Patent Document

[0001]    The invention relates to an electromagnetic actuator having permanent magnets arranged in the form of a V in an electromagnetically optimized arrangement. 
       BACKGROUND OF THE INVENTION 
       [0002]    Document FR 2 865 238 discloses an electromagnetic actuator having an actuating member associated with an armature that can move under the action of an electromagnet, comprising a coil and a core suitable for channeling the flux of the coil so as to form a return path in the armature, the core having a base from which branches extend, including a central branch around which the coil extends. The electromagnet comprises two permanent magnets which are incorporated into the core in such a way that the latter channels the flux of the permanent magnets so as to form a return path in the armature, the flux of the coil passing through the magnets. In one of the embodiments illustrated in that document, the permanent magnets are placed obliquely in the lateral branches of the core, thereby making it possible to house, in the core, magnets having a length substantially equal to the height of the coil without correspondingly increasing the height of the electromagnet. 
         [0003]    However, such an arrangement means that the laminations of the core have to be cut so as to allow the magnets to be inserted, thereby mechanically weakening the laminations and posing assembly problems. Furthermore, it is necessary to leave connecting portions behind on the laminations in order to keep the cut parts of the laminations together, the linking portions thus forming as many short circuits, which are saturated by the flux of the neighboring magnet. 
       SUBJECT OF THE INVENTION 
       [0004]    The subject of the invention is an electromagnetic actuator having oblique magnets that has a higher electromagnetic efficiency. 
       BRIEF DESCRIPTION OF THE INVENTION 
       [0005]    To achieve this objective, the invention provides an electromagnetic actuator, having an actuating member associated with an armature and capable of moving under the action of at least one electromagnet, which comprises: a coil; a core designed to channel the flux of the coil so as to form a return path in the armature, the core having a base from which branches extend, including a central branch around which the coil extends; and two permanent magnets which, are associated with the core so that the latter channels the flux of the permanent magnets so as to form a return path in the armature, the flux of the coil passing through the magnets. According to the invention, the two permanent magnets are placed in the central branch of the core so as to form a V, which separates the central branch into a support part, which supports the permanent magnets and is integral with the base, and an end part lying above the permanent magnets, so that any section of the core or of the armature through which the flux of one or other of the permanent magnets can pass has an area large enough to avoid saturation of said section by this flux. 
         [0006]    Thus, the core is separated into a main part, incorporating the part for supporting the magnets, the access to which, for positioning the permanent magnets, is completely free, and an end part, which is attached to the magnets placed on the support part so as to lie above them, the end part being centered by itself on the V formed by the permanent magnets and having no contact with the support part so that the risk of a short circuit between the support part and the end part is very low. 
         [0007]    The sufficient area of the sections of the core or of the armature furthermore avoids any saturation by the flux of the permanent magnets, thereby helping to optimize the electromagnetic efficiency of the actuator. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0008]    The invention will be more clearly understood in the light of the following description with reference to the figures of the appended drawings in which: 
           [0009]      FIG. 1  is a partial schematic sectional view of an actuator according to the invention; 
           [0010]      FIG. 2  is a partial schematic view of the actuator of  FIG. 1 , illustrated in the course of being mounted; and 
           [0011]      FIG. 3  is a partial schematic sectional view of an actuator according to the invention. 
       
