NON-LINEAR ELECTROMAGNETIC VIBRATION FLUID COMPRESSION DEVICE

Abstract: A non-linear, electromagnetic, vibration compression mechanism comprising a non-linear electromagnetic vibration device and a piston-cylinder, plunger-cylinder, or mem­ brance type pump. A reciprocating compression section of the device may be axially arranged at a front or rear por­ tion of the electromagnetic vibration device to form a coaxial compression device. Compression elements may also be installed on the lateral right and left sides or top and bottom of the electromagnetic vibrator to act non-coaxially but in parallel with the vibrator. The electromagnetic vibrator may drive one compression cylinder or several cylinders simultaneously. The reciprocating fluid compres­ sion device of the instant invention may be used to com­ press gas as well as liquid.

Description: RELATED APPLICATION This application is related to applicant's copending application serial ........ entitled "Non-Linear Elec­ tromagnetic Vibration Device" filed on even date here­ with. BACKGROUND AND FIELD OF INVENTION The instant invention relates to a non-linear, elec­ tromagnetic vibration fluid compression device. It is operative to effect gas volume changing and to transport liquid and its pressure operations. Conventional reciprocating fluid compression devices usually employ a rotary motor as a power source and then converts the rotary motion into reciprocating motion using a transmission mechanism. In this sense, its structure is complex and bulky, and its efficiency is generally low. Furthermore, the transmission mechanism can be easily damaged. If an electromagnetic vibrating device is used as a power source for reciprocating fluid compressor, direct transmission and resonance may be effected and energy con­ servation can be relatively enhanced. However, there are usual disadvantages associated with linear type electromag­ netic vibration devices, such as small amplitude, unstable vibration characteristics, and limited discharge and work­ ing pressure. Therefore, ordinary fluid compression devices using linear electromagnetic vibration devices as a power source unavoidably possess problems in the form of inadequate displacement, working pressure, and lack of efficiency and stability. Ordinary compressors utilizing electromagnetic vibra­ tors are generally inadequate to achieve sufficient preci­ sion of directional vibration. Consequently, cylinders, pistons, or other parts of a working compressor are easily jammed, stuck, or otherwise subjected to non-uniform wear, resulting in unnecessary and extensive damage to the com­ pressor embodying the vibrator. The problem becomes espe­ cially pronounced, to a degree hindering normal use, when the electromagnetic vibrator is not coaxially mounted with respect to the compressor cylinder. For this reason, ordi­ nary compressors utilizing an electromagnetic vibrator as a source of power may be properly and effectively operated only in low demand conditions. In an attempt to alleviate some of these problems, it has been known to employ a multi-stage link in fluid com­ pression devices. However, this modification significantly complicates the structural configuration and achieves rela­ tively little improvement in performance. Still further, because of the low orientation accuracy in an ordinary electromagnetic vibrator, the vibrator and other components of the compression device are most often arranged coaxially to prevent uneven wear and sticking between cylinders and corresponding pistons. Thus, recip­ rocating fluid compression devices using an ordinary elec­ tromagnetic vibrator as a power source can be used only in certain applications where high performance is not essen­ tial. The difficulties suggested in the preceding are not intended to be exhaustive, but rather are among many which may tend to reduce the effectiveness and satisifaction with prior fluid compression devices. Other noteworthy problems may also exist; however, those presented above should be sufficient to demonstrate that fluid compression devices appearing in the past will admit to worthwhile improvement. OBJECTS OF THE INVENTION It is therefore a general object of the invention to provide a novel, non-linear electromagnetic vibration fluid compression device which will obviate or minimize difficulties of the type previously described. According to the present invention there is provided a non-linear, electromagnetic vibration, fluid compression device comprising a non-linear electromagnetic vibration device having a first vibration part, a second vibration part, an electromagnetic source comprising an armature included in one of said parts and an electromagnetic core included in the other of said vibration parts, means for operably connecting the first and second vibration parts to permit relative motion there between, said means including at least one non-linear, bellows plate spring, and electrical power means for supplying electrical current to the electromagnetic source for electromag­ netically inducing movement of the armature within the core in opposition to a non-linear restoring spring force of the connecting means whereby a resonant, non-linear electromagnetic vibration may be induced between the first and the second vibra­ tion parts; and a first compression cylinder including a piston received therein for reciprocating motion, the piston being operably connected to one of the first and second vibration parts, and the cylinder being operably connected to the other of the first and second vibration parts, whereby relative oscillating motion of the first and second vibration parts induced via action of the connecting means is converted to reciprocating piston motion in the first compression cylinder. The preferred fluid compression device embodying a non-linear, electromagnetic vibration device may be properly and effectively operated in a wide range of variable demand conditions. It embodies a non-linear, electromagnetic vibration with a high level of precision in directional vibration with a highly efficient and stable operation. The device is capable of high amplitude vibrations during compressor operations and is generally frictionless in operation. The preferred arrangement is low in maintenance and capable of being sealed within a container for extended operation. BRIEF SUMMARY OF A PREFERRED EMBODIMENT The invention as disclosed presents a reciprocating fluid compression device including as the power source a novel, non-linear, electromagnetic vibration devices in­ vented by the applicant herein and the structure of which is disclosed in detail in a separate patent application. The vibrator has high efficiency, stability, orientation accuracy, and large amplitude, and has many adaptive forms suitable for compression devices of different requirements. The non-linear, electromagnetic vibration device employed in a preferred embodiment of the instant recipro­ cating, fluid compression device includes an electromagnet, a frame, a linking block, and at least one segmented, co­ rugated leaf spring set. The center of each corrugated leaf spring is connected to an armature of the electromag­ net through the linking block. The two ends, of each cor­ rugated leaf spring, are connected to the core of the elec­ tromagnet through the frame. An air gap is selectively maintained between the core and armature of the electro­ magnet. Two corrugated leaf spring sets may be mounted respectively at opposing ends of the vibrator, or the vibrator may include only one corrugated leaf spring set with that set being mounted at one end of the vibration device. When a pulsating vibration-exciting current is set up in the coil of the electromagnet, the core and armature of the electromagnet, together with the corrugated leaf spring sets, drive a main vibrating part and a relative vibrating part, via electromagnetic force and non-linear elastic restoring force, to vibrate in a non-linear manner at a frequency corresponding to