverse regeneration, and the functioning electron is regenerated toward rotation to 90 degrees ( a t this point electron precession stops completely;, which is the maximum regeneration, and all operations stop at this point with no possibility of pole reversal. This is the stage in which strong paramagnetic resonance at about 3 cm. wavelength can be obtained by an external magnet. As stated in the foregoing, alternate control of adjacent molecules is now interferred with, and the adjacent molecules also stop operation step by step, but very slowly at the beginning. In time, when sufficient number of molecular mechanisms have become inoperative, the loss of the original peripheral ag- netic field between adjacent molecules causes the strings of supply atoms to the RNA and DNA sources to recede, and because of the processional radiation of the functioning electron has stopped at this point, the released RNA electrons are now drawn to the positive atoms in the RNA source. The direction of withdrawal of these electrons is such that the functioning electron keeps rotating in the same direction that it had rotated to 90 degrees, and makes a complete 180 degree pole reversal, instead of returning to its normal polar orientar tion. This is the condition in whic Para cannot be obtained - it stops completely, but can be resonated by electromagnetic radiation at about decimeter wavelength. This is because the functioning electron is bound to the 180 degree pole reversed orientation so strongly that it will require much stronger magnetic field to rotate the electron from its new polar position, except by resonant radiation. In "other words, without the help of RNA electrons in the molecule, external magnetism alone cannot influence the functioning electron for polar normalization. Treatment of cancerous state As explained above, the RNA and DNA sources in a mole¬ cule b ecome separated from their strings of supply atoms only after some number of molecules from normal molecules become inoperative, because of a threshold volume in which they are forced to lose their magnetic hold of their supply strings. Thus, those inoperative molecules that are in the vicinity of normally operating molecules, have their RNA and DNA sources still intact with their respective strings of atoms, so that an external influence upon these functioning elec¬ trons from a direction at right angle to the pole disoriented positions will rotate these electrons to 90 degree angle by the regenerative help of released RNA electrons. If now we change the direction of this influencing field to the direc¬ tion of the electron's normal polar orientation, the released RNA electrons will now be removed by degenerative DNA relea¬ sed atoms, and the functioning electrons will be reoriented to their normal polar states for normal, operation. Thus, all that is necessary is external influencing field from two proper directions. Since this is not possible to predetermine, however, we may arrange thi3 external field to undergo angular changes in direction in three dimensions to obtain the desired treatment. As stated in the foregoing, the curing action starts from those inoperative molecules which have their RNA and DNA sources still intact with their respective supply strings, which means that cure starts from the outer periphery of the growth, and not from the center. Since only few degrees of electron rotation is required to start regeneration, a field strength anywhere between 800 gauss to seven thousand gauss can be used, non-critic lly. Brief description of the drawings Fig. 1 illustrates partly diagramatic view of a rectan¬ gular assembly of magnetic coils Ml, U2 and M3, wound around a rectangular tubing through which the patient is inserted for treatment. A perspective view of M1-M3 is shown at A of Fig. 1. in conjunction " with these coils, there is included a distributor arrangement for energization of the coils in a * 3 * » l !-* • specific sequence, for producing the required magnetic field in the body for treatment. Fig, 2 is a chart showing exemp¬ lary sequence of energization of the magnetic coils Ml-JO. And Fig. 3 is an alternate version of the distributor, and switching arrangementof Fig. 1, Best mode of carrying out the invention In Fig. 1, there are used three magnetic coils Ml, M2 and M3, which are wound around a rectangular tubing 1, for producing three separate magnetic fields mutually perpendicu- lar relative to each other, transversely to the longitudinal axis of the inner space of the rectangular tubing. For example, he first field is produced by the magnetic coil M3 > which is wound around the rectangular tubing, to produce a magnetic field in a first direction longitudinal through the two open ends of tubing. The second field is produced by the coil M2, which is split into a pair of series-connected coils, for producing transverse field, perpendicular to the longitudinal axis in the first direction. And the third field is produced by the coil Ml, which is split into a pair of series-connected coils, for producing a transverse field perpendicular both to the longitudinal axis in the first direction, and to the field in the second direction. Thus, when the coils Ml and M2 are energized by a quadrature phased sine wave