Abstract:
A linear oscillator includes a reciprocating moving part, a case to contain the moving part, and an amplitude control spindle moveably supported in the case. The moving part and the amplitude control spindle reciprocate at a frequency approximately equal to the resonance frequency of the linear oscillator.

Description:
BACKGROUND OF THE INVENTION  
         [0001]    1. Field of the Invention  
           [0002]    The invention relates to a linear oscillator in which a moving part thereof reciprocates.  
           [0003]    2. Description of the Related Art  
           [0004]    There has been employed such a linear oscillator using a motion direction converting mechanism to convert a motor revolutionary motion into a reciprocating linear motion that can be used in a driving part for use in mechanical control or of an electric razor or a power tooth brush.  
           [0005]    In this case, however, there would rise various problems due to a mechanical loss or noise occurring at the motion direction converting mechanism and a difficulty in miniaturization.  
           [0006]    Besides the above, there has been known such a linear oscillator that uses no motion direction converting mechanism to reciprocate the moving part to axially by use of an electromagnetic force as well as by use of a resonance frequency determined by a spring force of a spring member having the moving part as a spring oscillation system and a mass of the moving part, however this causes high vibration because of inertia force of the moving part.  
         SUMMARY OF THE INVENTION  
         [0007]    In view of the above, it is an object of the invention to provide a linear oscillator that gives a low vibration and small noise and can be miniaturized.  
           [0008]    Thus, an aspect of Claim  1  is a linear oscillator comprising a moving part moving reciprocally, a case containing the moving part, and an amplitude control spindle supported in the case to be movable, in which the moving part and the vibration control spindle reciprocate at a resonance frequency or in its vicinity. The amplitude control spindle is thus provided to conduct control so as to absorb or increase an amplitude due to a reaction of the moving part when it is reciprocating.  
           [0009]    An aspect of Claim  2  is the linear oscillator according to Claim  1  comprising an electromagnetic driving part reciprocating the moving part and a spring member making up a spring oscillation system disposed at least between the case and the moving part and between the case and the amplitude control spindle, in which a resonance frequency of the spring oscillation system is equal to that of the linear oscillator and in its vicinity.  
           [0010]    An aspect of Claim  3  is the linear oscillator according to Claim  1 , in which the moving part and the amplitude control spindle moves in phases opposite to each other and reciprocate at a resonance frequency.  
           [0011]    An aspect of Claim  4  is the linear oscillator according to Claim  2 , in which the spring member includes a first spring disposed between a fixed part including the case and the electromagnetic driving part and the moving part, a second spring disposed between the moving part and the amplitude control spindle, and a third spring disposed between the amplitude control spindle and the fixed part.  
           [0012]    An aspect of Claim  5  is the linear oscillator according to Claim  1 , wherein the electromagnetic driving part includes a coil, to use its coil current in order to enable controlling the reciprocating motion.  
           [0013]    An aspect of Claim  6  is the linear oscillator according to Claim  5 , in which the electromagnetic driving part includes a coil surrounding an outer periphery of the moving part, second yokes disposed at both ends of the coil, a pair of permanent magnets which are provided at an end face of each of the second yokes and also which are magnetized symmetrically with respect to the center of the coil, and first yokes provided on the sides of the permanent magnets opposite to the second yokes.  
           [0014]    An aspect of Claim  7  is the linear oscillator according to Claim  1 , in which a shaft for taking out a motion output is connected as a connection element to the moving part or the amplitude control spindle.  
           [0015]    An aspect of Claim  8  is the linear oscillator according to Claim  4 , in which the second spring is stronger than the first and third springs.  
           [0016]    An aspect of Claim  9  is the linear oscillator according to Claim  1 , in which the amplitude control spindle is provided with a rocking preventing means for preventing rocking.  
           [0017]    An aspect of Claim  10  is the linear oscillator according to Claim  2 , in which the spring member is formed of a coil spring and the mass of the amplitude control spindle and its connection element is larger than the mass of the moving part and its connection element.  
