ROTATION DETECTING MEANS FOR A ROTATING BODY

Abstract: The invention discloses a rotation detecting means for detecting the rotation state of a rotating body, in which a magnetic recording medium (4) on which N and S magnetic poles are alternately recorded at a constant interval is fixed symmetrically with respect to a rotary shaft of a rotating body (3) whose rotation state is to be detected, and an MR element (5) comprising magnet-­ resistive elements (R₁₁, R₁₂, R₂₁, R₂₂) is mounted at a fixed position relative to the magnetic recording me­ dium so that the rotation state of the rotating body can be detected from variation of the values of resistance of the magnet-resistive elements caused by the rotation of the body. N and S poles are recorded on the magne­ tic recording medium (4) with a small pole pitch P. The magnet-resistive elements (R₁₁, R₁₂, R₂₁, R₂₂) are formed to have a width sufficiently smaller than the pole pitch. The magnet-resistive elements constitute a first group (R₁₁, R₁₂) and a second group (R₂₁, R₂₂) the magnet-resistive elements of each group being disposed with an interval equal to the pole pitch or half the pole pitch. The magnet-resistive elements are disposed in such a manner that the interval between the groups is deviated from the pole pitch, whereby a circuit compris­ ing these magnet-resistive elements can detect the rotation of the rotating body.

Description: This invention relates to a rotation detecting means for detecting the rotation position, rotation direction and rotation speed of a rotating body of the kind referred to in the pre-characterising parts of patent claims 1 and 3. In a prior art rotation detecting means for a rotating body, as disclosed in Japanese Patent Publication (Post-Examined) No. 41335/79 and Japanese Patent Publication (Laid-Open) No. 48379/79, a magnetic medium on which N and S poles are magnetized alternately at a constant interval is disposed with its center at the rotation axis of the rotating body, and two magnet-resistive elements disposed with an interval equal to half the pole pitch are mounted at fixed positions relative to the magnetic medium. The two magnet-resistive elements are connected in series, and a d.c. voltage is applied in order to pick up a signal related to the rotation state of the rotating body from a connection point of both magnet-resistive elements. Further, U.S. Patent US―A―4,039,936 discloses a rotation detecting means for a rotating body, in which a voltage dividing circuit is connected in parallel with a series circuit of the above-mentioned magnet-resistive elements to form a bridge circuit, and a signal related to the rotation state of a rotating body is taken out from this bridge circuit. Further, Japanese Patent (Laid-Open) No. 120547/78 discloses a rotation detecting means for a rotating body, in which two pairs of series circuits of the above-mentioned magnet-resistive elements are used to detect two rotation state signals with different phases. Still further, Japanese Patent (Laid-Open) No. 115257/79 discloses a similar means for detecting a multiplicity of signals with different phases by using a multiplicity of magnet-resistive elements. These rotation detecting means for a rotating body are often applied to detection of the rotation speed of a motor, the rotation direction thereof and the rotation angle from a reference value when the motor-driven body is under drive control. In order to obtain an accurate drive control, it is necessary to detect the rotation states of the rotating body, that is, the rotation speed, rotation direction and rotation angle. For this purpose, it is required that N and S poles recorded on a magnetic recording medium that is mounted on the rotating body are formed at a small interval. Further, the small interval is inevitable for miniaturization of the means. Therefore, magnetic resistive elements for discriminating and detecting magnetic poles with such a small interval must have a sufficiently small width compared to the pitch of the magnetic poles in the moving direction of the magnetic recording body. These requirements are disclosed in none of the cited references. No construction satisfying these requirements is shown therein. Requirement of a small size means is satisfied by miniaturization of a pick-up including a magnet-resistive element, that is, a small construction of magnet-resistive effect metal elements (hereinafter referred to as an MR element). Therefore, it will be convenient, if terminal parts from the magnet-resistive element to a detecting circuit is constructed in such a manner that they are adjacent to each other. Further, if magnet-resistive elements, conductor parts for mutual connection thereof and terminal parts are to be formed on an insulator substrate, it is preferable that MR elements be formed with the same material at