current, the polar orientation of the field in the rectangular tubing 1 will rotate circularl in a first plane. ' When the coils Ml and M3 are energized by the same wave cur¬ rent, the field will rotate in second plane, perpendicular to the first plane. And when the coils M2 and M3 are energized by the same wave current, the field will rotate in.a third plane, perpendicular to the first and second planes. Further, when Ml and M2, M3 are energized by the current, t he field will also rotate circularly, but in this case, at an angle ϊ $ degree with respect to the first and socond planes. By these examples, therefore, it is seen that the assembly arrangement of the coils M1-M3 i3 capable of producing a magnetic field in the spacing ofthe tubing 1, the polar orientation of which can be changed in -any direction and plane, as desired. It will be noted, however, that the rectangular windings of the coils, especially the coil M3, will not produce uniform field in the central region of the tubing 1. But such imperfection is allowable for the purpose herein, because electron polar normalization can be established under wide variations of angular directions through which the field is applied. If desired, however, the assembly can be cylindrical, or square, as shown at A. The current applied to the magnetic coils M1-M3 is supplied by the R-F generator in block 2, from its output transfo∑-mer comprising L9 and 10, One of the terminals of L10 is connected in parallel with one ofthe terminals ofMl, M2 and M3, and the other terminal of L10 is connected to ground for establishing closed circuits with the other termi¬ nals of Ml to M3 connected in series with the pairs of diodes Dl, D2; D3 > *D-+; D , DO, and the pairs of ENJ » control transistors Ql, 2 Q3, and Q5, Q6, respectively, connected to ground. The NPN and PNP transistors Ql to Qό re normally ren¬ dered non-conductive by negative and positive bias supply voltages Bl and B2. The alternating sine wave voltages across the secondary inductance L7 to L2 are connected to the base electrodes of transistors Ql to Q6, respectively, in series with the output circuits (not shown of the one-shots in blocks 3 to 8, respectively, and the bias batteries Bl, B2, to ground. The * bias voltages of Bl and B2 in series with the output operating voltages of the one-shots, and the peak output voltages across the secondary coils L2 to L7 are so prβad- justed that, during operation of one of the one-shots, for esample, the block 3, the NPN transistor Ql becomes conduc¬ tive only during the positive half cycle of the alternating wave from LI, and during operation of anyone of the one-shots, for example, the block I., the PNP transistor Q2 becomes con¬ ductive, only during the negative half cycle of the alter¬ nating wave from L6. Thus, the outputs of one-shots in blocks 3, 5 an 7 are arranged to produce at their outputs positive pulse voltages, and the outputs of one-shots I., 6 and 8 are arranged to produce negative pulse voltages. The operating duty cycles of the one-shots 3 and 8 are preadjus- ted to be a little longer than one half cycle period of the alternating wave from LI, to make sure that the transistors are kept active during a complete half cycle period of the alternating wave, which may be a standard commercial 6θ . cycle, or I.0 cycles per second, in different countries. If greater time period than a half cycle of the sine wave is desired to be devoted to energization of the magnetic coils, then the operating duty cycles of the one-shots 3-8 can be lengthened, up to the full time periods devoted between dif¬ ferent coil energizations by the switchings to the coils Ml- M3. In this case, the energization of coils Ml to M3 will be only during periodic half cycles of the sine wave from LI, because during the alternate half cycle periods one of the pairs of transistors remain inoperative. The operating distribution of these one-shots is con¬ trolled by the outputs of distributor in block 9* tn e sequen¬ tially operating outputs of which are coupled to the ulti- inputs of the OR-gates in blocks 10 to 15, in prearranged sequence nd combinations. The comman outputs of OR-gates 10 to l5 are coupled to the operating inputs of the one-shots 3 ' to 8, respectively, for operation. As mentioned in the foregoing, the- outputs of one-shots 3, 5 and 7 should produce positive pulses at their outputs, and the one-shots I4., 6 and 8 should produce negative pulses. Thus, it may be neces¬ sary that the inputs of one-shots 3, 5, 7 and I, 6, 8 *re of opposite polarities. For this reason, the voltage inverters l6, 17 and 18 are included in the drawing. But such an arrangement depends on how the internal circuits of commer¬ cially available integrated devices are designed. Then again, when the magnetic coils Ml to M3 are designed for low frequen¬ cy operation, for example, at 6θ cycles per second, they may require high current energization, and therefore, the transis- 0 tors Ql to Q6 should also be capable of delivering these high currents. Thus, the commercially available one-shots might need amplifiers to drive the inputs of these transistors. If R-F is used for the coils M1-M3, the R-F may first be 100 percent amplitude modulated by the half sine waves from coil 5 LI. It will be