           [0018]    An aspect of Claim  11  is the linear oscillator according to Claim  2 , in which the spring member is formed of a leaf spring and the mass of the amplitude control spindle and its connection element is smaller than the mass of the moving part and its connection element.  
           [0019]    An aspect of Claim  12  is the linear oscillator according to Claim  6 , in which at least a portion facing the electromagnetic driving part in the case is formed of an electromagnetic substance and the thickness of the portion facing the electromagnetic driving part is 7% or larger of an outer diameter of the permanent magnet.  
           [0020]    An aspect of Claim  13  is the linear oscillator according to Claim  6 , in which a magnetic flux increasing means is provided which increases magnetic flux running toward the moving part.  
           [0021]    An aspect of Claim  14  is the linear oscillator according to Claim  6 , in which a first yoke has a triangular cross section which has its sloped side facing the case.  
           [0022]    An aspect of Claim  15  is the linear oscillator according to Claim  7 , in which part or the whole of the shaft is made of a nonmagnetic substance.  
           [0023]    An aspect of Claim  16  is the linear oscillator according to Claim  15 , in which only a portion of the moving part passing through the shaft is made of a nonmagnetic substance.  
           [0024]    An aspect of Claim  17  is the linear oscillator according to Claim  6 , in which the yoke or the moving part is provided with an eddy current loss reducing means for reducing an eddy current loss.  
           [0025]    An aspect of Claim  18  is the linear oscillator according to Claim  17 , in which the moving part has an amplitude-directional slit formed therein.  
           [0026]    An aspect of Claim  19  is the linear oscillator according to Claim  6 , in which the moving part has a large diameter portion at its both ends in its reciprocating direction and a small diameter portion at its center in such a configuration that a boundary between the large diameter and small diameter portions roughly agrees with the end faces of the second yokes on the side of the coil and both end faces of the moving part in its reciprocating direction roughly agree with the end faces of the permanent magnets on the sides of the first yokes respectively.  
           [0027]    An aspect of Claim  20  is the linear oscillator according to Claim  6 , in which a gap between the outer circumferential surface of the moving part and the inner circumferential surface of the yoke is non-uniform in an revolutionary direction.  
           [0028]    An aspect of Claim  21  is the linear oscillator according to Claim  7 , comprising a revolution restricting means for restricting revolution of the shaft.  
           [0029]    An aspect of Claim  22  is the linear oscillator according to Claim  21 , in which the spring member acts as the revolution restricting means. 
       
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0030]    [0030]FIG. 1 is a cross-sectional view of one embodiment of the invention;  
         [0031]    [0031]FIG. 2 shows a model of the embodiment;  
         [0032]    [0032]FIG. 3 is a cross-sectional view of another embodiment of the invention;  
         [0033]    [0033]FIG. 4 is a cross-sectional view of further embodiment of the invention;  
         [0034]    [0034]FIG. 5 is a cross-sectional view of still further embodiment of the invention;  
         [0035]    [0035]FIG. 6 is a cross-sectional view of an additional embodiment of the invention;  
         [0036]    [0036]FIG. 7 is a cross-sectional view of an additional embodiment of the invention;  
         [0037]    [0037]FIG. 8 is a cross-sectional view of an additional embodiment of the invention;  
         [0038]    [0038]FIG. 9 is a cross-sectional view of an additional embodiment of the invention;  
         [0039]    [0039]FIG. 10 is a cross-sectional view of an additional embodiment of the invention;  
         [0040]    [0040]FIG. 11 is a cross-sectional view of an additional embodiment of the invention;  
         [0041]    [0041]FIG. 12 is a cross-sectional view of an additional embodiment of the invention;  
         [0042]    [0042]FIG. 13 is a perspective view of the plunger of the above embodiment;  
         [0043]    [0043]FIG. 14 is a cross-sectional view of an additional embodiment of the invention;  
         [0044]    [0044]FIG. 15 is a cross-sectional view of an additional embodiment of the invention;  
         [0045]    [0045]FIG. 16A is a cross-sectional view taken along line A of FIG. 15, FIG. 16B is that taken along line B of FIG. 15, and FIG. 16C is that taken along line C of FIG. 15;  
         [0046]    [0046]FIG. 17 is a cross-sectional view of an additional embodiment of the invention;  
         [0047]    [0047]FIG. 18 is a cross-sectional view of an additional embodiment of the invention;  
         [0048]    [0048]FIG. 19 is a cross-sectional view of an additional embodiment of the invention;  
         [0049]    [0049]FIG. 20 is a cross-sectional view of an additional embodiment of the invention;  
         [0050]    [0050]FIG. 21A is a cross-sectional view of an additional embodiment and FIG. 21B, a partial end elevation thereof; and  
         [0051]    [0051]FIG. 22 is a cross-sectional view of an additional embodiment. 