that of an exciting fre­ quency. The instant fluid compression device, according to a preferred embodiment, employs a simple single stage link structure connecting the armature of the non-linear, elec­ tromagnetic vibration device to the piston of at least one corresponding reciprocating compression cylinder. The vibration device has portions thereof fixedly connected to said at least one corresponding reciprocating compression cylinder. Each piston of a respective compression cylinder is coupled to the electromagnetic armature through an asso­ ciated single stage link member and a support block to which an end of the electromagnetic armature is fixed. In one embodiment a reciprocating compression cylinder can be fixedly linked to the front or rear side of the non-­ linear electromagnetic vibrator in a coaxial manner. Two or more reciprocating compression cylinders can also be fixedly linked concurrently to both right and left sides or the top and bottom, or other portions of the non-linear electromagnetic vibration device in a non-coaxial manner therewith. The overall combination is operative as a fluid compressor suitable for use in various refrigeration or other pump-type applications. BRIEF DESCRIPTION OF THE DRAWINGS FIGURE 3 is a partially cross-sectioned view of fluid compression piston and cylinder assemblies mounted upon opposing sides of a non-linear, electromagnetic vibration device as shown in FIGURE 1. FIGURE 1 illustrates an axonometric view of a non-­ axially arranged dual cylinder, reciprocating fluid com­ pression device, according to a preferred embodiment of the instant invention. FIGURE 2 illustrates an exploded view of a non-linear, electromagnetic vibration device for use in a reciprocating fluid compression device, shown in FIGURE 1, according to a preferred embodiment of the instant invention. FIGURE 4A illustrates an axonometric view of the com­ pression cylinder component of a reciprocating fluid com­ pression device according to one embodiment of the instant invention. FIGURE 4B illustrates an exploded view of a compres­ sion cylinder component featured in FIGURE 4A. FIGURE 5 illustrates a partially cross-sectioned view of a lubricating oil plunger pump for use in the recipro­ cating fluid compression device according to one embodiment of the instant invention. FIGURE 6 illustrates a coaxially arranged, single cylinder, non-linear, electromagnetic reciprocating fluid compression device according to an alternate embodiment of the instant invention. FIGURE 7 illustrates an electrical circuit for supplying working frequency current. DETAILED DESCRIPTION Terminology Prior to providing a detailed description of various preferred embodiments of the invention it may be worthwhile to briefly stablish operative terminology in connection with the subject non-linear electromagnetic device. In the instant invention the drive for the compressor comprises an electromagnetic oscillation installation which may be regarded as a bipolar oscillating system. The core of the electromagnet and other structures fixedly connected thereto in combination constitutes a first vibrating part of a given mass M1. On the other hand, the armature of the electromagnet and other structures fixedly connected there­ to in combination constitutes a second vibrating part of a given mass M2. During oscillation, these two oscillating parts make reciprocating motion relative to their respec­ tive static positions prior to such oscillations. The corresponding amplitudes of oscillation of these vibrating parts are inversely proportional to the associated given mass as given by the equation A1/A2 = M2/M1 wherein A1 and A2 represent respective amplitudes and M1 and M2 represents respective masses of the vibrating parts. Of these two vibrating parts, the one of comparatively smaller total mass has comparatively larger amplitude, and is referenced herein as the main oscillating or main vibrating part. The other vibrating part of larger mass and smaller oscillation amplitude is referenced herein as the relative oscillating or relative vibrating part. The total amplitude of the bipolar system, A, is the sum of the main vibrating part and the relative vibrating part amplitudes, A1 + A2. If the mass ratio M2/M1 is greater than ten (10), that is A1 is 10 times A2, then the whole electromagnetic oscillating system can be regarded as a single proton oscillating sys­ tem. In this event, the total amplitude value A may be regarded as being approximately equal to A1. Similarly, it is possible to adjust the amplitude ratios of the two vibrating parts by adjustments in their respective mass. Accordingly, depending on the manner of connection of various system components to the electromagnet core or to the electromagnet armature, main and relative vibrating parts of various different mass, configuration, and oscil­ lation amplitude may be formed. Structure and Operation Referring now to the drawings wherein like numerals indicate like parts, Figures 1-3 show a preferred embodi­ ment of the instant invention, comprising a compressor unit employing a single stage link structure for connection to respective reciprocating piston-cylinder units, and a non-­ linear, bellows spring plate, electromagnetic vibration device as a source of vibration for the compressor. In reference to Figures 1 and 2, the non-linear elec­ tromagnetic vibrator comprises an electromagnet frame 5, waveform plate spring sets 13, and armature link blocks 8 and 10. The central structure 1 includes an electromag­ net. The electromagnetic armature 6 is fixedly coupled at its opposing ends to armature link blocks 8 and 10 which are in turn connected to a central portion of a respective sectionalized waveform plate spring set 13 in-between two sections of each plate spring in the corresponding spring set. Portions of the frame 5 are fixedly connected to the opposing ends of each sectionalized waveform plate spring set. When the vibrator is in operation, the armature 6 oscillates in a direction generally perpendicular to the primary disposition of the sectionalized waveform plate spring sets. A dual-piston-cylinder type non-linear electromagnetic vibration air compressor is shown in Figure 1. The power source of the said air compressor is a non-linear, bellows spring, electromagnetic vibration device spearately illus­ trated in Figure 2 in which an electromagnetic core 1 of the electromagnet is riveted to a base 2 by means of rivets 3 to form a single unit. The electromagentic core con­ nected to a generally U-shaped frame 5 by means of a screw 4 on each side of the frame. An armature 6 of the electromagnet is riveted to upper and low linking plates 7 and is connected to a front link­ ing block 8 by means of welding or the like. An electro­ magnetic coil 9 is placed in the core assembly of the elec­ tromagnet and the armature assembly is inserted toward a rear linking block 10 after passing through an inner hole of the core 9. An upper cover 11 presses tightly against the electromagnet core by means of screws 12. Two sets of sequentially arranged corrugated leaf springs (i.e. bellows or sectionalized waveform plate springs) are placed at the two ends of the frame 5 respec­ tively. Each leaf spring is separated by means of a washer 14. Although only a front and end spring are shown in the drawings, each spring set 13 may comprise a plurality of individual springs separated by the thin spacer washers 14. At the center and two ends of each bellows leaf spring set 13 there are three assembly sections, each plate having two punched assembly holes through each assembly section. A pressing plate 15 is located at the outer side of the two sets of corrugated leaf spring sets 13 and tightly presses the corrugated bellows spring against the frame 5. At the center of each end of the electromagnetic vibrator is pressing strap 16 which tightly presses the central assem­ bly portion of the corrugated bellows springs 13 against a corresponding end block. At each of the