Abstract:
A claw pole type motor includes first and second claw poles opposed to each other and each including a radial yoke portion having an inner diameter side and an outer diameter side, a plurality of pole portions arranged on the inner diameter side, and axially extended, and an outer peripheral side yoke portion extending on the outer diameter side. A stator core is provided having an inner diameter side, and is formed so as to cause the pole portions of the first claw pole to be meshed with the pole portions of the second claw pole. A rotor is arranged on the inner diameter side of the stator core with a circumferential gap being defined therebetween. In order to provide high efficiency while simplifying manufacturing, the first and second claw poles are formed by compacting of magnetic powder.

Description:
CROSS-REFERENCE TO RELATED APPLICATIONS  
       [0001]     This application is a continuation of U.S. application Ser. No. 11/376,091, filed Mar. 16, 2006, and which said application claims priority from Japanese patent applications JP 2005-079282, filed Mar. 18, 2005 and JP 2006-066882, filed Mar. 13, 2006, the entire contents of which are hereby incorporated by reference. 
     
    
     BACKGROUND OF THE INVENTION  
       [0002]     (1) Field of the Invention  
         [0003]     The present invention relates to a multiple phase claw pole type motor used in the fields of industry, home electric appliances, motor vehicles, and the like, and, more particularly, to a multiple phase claw pole type motor having an improved stator iron core.  
         [0004]     (2) Description of Related Art  
         [0005]     Claw pole type iron cores are attracting attention which are provided in ordinary rotating electric motors for the purpose of improving the rate of use of magnetic fluxes by increasing a winding factor of windings, as disclosed in JP-A-2003-333777 for example.  
         [0006]     In the conventional rotating electric motor having a claw pole type iron core, claw poles of the iron core are formed by laminating a rolled plate and, therefore, can only be obtained in a simple shape. Therefore, the conventional rotating electric motor cannot be obtained as a desirable high-efficiency motor.  
       BRIEF SUMMARY OF THE INVENTION  
       [0007]     An object of the present invention is to provide a multiple phase claw pole type motor with high efficiency having claw poles easily manufacturable.  
         [0008]     To achieve the above object, in a multiple phase claw pole type motor having a plurality of claw poles including a claw portion extending in an axial direction and having a magnetic pole surface facing a rotor in a state of being separated from the rotor by a small gap, a radial yoke portion extending radially outwardly and perpendicularly from this claw portion, and an outer peripheral yoke extending from this radial yoke portion in the same direction as the direction of extension of the claw portion, a stator core formed by alternately placing the claw poles in a circumferential direction so that a distal end of each claw portion faces the radial yoke of an adjacent one of the claw poles and having a stator constructed by sandwiching an annular coil with the adjacent claw poles of this stator iron core, the present invention makes the claw poles formed with a magnetic compact having a DC magnetizing property of its flux density becoming 1.7 teslas when 10000 A/m of magnetic field is applied.  
         [0009]     The claw pole is formed by compacting a magnetic powder as described above. The claw pole can therefore be formed so as to have a complicated shape. Also, a high-efficiency motor can be obtained by using a magnetic compact having a DC B-H curve of its flux density becoming 1.7 teslas when 10000 A/m of magnetic field is applied.  
         [0010]     According to the present invention, as described above, a multiple phase claw pole type high-efficiency motor having claw poles easily manufacturable can be obtained.  
         [0011]     Other objects, features, and advantages of the present invention will become clear from the following description of embodiments of the present invention relating to accompanying drawings. 