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
       [0012]    As shown in  FIG. 1 , the electromagnetic actuator of the invention comprises an electromagnet  1  with a core  2  and a coil  3 . The electromagnet  1  exerts an electromagnetic force in a controlled manner on an armature  4  integral with a pushrod  5  that can move along the X axis. 
         [0013]    Such an actuator is, for example, used to actuate an internal combustion engine valve, the actuator being placed in such a way that the pushrod  5  extends along the sliding axis of the valve. As is known, the actuator includes another electromagnet (not shown) that extends opposite the electromagnet  1  so as to selectively attract the armature  4  in the opposite direction. The end of the pushrod  5  and the end of the valve are returned to each other by opposing springs (not shown) that define an equilibrium position of the pushrod/valve assembly in which the armature extends substantially at mid-path between the two electromagnets. 
         [0014]    The core  2  of the electromagnet  1  has a base  10  from which two lateral branches  11  and a central branch extend, the coil  3  extending around said central branch. The central branch comprises two portions  12  with facing inclined faces integral with the base  10 . 
         [0015]    The portions  12  form a support part, for supporting the core  2 , said part being designed to accommodate permanent magnets  13  so that the latter extend obliquely to the X axis and form a V, the point of which here is turned toward the base  10 . A wedge  14  forming an end part of the central branch is thus formed in the V. 
         [0016]    The path of the flux lines generated by the permanent magnets  13 , which pass through the core  2  so as to form a return path in the armature  4 , is depicted as the bold dashed lines in  FIG. 1 . The wedge  14  has an end face  15  in which a groove  17  lies parallel to the permanent magnets  13 . The groove  17  ensures that there is a sharp separation between the respective flux lines of the two permanent magnets  13  that pass on either side of the groove  17 . 
         [0017]    As may be seen in  FIG. 2  (in which the core is illustrated upside-down with respect to  FIG. 1 ), the actuator is mounted as follows. After having formed the core  2  by assembling the laminations that form the base  10 , the lateral branches  11  and the support portions  12 , the permanent magnets  13  are put into position on the support portions  12 . In this regard, the support portions  12  include steps  50  making it easier to position the magnets  13 . After having formed the wedge  14 , by assembling the corresponding laminations, the wedge  14  is then attached to the permanent magnets  13  as indicated by the arrow. The wedge  14  then lies above the permanent magnets  13  and is self-centered by the V formed by the permanent magnets  13 . 
         [0018]    To keep the whole assembly in place, nonmagnetic clamps  18  are used, each of these having, on the one hand, an elongate part (visible in cross section in  FIG. 1 ) that is housed in the groove  17  of the active face  15  of the wedge  14 , and on the other hand, braces that extend into holes passing through the wedge  14 , then between the permanent magnets  13  and finally in holes in the core  2  (these not being visible) so as to be fastened to the latter, for example by screwing or by riveting (as a variant, the braces could pass through the core  2  so as to be fixed directly to the body  100 ). 
         [0019]    The clamps make it possible to exert a compressive force so as to take up, or even eliminate, the residual gap that may remain owing to the manufacturing tolerances between, on the one hand, the support portions  12  and the permanent magnets  13  and on the other hand, the permanent magnets  13  and the wedge  14 . This gap take-up allows the magnetic efficiency of the actuator to increase. 
         [0020]    As may be seen in  FIG. 3 , the geometry of the core  2  imposes on the central branch of the latter critical passage sections for the flux lines of the permanent magnets  13 . First critical sections S 1  extend in the wedge  14  between one of the ends of the permanent magnets  13  and the central axis X. Second critical sections S 2  each extend in one of the bearing portions between one of the ends of the corresponding permanent magnets  13  and the angle formed by the base  10  and the bearing portion  12 . Finally, third critical sections S 3  extend in the wedge  14  between an external face and the groove  17 . 
         [0021]    Each of these critical sections S 1 , S 2 , S 3  has a minimum area through which the entire flux of one of the permanent magnets  13  passes. 
         [0022]    Moreover, the armature  4  also has fourth critical sections S 4  through which the entire flux of one or other of the permanent magnets  13  passes. 
         [0023]    It is known that the constituent ferromagnetic material of the core  2  and of the armature  4  has a saturation threshold above which it becomes increasingly difficult to make additional flux pass through a given passage section. It is important, when in only the flux generated by the permanent magnets  13 , for the constituent material of the core  2  and of the armature to work, in the critical sections S 1 , S 2 , S 3 , S 4 , below the saturation threshold so as to retain the possibility of the flux generated by the coil passing through them and thus providing said coil with an acceptable efficiency. To do this, the critical sections S 1 , S 2 , S 3 , S 4  should have sufficiently large areas. 
         [0024]    The width of the core  2  in the sections S 1 , S 2 , S 3 , is called d 1 , d 2 , d 3  respectively. If L is the length of the core (measured along a direction perpendicular to the plane of the figure), the critical sections S 1 , S 2 , S 3  have respective areas: 
         [0000]        A 1 =L×d 1 ; A 2 =L×d 2; and  A 3 =L×d 3. 
         [0025]    Likewise if d 4  is the width of the armature in the section S 4  and if the length of the armature is taken to be approximately L, the area of the section S 4  is A 4 =L×d 4 . 
         [0026]    As regards the flux of the permanent magnets  13  this is approximately proportional to the area of the surface of the permanent magnets in contact with the core. If H is the height of the permanent magnets, this area is 
         [0000]    
       