two ends of the non-linear electromagnetic vibrator four screws 17 respec­ tively pass through assembly holes at two ends of the pressing plate 15 as well as assembly holes at two ends of the corrugated leaf spring set 13 and screws down into holes at two ends of frame 5. At the center of each end of the electromagnetic vibrator two screws 17 pass through assembly holes of the pressing strap 16 and assembly holes at the central assembly plate of the corrugated leaf spring set 13 and screw down into holes at the center of front linking block 8 and rear linking block 10 forming a non-­ linear, bellows plate spring, electromagnetic vibration device. The sectionalized bellows (waveform) plate spring sets are non-linear elastic components. The non-linear charac­ teristics may be conveniently selected and designed to suit different application environments. In the overall vibra­ tion assembly, each waveform plate spring of one configu­ ration may be used in combination with waveform plate springs of the same or other kinds to suit the particular requirements of different application environments. These sectionalized plate springs have smooth non-linear charac­ teristics and a wide range of potential behavior in combi­ nation to support a correspondingly wide range of desirable flexibility and rigidity. There is very minimal internal damping, and a very long fatigue life. The plate springs provide high precision in directional motion, and high adjustability for self-adapting control. In all these aspects the subject invention manifests optimal performance in comparison with common linear springs, sectionally linear composite springs, and other existing non-linear springs. The number of waveform plate springs in each spring set 14 may be varied and selectively adjusted to vary the vibration frequency responsive to an exciting frequency from a source. If the number of plate springs is raised to equal the square of an integral times the number required for a harmonic response, the vibration frequency may be multiplied a corresponding integral times. Similarly, if the number of plate springs is made to equal the square of an inverse integral times of the number required for a harmonic response, then the vibration frequency can be made to equal an inverse integral times of the exciting fre­ quency. In this manner, frequency conversion and multipli­ cation under harmonic resonance can be achieved via mechan­ ical adjustments of the number of plate springs. The need for a complex electronic frequency converter is completely eliminated. With the subject vibration assembly, the reso­ nance state can be persistently maintained under no load, or varying rated load conditions. The concept is based on the unique characteristic of strong non-linear systems in being able to generate harmonic resonance. The spring-set stiffness may be varied by varying the number of plate springs, and thus can be made to equal the square of an integral or of an inverse integral times the degree of stiffness under harmonic response. The inherent vibration frequency may be raised an integral times or an inverse integral times by combined adjustments in the mass of vi­ brating parts and the vibration stiffness. Accordingly, the subject vibration assembly is able to achieve harmonic resonance characteristics in mechanical vibration as in non-linear electromagnetic wave vibration. The instant device enables frequency multiplication and frequency con­ version of harmonic response to be achieved for resonance type mechanical vibration without requiring an independent electronic frequency converter device. When the vibration device is activated, an electrical exciting current flows through coil 9 (note Figures 2 and 7), pulsed attraction is generated by electromagnetic action. The spring-sets are correspondingly elastically flexed in unison towards a common direction along a linear axis parallel to the longitudinal axis of the upper con­ necting plate 7. Because the springs are sectionalized, and because opposing ends of each section of each plate spring are couple to different vibrating parts, main and relative, as discussed above, two self-reciprocating par­ allelograms are formed which share a mjaor side along an axis parallel to the central longitudinal axis of the upper connecting plate 7. Each side wall of frame 5 constitutes the other major side of each parallelogram, and a corre­ sponding section of each plate spring collectively forms every minor side of each of said two parrallelograms. The whole electromagnetic vibration device is separated from other elements of the compressor by means of four isolating springs 18 and forms an independent dual-­ mass vibration system. When an alternative vibration-exciting current is set up in the electromagnetic coil 9, pulsating electromagnetic force is created between the electromagnetic core 1 and armature 6 and, together with the non-linear elastic re­ storing force exerted by the non-linear bellows plate spring sets 13, generates forced vibration at a frequency equal to the frequency of the vibration-exciting current produced from a conventional electrical source such as shown schematically in Figure 7. A main vibrating mass is composed of the armature assembly, front linking block 8 and rear linking block 10. A relative vibrating mass is composed of the electromagnetic core assembly, frame 5, upper cover 11 and front and rear pressing plates 15. When the inherent frequency range is modulated by means of changing the number of springs in the corrugated, bellows plate, spring set 13 so that the electromagnetic vibration is near resonant state at the frequency of the vibration-­ exciting current. It has been found that a designed ampli­ tude of 6-7 mm can be reached when the exciting frequency is 50 Hz, and non-linear vibration characteristics can be obtained. In a preferred embodiment of the instant invention a solenoid type electromagnet is utilized. In comparison with a common n or E type electromagnet, the solenoid type has a larger electromagnetic attractive force and travel, and is much easier to connect its two ends to double elas­ tic components, and to carry out position fixing and air gap trimming. In addition, the structure of the entire electromagnetic vibrator is made power-head-like so that it is easy to connect to and maintain. The core, upper cover and adjoining frame to the core, the armature, and front and rear support blocks of the armature all can be used as the unit for producing the principal vibration. In this manner, the structure can be employed flexibly and mechani­ cal vibration can be sent out conveniently through attach­ ments with simple connecting parts at a number of alterna­ tive positions. A significant breakthrough in the technical field of non-linear vibrating machines made by the present invention lies in the fact that subject springs have been selected to exhibit exponential/sine waveforms. A curve for shifting its standard rigidity is determinable and the parameters for the springs optimal working characteristics are con­ veniently selectable. This type of non-linear vibration not only depends upon the average rigidity of the vibratory elastic component but has also a close relationship with its rigidity curve and structural damping. The exponen­ tial/sine waveform spring adopted in the present invention has smaller structural damping than other springs and the relationship between stress and strain is approximately a logarithmic function. Let "f" be the stress and "ℓ" the strain. Then ℓ = α1n(1+βf), where α and β are parameters which can be determined by the method of least square from experimental data. Con­ versely, "f" can be written as an exponential function of the strain: Its rigidity function is found to be Calculations by microcomputer show that the vibration type non-linear spring with such rigidity function exhibits a stable periodic vibration (under rather extensive external force conditions and for certain amplitudes). The computer