one time by the evaporation method, etc. in order to have improvement in mass production and cost reduction. In this case, since the conductor parts cause a magnet-resistive effect, some countermeasure would be necessary to avoid any influence of magnetic poles recorded on the magnetic recording medium. However, the cited references describes nothing on these points. Particularly, an MR element having a plurality of bridge circuits formed therein to detect plural signals has a large shape, since the number of magnet-resistive elements is large. Because of this, an irregularity of evaporation can appear easily, which causes a variation in the characteristic of each bridge circuit. Moreover, simultaneous formation of all the elements becomes difficult. Thus, a problem degrading mass productivity arises. Another problem is that a large number of terminals make a complicated printing. From GB―A―2 034 053 a magnetoresistive displacement sensing transducer is known, which employs a plurality of sensors, comprising each a plurality of magnetically biased magnetoresistive stripes. Each sensor produces a signal in response to a displacement with respect to a magnetic grating arranged on a body the displacement of which is to be measured. The phases of signals from the plurality of these sensors are relatively displaced by less then 180° to permit determining direction of displacement and to increase accuracy through interpolation. A signal processing unit uses combinations of signals of these sensors to retain a value corresponding to the position of the transducer relative to the grating. This transducer is of large length along the direction of displacement of the grating making it difficult to use it in a rotational displacement sensor. If the sensors are arranged on a flat substrate the distance between magnetoresistive stripes and the grating varies in accordance to their location on the substrate, whereby the accuracy of the transducer is affected. To deposit the transducer circuit on a curved substrate is very complicated and expensive. Further the large number of elements to be printed degrades mass productivity of such a transducer. The object of this invention is to provide a rotation detecting means for a rotating body with a small size and good mass productivity. According to the invention this object is solved by a rotation detection means of the kind referred to in the pre-characterising parts of patent claims 1 and 3 comprising the features disclosed in the characterising parts of patent claims 1 and 3. The rotation detecting means according to the invention employs only one sensor and no bias magnetic field is needed. Further only four magnetoresistive elements are used whereby the size of the rotation detecting means is made very small and the mass productivity increased. This and other objects and advantages of this invention will become more apparent from the following detailed description made in conjunction with the accompanying drawings, in which; Fig. 1 is a diagram showing one example of the whole construction of this invention; Fig. 2 is an explanatory diagram showing one embodiment of the main part of this invention; Fig. 3 is a diagram showing the circuit construction of Fig. 2; Fig. 4 shows output waveforms in the operation of the embodiment shown in Fig. 2; Fig. 5 is an explanatory diagram showing a modification of the embodiment shown in Fig. 2; Fig. 6 is a diagram showing the circuit construction of the embodiment shown in Fig. 5; Fig. 7 is an explanatory diagram showing another embodiment of the main part of this invention; Fig. 8 is a diagram showing the circuit construction of the embodiment shown in Fig. 7; Fig. 9 shows wave forms at main parts of the circuit shown in Fig. 8; Fig. 10 is a circuit construction diagram showing one application example of this invention; Fig. 11 is a detailed view of the main part of the circuit of Fig. 10; Fig. 12 shows wave forms for explaining the operation of the circuit of Fig. 11; Fig. 13 is a detailed view of another main part of the circuit of Fig. 10; Fig. 14 shows wave forms for explaining the operation of the circuit of Fig. 13; Fig. 15 is a detailed view of still another main part of Fig. 10; and Fig. 16 shows wave forms for explaining the operation of the circuit of Fig. 15. In Fig. 1, a magnetic recording medium 4 with magnetic records is mounted on a rotary disk 3 fixed to a rotary shaft of a rotating body 1. An MR element 5 is mounted at a fixed position oppositely to the magnetic recording medium 4 with a small interval therebetween. The magnetic recording medium 4 may be formed either by adhering a magnetic tape or by attaching a magnetized magnetic substance. N and S poles are alternately recorded with an equal spacing therebetween. The MR element 5 has four magnet-resistive elements R₁₁, R₁₂, R₂₁ and