      
       A=L×H.  
      
     
         [0027]    To avoid the critical sections being saturated, it is necessary to given an upper limit to the ratio of the flux to the area of the critical section in question, and therefore to limit the ratios: 
         [0000]        r 1 =A/A 1 ; r 2 =A/A 2 ; r 3 =A/A 3; and  r 4 =A/A 4. 
         [0028]    The upper limit of these ratios depends on the nature of the constituent material of the core  2  and of the armature  4 . The upper limit of the ratios r 1 , r 2 , r 3 , r 4  is preferably equal to:
       3.2 for a core or armature made of silicon-iron;   3.75 for a core or armature made of 17/18% cobalt-iron; and   4.15 for a core or armature made of 48/50% cobalt-iron.       
 
         [0032]    Since the length L comes into the expressions for the areas A, A 1 , A 2 , A 3  and A 4  it should be noted that these ratios may also be expressed as r 1 =H/d 1 , r 2 =H/d 2 , r 3 =H/d 3  and r 4 =H/d 4  so that the ratios represent length ratios. 
         [0033]    As may be seen in  FIG. 3 , the core  2  illustrated here is such that the wedge  14  terminates in a point approximately at those ends of the permanent magnets  13  which are opposite the ends where the sections S 1  are taken in the wedge  14 . Likewise, the bearing portions  12  terminate in a point at those ends of the permanent magnets  13  which are opposite the ends where the sections S 2  are taken in the bearing portions  12 . In this configuration, the tangent of the half-angle φ of the V formed by the permanent magnets  13  is approximately equal to d 2 /H or d 1 /H, i.e. the inverse of the ratios r 1  and r 2 . 
         [0034]    This therefore amounts to giving the ratios r 1  and r 2  an upper limit or to giving the half-angle φ at the apex of the V a lower limit. The lower limit of the half-angle φ of the apex of the V is preferably equal to:
       17° for a core made of silicon-iron;   13.5° for a core made of 17/18% cobalt-iron; and   12° for a core made of 48/50% cobalt-iron.       
 
         [0038]    These values make it possible to prevent saturation in the critical sections under just the flux of the permanent magnets  13 . In any event, the half-angle φ at the apex of the V will be chosen to be equal to or greater than 10°. 
         [0039]    However, the ratios r 1 , r 2 , r 3 , r 4  should not be too small as otherwise this would lead to excessively large passage sections limiting the efficiency of the permanent magnets  13 . In practice, the ratios r 1 , r 2 , r 3 , r 4  are preferably chosen to be equal to or greater than 2. In terms of angle, this condition amounts to limiting the half-angle φ of the V to a value equal to or less than 25°. 
         [0040]    The invention is not limited to what has just been described, rather quite to the contrary it encompasses any variant falling within the scope defined by the claims. 
         [0041]    In particular, although actuators have been illustrated here in which the permanent magnets form a V, the tip of which is turned toward the base of the core, it will also be possible to place the magnets in such a way that they form a V with the tip directed toward the armature. The magnet support part of the base will have inclined faces no longer facing each other but being turned toward the lateral branches, whereas the end part of the central branch will no longer have a wedge shape but a hat shape. 
         [0042]    Although critical sections have been considered here in the central branch, it is obvious that the limits that apply to the ratios r 1 , r 2 , r 3 , r 4  also apply to any similar ratio associated with any section taken in the rest of the core or of the armature, said ratio then being equal to the area of the surface of the permanent magnet to the area of the relevant section.

Technology Category: 5