has also drawn out its stable limiting rings of the phase space under various parameter conditions. Even with an elastic vibration component of excellent performance, normal operation of a vibrating machine still cannot be fully ensured with conventional systems. This is because external conditions may vary in different ways when the machine is in operation. Thus, for example, when it is used for cutting, the damping in cutting would vary with the change of the hardness and dimension of the work piece being cut; when it is used for conveying and sifting of material, the quantity and variety of the material would entail change in the vibrating mass; and when it is used in compressing gases (vibratory compressor), which is equiva­ lent to attaching a gaseous spring, the change of rigidity curve would arise. The change in these conditions would affect the type of respective vibrations and may cause them to transfer from the near resonance area to the far reso­ nance area and to come out of stable limiting rings and get into a non-stable state, with the result that the vibrating machine either could not operate normally or would exhibit reduced performance during operation. The present invention has effected three kinds of vibration control, viz: Damping control (stability control for varying damp­ ing); Rigidity control (stability control for varying rigid­ ity); and Mass control (stability control for varying mass). The fundamental principle of control is the method of feedback function, i.e., a preset feedback (self-compensat­ ing) function is to be formed by designing electromagnetic, elastic, and mass damping systems. Once the working condi­ tions of a vibrating machine undergoes a change within a certain range, the feedback function would automatically play a role to control and offset the change in external conditions so that the machines may continue to work nor­ mally. The feedback function is implemented by the following procedures: (a) Procedure of Electromagnetic Feedback As the amplitude of vibration decreases with the in­ crease of external damping, the velocity of vibration, and, therefore, the resistance of the coil, is reduced, leading to the increase of the current. The result is the increase of the amplitude. This control effect is called electro­ magnetic feedback, which is particularly manifested as the increase of power with increase of external damping (work­ ing damping). To exploit the feedback effect to the ut­ most, the present invention has made the optimum selection of the gap between the electromagnet and yoke and has used a plug-in yoke so that the maximum feedback effect can be obtained without any collision. The hard spring which the present invention has adopted causes the vibrating body to reduce its velocity abruptly when it reaches the limiting position, which also contributes to the maximum exploita­ tion of this control effect. Moreover, in the design of the coil-rectifier circuit, various forms such as full-­ wave, full-wave rectification, half-wave rectification, and "full-wave (electromagnet) x full-wave rectification (yoke)" may be employed to meet different working require­ ments. (b) Procedure of Preset Stress In the course of the design, working area, i.e., near resonance, is chosen not only according to the curve of the elastic component, but by matching the selection of para­ meters the component is made to work outside the working area. Once either the external damping or the mass in creases, the elastic component would return from the out­ side to the inside of the working area. The resonance force inside the working area would assist to compensate for the deterioration of external conditions so that the machines can operate normally. (c) Procedure of Auxiliary Springs In the design of vibrating machines, beside the elas­ tic component producing the principal vibration, several sets of auxiliary springs may be installed to meet any possible variation of external conditions. When external changes interfere with the mass and rigidity, these auxil­ iary springs, would to varying degrees, play a part auto­ matically, resulting in compensatory changes in the rigid­ ity of the vibration system so that the machines can operate normally. The above control procedures may be used either sepa­ rately or jointly with one or more of them together. In a specific design, differential equations may be formulated on the basis of test data to be solved by simulation and, if necessary, a computer may be used for optimizing operat­ ing conditions. Bellows (Waveform) Type Plate Springs Non-linear rectangular bellows type plate spring group is a generally significant operating element of the subject invention by which the main characteristics of the elec­ tromagnetic vibration facility and hence, those of the vibration machinery using such facility as its power source are determined. The main characteristic of this element is the appli­ cation of thin bellows type plate spring pieces with a generally rectangular outer dimension, and separate segment sine configuration or exponential function and the spaced lamination of such plate springs into a group. Each bellows type plate spring piece has an assembly hole or separate segment assembly plane, so as to use a bolt for fixing and restraining it. Aluminum washer shims may be used between these assembly planes, so that friction may be avoided, when deformation between plate springs is pro­ duced. The main characteristics of the subject bellows type plate springs may be described in some detail as follows: (a) Constructed by Thin, Rectangular Plate Spring Piece A conventional plate spring piece used in electromag­ netic vibration machinery is constructed by a thick (2mm) rectangular plate spring piece. There is neither a bellows configuration nor assembly hole on it. The pieces are used in a non-fixed-restraint mode, with the plate spring lami­ nated in a group, and comprising elastic elements with linear elastic characteristic. There were also previously known single-piece, thick, circular plate spring pieces with concentric circle series washer elements, forming a non-linear characteristic or deformation with separate segment linearity to a definite stage and thereafter pre­ senting a non-linear characteristic. The bellows type plate spring of the subject invention is composed of thin, generally rectangular plate spring pieces. Each bellows type plate spring piece is generally 0.3- 1.5 mm thick. To compare the thin type plate-spring piece with thick type plate-spring piece, we find that the inter­ nal damping of the former decreases exponentially, when they are laminated in a group and used. Total damping is still less than that of a comparatively thick type plate-­ spring piece with the same rigidity, but the strength of the transverse bream constructed by the former increases with the increase in total area of cross section. In com­ paring rectangular bellows type springs with disc shape bellows type springs or with rectangular plate springs, it is found that the internal damping determined by the con­ struction factor is also much smaller. When a generally rectangular bellow type plate spring is in the state of working deformation, deformation in a rectangular bellows type plate spring through the bending or twisting action on a vertical line of the bellows may be much higher than that of various conventional plate springs (such as rectangular, non-bellows or disk shape, bellows plate springs) and that of rubber springs under the same action force; yet, in the direction of non-working deformation, there is a very large mono-directional rigidity. Therefore, when the subject invention is used in a vibration facility, and vibration motion is produced, both large vibration amplitude and high orientation is obtained. Each generally rectangular plate spring may have a shaped outer dimensions, such as straight, convex or con­ cave. (b) Vertical Bellows with Sinusoidal Configuration Or Exponential Function As