observed that the OR-gates; one-shots; and the diodes in operation act as switching circuits, and therefore, other suitable switching means may also be utilized, operated under control of the distributor. A segment of the special coupling arrangement of the 20 outputs of distributor 9 to the inputs of OR-gates 10 to 15 is shown to concur with the sequence of magnetic coil energization, as shown by the chart of Fig. 2. For example, in a reference starting point (number 1 of the chart) of coil energization, a positive current is passed through the coil 25.Ml, which produce a first magnetic field in a first direction toward a first plane between its series connected windings, transverse the longitudinal axis of the rectangular opening of the tubing 1. In the second step of coil energization sequence, a positive current is passed through the coil M2, 30 which produces a second magnetic field in a second direction toward a second plane perpendicular to the first plane, between its series connected windings, transverse said longi¬ tudinal axis of the tubing 1. And in the third step of coil ■ energization, a negative current is passed through the coil M3 » which produces a third magnetic field in a third direc¬ tion toward a third plane perpendicular both to the firet and second planes, transverse said longitudinal space. These steps of coil energization are continued to the twelvth step, for rotation of the field in 90 degree angular steps within mutually perpendicular first, second and third planes. When rotation of the field is desired to occur in i|_5 degree angu¬ lar steps, then the sequence of steps 13 to 16 may be used, as example - but the simultaneous availability of oppositely polarized R-F voltage is not shown in Fig. 1, as required in the step 16 of the ch a rt in Fig. 2. Also, if rotation of the field is desired to occur in more than three planes, then the sequence of the steps 17 to 2J_J_ c be used, as example. By these examples, accordingly, it is 3een that the magnetic field produced in the space region of the tubing 1 can be rotated in any direction and plane, as desired, by modify¬ ing the couplings from the output of the distributor in block 9, to the multi-inputs of the OR-gate in blocks 10 to 15. For fast operation of the magnetic coils Ml to M3, however, the sequence of coil energization from the first to the twelvth switching of the chart in Fig. 2 will suffice for practical purposes. For this reason, a manual switch may be incorpo-- rated with the arrangement of Fig, 1, so that the technician in charge can decide which mode to use. The time period of a depolarized functional electron to rotate to its normal polar orientation is about one eighth of a second, as the shortest time period, and one half second as the longest period. Therefore, the rectified half cycles of the a-c voltage from the coil 8 (circuit not shown; may be counted by the counter 19, and operate the distributor 9 at every predetermined count, as shown. The distributor 19 is shown with extra outputs, for operation of other sets of magnetic coils that may be placed a t different segments of the body for simultaneous tratment as desired. Modified arrangement of Fig. 1. In Fig. 1, the magnetic coils Ml to M3 are shown to be high frequency inductances, which are energized by the R-F generator in block 2. The preference between high frequency coils and low frequency coils is a matter of choice for practical purposes, because in using low frequency coils, for example 6θ cycles, the coils would require large number of copper wire, which will add bulk and weight to the appara- tus. But at commercial/cycle line, the power is readily available, either directly, or through a transformer, if higher voltage is required. Whereas, at high frequency opera¬ tion, the weight of the coils Ml to M3 can be light, but an R-F generator is required. Also, the high frequency field will cause heat in the body. In either case, a radiation 3hield may be preferred to be used surrounding the coils. In high frequency operation, the shielding material Is conven¬ tional, but for low frequency operation, magnetic shielding material " is used, for example, the MU metal. In the case that 6θ cycle line power is preferred for energizing the coils Ml- M3» the distributing arrangement of Fig. 3 Ja y be used. In Fig. 3, the pulse-formers " in blocks 20 and 21 derive pulse signals from the a-c source in block 22, as shown graphically by waves at the right hand side of blocks 20- 22. The output pulses of blocks 20 and 21 are mixed in the 0R-gate in block 23, and applied to the input of the distri¬ butor 2-4-, which operates at the crossing points of the upper and lower lobes of the a-c sine wave. The distributor _ counts the half cycles of the a-c source to a predetermined count, and the last two outputs of _h.e predetermined counts are mixed at the two inputs of the 0R-gate in block 25. The last output is applied to one of the inputs of OR-gate 50, for impressing upon its clear input, for a new start of counting. SU! • > _ . TUTΞ SHEET The output of OR-gate 25 is applied to the input of the dis¬ tributor in block 26, which makes two distinct operations at every predetermined count ofthe counter _ . This provides two output operations of the distributor 