R₂₂, as shown in Fig. 2. Each magnet-resistive element has a width sufficiently smaller than the pitch of N and S magnetic poles that are recorded on the magnetic recording medium. The elements R₁₁ and R₁₂, and R₂₁ and R₂₂, are connected in series with each other by low resistance parts C₁ and C₂, respectively, to form two groups of magnet-resistive elements, these groups are connected in series with each other by an additional low resistance part T. As shown in Fig. 3, the connection part T and low resistance parts V₁, V₂ at both ends form a three-terminal circuit. The MR element consists of magnet-resistive elements R₁₁, R₁₂, R₂₁ and R₂₂, and low resistive parts C₁, C₂, T, V₁ and V₂, which are formed by evaporating a ferromagnetic material such as permalloy on an insulator substrate 5B. The pattern is formed on one chip. Low resistance parts are realized by forming their widths sufficiently larger than those of the magnet-resistive elements. Therefore, the magnet-resistive elements and low resistance parts can be formed by the same material. Since the MR element can be fabricated by the same material at one time, the mass producibility is greatly improved. Furthermore, since the resistance of the parts other than those of the magnet-resistive elements can be neglected, the sensitivity of the MR element can be enhanced. The intervals between the magnet-resistive elements R₁₁ and R₁₂, and R₂₁ and R₂₂, are shown to be equal to the pitch P between N and S poles which are recorded on the magnetic recording medium 4. However, the intervals may take any value that is an integer multiple of P. Although the magnet-resistive elements R₁₂ and R₂₁ are shown to be spaced by P/2, the interval between R₁₂ and R₂₁ may take any value that is an odd multiple of P/2. Therefore, the interval between the magnet-resistive elements of the R₁₁ and R₁₂ group and those of the R₂₁ and R₂₂ group becomes an odd integer multiple of P/2. The magnet-resistive elements decrease their resistances with an increase of the intensity of a magnetic field independently of the N and S poles. Therefore, the magnet-resistive elements R₁₁ and R₁₂ which are spaced by an integer multiple of P vary their resistances by the same value. On the other hand, the elements R₁₁ and R₂₁, or the elements R₁₂ and R₂₂ which are spaced by an odd integer multiple of P/2 vary their resistances with a phase difference of 180°. If a voltage is applied across the terminals V₁ and V₂ and the body 1 is rotating, an a.c. voltage as shown in Fig. 4 can be detected at the intermediate terminal T. In this figure, the interval between the magnetic recording medium and the MR element which gives a wave form G₁ is smaller than that which gives a wave form G2. As can be understood from Fig. 4, when the interval is varied, all the resistances vary in the same way. Thus, the center value of the output voltage at the intermediate terminal is not changed by the variation of the interval but kept at a constant value v. Only the amplitude of the a.c. voltage varies. Therefore, not only signal processing can be made stably through d.c. amplification but also accurate signal detection becomes possible even when the rotating body 1 stops. Since the interval between the groups of magnet-resistive elements is made equal to an odd integer multiple of P/2, as mentioned before, magnet-resistive elements in each group vary their resistances alternately with the rotation of the rotating body 1. The rate of variation of the resistances is from 2 to 6%. Hence, the increment variation of the output voltage between the terminals V₂ and T is also from 2 to 6%. Especially, since the three terminals are positioned adjacent on the same side, as shown in Fig. 2, printing of lead wires from the MR elements can be easily done. This serves also for miniaturization of the MR element. Fig. 5 shows a modified example where the construction of Fig. 2 is made to be a bridge type. Namely, a series connection of resistive bodies R a , R b , R c and R d is connected across the power supply terminals V₁ and V₂, and resistive bodies are connected with each other by low resistance parts C₃, C₄ and T. These resistive bodies R a , R b , R c and R d and low resistance parts C₃, C₄ and T₀ are formed with the same material as the magnet-resistive elements. However, in order not to have any influence of the recorded poles one the magnetic recording medium, the resistive bodies R a , R b , R c and R d are positioned distant from the magnetic recording medium. The equivalent circuit of the construction of Fig. 5 is expressed by a bridge circuit, as shown in Fig. 6, where an output signal can be obtained between the terminals T₀ and T. In Fig. 5, R c , R d and T₀ may be omitted, and C₃ and C₄ may be formed in one united body as T₀. Next, another example with two bridge circuits is shown in Fig. 7. As an