Technical field The invention is thus based on high performance electric miniature motors. These are e. g. used in mobile tele- phones where a mass, which is mounted eccentrically on the shaft of the motor, upon rotation causes the mobile telephone to vibrate, whereby the user of the telephone is wirelessly made aware that there is an incoming call on the telephone. This illustrates a situation where the motor according to the invention may be used to advan- tage, and the example should not be taken to restrict the invention.

To provide a sufficiently high performance and speed for the motor, it is an advantage to use a permanent magnet as a rotor. This, however, normally causes problems in connection with motors of this size, since eddy current losses are created in the stator because of the rotating magnetic field that is established when the magnet ro- tates. In large motors, this problem is normally overcome by laminating the magnetic part of the housing/stator to the motor. Laminated magnetic cores are known for avoid- ing eddy current losses in magnetic cores in motors and transformers, etc., said core being composed of a plural- ity of individual sheets which are electrically insulated from each other at least partly, so that the stack of sheets has an at least significantly reduced electrical conductivity transversely to the planes of the sheets, that is in the direction of stacking.

In the field of high frequency technique it is known to use sintered magnetic elements of ferrite material.

Drawbacks of the prior art The above solutions to the problem of eddy current losses in the stator of miniature motors have certain drawbacks.

For example, lamination of the stator in an axial direc- tion is rather expensive, since the stator of miniature motors has a very small wall thickness, and it adds con- siderably to the costs when the magnetic core of the sta- tor has to be assembled from a plurality of small ring- shaped sheet elements with a sufficiently high precision.

The use of sintered elements is likewise inexpedient be- cause of the necessary small thickness of material, since the stator hereby gets a too low ultimate strength, and also it is difficult to make a stator of a sintered mate- rial, such as ferrite, with sufficiently narrow toler- ances.

A miniature motor of the above-mentioned type is known from an article or advertisement Tiny motors packed with precision published in Machine Design, 9th July 1998, page 58. This motor, however, also has drawbacks. The mo- tor uses a wound coil made by a process wherein the coil threads must be wound very closely together and be posi- tioned with great precision because of the small size in order to achieve a suitably high performance in the very small and compact coil. A very high degree of precision is required for such a process, which makes the process cumbersome, and the resulting motor is therefore expen- sive.

Furthermore, this known motor has no commutator brushes.

This requires additionally complicated and cost-increas-

ing control electronics which is used for keeping track of and determining the angular position of the rotor relative to the stator coil, so that the correct part of the coil can be activated to affect the magnet expedi- ently. The high speeds of rotation moreover make very great demands on the control electronics. An additional drawback of the use of the external control electronics is that the electronics per se takes up much space rela- tive to the miniature motor. This manifests itself par- ticularly in connection with mobile telephones where size, weight and price are very much competitive parame- ters.

Object of the invention The object of the present invention is to provide a com- pact high performance miniature motor with a high speed of rotation, which also consists of simple components and is thereby easy and simple to manufacture.

Summary of the invention The invention provides a high performance miniature motor with a low eddy current loss and containing quite few simple elements, such as bearings, a double-sided flexible circuit board provided with coil parts on both sides, a spring used as a commutator brush, a permanent magnet used as a rotor, etc. This allows a very simple and inexpensive manufacturing method for the motor.

The problem of eddy currents in the housing when the mag- net rotates is solved in the following manner according to the invention.

In a preferred embodiment, the motor housing is formed by a plurality of non-plane subelements which are provided

with protruding parts and corresponding cavities to re- ceive protruding parts on another subelement so that the subelements have a self-centering effect when assembled.

This means that the housing is essentially electrically insulating in the longitudinal direction of the motor, since, in practice, the division into subelements gives an electrical division into layers which, otherwise, can typically be achieved only by an expensive lamination, so that eddy current losses are avoided entirely or reduced considerably. The housing is still magnetically conduc- tive, as is required for a stator in a motor.

According to a preferred embodiment, the electrical ter- minal wires are integrated on the flexible circuit board.

This ensures an additionally simple and flexible struc- ture, as the terminal wires do not have to be soldered on the coils, but have already been integrated. This gives an easy and inexpensive mounting of the motor in e. g. a mobile telephone.

In an expedient embodiment, the end part of the spring touching the commutator segments has a direction of wind- ing opposite to the direction of rotation of the shaft.

This ensures that the spring cannot inexpediently lose contact with the shaft, since the spring will be tight- ened additionally when the motor is used.