26, at every prede- termined count coincident with the timings of the positive and negative half cycles of the a-c input. Thus, at any required timing of energization of the coils M1-M3, either the positive or negative lobe of the a-c source is available, even though there occurs a half cycle timing difference between the two separate operations at the outputs of the distributor 26. In other words, the coils M1-M3 m y be con¬ nected to either the positive voltage or the negative vol¬ tage of the a-c line source, by selecting the proper timing during which the particular outputs coincide with a positive or negative lobe of the alternating cycle - disregarding the timing difference that occurs between the positive and negative lobes. To make it clearer how the outputs of the distributor 26 re selected for coil energization, and in reference to the chart in Fig. 2, assume that a positive voltage of the a-c source occurs at the number 1 output oft he distributor 26, This output is coupled to one o the multi _-_inputs of the OR-gate in block 27, which operates the set-reset trigger circuit in block 28, the output of which is amplified by the block 29 for operation of the relay Rϊl. The contact points 30, 31 and 32, 22 (as shown), and the control electrodes of controlled rectifiers Dl and D2 are connected to their anode electrodes in series with the current limiting resistors Rl and R2, for conduction. Thus, the magnetic coil Ml is ener- gized by the'positive lobe of the a-c wave. During the negative lobe of the a-c wave, the number 2 output of the distributor 26 operates, and this output having been coupled to one of the multi-input OR-gate in block 3l j _, the set-reset triggers 28, 35 and 3 operate in reset states for releasing the operations of the relays RY1-RY3, by way of the amplifiers 29, 37, 38. The contact points of the relays open, and current to the coils M1-M3 stop. Thus, after each half cycle period of the a-c voltage, during which anyone, or combination, of magnetic coils are energized, during the following half cycle periods of the a-c line voltage the' current through the magnetic coils are switched off, until the distributor in block 2 counts another predetermined number of half cycles of the a-c line voltage, for repetitive operation. In order to synchronize the timings of operations of the distributors 2_+ and 26, a pulse signal is derived from the last output (marked 59) ° * e distri¬ butor 26, by the one-shot in block I4.9, which applies this pulse signal to the clear input of the distributor 26, and simultaneously to the clear input of the distributor 2I4. by way of the OR-gate 50, so that the starting time periods of both distributors become coincident. Commercially available integrated circuits, however, contain feed-back connections to their clear inputs, and some of them may contain auxil¬ iary connections, which may be used to eliminate the OR-gate 50, and the one-shot ]_μ9» The number of outputs of the distributor in block 26 are marked by the numerals just below the output terminal connections, and the number of output terminals coupled to the inputs of the OR-gates 27, lj-7 and 1+.8 are marked by the numerals below the numerals just mentioned. The numerals just below the output terminals are shown for the purpose to indi¬ cate which output terminals are coupled to inputs of OR-gate in block 3k- * and which outputs are left open, in order to select the proper timings of the positive and negative lobes of the a-c sine wave, for energization ofthe magnetic coils Ml to M3. If simultaneous positive and negative voltages of the a-c line is available, however, such as across the sβcN->ndary of a center tapped transformer, then the parallel connected anode terminals of diodes Dl, D3, D5 may be connec¬ ted to one secondary terminal, and the parallel connected cathode terminals of diodes D2, D-4., 6 connected to the other secondary terminal of the transformer. By this availability of simultaneous positive and negative voltages of the a-c line, the output connections of the distributor to the OR- gates 27, 1+7, l can be simplified. The differentiating capacitors Cl to C13 are used to avoid direct connections 10 from the outputs of the distributor to the inputs of the OR- gates 27, k-7 and I4.8. This use, however, is not imperative, and they may be dispensed with, when proper integrated cir¬ cuits a∑*e selected. As described in the foregoing, the use of the commer- l5 cial a-c line at 60 cycles is only for convenience. Therefore, the a-c source in block 22 can be a source of different frequency, or, it may be bipolar d-c source. Also, in refe¬ rence to the distributor of Fig, 1, and the chart of Fig. 2, it may be desired to use only up to the twelvth switching of 20 the coils Ml to M3. Thus in Fig. 3, an auxiliary one-shot, such as the one-shot J4.9, may be connected to the thirteenth output terminal of the distributor 26, and a manual switch to select either the one-shot l|_9 or the auxiliary one-shot. In this case, the OR-gate may have three inputs, so that the 25 output of the auxiliary one-shot can be connected to the third input of gate 5 . The outputs of one-shot 1| and the auxiliary ' one-shot may then be mixed in a two input OR-gate for connec¬ ting to the clear