MR element 5, six thin film magnet-resistive elements R₁, R₂, R₁₁, R₁₂, R₂₁ and R₂₂ formed by a ferromagnetic material such as permalloy are disposed on a substrate 5B. T₀, T₁, T₂, V₁ and V₂ are terminals which form two bridge circuits with the magnet-resistive elements R₁ and R₂ as common sides. V₁ and V₂ are power supply terminals for the bridge circuits, and T₀, T₁ and T₂ are detection terminals. The magnet-resistive elements R₁ and R₂ serving as common sides are positioned distant from the magnetic recording medium 4 on the substrate 5B. The first bridge circuit consists of resistive elements R₁ and R₂ and magnet-resistive elements R₁ and R₁₂ on the opposite side, while the second bridge circuit consists of resistive elements R₁ and R₂ and magnet-resistive elements R₂₁ and R₂₂ on the opposite side. All the elements R₁₁, R₁₂, R₂₁ and R₂₂ are positioned adjacent to the magnetic recording medium 4. Now, define that half the wave length of the magnetic signals recorded on the magnetic recording medium 4, i.e. the pitch of the magnetic poles, is P. The magnet-resistive elsments R₁₁ and R₁₂ which are the components of the first bridge circuit are shifted by an odd integer multiple of P/4 from magnet-resistive elements R₂₁ and R₂₂ which are the components of the second bridge circuit. Further, magnet-resistive elements R₁₁ and R₂₁ are shifted by P/2 from magnet-resistive elements R₁₂ and R₂₂, respectively. In Fig. 8, since the magnet-resistive elements R₁ and R₂ are distant from the magnetic recording medium 4, the values of their magnetic resistance do not vary with the rotation of the magnetic recording medium 4. On the other hand, since the magnet-resistive elements R₁₁, R₁₂, and R₂₁, R₂₂ are adjacent to the magnetic recording medium 4, the values of their magnetic resistance vary with the rotation of the magnetic recording medium 4. Hence, outputs with a corresponding phase difference can be obtained between the terminals T₀ and T₁, and T₀ and T₂. Thus, when the detection terminals T₀ and T₁ are connected to a comparator, or an amplifier 6a, an output OUT 1 with a first phase related to the rotation of the rotating body 1 (cf. Fig. 1) is obtained. When the detection terminals T₀ and T₂ are connected to a comparator, or an amplifier 6b, an output OUT 2 with a second phase can be obtained. This relation will be explained next in more detail by using Fig. 9. Fig. 9(a) shows wave forms of a voltage u a between the terminals V₂ and T₀, a voltage u b between the terminals V₂ and T₁, and a voltage u d between the terminals V₂ and T₂. The voltage u a is independent of the rotation of the rotating body 1 and is a d.c. voltage which does not vary with rotation. When the magnet-resistive element R₁₁ is under the influence of the maximum magnetic field of N or S pole of the magnetic recording medium 4, the value of its magnetic resistance decreases. At this moment, the magnet-resistive element R₁₂ being at a position shifted by P/2 from R₁₁ is not influenced by the magnetic field of the N or S pole. Therefore, the voltage u b becomes smaller than u a . In this case, since the magnet-resistive elements R₂₁ and R₂₂ are lying in positions shifted by an equal distance from the center of N or S pole of the magnetic recording medium 4, they are subjected to a magnetic field of the same value. Therefore, the values of their magnetic resistance are decreased equally, and hence the voltage u d becomes equal to u a . As the rotating body 1 rotates and the magnet-resistive element R₂₂ is subjected to the maximum magnetic field, the element R₁₁ feels no magnetic field. Then, the voltage u d becomes smaller than u a . At this moment, since the magnet-resistive elements R₁₁ and R₁₂ are subjected to a magnetic field of the same value, the voltage u b becomes equal to u a . As the rotating body 1 rotates further, the magnet-resistive element R₁₂ feels the maximum magnetic field while R₁₁ feels no magnetic field. Hence, the voltage u b becomes larger than u a . Similar cycles as above are repeated. As a result, voltages u b and u d vary as shown in Fig. 9(a), giving two outputs with different phases. Since the values of magnetic resistance of the magnet-resistive elements are decreased by the magnetic fields of N and S poles in the same way, the frequency of the signals are twice as large as that of magnetic signals recorded in the magnetic recording medium 4. The output OUT 1 of the comparator 6a whose inputs are voltages u a and u b appears in the form of rectangular waves, only when the voltage u b is larger than u b , as shown in Fig. 9(b). The output OUT 2 of the comparator 6b appears as shown in Fig. 9(c). Although, in Fig. 6, the output OUT 1 has an advanced phase by 90° with respect to the output OUT 2, this phase relation is reversed if the rotation direction of the rotating body 1 is reversed. Thus, the