mentioned above, with generally rectangular bellows type plate spring pieces, the vertical bellows has a unique influence upon reducing the structural internal damping and assuring correctly oriented motion. Furthermore, there are various kinds of cross-sections of the bellows, whatever the overall outer dimension of the plate spring, such as sinusoidal configuration type, exponential function type and other different forms of bellows type cross-section. These kinds of plate spring pieces have excellent longevity in the fatigue type working state, because the deflection curve is very smooth and the rate of variation may approach an infinitesimal value. (c) Continuous Non-Linearity of the Elastic Characteristic Curve and the Versatile Selectivity of the Curve The elastic working characteristic of the vertical, bellows type spring piece of this invention presents the variation of continuous-non-linearity within the entire scope of working deformation from start to end. Many kinds of conventional non-linear springs, such as a non-cylindri­ cal spiral spring and so on, usually enter a region of non-­ linear characteristics only after they have been deformed to a specified extent, and some other non-linear springs, such as linear plate springs, non-linear spiral springs and some combinations of such springs constitute a non-linear characteristic curve by exhibiting separate segment linear characteristics. The generally rectangular, bellows plate spring of the subject invention not only has a pronounced, continuous, complete curve of non-linear elastic character­ istic, but also may selectively obtain many different kinds of characteristic curves of non-linear elasticity through changing the design parameters of plate-spring, such as its outer shape, thickness, different bellows shape cross-sec­ tion elastic waveform, depth of each bellow trough and different techniques of heat treatment. A transistor tri­ ode can be used as an example to explain the above men­ tioned situation. Every kind of transistor triode has its own amplification characteristic curve which may be selec­ ted according to a technical specification, and therefore, may satisfy different technical requirements of usage and control. Particularly, in the state of different external load fluctuations, if the proper curve of non-linear elas­ ticity character can be designed and selected, then proper non-linear feed-back characteristics can be achieved to maintain the stability of vibration of the entire system. (d) Fixed Restraint The generally rectangular, bellows plate-spring group of the the subject invention is different from conventional plate-spring groups. It adopts an assembly mode of fixed restraint with assembly holes which differ from that of conventional, single, non-linear springs. In addition, it utilizes a method of spaced lamination in a group for use, so, springs of this invention has both the characteristic of non-linear elasticity as well as versatile and unique modulation characteristics. The total rigidity of the vibration system can be modulated by increasing or reducing the number of pieces of the bellows plate-spring sets, to realize one order harmonic resonance or multiple order harmonic resonances. Under the conditions or resonance, owing to the above-mentioned characteristics of low inter­ nal damping and non-linear motion of the spring of the instant invention, it is possible to obtain much larger resonance amplitudes and spontaneous acceleration char­ acteristics than those of previously known linear and non-­ linear electromagnetic vibration facilities. Therefore, the energy consumption per unit of vibration strength de­ creases considerably, and a novel harmonic resonance type double frequency variation method is thus formed. To summarize, non-linear rectangular bellows plate spring group of this invention has main characteristic of fixed restraint in application, such as, separate segment sine configuration type or exponential function type bellows plate spring with thin and rectangular outer shape and laminating in group, therefore, its elasticity charac­ teristic curve has continuous non-linearity and versatile selectivity of characteristic curve. When it is used in electromagnetic vibration facility or various kinds of vibration machinery, if compared with any known linear or non-linear spring, it may obtain the best and the most stable performance characteristics of vibration in many respects, such as: convenience in design, selection and test of characteristics curve of non-linearity, minimum internal damping, large amplitude, large spontaneous accel­ eration and high precision orientation, one or more than one harmonic resonance, realization of double frequency variation of excited resonance, as well as high strength and long fatigue-resistant duration time. Solenoid Type Electromagnet A conventional electromagnetic vibration unit typical­ ly uses a shape "E" shape or "H" shape electromagnet. An electromagnetic vibration facility of this invention uses a solenoid type electromagnet wherein the armature is gener­ ally T-shaped and an electromagnetic core is generally U-­ shaped which may better concentrate its electromagnetic attraction in the magnetic field. Furthermore, the elec­ tromagnet of the instant invention is made to include unique electromagnetic elements. Silicon steel sheet of high silicon content is used to replace that of low silicon content as a basic material of the electromagnet. In this manner, larger electromagnetic attraction forces can be ob­ tained than that of a conventional unit. In addition, dual reciprocation structures of parallelogram shaped cross-sec­ tion can be easily constructed to include both front and rear sectionalized waveform plate spring sets on opposing sides of the electromagnet so as to assure a high precision fixed direction motion of the vibration system during sys­ tem operation. Control and Adjustment (a) Control and Adjustment of Performance Characteristics of One or More then One Harmonic Resonance In conventional linear and non-linear electromagnetic vibration facilities, only the form of a base wave reso­ nance can be used for performing resonance control and adjustment. According to the instant invention, harmonic resonance can be produced by adjusting the total rigidity of the non-­ linear spring sets in the vibration facility. Moreover, through an adjustment of the number, size, bellow shape, and heat treatment of the springs, the total rigidity can become the square of an integral fold or square of a frac­ tion of an integral fold of the predeterminable rigidity in harmonic response. A simultaneous adjustment of the vibrating mass and the total rigidity of the vibration system can yield a vibration frequency higher than that in base wave resonance by an integral fold or a fraction of an integral fold. Therefore, harmonic resonance characteris­ tics traditionally achieved via supplemental electrical controllers can be obtained mechanically. In this manner, frequency variation for excited resonance frequency can be realized without adding any frequency variation electrical devices. By adjusting the number of plate springs in one or more sectionalized waveform plate spring set to equal the square of an integral (n) times a number predeterminably required therein for the vibration device to achieve har­ monic response, one can yield an integral (n) times the vibration frequency of the source as the operating vibra­ tion frequency of the device. Similarly, by adjusting the number of plate springs in one or more sectionalized wave-­ form plate spring sets to equal the square of an inverse integral (1/n) times a number predeterminably required therein for the vibration device to achieve harmonic re­ sponse, one can yield an inverse integral (1/n) times the vibration frequency of the source as the operating vibra­ tion frequency of the device. An example of a determination of the number of spring plates is illustrated below: The number of plates