     
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS  
       [0052]    [0052]FIG. 1 shows one embodiment of the invention, in which a cylindrical plunger  1  made of a magnetic substance such as iron constituting the moving part housed in the case has a large diameter at its both ends and a small diameter at its center in such a configuration that through the plunger  1 , an output-take-out shaft  7  is pierced and fixed therein as a connection element and on the periphery of the plunger  1  is provided a coil  5 . At both axial ends of the above-mentioned annular coil  5  fixed on the inner surface of a shield case  10  acting as the case are provided annular permanent magnets  40  and  41  magnetized symmetrically with respect to the coil  5 , so that between the magnets  40  and  41  and the coil  5  are provided annular second yokes  30  and  31 , and on the sides of the magnets  40  and  41  opposite to the yokes  30  and  31  are provided annular first yokes  20  and  21  respectively. Those coil  5 , permanent magnets  40  and  41 , and yokes  30 ,  31 ,  20 , and  21  are combined to make up an electromagnetic driving part. Between one end face of the above-mentioned plunger  7  and the shield case  10  is provided a spring  60 , while between the other end face of the plunger  7  and the shield case  10  are provided a spring  61 , an amplitude control spindle  9 , and a spring  62  in this order. A spring member (springs  60 ,  61 , and  62 ) is provided as a spring oscillation system for energizing the moving part axially, supporting the amplitude control spindle to the case to be movable. The plunger and the amplitude control spindle reciprocate at a resonance frequency of the spring oscillation system. This resonance frequency is equal (or vicinal) to that of the linear oscillator. Although the spring member (springs  60 ,  61 , and  62 ) employs a coil spring easy to obtain a relatively large amplitude, any other appropriate springs may be used.  
         [0053]    When the coil  5  has no current flowing therethrough, the plunger  1  stands still at a shown position where a magnetic force which the permanent magnets  40  and  41  have on the plunger  1  via the yokes  20 ,  30 ,  21 , and  31  is balanced with a spring force of the springs  60 ,  61 , and  62 . When the coil  5  has a current flowing in one direction therethrough, the magnetic flux of either one of the two permanent magnets  40  and  41  is weakened and so the plunger moves toward the other magnet as against the force of the spring  60 , and when the coil  5  has a current flowing in the opposite direction therethrough, on the other hand, the plunger  1  still moves in the opposite direction, so that by flowing an alternating current through the coil  5 , the plunger  1  reciprocates axially, thus enabling controlling of the reciprocating motion by a coil current.  