     
    
     BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS  
       [0012]      FIG. 1  is an exploded perspective view of a first claw pole and a second claw pole used in a first embodiment of a three-phase claw pole type motor according to the present invention;  
         [0013]      FIG. 2  is a perspective view partly in section of a part of stator iron cores for three phases obtained by assembling the first and second claw poles shown in  FIG. 1 ;  
         [0014]      FIG. 3  is a schematic longitudinal sectional view of the entire three-phase claw pole type motor according to the present invention;  
         [0015]      FIG. 4A  is a sectional view taken along line A-A in  FIG. 3 ;  
         [0016]      FIG. 4B  is a sectional view taken along line B-B in  FIG. 3 ;  
         [0017]      FIG. 4C  is a sectional view taken along line C-C in  FIG. 3 ;  
         [0018]      FIG. 4D  shows the construction of an inductor type rotor;  
         [0019]      FIG. 4E  shows the construction of a rotor having an inductor and magnets;  
         [0020]      FIG. 4F  shows the construction of a salient pole type rotor;  
         [0021]      FIG. 5A  is a diagram showing B-H curves of various iron core materials;  
         [0022]      FIG. 5B  is a diagram showing B-H curves of various iron core materials;  
         [0023]      FIG. 6A  is a diagram showing a mesh model of the iron core and the results of computation on the various iron core materials using three-dimensional magnetic field analysis;  
         [0024]      FIG. 6B  is a diagram showing the results of calculation of output torque of the motor constructed of various iron core materials;  
         [0025]      FIG. 6C  is a diagram showing the relationship between the flux density and the output torque of the motor, constructed of various iron core materials, at 10000 A/m;  
         [0026]      FIG. 6D  is a diagram showing the relationship between the claw pole thickness and the output torque of the motor constructed of an SMC (Soft Magnetic Composite);  
         [0027]      FIG. 6E  is a diagram showing the relationship between the flux density and the output torque of the motor, constructed of various iron core materials, at 10000 A/m;  
         [0028]      FIG. 7A  is a sectional view showing a main flux and a leakage flux in the claw pole;  
         [0029]      FIG. 7B  is developed plan view showing a leakage flux in the claw pole;  
         [0030]      FIG. 8  is a diagram showing the results of computation of the relationship between the shape of the claw portion of the claw pole and the effective value of the linkage flux using three-dimensional magnetic field analysis;  
         [0031]      FIG. 9  is a perspective view partly in section of a second embodiment of the three-phase claw pole type motor according to the present invention;  
         [0032]      FIG. 10  is a sectional view partly in section of a third embodiment of the three-phase claw pole type motor according to the present invention;  
         [0033]      FIG. 11  is a perspective view partly in section of a fourth embodiment of the three-phase claw pole type motor according to the present invention;  
         [0034]      FIG. 12  is a sectional view partly in section showing the relationship between the magnetic poles and the claw poles shown in  FIG. 11 ;  
         [0035]      FIG. 13  is an exploded plan view showing an example of modification of the fourth embodiment;  
         [0036]      FIG. 14  is an enlarged view partly in section of a fifth embodiment of the three-phase claw pole type motor according to the present invention;  
         [0037]      FIG. 15  is a partly exploded perspective view of a sixth embodiment of the three-phase claw pole type motor according to the present invention;  
         [0038]      FIG. 16  is a partly exploded perspective view showing an example of modification of the sixth embodiment;  
         [0039]      FIG. 17  is a perspective view of a claw iron core of a seventh embodiment of the three-phase claw pole type motor according to the present invention;  
         [0040]      FIG. 18  is a perspective view of a claw iron core of an eighth embodiment of the multiple phase claw pole type motor according to the present invention;  
         [0041]      FIG. 19  is a perspective view showing an example of modification of claw poles;  
         [0042]      FIG. 20  is a perspective view showing another example of modification of claw poles;  
         [0043]      FIG. 21  is a perspective view showing still another example of modification of claw poles;  
         [0044]      FIG. 22A  is a diagram showing the results of measurement of the induced electromotive force of the claw pole type motor using iron plates such as SPCC;  
         [0045]      FIG. 22B  is a diagram showing an induced voltage waveform at the rotating speed of 250 r/min; and  
         [0046]      FIG. 22C  is a diagram showing an induced voltage waveform at the rotating speed of 1000 r/min. 
     
    
     DETAILED DESCRIPTION OF THE INVENTION  
       [0047]     Hereafter, a first embodiment of a multiple phase claw pole type motor according to the present invention will be described on the basis of FIGS.  1  to  4 .  
         [0048]     A three-phase claw pole type motor is constructed by a rotor  2  constructed on a rotating shaft  1 , a stator  5  formed concentrically with this rotor  2  in a state of being separated from the same by a small gap formed in a circumferential direction, and a stator frame  7  on which the stator  5  is supported. The rotating shaft  1  is rotatably supported on opposite ends of the stator frame  7  by bearings  8 A and  8 B.  