may be obtained by using the following equation Once K (χ) has been determined, the number of plates can be determined according to this equation. The wave shape and the plate form are important to the spring characteristic design. The spring design can be solved theoretically as well as exper­ imentally. The spring characteristic depends on the wave shape, the number of waves, the form of the plate and the applied constraint conditions. The spring design must meet the following requirements: (1) The spring characteristic must comply with the vibration characteristic. (2) The spring fatigue life must satisfy long-­ term operating conditions. As the applications of springs are extensive, springs used on various vibrating machines may be different from each other. Various springs may be designed qualitatively according to the following comments to determine their parameters, then modi­ fied by routine experiments. I. Spring Characteristic Using the following terminology: K (χ) is the spring characteristic r is the radius of wave shape S is the plate thickness b is the plate width ℓ is the plate length n is the number of waves The spring characteristic K (χ) will be proportional to S³. proportional to b, inversely proportional to ℓ², inversely proportional to r² (using an equivalent arc for other curves), proportional to , if the spring material has been determined (consider every wave as a spring, then spring with n waves is equivalent to n shorter springs connected in series. Therefore II. Selection of Spring Shape A. Wave Shape: In determining the wave shape of a spring, a matter of main concern is the fabricating method and its fatigue strength. The sinusoidal and exponential reduction curves are superior to others. Research results of large deflection theory indicates that all n th -order differentiable curves and combined curves will not cause stress concentrations, thus behave better for shock resistance and fatigue resis­ tance. Other curve shapes can not be used, however, that forementioned curves are better. In cases of large changes of ac­ celeration, the forementioned curves are greatly preferred. B. The plate form may be tailored to comply with the stress distribution and adjustment of the spring characteristic, provided the directional vibration requirement has been met. Referring again to the above equation (1), resonance will take place so long as W(χ)=nω₂ (where n=1,2,3...k or n=1,1/2,1/3....1/k) with the operating frequency of power supply being ω₁, it is so called harmonic resonance, which is non-linear vibration characteristic. In application, W(χ) is selected as required, then K(χ) can be determined based on the inertia mass "m", where K(χ) is the general characteristic of the springs required by the system. It is possible to design the spring according to K(χ), suppose the characteristic of each spring is R(χ), then R(χ)=K(χ)/n, where n is the number of the plate springs. In an air compressor as an example (to be described in detail below) assume the motion equation of the compressor; m+r(,) + K(χ) = F (t) will satisfy the operating requirements. The compressor cylinder acts as an air-spring K₁(χ) during the compress­ ing process. Now a spring K₂( χ) needs to be added in series K( χ) = K₁( χ) + K₂( χ) to meet the operating re­ quirements. Then K₂( χ) may be determined by the relation­ ship K₂( χ) = K( χ) - K₁( χ). Knowing or selecting the above referenced variables enables the characteristic and the number of springs to be designed as discussed above. Alternatively, given the structural arrangement disclosed herein, one skilled in the art will be able to quickly select a desired number of characteristics of the spring sets by routine experimentation. (b) Control and Adjustment of the Stability of Performance Characteristics Conventional linear electromagnetic vibration devices and vibration machinery are very limited in the region of the stability of performance characteristics under the conditions of fluctuating external loads. Accordingly, complicated electrical control mechanisms are frequently required to improve the stability of performance charac­ teristics. Some existing non-linear type electromagnetic vibration devices, such as rubber spring electromagnetic vibration units and the vibration machinery constructed with it, have been slightly improved in performance stabil­ ity owing to the feedback of non-linearity characteristic curve, but an electrical control mechanism is still needed and it is very difficult to control and adjust the self-­ feedback. No matter how external loads are fluctuated in the form of mass variation, rigidity variation or damping vari­ ation and so on, an electromagnetic vibration device according to the instant invention using non-linear bellows plate-spring groups, by taking such spring group as power source and adding a non-linear type elasticity control element according to the requirements, may utilize the self-feedback of the non-linear type elastic element to control and adjust the performance characteristics in a compartively large range by selecting and fitting the proper control spring matching the non-linear elasticity curve according to the scope of external load fluctua­ tions. Therefore, the vibration system can maintain a stable state of resonance within the scope of load fluctua­ tion from start to end. In this manner, the stable performance characteristics can be obtained without adding any electrical control mechanism. Turning now to Figures 2 and 3, a bore 19a is located at opposing sides of the front armature link block 8. A respective rod link 19 has one end releasably coupled to a corresponding bore 19a in block 8 and extends through a cut-out portion 19b in said frame 5. A mechanical link joint 56 is used to couple the rod link 19 to a piston 21 operably received within a compressor cylinder 23. One cylinder is preferably positioned on opposing peripheral areas of the central structure. The rod link 19 operably transfers motion of the vibrator at its vibration frequency to piston motion and thus to corresponding compression strokes per minute. The full amplitude of vibrator vibration corresponds to the range of compression stroke. Referring specifically to Fgiures 4A and 4B a piston is located within each compression cylinder 23. The compression cylinder is fixed via fasteners to a lateral wall of the vibrator frame 5. A similar assembly is pre­ ferably arranged for balance on both sides of the vibrator, as shown in Figure 1, resulting in a compression device having a single vibrator source and balanced dual compres­ sion cylinders including respective pistons therein. Alternative embodiments may be reasonably constructed by one with ordinary skill in the art. For instance, the compressor unit may have only one compression cylinder. A different embodiment may position dual cylinders in front and behind, or on top and below of the vibrator, as opposed to on either side as shown in figure 1. In addition, more than two compression cylinders may be efficiently accommo­ dated in a similar manner via the novel structure dis­ closed. When cylinders are mounted in front and behind of the vibrator, the assembly is of coaxial configuration. A non-coaxial configuration is represented where cylinders are located laterally or vertically from the axis of vibra­ tion of the vibrator. When the dual balanced compressors are utilized or an axial compressor is featured, a balanced condition exists which is a low friction, low maintenance condition and will admit to use of a sealed enclosure for the vibration assem­ bly. Figure 4A illustrates a perspective view of the rod and piston/cylinder assembly as non-coaxially mounted to the electromagnetic vibrator. Figure 4B is an exploded view of the compressor unit shown in Figure 4A. In order to eliminate axial error in assembly, a slid­ ing block 22 is arranged in the connecting head 56 which links the connecting rod 19 and piston 21. Driven by the front linking block 8, piston 