         [0054]    If, in this case, attention is paid to the axial motion of such moving parts as the plunger  1 , the shaft  7 , and the amplitude control spindle  9 , it is known that there are provided the above-mentioned springs  60 ,  61 , and  62  made up of a coil spring to permit this linear oscillator to be handled as such a three-mass-point system oscillation modes as shown in FIG. 2, so that if it is assumed that the electromagnetic driving part having the coil  5  as the main body and the shield case  10  act as the fixed part and that m 1  represents mass of the moving part, m 2  represents mass of the vibration control spindle, m 3  represents mass of the fixed part, k 1  represents a spring coefficient of the spring  60 , k 2  represents a spring coefficient of the spring  61 , k 3  represents a spring coefficient of the spring  62 , c 1  represents an attenuation coefficient of the spring  60 , c 2  represents an attenuation coefficient of the spring  61 , and c 3  represents an attenuation coefficient of the spring  62 , the motions at the time of free oscillation of those three mass points of the above-mentioned oscillation system can be determined by motion equations (1), (2), and (3) and also, if values of m 1 =m 2 , k 1 =k 3 , c 1 =c 3 , and m 3  is sufficiently large as compared to m 1  and m 2 , equations (4) and (5) can be solved by solving the above-mentioned equations, where the attenuation term is omitted in the equations (4) and (5).  
                 m1        x   ¨        1     +     c1        (         x   .        1     -       x   .        3       )       +     c2        (         x   .        1     -       x   .        2       )       +     k1        (     x1   -   x3     )       +     k2        (     x1   -   x2     )         =   0           (   1   )                   m2        x   ¨        2     +     c2        (         x   .        2     -       x   .        1       )       +     c3        (         x   .        2     -       x   .        3       )       +     k2        (     x2   -   x1     )       +     k3        (     x2   -   x3     )         =   0           (   2   )                   m3        x   ¨        3     +     c1        (         x   .        3     -       x   .        1       )       +     c3        (         x   .        3     -       x   .        2       )       +     k1        (     x3   -   x1     )       +     k3        (     x3   -   x2     )         =   0           (   3   )               f1   =       1     2      π              k1   m1                 (   4   )               f2   =       1     2      π                k1   +     2      k2       m1                 (   5   )                               
 
         [0055]    Frequencies f 1  and f 2  thus obtained as two solutions are each a resonance frequency and, therefore, in an oscillation mode of the resonance frequency f 1  of the primary side (lower order side) of Equation (4) the moving part and the amplitude oscillation spindle  9  move in a same phase and in an oscillation mode of the resonance frequency f 2  of the secondary side (higher order side) of Equation (5) the moving part and the amplitude control spindle  9  move in phases opposite to each other; so that when the moving part is reciprocated axially by flowing through the coil  5  a current having a frequency in the vicinity of this secondary side resonance frequency f 2 , the amplitude control spindle  9  moving in the opposite phase cancels inertia force of the moving part, which in turn cancels an inertia force of the amplitude control spindle  9 . In this state, further, the two mass points of the moving part and the amplitude control spindle  9  would move so as to balance their respective inertia forces to thereby give a great effects of canceling the inertia forces by means of the counteraction, thus minimizing the force transmitted from these two mass points (the moving part and the amplitude control spindle  9 ) to the fixed part side hence the amplitude of the linear oscillator.  
         [0056]    As may be obvious from the above equation (5), to keep the secondary side resonance frequency f 2  at a constant value, it is necessary to set the spring coefficient k 2  of the spring  61  at a large value and the spring coefficients k 1  and k 3  of the springs  60  and  62  at small values. If the spring coefficients k 1  and k 3  of the springs  60  and  62  respectively are thus set smaller, the amplitude control spindle  9  receives a less force from the fixed part, resulting in a larger stroke of the moving part.  
         [0057]    Also, the mass of the amplitude control spindle  9  should preferably be larger than that of the moving part. This is because, when they move in the vicinity of the secondary side resonance frequency f 2 , the two mass points of the moving part and the amplitude control spindle  9  would move so as to balance their inertia forces, so that the moving part having smaller mass obtains a larger oscillation amplitude than the amplitude control spindle  9  having larger mass, thus making it possible to increase the stroke of the moving part. If they move at the lower order side resonance frequency, on the other hand, the amplitude control spindle and the moving part move in the same direction, thus making it possible to increase the amplitude of the moving part. Also, if it is possible to move them at alternating frequencies of the lower order and higher order sides, a stroke increase and an amplitude increase can be switched according to the application.  