direction of rotation can be discriminated. According to the embodiment of this invention performing the above-mentioned operation, the detection of rotation of a rotating body is possible. Furthermore, since magnet-resistive elements R₁ and R₂ placed in positions where their values of magnetic resistance do not vary with the rotation of the magnetic recording medium 4 are used as common sides of two bridge circuits, miniaturization of the MR element 5 can be realized. In the fabrication process of magnet-resistive elements, any irregularity of evaporation can be avoided, which facilitates an easy printing. This further helps the mass producibility much. Although the above mentioned embodiment related to a case with two bridge circuits, it may also be applied to a multi-phase case with more than two bridge circuits with the same effect. For example, three bridge circuits may be prepared so that the phases of the output signals have a difference of 120° from each other by disposing the two magnet-resistive elements in each bridge circuit shifted by P/3 from each other. Next, an example in which this invention is applied to a motor driving circuit will be explained with reference to Figs. 10 to 16. In Fig. 10, an H type bridge circuit of transistors 20, 21, 22 and 23 and another bridge circuit of diodes 24, 25, 26 and 27 are connected to a power supply E. Namely, the positive pole of the power supply E is connected with the collectors of transistors 20 and 22 and the cathodes of diode 24 and 26, while the negative pole is connected with the emitters of transistors 21 and 23 and the anodes of diode 25 and 27. The emitter of transistor 20, the collector of transistor 21, the anode of diode 24 and the cathode of diode 25 are connected with the one terminal of a motor 1. The emitter of transistor 22, the collector of transistor 23, the anode of diode 26 and the cathode of diode 27 are connected with the other terminal of the motor 1. The shaft of the motor 1 is coupled to a rotation detecting means R of this invention. A revolution signal 10, or the output of the rotation detecting means R, is introduced into a rotation direction detecting circuit DD, a position detecting circuit PD and a speed detecting circuit SD. A revolution direction signal 11, or the output of the rotation direction detecting circuit DD, is supplied to a microcomputer circuit 9 and the position detecting circuit PD. A position signal 12, or the output of the position detecting circuit PD, and a speed signal 13, or the output of the speed detection circuit SD are supplied also to the microcomputer circuit 9. Further, position instruction 18 and maximum speed instruction 19 are introduced to the microcomputer circuit 9 from extermal means. The microcomputer circuit 9 supplies a duty signal 14 and a forward-reverse rotation signal 15. A forward revolution output 16, or the output of a drive circuit 8, is supplied to the bases of transistors 21 and 22. A reverse rotation output 17, or another output of the drive circuit 8, is supplied to bases of transistors 20 and 23. The operation of the above construction is as follows. First, a position instruction 18 and a maximum speed instruction 19 are given to the microcomputer circuit 9, which reads in the speed signal 13 for examining the speed of the motor 1 and also the position signal 12 for examining the position of the motor 1. After calculation, the microcomputer circuit 9 gives to the drive circuit 8 a duty signal 14 for determining a voltage to be given to the motor 1 and a forward-reverse rotation signal 15 for determining the rotation direction of the motor 1. In the case of forward rotation, the drive circuit 8 gives the forward rotation output 16 to make transistors 21 and 22 conductive in accordance with the duty signal 14 and give a rotational force to the motor 1. At first, the position signal 12 of the motor 1 is different from the position instruction 18. This tends to increase the duty of the voltage given to the motor 1 and accelerate its rise time. As the speed of the motor 1 increases and the speed signal 13 approaches to the maximum instruction 19, the motor 1 generates a reverse rotation signal 17, in order to stop at the position instruction 18. As a result, transistors 20 and 23 are made conductive. This gives a damping force to the motor 1 so that the motor 1 may stop stably at the position instruction 18 as soon as possible. Each block as shown in Fig. 10 will be explained in more detail next. In the rotation direction detecting circuit DD shown in Fig. 11, a reference numeral 51 denotes a D type flip-flop. The one revolution signal OUT 1 of the rotation detecting means R shown in Fig. 9 is supplied to a clock terminal 52, while the other revolution signal OUT 2 is supplied to the input of a D terminal 53. The input of the clock terminal 52 