21 reciprocates at one end in cylinder block 23 at a frequency and amplitude equal to those of the non-linear, harmonic electromagnetic vibra­ tor. A valve package comprising an inlet valve 25, valve plate 26, outlet valve 27, and cylinder head 28 is mounted on the other end of the cylinder 23 by means of screws 24. During each backward stroke of the piston 21, the inlet valve 25 is opened automatically and air is sucked into cylinder 23 through an inlet hole at an upper center of the cylinder head 28 and inlet pipe. During each com­ pressing stroke of the piston 21, the inlet valve is closed automatically onto the valve plate 26, and outlet valve 27 is opened automatically. Air in cylinder 23 is then com­ pressed by piston 21 and is exhausted out of the compres­ sing cylinder through an exhaust hole. Compressed air travels through an exhaust pipe connector 29 fitted on cylinder head 28, an exhaust pipe 30, a five-way pipe fit­ ting 31, and enters a compressed air container 32. Com­ pressed air may then be accessed, as desired, through an air-supply valve 33. High exhaust pressure can be obtained by means of adjusting the position of the dead point of the working stroke of the piston 21 to reduce the gap between the piston crown and inlet valve 25 to be sufficiently small by the end of the working stroke of the piston. The pressure within cylinder 32 can be indicated by a conventional pressure gage 34 connected to the five-way pipe fitting 31. The maximum output pressure the air com­ pressor can reach is approximately 12-20 kg/cm² when the diameter of the piston 21 is 36 mm. Under a rated working pressure of 6 kg/cm², the said dual-cylinder compressor can stably produce 0.025 m³ compressed air per minute. The required working pressure range can be adjusted freely by means of a pressure regulator 35 connected to the five-way pipe fitting 31. The starting current of the electromag­ netic vibrating air compressor is not higher than the operating current and the said compressor can be started frequently under pressure. In addition, the compressor can always work close to resonant state within the changing range of working pressure. The whole electromagnetic vibrating air compressor device is installed on a base 36 by means of four isolating springs 18 (note Figures 1 and 2). A certain amount of lubricating oil is contained within the base 36. Figure 5 illustrates in detail a manner of connection between the electromagnetic vibration device and the base. In this connection a linking plate 38 is fitted under the front linking block 8 of the electromagnetic vibrator by means of a screw 37. A plunger 40 of a plunger pump which is in­ stalled on the frame 5 by screw 47 may then be driven against restraining forces of compression springs 39. The plunger 40 reciprocates in the plunger cylinder block 41 and pumps lubricating oil through a suction pipe 43 with a filter 42 from an oil sump in the base 36 and through one-way valves 44, 45 and an outlet three-way pipe fitting 46 supplies lubricating oil at a required rate to the pistons 21 of the two air compressing cylinders. The lubricating oil returns to the storage sump of the base 36 through pistons 21 and over the oblique plane of the base and can be re-circulated again. Figure 6 is an axonometric drawing showing a non-­ linear vibration power source and a compressing cylinder assembly of a single-cylinder non-linear electromagnetic air compressor whose compressing cylinder assembly and electromagnetic vibrator are arranged coaxially. The basic structure of the compressor is similar to the first embodi­ ment shown in Figures 1-5, except that the compression cylinders) are coaxially mounted. In a simplified struc­ ture, the two sets of corrugated leaf springs on opposing sides of the vibration assembly are combined into one set and are installed at one end of the electromagnetic vibra­ tion device. A compressing cylinder 23 is directly fitted onto the frame 5 at another end of the electromagnetic vibration device, by means of screws 20. A piston 21 of the axial compressor is connected to the main vibrating section through connecting frame 49 which is fitted on the rear linking block 10 by means of screws 48. Alternatively, the corrugated bellows spring sets need not be combined and relocated, and each compression cylin­ der may be mounted outside of a corresponding spring set while fixedly connected to the frame 5 via bolts 17 through plate 15 with a piston 21 coupled to elements 10. In this alternative manner, one or more than one compression cylin­ der may be mounted coaxially to the vibration assembly without rearrangement of a spring set. The air compressing procedure of these coaxial embodiments is similar to that of above described non-coaxial embodiments. Summary Of The Major Advantages A non-linear electromagnetic vibration device employed in the instant non-linear compression device has a higher range of vibration amplitude than an ordinary vibrator. At certain optimal exciting frequencies, it may achieve a vibration amplitude twice or more times as large as a con­ ventional electromagnetic vibrator. Moreover, the non-­ linear electromagnetic vibrator exhibits an enhanced degree of working stability. This stability persists even under harsh conditions of drastically varying load, because of a high degree of adaptability characteristic of non-linearity of the vibration device. At the same time, the precision of directional vibration is enhanced because of a non-linear electromagnetic vibrator is ordinarily of a parallel quad­ rangle structure. Whether a coaxial or non-coaxial configuration is employed, the subject invention includes a novel compressor structure employing a non-linear electromagnetic vibrator and is free of seizure and non-uniform wear problems asso­ ciated with compressors of the prior art. Furthermore, a simple single stage link structure is employed, which greatly reduces the complexity of the device and expands its range of application utility. As compared to conventional linear electromagnetic vibrating reciprocating fluid compressing devices, the present device has a simpler structure and can obtain greater working displacement and higher working pressure. In addition the device can always stably work close to a resonant state in a large range of pressure changes -- from null working pressure (0 kg/cm²) to a maximum working pres­ sure. The subject device has a stable working current and does not rise when working pressure increases and can fre­ quently start at any time without difficulty under null load or under pressure. The present device has accurate motion orientation and can avoid sticking between piston and cylinder and uneven wear whether it is coaxially or non-coaxially arranged with multicylinders. The present device can save approximately 50% on energy usage as com­ pared with rotary motor powered reciprocating fluid com­ pressing devices having a similar displacement and working pressure. The present device can be composed of a non-linear electromagnetic vibrator and different kinds of reciprocat­ ing compression cylinder assemblies and can be widely used in different application environments including those of a refrigerating compressor, an air compressor, and pumps. The novel structure of the subject invention produces a larger discharge with a simple configuration. A high working pressure may be achieved. The compression unit can operate steadily and persistently in or near a resonance state despite variations in load pressure. Furthermore, the working current does not rise when the load pressure is increased nor does it fall when the device is in resonance. Alternative Embodiments In describing the subject invention, reference has been made to preferred embodiments. Those skilled in the art, however, and familiar with the disclosure of the sub­ ject invention, may recognize additions, deletions, substi­ tutions, modifications and/or other changes which will fall within the purview of the invention.