Brief description of the drawings The invention will be described more fully below with reference to the drawing, in which Figure 1 shows a schematic section longitudinally through a motor according to a preferred embodiment of the inven- tion,

Figure 2 shows an element for building the stator in the motor in figure 1, Figure 3 shows a side (the front side) of a developed flexible circuit board according to an embodiment of the invention, Figure 4, seen through one side, shows another side (the rear side) of a developed flexible circuit board accord- ing to an embodiment of the invention, and Figure 5 shows a schematic section transversely trough a folded/coiled-up cylinder of a flexible circuit board as well as three commutator segments according to an embodi- ment of the invention, said cylinder being placed around the commutator segments.

Detailed description of the invention Figure 1 shows a schematic section longitudinally through a motor according to a preferred embodiment of the inven- tion. The motor comprises a stator (10) of magnetic soft material shaped as a substantially cylindrical tube which is composed of elements as shown in figure 2.

Figure 2 shows an element (50) for building the stator in the motor in figure 1. The element (50) consists of mag- netic soft material and has the shape of a ring or a short length of tube with two interconnected sections, a first section (51) and a second section (52). The first section (51) has an external diameter which corresponds to the internal diameter of the second section (52), so that the first section may be received in the second sec- tion on a second element with a suitable degree of fric- tion.

When building a stator for the motor in figure 1, a suit- able number of elements (50) are arranged on a mandrel where they are pressed together so that the narrow first sections (51) of the elements are pressed into the wide second sections (52) of the adjacent elements. This re- sults in the formation of a tubular element which is used as a stator in a motor as shown in figure 1. The mandrel serves as an aid in the assembly and has the effect that the resulting stator is not curved, but rectilinear.

The stator is thus divided into individual parts sepa- rated in its longitudinal direction, which causes eddy current losses to be reduced significantly, thereby im- parting a greater efficiency to the motor.

The elements (50) for building a stator are self-center- ing because they each have two sections which fit into each other and enclose each other at least partly. This self-centering effect may be achieved by other embodi- ments of the elements. For example, the elements may be shaped as a frusto-conical shell, or they may have pro- jections on one side with corresponding cavities on the other side.

Figure 1 also shows that one end of the shaft (3) has mounted thereon a mass (55) which is arranged eccentri- cally relative to the shaft.

Two bearings (4,5) are provided at the ends of the sta- tor (10), one bearing (5) of which serves as a commutator with commutator segments. Rotatably secured in the bear- ings (4,5) is a shaft (3) with electrical connection to the bearing (4) through a screw spring (7) which is in constant electrical contact with the bearing (4) and thus serves as a slip-ring contact. The bearing (4) may be formed with an unbroken slip-ring or be identical with

the bearing (5) at the opposite end with commutator seg- ments. The advantages of this in terms of production are evident. Alternatively, the bearing (4) per se may be conductive and be made of known conductive materials for such bearings, such as bronze or conductive plastics, thereby obviating the spring (7). Fixedly mounted on the shaft (3) is a permanent magnet (1) which is magnetized in a radial direction and serves as a rotor. Further, an electrically conducting screw spring (9), which serves as a commutator brush, is mounted on the shaft (3). The spring (9) has an end part (11) which is pressed onto a part of the shaft which has a slightly increased diame- ter, whereby the spring (9) is kept in position on the shaft by its own mechanical tension. The contact springs (7,9) have opposite directions of winding, but are oth- erwise identical.

Three commutator segments are provided on the bearing (5), of which only a single one (6) is visible in figure 1. The three commutator segments are placed with 120 de- grees between each other, and by rotation of the shaft (3) the free end of the spring moves across the three commutator segments and make alternately contact with them individually. The motor may optionally have more than three commutator segments with their respective coils attached.

The electrical connection to the motor has one commutator brush and one slip-ring contact with permanent electrical contact, where other motors have two commutator brushes on the same commutator. The structure with just one com- mutator brush selected here is advantageous, because the wear on the commutator segments is thereby substantially halved, it being mainly the power interruptions that sub- ject the metal parts of the commutator to wear. Moreover,

this structure is advantageous, because also less elec- trical noise is generated hereby.