         [0049]     The rotor  2  is constructed by a rotor iron core  3  formed concentrically with the rotating shaft  1 , and a plurality of magnetic poles  4  formed of permanent magnets fixed on the outer periphery of the rotor iron core  3 . The stator  5  is constructed by stator iron cores  6 U,  6 V, and  6 W, and annular coils  13  wound on the stator iron cores  6 U,  6 V, and  6 W. The stator iron cores  6 U,  6 V, and  6 W are supported on the stator frame  7 , and the rotating shaft  1  is rotatably supported by the bearings  8 A and  8 B on the opposite ends of the stator frame  7 .  
         [0050]     Each of the stator iron cores  6 U,  6 V, and  6 W is constructed by a first claw pole  9 A and a second claw pole  9 B. Each of the first claw pole  9 A and the second claw pole  9 B is constructed by a claw portion  10  having a magnetic pole surface  10 F extending in an axial direction and facing the rotor  2  while being separated from the same by the small gap, a radial yoke portion  11  extending radially outwardly and perpendicularly from the claw portion  10 , and an outer peripheral yoke  12  extending from the radial yoke portion  11  in the same direction as the direction of extension of the claw portion  10 . Each of the radial yoke portion  11  and the outer peripheral yoke  12  has a circumferential length L 2  twice or longer than the circumferential length L 1  of the claw portion  10 . The claw portion  10  is connected to one side along the circumferential direction of the radial yoke portion  11  having the circumferential length L 2 . The outer peripheral yoke  12  has an axial length L 4  of about ½ of an axial length L 3  of the radial yoke portion  11 .  
         [0051]     The first claw pole  9 A and the second claw pole  9 B are formed into shapes identical to each other by compacting a magnetic powder in a die. In this way, a complicated magnetic pole structure can be obtained in comparison with those constructed by laminating silicon steel plates.  
         [0052]     The first claw poles  9 A and the second claw poles  9 B formed as described above are alternately arranged in the circumferential direction so that the end of the claw portion  10  faces the inside diameter side of the radial yoke portion  11  of the adjacent claw pole  9 A or  9 B, thus forming the stator iron core  6 U incorporating the annular coil  13 U. The stator iron cores  6 V and  6 W incorporating the annular coils  13 V and  13 W are formed in this way and placed by the side of the stator iron core  6 U in the axial direction with shifts of 120° in terms of an electrical angle, as shown in  FIGS. 4A  to  4 C, thus constructing the three-phase claw pole type motor having the same number of magnetic poles  4  as the number of claw portions  10 , i.e., sixteen magnetic poles  4 . These three groups of stator iron cores  6 U,  6 V, and  6 W are encapsulated in a molded insulating resin to obtain the stator  5  in which the first claw poles  9 A, the second claw poles  9 B, and the annular coils  13 U,  13 V, and  13 W are combined integrally with each other.  
         [0053]     The construction of the rotor  2  is not limited to the construction of arranging the magnets  4  on its surface, but it is possible to obtain running torque so long as the rotor  2  is a rotor, which constructs a pole, such as a rotor which has saliency as shown in  FIG. 4F , a cage type inductor shown in  FIG. 4D , and a rotor which has magnets and an inductor as shown in  FIG. 4E .  
         [0054]     As described above, a complicated magnetic pole construction, in other words, a magnetic pole construction capable of improving the motor efficiency can be obtained by forming the first claw poles  9 A and the second claw poles  9 B by compacting a magnetic powder.  
         [0055]      FIGS. 5A and 5B  show the results of measuring the B-H curves of each raw material. This measurement was performed by a ring sample type measuring method (JIS H 7153), and shows DC B-H curves. Iron core bodies formed by compacting a magnetic powder (soft magnetic composites i.e. SMCs  1 ,  2 , and  3 ) ordinarily have a magnetic permeability lower than that of laminated iron cores formed of a rolled plate (SPCC t0.5, SS400) and laminated iron cores formed of a silicon steel plate (50A1300, 50A800). The maximum flux density of the former is also lower than that of the latter. Further, even if they have the completely same shape, the iron cores (SMCs) formed by compacting a magnetic powder differ in B-H curves by compounding ratios of an iron powder and a resin binder, and the like. As shown in  FIG. 5B , the flux density of the SMC  1  obtained when a magnetic field of 10000 A/m is applied to its compact is 1.7 teslas or more, and when 80000 A/m, which is large magnetic field strength is applied, the flux density exceeds 2 teslas. On the other hand, the flux density of the SMC  2  obtained when the magnetic field of 10000 A/m is applied to its compact is 1.6 teslas, and when 80000 A/m, which is large magnetic field strength is applied, the flux density is 1.8 teslas or so. As for an SMC  3 , its flux density obtained when the magnetic field of 10000 A/m is applied to its compact is only 1.26 teslas, and when 80000 A/m, which is large magnetic field strength is applied, the flux density is less than 1.5 teslas. It can be expected that the obtained torque of the SMC  3  where the flux density as an SMC is low is also small when it is used in a motor.  