Claims: 1. A non-linear, electromagnetic vibration, fluid compres­ sion device comprising: a non-linear electromagnetic vibration device having a first vibration part including, an electromagnetic armature, and an electromagnetic coil mounted about said arma­ ture; a second vibration part including, a generally U-shaped electromagnetic core mounted about said armature and said coil, a free end portion of said armature extends into said generally U-shaped electromagnetic core to a posture wherein the free end of the armature is adjacent to but spaced from a base portion of said generally U-shaped electromagentic core; means for operably connecting said first vibration part to said second vibration part to permit relative motion between said first vibration part and said second vibration part; said means for operably connecting said first and second vibration parts including, at least a first generally rectangular, non-­ linear, bellows plate spring wherein one portion of said spring is operably connected to said first vibration part and another portion of said spring is operably connected to said second vibration part; electrical power means connected to said electromag­ netic coil for supplying electrical current pulses to said coil and electromagnetically inducing movement of said armature within said core in opposition to a non-­ linear restoring spring force of said at least one generally rectangular, non-linear bellows plate spring operably extending between said first vibration part and said second vibration part, whereby a resonant, non-linear electromagnetic vibration may be induced between said first vibration part and said second vibration part; a first reciprocating-type compression cylinder in­ cluding a piston received therein for reciprocating motion, said piston being operably connected to one of said first and second vibration parts, and said cylinder being operably connected to the other of said first and second vibration parts; whereby relative oscillating motion of said first and second vibration parts induced via action of said non-­ linear bellows plate spring is converted to recipro­ cating piston motion in said first compression cylin­ der. 2. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 1 wherein: said first portion of said pump comprises a piston; and said second portion of said pump comprises a cylinder. 3. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 1 wherein: said first reciprocating compression cylinder is non-­ coaxially mounted with respect to a major axis of said first and second vibration parts; and a first link means for connecting said piston to said one of said first and second vibration parts. 4. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 1 and further comprising: a second reciprocating-type compression cylinder in­ cluding a piston received therein for reciprocating motion, said piston being operably connected to one of said first and second vibration parts, and said cylinder being operably connected to the other of said first and second vibration parts; whereby oscillating motion of said first and second vibration parts induced via action of said non-linear bellows plate spring is also converted to reciprocat­ ing piston motion in said second compression cylinder. 5. A non-linear fluid compression device as recited in claim 4 wherein: said first reciprocating compression cylinder is non-­ coaxially mounted with respect to a major axis of said first and second vibration parts; a first link means for connecting said piston to said one of said first and second vibration parts; said second reciprocating compression cylinder is non-­ coaxially mounted with respect to a said major axis of said first and second vibration parts; and a second link means for connecting said piston to said one of said first and second vibration parts. 6. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 5 wherein: said major axis of vibration of said first and second vibrati parts and said axes of piston reciprocation of said first and second reciprocating compression cylinders are arranged in parallel. 7. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 5 wherein: each of said first and second linking means includes a support block to which an end of said electromagnetic armature is connected, and a link member fixedly con­ necting a corresponding piston to said support block; and each of said link members includes a rod having a major axis disposed substantially perpendicular to said major axis of vibration of said first and second vibration device. 8. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 1 wherein: said first reciprocating compression piston and cylinder is coaxially mounted with respect to a major axis of vibration of said first and second vibration parts. 9. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 1 wherein said second vibration part further comprises: a generally U-shaped frame surrounding and receiving said generally U-shaped electromagnetic coil and being releasably connected to the lateral surfaces of said core. 10. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 9 wherein: said cylinder is securely connected to said U-Shaped frame, and said piston is operably connected to said electromag­ netic armature. 11. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 10 wherein said first vibration part further comprises: a first linking block connected to said electromag­ netic armature. 12. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 11 wherein: said armature comprises a generally T-shaped configu­ ration and the length of a leg element of the T-shaped armature is such that the gap between the free end of the leg element of the armature with respect to the base portion of the U-shaped electromagnetic core is equal to a gap that exists between the arm portions of the T-shaped armature and end most leg portions of the U-shaped electromagnetic core. 13. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 12 wherein said first vibration part further includes: a second linking block connected to said electromag­ netic armature and extending adjacent to but spaced from the exterior of said electromagnetic core, said second end unit being in alignment with said first end unit: and means for operably connecting said leg element of said armature to said second end unit. 14. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 13 wherein said at least a first generally rectangular, non-linear, bellows plate spring comprises: A plurality of generally rectangular, non-linear bellows, plate springs which are stacked together but spaced apart into a mutally parallel array of generally rectangular, non-linear bellows, plate spring sets. 15. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 14 and further comprising: a plurality of generally rectangular, non-linear bellows, plate spring sets extending between said first vibration part and said second vibration part. 16. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 15 wherein: the number of plate springs in each said generally rectangular, non-linear bellows plate spring sets equals the square of an integral (n) times of a number predeterminably required therein for the vibration device to achieve harmonic resonance. 17. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 15, wherein: the number of plate springs in each said generally rectangular, non-linear bellows plate spring sets equals the square of an inverse integral (1/n) times of a number predeterminably required therein for the vibration device to achieve harmonic resonance. 18. A non-linear, electromagnetic vibration, fluid compres­ sion device as defined in claim 1 and further com­ prising: lubricating fluid pump means connected between said first vibration part and said second vibration part for delivering lubricating fluid to said first reciprocating-type compression pump. 19. A non-linear, electromagnetic vibration, fluid compression device comprising a non-linear electromagnetic vibration device having a first vibration part, a second vibration part, an electromagnetic source comprising an armature included in one of said parts and an electromagnetic core included in the other of said vibration parts, means for operably connecting the first and second vibration parts to permit relative motion there between, said means including at least one non-linear, bellows plate spring, and electrical power means for supplying electrical current to the electromagnetic course for electromag­ netically inducing movement of the armature within the core in opposition to a non-linear restoring spring force of the connecting means whereby a resonant, non-linear electromagnetic vibration may be induced between the first and second vibra­ tion parts; and a first compression cylinder including a piston received therein for reciprocating motion, the piston being operably connected to one of the first and second vibration parts, and the cylinder being operably connected to the other of the first and second vibration parts, whereby relative oscillating motion of the first and second vibration parts induced via action of the connecting means is converted to reciprocating piston motion in the first compression cylinder.

Inventors: CAO, PEI SHENG
Applicants: SHANGHAI NEW MECHANICAL TECHNOLOGY DEVELOPMENT CENTRE
Application year: 1986
Main classification: H02K33
IPC codes: F04B17, H02K33