Figures 3-4 show a flexible circuit board (2) in the form of a flexible foil with coils that may be impressed or etched by means of prior art techniques. The commutator segments in the bearing (6) are each electrically con- nected to a coil (12,15; 13,16; 14,17), on a flexible circuit board (2) in the form of a flexible foil with coils, through their respective connecting points. A positive voltage is applied to all the coils (12,15; 13, 16; 14,17) from a positive terminal wire (+) on the flexible circuit board (2), while a negative voltage (or earth) is applied to the shaft (3) via the electrically conducting bearing (4) through a connecting point between the electrical bearing (4) and a negative terminal wire (-) on the flexible circuit board (2). When the spring (9) touches a commutator segment, a current will flow in the coil concerned (12,15; 13,16; 14,17) to which the commutator segment is electrically connected. The current will create a magnetic field in the longitudinally ex- tending conductors of the coil concerned (12,15; 13,16; 14,17), that is the parts which extend in an axial di- rection, and this magnetic field affects the magnet (1) by a force and causes rotation of the magnet (1) and thereby the shaft (3), the coils (12,15; 13,16; 14,17) being secured relative to the housing.

When assembling the motor, the coiled-up flexible circuit board with coils is first inserted into the stator hous- ing so that it engages and is held firmly against the in- ner wall of the housing because of the outwardly directed pressure from the coiled-up flexible circuit board. Then, a first bearing is secured by a simple axial movement for insertion into one end part of the housing, so that the flexible circuit board is additionally stretched and se-

cured against the interior of the housing. The shaft with the magnet secured, i. e. the entire rotor, is positioned centrally in this bearing. A spring is pressed axially on the shaft, which spring is to serve as a commutator brush, e. g. so that it engages the magnet or is otherwise fixed axially. A second bearing provided with commutator segments is then moved axially into the other end part of the housing until electrical contact between the commuta- tor brush and a commutator segment is detected. Then, the second bearing is pressed additionally into the motor housing (e. g. 0.1-0.2 mm) so that the spring is firmly fixed between the magnet and the second bearing. The lat- ter pressure particularly ensures a well-defined contact force between the commutator brush and the commutator segments, thereby ensuring a good and stable electrical connection between the commutator segments and the shaft with minimum wear.

Preferably, the rotor with the spring (9), which touches the commutator segments with its end part, has a direc- tion of rotation which means that friction between the spring (9) and the commutator segments causes further tightening of the spring.

Figure 3 shows a side (the front side) of a developed flexible circuit board (2) according to an embodiment of the invention. The figure shows three subcoils (12,13, 14) positioned on one side of the flexible circuit board (2). The subcoils (12,13,14) are connected through the connecting points (25,26,27) to their respective other subcoils (see figure 3 and the description below) which are present on the other side of the flexible circuit board (2). Each coil (12,13,14) has a connecting point (21,22,23) of its own to the respective connected com- mutator segment. A connecting point (24) ensures that the

negative voltage (or earth) fed from the negative termi- nal wire (-) (see figure 4) is fed to the bearing (4).

The configuration of the subcoils (12,13,14) has been made with a view to utilizing the area of the flexible circuit board (2) as well as possible with respect to the number of windings on each coil. The flexible circuit board (2) is rolled into a cylinder with substantially two layers (they have a small overlap, see figure 5), so that the coil centres (25,25' ; 26,26' ; 27,27') are mu- tually offset by substantially 120 degrees. The cylinder with the two layers gives a total of about 720 degrees on which the coils may be distributed. Each pair of coils has an extent in the peripheral direction corresponding to 240 degrees. The shown arrangement of the coils on the flexible circuit board means that each coil consists of a small subcoil and a large subcoil positioned on their re- spective sides of the flexible circuit board (2). The large coil part (12,14,16) for each coil must have a certain extent in the peripheral direction to enclose the magnet (1) sufficiently to cause rotation of this (see figure 4). This is satisfied particularly expediently by this invention in that each coil comprises a pair of coils with a large and a small subcoil, the large sub- coils alternately being present on the one and the other side of the flexible circuit board. If the large subcoils were arranged on the same side of the flexible circuit board, there would not be sufficient space on the one side of the flexible circuit board while still maintain- ing two layers (with a small overlap). Thus, by position- ing at least one subcoil on the other side space is pro- vided for the rest of the large subcoils, while providing extra space that is utilized by the invention for the re- spective small coil part (13,15,17) in order to in- crease the effective number of windings for each coil, resulting in a greater effective capacity per coil. This

gives a very high utilization ratio of the coil area on very restricted space.