works at the rising edge. The rotation direction signal 11, or the output of the flip-flop 51, is maintained at the level "1", as shown in Fig. 12, because if the revolution signal OUT 2 is advanced from the revolution signal OUT 1 of the two-phase outputs of the rotation detecting circuit R, the OUT 2 signal (input to the D terminal 53) is always at the ‴1 " level when the OUT 1 signal (clock signal) rises. When the rotation direction changes and the revolution signal OUT 2 lags behind the revolution signal OUT 1, the OUT 2 signal (input to D terminal) is at the "0" level when the OUT 1 signal (clock input) rises as can be seen from Fig. 12(A). Thus, the revolution direction signal 11 from the output terminal 54 of the flip-flop 51 is set at the "0" level. In this manner, the rotation direction can be detected from the rotation direction detecting circuit 5. Next, the position detecting circuit PD will be described in more detail with reference to Fig. 13. The circuit consists of an UP/DOWN counter 61 and a latch 62. The revolution signal 10 is used as a clock input to the UP/DOWN counter 61 while the revolution direction signal 11 is used as an UP/DOWN input. Outputs P₀ to P n of the UP/DOWN counter 61 are connected with the inputs of the latch 62. The position signal 12 is derived from the outputs of the latch 62. To a strobe terminal of the latch 62, a strobe signal 63 for latch is supplied. Further, the UP/DOWN counter 61 and the latch 62 have a reset terminal for receiving a reset input 64. The operation of the construction of Fig. 13 can be understood from time charts as shown in Fig. 14. The revolution signal 10 at the clock input is counted by the UP/DOWN counter 61. While the revolution direction signal 11 is at the "1" level, the counter 61 counts up as an UP counter, so that the counter output signals of the counter 61 vary as shown by P₀ to P₂. However, when the rotation of the motor 1 is reversed, the revolution direction signal 11 becomes "0" as shown in Fig. 14(A). The counter 61 counts down as a DOWN counter. The strobe signal 63 is supplied to the latch 62 at each prescribed time to latch the content of the UP/DOWN counter 61 and keep the position signal 12 always at a new value. At a moment when a new position instruction 18 is introduced into the microcomputer 9, both the UP/DOWN counter 61 and the latch 62 are reset by supplying a reset signal 64. The speed instruction circuit SD consists of a counter 71 and a latch 72, as shown in Fig. 15. The revolution signal 10 from the rotation detecting means R is supplied to the clock input of the counter 71, while a counter enable signal 73 with a prescribed period is supplied to an enable terminal. A counter reset signal 74 is supplied to a reset terminal. Output signals S₀ to S n of the counter 71 are the inputs to the latch 72. The outputs of the latch 72 constitute the speed signal 13. A latch strobe signal 75 is supplied to the latch 72. The operation of the circuit construction can be understood from time charts as shown in Fig. 16. The counter 71 continues to count the revolution signal 10 so long as the counter enable signal 73 is present, and generates output signals S₀ to S n . By the latch strobe signal 75 of the latch 72, the content of the output signals S₀ to S n is latched. At a next moment, the counter 71 is reset by the counter reset signal 74 to prepare for following countings. Since the revolution signal 10 is counted for a prescribed period as determined by the presence of the counter enable signal 73, a value proportional to the speed of the motor 1 can be obtained as the speed signal 13. The present invention may be applied to rotation control of various rotating bodies other than the above-mentioned examples. As described before, this invention is also applicable to a case in which the record interval in the magnetic body 5B is extremely narrow; that is, the signal density is extremely large. A further merit of this invention lies in the fact that the accuracy of forming the magnet-resistive elements is scarcely influenced by each pattern as formed on one chip, or by the method of formation. In summary, this invention provide a rotation detecting means for a rotating body, in which even if the spacing between the MR element and the magnetic recording medium on a rotating body varies, the center voltage of the outputs at the terminals of the magnet-resistive elements is maintained at a constant level, and additionally the sensitivity of the output signals is increased. Therefore, the invention can enjoy an excellent effect. Further, according to this invention the number of magnet-resistive elements and terminals used for the formation of an MR element can be reduced. Therefore, the magnet-resistive element can be fabricated in a small size. This is effective in improving the mass producibility.