         [0058]    [0058]FIG. 3 shows another embodiment. In this embodiment, the springs  60 ,  61 , and  62  are all made of a leaf spring. In this case, the mass of the amplitude control spindle  9  should preferably be made smaller than that of the moving part. By thus employing a leaf spring, not only the mass of the spring as a standalone element can be made lighter easily but also its whole length can be decreased easily, besides which the mass of the amplitude control spindle  9  can be made smaller than that of the moving part, thus realizing a linear oscillator light-weighted as a whole with an extremely small amplitude.  
         [0059]    [0059]FIG. 4 is further embodiment according to Claim  7 , in which as the connection element the output-take-out shaft  7  is provided not to the plunger  1  but to the amplitude control spindle  9 . In this case also, almost the same motions can be obtained as those of the above-mentioned linear oscillator and, besides, it is possible to dispose opposite to that shown in FIG. 1 the position of the magnetic circuit portion including such as the permanent magnet  5 , which is usually supposed to have a large mass, thus enhancing the gravity position in height of the equipment as a whole and the freedom degree in product designing of, e.g., a distance with respect to the power supply. Also, the light-weighting of the amplitude control spindle  9  directly leads to the increasing of the linear oscillator stroke, so that these two merits can be united easily and, further, a member to be attached to the output-take-out shaft  7  can be designed as part of a mass component of the amplitude control spindle  9 , to decrease the initial mass of the amplitude control spindle  9  by that much, thus obtaining a more light-weighted and less vibrated linear oscillator.  
         [0060]    [0060]FIG. 5 shows a still further embodiment according to Claim  12 , in which the thickness of the shield case  10  formed of a magnetic substance is 7% or more of that of an outer diameter of the permanent magnets  40  and  41  and there is formed an air gap between the inner surface of the shield case  10  and the outer surface of the permanent magnets  40  and  41  and also the yokes  20 ,  21 ,  30 , and  31  to thereby give a sufficient shielding effect, thus obtaining a linear oscillator having no influence on a pace maker etc. In such a case, the shielding effect is improved when at least a portion of a case such as the shield case  10  which faces the electromagnetic part is formed of a magnetic substance and has a thickness of 7% or more of the outer diameter of the permanent magnet.  
         [0061]    [0061]FIG. 6 shows an additional embodiment according to Claims  13  and  14 , in which the yokes  20  and  21  have a triangular cross section so that their surfaces facing the shield case  10  may be a slope. The yokes  20  and  21  and the shield case  10  can be separated from each other to thereby decrease the quantity of magnetic flux running toward the shield case  10 , thus improving the driving thrust of the plunger  1 , which is the moving part.  
         [0062]    As shown in FIG. 7, almost the same effects as above can be obtained even when the outer diameter of the yokes  20  and  21  is made smaller than that of the permanent magnet  5  to thereby give a space with respect to the shield case  10 . In this case, as shown in FIG. 8, the yokes  20  and  21  can be provided with a thin layer made of a magnetic substance covering the permanent magnet  5  entirely to thereby suppress the demagnetizing effect of the permanent magnets  40  and  41 .  
         [0063]    Besides, as shown in FIG. 9, the permanent magnets  40  and  41  can be formed frusto-conical to thereby increase the quantity of magnetic flux running toward the movable plunger  1 , which contributes to the thrust.  
         [0064]    [0064]FIG. 10 shows an additional embodiment according to Claim  15 , in which the shaft  7  passing through the movable plunger  1  is made of a nonmagnetic substance. This leads to an improvement in the thrust and also prevents the leakage of magnetic flux through the shaft  7 .  
         [0065]    [0065]FIG. 11 shows an additional embodiment according to Claims  15  and  16 , in which a portion of the shaft  7  which passes through the movable plunger  1  is made of a nonmagnetic substance. A portion of the plunger  1  which is exposed to the outside is made of a highly wear resistant metal material and a portion which is pressed into the plunger  1  is made of a nonmagnetic substance to thereby enable improving the thrust without deteriorating the wear resistance.  