         [0056]      FIGS. 6B  to  6 E show the results of calculation of the output torque of motors in three-dimensional magnetic field analysis using a finite element method. First, a mesh model is shown in  FIG. 6A . In this example, one cycle of electrical angle (equivalent to a machine angle of 45°) of a three-phase claw pole motor with outside diameter size of φ60 mm and 8 poles is modeled.  FIG. 6B  shows the result of calculation of the output torque, obtained when a current is given to a coil of each phase using this model, using the B-H curves of each material. In the consequence of calculation on the condition that shapes of the motors were completely the same, it was found that, as for the output torque of the motors, the higher a magnetic permeability of a material was, the higher the output torque was. That is, according to the results of calculation with four kinds of materials shown in  FIG. 5B , the torque of SPCC is the largest, and the torque of the SMC  3  is the smallest.  FIG. 6C  shows this relationship with taking the flux density at the time of 10000 A/m as a horizontal axis and taking the output torque as a vertical axis. It was found that the output torque became large in proportion to the flux density.  
         [0057]     Next, since the SMC can obtain its core shape by compacting, it is possible to employ a pole shape which improves efficiency, as described previously. A specific method is to change pole thickness, which was a limit for SPCC, or the like.  FIG. 6D  shows the results of calculation with having increased the thickness of the SMC and having performed the same calculation as the above. It becomes clear that, when the thickness of claws of the SMC increases under the same conditions of the field magnets and the motor size, the output torque had an optimal value.  FIG. 6E  shows the result of plotting with superposing this optimal value on  FIG. 6C  having been explained previously. It was confirmed that the SMC  1  exceeded the limit torque in the case of construction from SPCC.  
         [0058]     Hence, in this embodiment, it is easy to manufacture the claw poles  9 A and  9 B and is possible to obtain a multiple phase claw pole type motor highly efficient than a conventional iron plate bending type claw pole motor by not only performing the compacting a magnetic powder to form the claw poles  9 A and  9 B, but also constructing a claw pole stator core of the SMC compact which has DC magnetizing properties of 1.7 teslas or more when a magnetic field of 10000 A/m is applied to the SMC compact.  
         [0059]     In addition, since the multiple phase claw pole motor constructed of the SMC core is hardly influenced by an eddy current loss, it is also advantageous to be able to be driven at an RF (radio-frequency). Although the comparison of the output torque in  FIG. 5  mentioned above was at low speed (a frequency area with slight influence of an eddy current), properties of the motor constructed of the SMC core will further improve in an RF.  FIG. 22A  shows the relationship between the revolution speed and the effective value of no-load induced electromotive force. In a claw pole motor constructed from iron plates such as SPCC, when the revolution speed becomes large, an eddy current flows inside the iron plates in a direction of obstructing magnetic fluxes. Then, owing to a denial operation of the magnetic fluxes by the current, a waveform of the induced electromotive force is distorted as shown in  FIG. 22B , and an effective value becomes small. On the other hand, in the claw pole motor whose core is constructed of the SMC, since an eddy current hardly flows, it becomes an effective value of the induced electromotive force linear to a frequency (revolution speed). Hence, although the conventional claw pole type motor with the conventional claw poles could not be used for an application at high revolution speed, the claw pole motor constructed of the SMC core can be driven at high revolution speed (high frequency area).  
         [0060]     In addition, because the eddy current hardly flows it is also possible to correspond to a PWM method of control system which performs a pulse division of a sinusoidal voltage and driving. PWM is a drive system of obtaining an effective value of a voltage in a pulse-like voltage. Since a switching frequency of those pulses is usually about 10 times of a maximum frequency of a drive current of a motor, that is, a very high frequency, an eddy current arises by its RF component. Hence, since iron loss becomes large in a conventional claw pole motor constructed from iron plates, the motor has become an inefficient motor. Since the eddy current hardly flows, the claw pole type motor of the present invention which is constructed of the SMC core can be driven.  