input of the distributor 26, In reference to the output terminals of the distributor 30 26, there are shown 59 output terminals. But this is only exemplary, and any number of outputs for d ifferent modes of operation m a y be used, for example, arranging the couplings fron these terminals for allowing energization of the coils M1-M3 during two or more periodic half cycles of the same sign, instead of only during one half cycle period of the a-c line wave. In reference to the rectangular assembly of the mag- netiσ coils M1-M3, these coils may be extended longitudinally, along the length of the body to be treated, so that the whole body can be treated by the same magnetic field, for fast treatment. But if such large volume of tissue matter is not desirable to be treated simultaneously by the same field, advantage can be taken from the fact that, after each pulsed field application the electron pole normalization is conduc¬ ted in the tissue by self regeneration, as described in the foregoing. Thus, after a pulsed magnetic field i3 applied to a segment of the body, another segment of the body is ready to receive a magnetic field while the first segment is in a process of self regeneration. Therefore, instead of contruc- ting the coils M1-M3 in one piece extending the length of the body, they can be made in narrow moduleβ, for example, 2.,% centimeter wide, and operate these modular arrangements sequentially, for example, by the distributor in block 19 of Fig. 1. In fact, these modules can be made ring like, and plugged in on a base holder. This way, the weight of the magnetic coils can be reduced for mobility. If high frequency is used by the generator in block 2, it may be at standard frequency for diathermy purposes, for example, at 13«56 megahertz. The standard power requirements will satisfy for the present purpose. Also, in reference to the coils M1-M3, the body shape relative to the coil M3 is such that inductive radiation is necessary for producing the longitucinal field through the body, tfhereas, the inductances of Ml and M2 are parallel devices around the body. Thus, in the case of high frequency field application, the pairs of coils Ml and M2 can be pairs of capacitive plates, while the coil 3 can be inductive. Or, the coils Ml, M2 and M3 can be three pairs of spaced parallel capacitive plates, the elec¬ tric field radiations between the three pairs of plates projecting toward a central area crossing transversely mutually perpendicular relative to each other, The foregoing and other advantages obviously indicate that arious other modifications, substitutions of parts, and adaptations can be made without departing from the true spirit and βcope of the invention. ' • -

Claims: Claims Apparatus for treating biological ailments resulting from depol a rized electrons in three dimensionally arrayed molecular mechanisms in the tissue matter, comprising an assembly of first, second and third energizable radiators, for radiating electron- attracting fields from directions toward a treatment area, where the polar -axes of said radiations cross transversely perpendicular relative one another; a bipolar energizing source; first, second and third pairs of controlled rectifier means interconnecting the energizing source and the first, second and third radiators, respectively, each rectifier means having a respective control means; first, second and third pairs of switching means, each pair having a plura- lity of inputs and a pair of outputs connected to a respective pair of the rectifier control means; and means operable to distribute successive switching signals selectively to the switching means for selec¬ tive energization of the radiators, the said distri- butor means having a plurality of outputs coupled to the inputs ofthe switching means in an order of sequence such that, in operation the radiated field at said area changes in direction lying successively and with 180 degree polar reversals substantially in at least three mutually perpendicular planes, for normalizing said depolarized electrons. , Apparatus for treating biological ailments resulting from depolarized functional electrons in three dimen¬ sionally arrayed molecular mechanisms in the tissue matter, comprising an assembly of first, second and third energizable radiator means, for radiating • electron-attracting fields from directions toward * a treatment area, where the polar axes of said radia- sue s - 'f -- 1 tions cross transversely perpendicular relative to each other ; a bipolar alternating wave energizing source; first, sevond and third Pairs of controlled rectifier means interconnecting the bipolar energizing ' 5 source and the first, second and third radi ator means, respectively, each rectifier means having a respective control means; first, second and third OR-gates, each gate having plurality of mixing input 3 and an output; coupling means from the outputs of said first, second 0 and third OR-gates to the pairs of control means of . said first, second and third pairs of rectifier means, respective l y, f° r operating each pair of the recti¬ fiers at a time, whereby allowing anyone of said radiators to be energized by either lobe of said 5 alternating wave source that may be present at a time of operation of said OR-gate s; ' and a distributor means under control of the alternations of said source , for di stributing operating signals to the plurality of inputs of said first, second and third OR-gates in 0 an order of selective sequence and timing of the alternations of said source, such that, the polar orientation of the field radiated to the region of said area of the body by the selective energization of said radiators changes in angular directions lying successively and with 180 degree polar reversals substantially in at least three mutually perpendi¬ cular planes, for effecting electron polar normali¬ zation in the said area of the patient. 