Figure 4, seen through one side, shows another side (the rear side) of a developed flexible circuit board. The figure shows three subcoils (15,16,17) which each are electrically connected to the three subcoils (12,13,14) on the other side of the flexible circuit board through the connecting points (30). Also visible are electrical terminal wires (+,-) which feed the coils with positive voltage and negative (optionally earth) voltage, respec- tively. The positive voltage from the positive terminal wire (+) is fed to all the coils through the connecting points. When the spring (9) touches one of the commutator segments, an electrical circuit is created, consisting of the positive terminal wire (+), the coil connected to the touched commutator segment, the touched commutator seg- ment, the spring (9), the shaft (3), the spring (7), the bearing (4) and the negative terminal wire (-) through the connecting point. The current flowing in this circuit will create a magnetic field in the longitudinal conduc- tors of the connected coil, which magnetic field affects the magnet (1) by a force and causes rotation of the mag- net (1) and thereby the shaft (3), the coils (12,15; 13, 16 ; 14,17) and the flexible circuit board (2) being se- cured to the housing.

Alternatively, all six subcoils may be the same on both sides of the flexible circuit board so that each of the subcoils has an extent in the peripheral direction corre- sponding to 240 degrees.

Figure 5 shows a schematic section transversely through a folded/coiled-up cylinder (40) of the flexible circuit board (2) and the three commutator segments according to an embodiment of the invention, the cylinder being posi-

tioned around the commutator segments. In the figure, (41) designates the contact point between the spring (9) and the active commutator segment. The active commutator segment is connected to its respective coil at the con- necting point (42), which corresponds to the connecting point (23) in figure 3. The solid lines on the cylinder (40) schematically indicate the position of the conduc- tors in the longitudinal direction in the coil. (43) and (43') designate the one half and the other half, respec- tively, of the large coil part of the coil positioned on one side of the flexible circuit board (2), while (44) and (44') designate the one half and the other half, re- spectively, of the large coil part of the coil positioned on the opposite side of the flexible circuit board (2).

The figure also shows the angle a between the contact point (41) seen in relation to the centre of the shaft (not shown) and the direction of magnetization shown as the arrow from S and N. x and * respectively indicate the current direction in and out of the plane.

The situation in figure 5 outlines for example an initial position/start position in which the shaft is at rest. If the voltage terminals (+,-) are activated, then, as stated above, there will be an electrical circuit con- sisting of the positive terminal wire (+), the coil (43, 43', 44,44') connected to the touched commutator seg- ment, the touched commutator segment, the spring (9), the shaft (3), the electrically conductive bearing (4) and the negative terminal wire (-) through the connecting point, and a current will flow in the coil (43,43', 44, 44') as indicated by the current directions x and e. At (43) and (44) the current in the conductors (which extend into the plane) and the magnetic field illustrated by the arrow from S and N will create a force which affects the conductors (43,44) anti-clockwise. Since the conductors are secured to the housing (10), the shaft (3), on the

contrary, will be affected by the conductors clockwise.

At (43') and (44') the current goes out of the plane, and the conductors (43', 44') will be affected by a force anti-clockwise, which causes the shaft (3) to be affected clockwise since the conductors are secured to the housing (10). These two cooperating forces will thus rotate the shaft (3) clockwise, as indicated by the bent arrow. This force application will continue until the spring (9) no longer touches the commutator segment, and the electrical circuit is thereby interrupted. The moment of the shaft (3) and the magnet (1) will cause the shaft (3) to still move until the spring (9) touches the next commutator segment and a new electrical circuit is created, contain- ing the next coil which is offset 120° relative to the preceding one. The current in the new electrical circuit and the magnetic field will now create a force in a man- ner similar to the one above, merely offset 120°, and will rotate the shaft (3) and the magnet (1) addition- ally. This process will repeat itself and the shaft will continue to rotate, until the voltage on the terminal wires (+,-) is no longer fed.

The two bearings (4,5) of the motor are shaped as plugs that are inserted in an axial direction into the stator with parts of the flexible circuit board disposed between the bearings and the stator (10). Only the coil parts in which the conductive paths extend in the axial direction of the motor apply a moment of force to the magnet of the rotor, and these coil parts have the same extent in an axial direction as the magnet.

The parts of the conductive paths on the flexible circuit board which do not exclusively extend in the axial direc- tion of the motor, are present outside the ends of the magnet and preferably between the bearing plugs and the stator. This position is particularly advantageous, since

these conduction parts thereby do not take up space, and the motor can therefore be made particularly compact. At one end of the motor, electrical currents flow in these parts one way round in the peripheral direction, and at the other end of the motor, currents of the same magni- tude flow the other way round. These currents will there- fore balance each other so that, in operation, the rotor is not affected by any net force in an axial direction.

This is an advantage, because the contact force is thereby just determined by the structure and not by the conditions of operation.