         [0061]     On the other hand, large torque pulsation occurs in the case of use of the iron core formed by compacting a magnetic powder, such that the magnitude of pulsation is ⅓ of the average torque. The cause of this torque pulsation is a large distortion in the waveforms of voltages induced in the annular coils  13 U to  13 W by local magnetic saturation in the claw poles  9 A and  9 B. Such a waveform distortion is also caused by an interpole leakage flux or an in-pole leakage flux.  
         [0062]     These leakage magnetic fluxes will be described with reference to  FIGS. 7A and 7B .  FIG. 7A  shows a flow of a main flux Φ. The main flux Φ emerging from one N magnetic pole in the magnetic poles  4 , for example, enters the claw portion  10  of the first claw pole  9 A through a gap, enters the claw portion  10  of the second claw pole  9 B from the claw portion  10  of the first claw pole  9 A in linkage to the annular coil  13 , and enters the S magnetic pole  4  from the claw portion  10  of the second claw pole  9 B through the gap, thus forming a magnetic path returning to the N magnetic pole  4 . Apart from the main flux Φ, an interpole leakage flux Φ 1  exists. If the interpole size SO between the claw portions  10  of the first and second claw poles  9 A and  9 B is smaller than the gap size between the magnetic poles  4  and the claw portions  10 , the interpole leakage flux φ 1  forms a magnetic path by shortcutting between the claw portions  10  without linkage to the annular coil  13 , resulting in reduction in a rate of use of the magnetomotive force of the magnetic poles  4  formed of permanent magnets. The interpole size SO between the claw portions  10  may be increased by considering this phenomenon. However, if the interpole size SO is increased, the width of the magnetic pole surface  10 F is so small that the effective value of the linkage flux of linkage between the main flux Φ and the annular coil  13  is considerably reduced. It is not advisable to adopt such an easy way of increasing the interpole size SO.  
         [0063]     Further, the generation of an in-pole leakage flux Φ 2  is a phenomenon in which, as shown in  FIG. 7B , part of the main flux Φ entering the claw portion  10  of the first claw pole  9 A enters the radial yoke portion  11  of the adjacent second claw pole  9 B facing the first claw pole  9 A from the distal end of the first claw pole  9 A by forming the in-pole leakage flux Φ 2 , and flows in the radial yoke portion  11  in the circumferential direction to form a magnetic path reaching the claw portion  10  of the second claw pole  9 B. To reduce this in-pole leakage flux Φ 2 , a sectional area of the distal end of the claw portion  10  may be reduced by increasing the angle θk of the magnetic pole surface  10 F or the gap dl between the distal end of the claw portion  10  and the radial yoke portion  11  may be increased. These measures to reduce the in-pole leakage flux Φ 2  entails the drawback of reducing the area of the magnetic pole surface  10 F and thereby reducing the effective value of the linkage flux as in the above-described case. It is not advisable to adopt these measures.  
         [0064]      FIG. 8  shows the results of computation of the relationship between the interpole size SO and the effective value of the linkage flux using the above-mentioned three-dimensional magnetic field analysis.  
         [0065]     As is apparent from  FIG. 8 , the effective value of the linkage flux can be increased by increasing the angle θk of the magnetic pole surface  10 F and by reducing the interpole size SO of the adjacent claw portions  10 . However, if the effective value of the linkage flux is increased, the leakage fluxes (Φ 1 , Φ 2 ) are also increased to cause an increase in distortion of the waveform of the induced voltage, as described above.  
         [0066]     A second embodiment of the three-phase claw pole type motor in accordance with the present invention arranged to solve the above-described problem due to the leakage fluxes (Φ, Φ 2 ) and capable of maintaining a high effective value of the linkage flux will be described with reference to  FIG. 9 . In  FIG. 9 , the same reference characters as those in the figure showing the first embodiment indicate the same component parts. The description of the same component parts will not be repeated.  
         [0067]     In this embodiment, the angle θk of the magnetic pole surface  10 F is increased and the thickness T of the claw portion  10  is increased. Also, the thickness T is gradually increased along a direction from the distal end of the claw portion  10  toward the radial yoke portion  11 .  