         [0066]    [0066]FIG. 12 shows an additional embodiment according to Claim  17 , in which the yokes  20 ,  21 ,  30 , and  31  are formed into a stack structure made of a thin sheet to thereby decrease an eddy current loss. The eddy current loss can thus be reduced and its effects increase with the increasing operating frequency. Almost the same effects can be obtained by forming the movable plunger  1  into a stacked structure. Such a structure can be formed also by blanking the material to thereby reduce the manufacturing costs.  
         [0067]    [0067]FIG. 13 shows an additional embodiment according to Claim  18 , in which to reduce the eddy current loss, the movable plunger  1  has a plurality of slits  11  formed therein in the amplitude direction. Those slits  11  can greatly decrease the magnitude of an eddy current when it flows in the axial direction of the plunger  1 , which is the main direction in which the magnetic flux runs. In this case also, the plunger  1  can be formed into a stacked structure made of a magnetic substance to thereby mitigate the difficulty in processing and increase the demagnetizing effect due to the iron loss.  
         [0068]    [0068]FIG. 14 shows an additional embodiment according to Claim  19 , in which when the plunger  1  (moving part) having a large diameter portion at both ends, in its reciprocating direction, and a small diameter portion at its center is present at a neutral position, the boundary between the large diameter and small diameter portions roughly agrees with the end face of the yoke  30  and  31  on the side of the coil  5  and both axial end faces of the plunger  1  roughly agree with the end faces of the permanent magnets  40  and  41  on the sides of the yokes  20  and  21  respectively. A detent force roughly at the neutral position can be reduced to almost zero and so can be ignored in the designing of a relevant resonance system taking into account only the spring coefficient of the spring member, thus facilitating the designing.  
         [0069]    [0069]FIGS. 15 and 16 show an additional embodiment according to Claim  20 , in which the air gap between the outer peripheral surface of the movable plunger  1  and the inner peripheral surface of the yokes  20  and  21  is made non-uniform in a revolution direction. FIG. 16A shows a positional relationship between the plunger and the yoke in a cross-sectional view taken along a line A of FIG. 15, FIG. 16B shows that in a cross-sectional view taken along a line B of FIG. 15, and FIG. 16C shows that in a cross-sectional view taken along a line C of FIG. 15. Since the gap between the plunger  1  and the yokes  20  and  21  changes in revolution direction with changing stroke positions, the plunger  1  can have a revolution directional force with axial movements thereof, thus obtaining a rectilinear motion as well as a revolutionary motion simultaneously.  
         [0070]    [0070]FIG. 17 shows an additional embodiment according to Claim  9 , in which the shield case  10  has on its inner surface a guide (rocking preventing means)  15  for preventing the amplitude control spindle  9  from rocking. In this embodiment the spring member is formed of a coil spring and so the amplitude control spindle  9  may not carry out an ideal rectilinear motion because of a problem of a stress balance and may rock, in which case the amplitude control effect such as vibration absorption cannot sufficiently be obtained, which rocking of the amplitude control spindle  9  can be prevented by the guide  15  to thereby permit the amplitude control spindle  9  to move ideally.  
         [0071]    As shown in FIG. 18, the rocking of the amplitude control spindle  9  can be prevented also by providing the two or more spring  62  disposed between the amplitude control spindle  9  and the shield case  10 .  
         [0072]    Also, as shown in FIG. 19, the rocking may be prevented by providing sliding bearings  80  and  81  facing the shaft  7  in the amplitude control spindle  9 . A leaf spring, if used to form the spring member, would absorb the rocking, so that as shown in FIG. 20, the springs  61 ,  62  of the spring member which have one end thereof fixed to the amplitude control spindle  9  may be formed of the leaf spring to effectively prevent the rocking.  