3. Apparatus for normalizing the polar orientations of 0 depolarized ele ctrons in three dimensionally arrayed molecular mechanisms of the tissue matter, causing biological ailments, the apparatus comprising an a ssembly of first, second and third radiator me a ns for radiating electron- ttracting fields from directions toward a central area where the polar axes of said radiations cross transversely at right angles relative to each other, when energized; a bipolar energizing source; first, second and third pairs of controlled rectifier means interconnecting the energizing source and the first, second and third radiator means, respectively, each rectifier means having a respective control means; first, second and third pairs of switching means, each pair having a 0 plurality of inputs and a pair of outputs connected to a respective pair of he rectifier control means; and means operable to distribute successive switching signals selectively to the switching means for selec¬ tive energization of the radiators, the said distri- 5 butor means having a plurality of outputs coupled to the inputs of the switching means in an order of sequence such that, in operation the radiated field at said control area changes in direction lying successively and with 180 degree polar reversals 0 substantially in at least three mutually perpendi¬ cular planes, so that when an area of tissue contai¬ ning depolarized electrons is placed at said central area, s a id polar normalization will occur. k.. The apparatus as in preceding claims, wherein said 5 field radiators are electromagnetic radiators, comp¬ rising a first coil having a central longitudinal open space with a winding arranged to radiate a longi¬ tudinal first magnetic field through said open sp^ce, when energized; a second coll divided into a pair of 0 parallel spaced series connected coils, wound in an orientation to radiate a second magnetic field between the pair of s a id second coils, transversely perpendicular to the axis of the first field through said longitudinal space, when energized; a third coil divided into a pair of parallel spaced series connec¬ ted coils, wound in an orientation to radiate a third magnetic field, when energized, between the pair of the third coil, transversely perpendicular both to 5 theaxes of the first and second fields, through said longitudinal space, * . whereby forming a longitudinal open space adaptable for insertion of a segment of a body for treatment, for said polar normalization. 105. The method of treating biological ailments, resulting fromdepolarized functional electrons in three dimen- tionally arrayed molecular mechanisms of the tissue matter, the method comprising the steps of radiating controllable first, second and third bipolar electron 15 pole-attracting fields, from directions that are originally positioned in a singular plane, and the radiations of said fields cross each other at right angles transversely in a segment of the body of the patient under treatment; controlling the poles and 20 radiations of each of said radiations selectively, and selectively distributing the said controls of poles and radiation states in an order of sequence and combinations such that, the polar orientation of . the radiated field in said segment ofthe body changes 25 in direction lying successively and with l8θ degree polar reversals substantially in at least three mutually perpendicular planes, thereby effecting polar reorientation' of said depolarized electrons at said segment to their normal polar orientations. 6. Apparatus, or method claims, as set forth in claims 1 to 3, or 5, wherein the distribution of energiza¬ tion to said first, second and third radiators is in an order ot sequence and combinations such that, each of s a id 180 degree pole reversals of said field at the said area is established by at least two 90 degree angular steps, 7. The apparatus, or method claims, as set forth in claiτss 1 to 3, r 5, wherein the distribution of energiza¬ tion to sai first, second and third field radiators is in the form of pulses, 8. Apparatus as set forth in claim 2, wherein is.included a counter for counting the alternation of said alter¬ nating wave source; and means for changing the state of operation of said distributor means only at predetermined counts of said counter. 9. Apparatus for treating biological ailments in tissue matter, the apparatus being substantially as herein¬ before described with reference to, and as illustrated by, the accompanying drawings.

Inventors: KALFAIAN M
Applicants: KALFAIAN M
Application year: 1980
Main classification: A61N1
IPC codes: A61N1, A61N2