         [0068]     If the sectional area of the claw portion  10  is increased as described above, a high effective value of the linkage flux can be maintained. Also, local magnetic saturation regions in the first and second claw poles  9 A and  9 B can be reduced. As a result, the leakage fluxes (Φ 1 , Φ 2 ) are limited even if the interpole size SO is reduced by increasing the angle θk of the magnetic pole surface  10 F. Therefore, distortion in the waveform of the induced voltage can be reduced and torque pulsation can be limited.  
         [0069]      FIG. 10  shows a third embodiment of the three-phase claw pole type motor in accordance with the present invention. The third embodiment differs from the first embodiment in the sectional shape of the magnetic pole  4  in the rotor side.  
         [0070]     That is, in this embodiment, the magnetic pole  4  is formed so as to have a sectional shape with a convex curve such that a central portion in the circumferential direction is closest to the claw portion  10  while opposite end portions in the circumferential direction are remotest from the claw portion  10 .  
         [0071]     If a curved surface defined by such a convex curve is formed on the magnetic pole  4 , the main flux Φ can be made to flow concentrically from a center of the curved surface into the claw portion  10 . Also, the resistance of the magnetic flux path for the interpole leakage flux Φ 1  flowing in the claw portions  10  through the opposite end portions of the magnetic pole  4  in the circumferential direction as shown in  FIG. 7A  is increased by increasing the gap between the magnetic pole  4  and the claw portion  10 , thereby reducing the amount of leakage of this flux. As a result, the interpole leakage flux Φ 1  can be reduced without reducing the effective value of the linkage flux.  
         [0072]     A fourth embodiment of the three-phase claw pole type motor in accordance with the present invention in which the shape of the claw portion  10  is changed to reduce a leakage flux will be described with reference to  FIGS. 11 and 12 .  
         [0073]     The area of the magnetic pole surface  10 F of the claw portion  10  facing the magnetic pole  4  is increased to ensure a high effective value of the linkage flux. The area of the magnetic pole surface  10 F is increased by reducing the angle θk in the construction shown in  FIG. 1  so that the sides defining the angle θk are parallel to the axial direction. Also, the interpole size SO between the claw portions  10  of each adjacent pair of the first and second claw poles  9 A and  9 B is increased relative to the gap between the claw portions  10  and the magnetic poles  4 , but the interpole size So between portions of the claw portions  10  having a thickness t in the magnetic pole  4  side is reduced.  
         [0074]     If the claw portions  10  are formed in this manner, the flow of the interpole leakage flux Φ 1  into the portions having the thickness t, between which the magnetic path between the claw portions  10  is restricted, is limited, thereby reducing the interpole leakage flux Φ 1 .  
         [0075]     To reduce the in-pole leakage flux Φ 2 , the gap d 2  between the distal end of the claw portion  10  and the radial yoke portion  11  of the adjacent claw pole  9 A (or  9 B) may be increased.  
         [0076]     A leakage flux Φ 3  between adjacent pair of phases can be reduced, for example, by setting the gap d 3  between the distal end of the claw portion  10  in the U-phase side and the radial yoke portion  11  of the adjacent claw pole  9 A in the V-phase side to an increased value, as shown in  FIG. 13 .  
         [0077]      FIG. 14  shows a fifth embodiment of the three-phase claw pole type motor in accordance with the present invention.  
         [0078]     In this embodiment, to enable the main flux Φ to flow through the shortest distance, concave portions R 1  and R 2  formed of polygonal surfaces are respectively formed as an inner corner portion in the connecting portion between the claw pole  9 A or  9 B and the radial yoke portion  11  and an inner corner portion in the connecting portion between the radial yoke portion  11  and the outer peripheral yoke  12 . The concave portions R 1  and R 2  are formed by connecting a certain number of surfaces at certain angles. They may alternatively be formed of one curved surface or a certain number of curved surfaces.  
         [0079]     A sixth embodiment of the three-phase claw pole type motor in accordance with the present invention will be described with reference to  FIG. 15 . The same basic construction for increasing the effective value of the linkage flux between the first claw pole  9 A and the second claw pole  9 B and reducing leakage fluxes as that in each of the above-described embodiments is also used in this embodiment. The description of the basic construction will not be repeated.  