         [0073]    [0073]FIG. 21 shows an additional embodiment according to Claim  21 , in which a groove  70  formed in the shaft  7  is engaged with a protrusion provided on the shield case  10  to thereby restrict the axial revolution of the shaft  7  and the plunger  1  around that shaft (to provide a revolution restricting means). This mechanism can suppress unnecessary axial revolutions.  
         [0074]    [0074]FIG. 22 shows an additional embodiment according to Claim  22 , in which one end of the spring  60  formed of a coil spring is fixed to the shield case  10  and the other end thereof, to the plunger  1 . In this case, the spring  60  formed of a coil spring not only exerts a spring force in the axial direction of the plunger  1  but also provides the plunger  1  with a small-angle reciprocating revolution in the axial direction with axial compression and expansion. In this case, the spring  60  has a spring force also in the revolution direction, thus being able to give also a secured revolutionary motion by matching a revolutionary directional resonance frequency.  
         [0075]    As described above, according to the invention claimed here, it is possible to directly convert electric energy into a rectilinear reciprocating motion of the plunger without a motion converting mechanism for converting a revolutionary motion into a rectilinear motion and also cancel an unnecessary vibration using the amplitude control spindle in order to obtain a miniaturized linear oscillator with low noise and extremely low vibration, which is well suited for use as a driving part for mechanical control use or a driving part of an electric razor or a power tooth brush.  
         [0076]    According to Claim  8 , besides the above-mentioned effects of the invention, it is possible to increase the stroke of the moving part.  
         [0077]    According to Claim  9 , besides the above-mentioned effects of the invention, it is possible to suppress the rocking of the amplitude control spindle to thereby permit the amplitude control spindle to carry out in an ideal rectilinear motion, thus obtaining a sufficient vibration reducing effect.  
         [0078]    According to Claim  10 , besides the above-mentioned effects of the invention, it is possible to increase a stroke of the moving part.  
         [0079]    According to Claim  11 , besides the above-mentioned effects of the invention, it is possible to obtain a light-weighted and easy-to-use linear oscillator.  
         [0080]    According to Claim  12 , besides the above-mentioned effects of the invention, it is possible to obtain such a linear oscillator that has an improved magnetizing effect and has a magnetic leakage level low enough to have no influence on a pace maker etc.  
         [0081]    According to Claim  13 , besides the above-mentioned effects of the invention, it is possible to improve the thrust.  
         [0082]    According to Claim  14 , besides the above-mentioned effects of the invention, it is possible to further improve the thrust.  
         [0083]    According to Claim  15 , besides the above-mentioned effects of the invention, it is possible to improve the thrust and prevent magnetic flux leakage.  
         [0084]    According to Claim  16 , besides the effects of Claim  15  above, it is possible to improve the thrust without deteriorating a wear resistance.  
         [0085]    According to Claim  17 , besides the above-mentioned effects of the invention, it is possible to decrease an eddy current loss.  
         [0086]    According to Claim  18 , besides the effects of Claim  17  above, it is possible to greatly decrease an eddy current using slits when magnetic flux runs in a direction in which the moving part moves.  
         [0087]    According to Claim  19 , besides the above-mentioned effects of the invention, it is possible to reduce a detent force almost to zero at the neutral position to thereby facilitate, e.g. designing of a resonance system.  
         [0088]    According to Claim  20 , besides the above-mentioned effects of the invention, it is possible to generate a revolutionary directional force according to a stroke position to thereby carry out a rectilinear motion and a revolutionary motion simultaneously.  
         [0089]    According to Claim  21 , besides the above-mentioned effects of the invention, it is possible to restrict the revolution of the shaft to thereby suppress unnecessary revolution of the shaft.  
         [0090]    According to Claim  22 , besides the effects of Claim  21  above, it is possible to restrict revolution without any other member.  
         [0091]    Explanation of Reference Numerals  
         [0092]    [0092] 1  plunger,  
         [0093]    [0093] 5  coil,  
         [0094]    [0094] 7  shaft,  
         [0095]    [0095] 9  amplitude control spindle, and  
         [0096]    [0096] 10  shield case.