         [0080]     A three-dimensional shape can be integrally formed since the first claw pole  9 A and the second claw pole  9 B constructing each of stator cores  6 U,  6 V, and  6 W are formed by compacting a magnetic powder, as described above. Since the first claw pole  9 A and the second claw pole  9 B are formed so as to be identical in shape to each other, it is desirable to attach marks used as a reference at the time of assembly to the first and second claw poles  9 A and  9 B. Further, it is advantageous to provide a positioning function or an assembly guide function by forming the marks. Such a function is effective in improving the facility with which the component parts are assembled and reducing the assembly time.  
         [0081]     To provide such a function in this embodiment, recesses  14  and projections  15  capable of engaging with the recesses  14  are formed in the outer peripheral yoke  12  constructing the first claw pole  9 A and the second claw pole  9 B. The recesses  14  and the projections  15  are formed in the first and second claw poles  9 A and  9 B by being recessed and raised along the axial direction so as to be capable of fitting to each other when the first and second claw poles  9 A and  9 B are brought into abutment on each other. A recessed groove  14  and a projection  15  are formed at positions distanced by 180° in terms of electrical angle in the circumferential direction. Since the first and second claw poles  9 A and  9 B are perfectly identical in shape to each other, they can be compacted in one die.  
         [0082]     When the first and second claw poles  9 A and  9 B constructed as described above are assembled, they are fitted to each other by simply moving the projections  15  into the recesses  14  in the axial direction, with the annular coil  13  interposed between the claw portions  10  and the radial yoke portions  11 . Thus, the assembly can be easily completed.  
         [0083]      FIG. 16  shows an example of modification of the sixth embodiment. A lead wire channel  16  through which a lead wire  13 R corresponding to a winding-leading end and/or a wiring-trailing end of the annular coils  13  is laid to the outside is formed by integral compacting in each of the surfaces of the radial yoke portions  11  of the first and second claw poles  9 A and  9 B facing the annular coil  13 .  
         [0084]     If the lead wire channel  16  is formed in the radial yoke portion  11  in advance, the need for provision of an additional space for the lead wire  13 R is eliminated, thereby increasing the winding density of the annular coil  13  and enabling lead wires  13 R in the entire motor to be laid in a determined direction.  
         [0085]     While the facility with which the first and second claw poles  9 A and  9 B in the in-phase relationship are assembled is improved in the above-described sixth embodiment, an improvement in the facility with which the first and second claw poles  9 A and  9 B in an interphase relationship are assembled can be achieved in a seventh embodiment shown in  FIG. 17 .  
         [0086]     That is, a recess  16  and a projection  17  are formed in the radial yoke portion  11  side in the outer eripheral yokes  12  of the first and second claw poles  9 A and  9 B in an interphase relationship by being placed side by side in the circumferential direction, in addition to the recess  14  and the projection  15  shown in  FIG. 15 . Recesses  16  each capable of being fitted to one projection  17  provided at least in one place are formed at positions distanced by ±60° and ±120° in terms of electrical angle from the position of the projection  17 , thereby enabling the outer peripheral yokes  12  of the first and second claw poles  9 A and  9 B in interphase relationship to be positioned relative to each other with accuracy as well as facilitating the assembly.  
         [0087]      FIG. 18  shows an eighth embodiment of the multiple phase claw pole type motor in accordance with the present invention. Fitting holes  18  and a fitting projection  19  arranged in the axial direction are formed in the outer peripheral yokes  12  of the first and second claw poles  9 A and  9 B in interphase relationship, as are the projection and the recesses in the sixth embodiment. Also in this case, the same effect as that in the sixth embodiment is achieved.  
         [0088]     In each of the above-described embodiments, the first and second claw poles  9 A and  9 B are formed in correspondence with each pole. However, needless to say, a claw pole assembly  20  in which claw pole portions for one phase (360°) are formed integrally with each other as shown in  FIG. 19 , a claw pole assembly  21  in which claw pole portions for ½ phase (180°) are formed integrally with each other as shown in  FIG. 20  and a claw pole assembly  22  in which claw pole portions for ¼ phase (90°) are formed integrally with each other as shown in  FIG. 21  may be formed. In such case, the relationship between the positions at which the recesses  14  or  16  and the projections  15  or  17  are provided and the relationship between the positions at which the fitting holes  18  and the fitting projections  19  are provided may be angular relationships of integer multiples of ±60° and ±120° in terms of electrical angle.  
         [0089]     Although the above-mentioned description was made about embodiments, the present invention is not limited to them, but it is apparent to those skilled in the art that various changes and modifications can be made within the scope of the spirit of the present invention, and the attached claims.