Claims: 1. A rotation detecting means for a rotating body (1, 3) comprising: a magnetic recording medium (4) which is attached to said rotating body (1, 3) and has the form of a circular track whose centre is coincident with the axis of rotation of said rotating body, said track comprising N and S magnetic poles alternately recorded at a predetermined pitch P along said track and providing a magnetic field varying periodically in intensity along the track, two groups of magnetoresistive elements (R₁₁, R₁₂; R₂₁, R₂₂) disposed at a fixed reference position in front of said magnetic recording medium, the magnetoresistive elements (R₁₁, R₁₂; R₂₁, R₂₂) of each group being spaced apart of an interval of P or an integral multiple thereof in the rotation direction, the spacing between groups of magnetoresistive elements being equal to P/2 or an odd integral multiple thereof and the widths of said magnetoresistive elements in the rotation direction being made substantially smaller than the pitch P of said magnetic poles recorded on said magnetic recording medium (4), low resistivity parts (C₁; C₂) which connect said magnetoresistive elements of each group in series, a low resistivity part (T) which connects said two groups in series, and low resistivity parts (V₁, V₂) across which a prescribed voltage is applied to said two groups characterized in that the magnetoresistive elements are such that an increase in intensity of the magnetic field sensed thereby causes a decrease in their resistance, said decrease being independent of whether a N or S pole is being sensed each of said groups has only two magnetoresistive elements (R₁₁, R₁₂; R₂₁, R₂₂); all magnetoresistive elements (R₁₁, R₁₂; R₂₁, R₂₂) and the corresponding low resistivity parts (T; V₁, V₂; C₁, C₂) are formed integral as one piece, an output signal related to the rotation state of said rotating body is derived from said connection part (T) between said two groups, without any bias magnetic field being applied, in that said magnetic recording medium (4) and said magnetoresistive elements (R₁₁, R₁₂; R₂₁, R₂₂) are disposed opposite to each other with parallel directions of extension and in that all magnetoresistive elements (R₁₁, R₁₂; R₂₁, R₂₂) consist each of a single linear strip, the low resistivity parts (T, V₁, V₂) constituting terminlas connecting said two groups of linear strips in series and across which a voltage is applied, respectively, are positioned adjacent on the same side of said strips. 2. A rotation detecting means for a rotating body according to claim 1, characterized by voltage dividing resistive means (R a , R b , R c , R d , C₃, C₄, T₀) connected in parallel with said two groups of series connection, in which said output signal is derived between said connnection part (T) and a voltage dividing terminal portion (T₀) of said voltage dividing resistive means. 3. A rotation detecting means for a rotating body (1, 3) comprising: a magnetic recording medium (4) which is attached to said rotating body (1, 3) and has the form of a circular track whose centre is coincident with the axis of rotation of said rotating body, said track comprising N and S magnetic poles alternately recorded at a predetermined pitch P along said track and providing a magnetic field varying periodically in intensity along the track, two groups of magnetoresistive elements (R₁₁, R₁₂; R₂₁, R₂₂) at a fixed reference position in front of said magnetic recording medium, the widths of said magnetoresistive elements in the rotation directing being made substantially smaller than the pitch P of said magnetic poles recorded on said magnetic medium (4), low resistivity parts (T₁, T₂, V₁, V₂) comprising first parts (T₁, T₂) which connect correspondingly said magnetoresistive elements of each group in series and second parts (V₁, V₂) which connect the two groups in parallel to apply a prescribed voltage to each group, output signals related to the rotation state of said rotating body being derived from said first connection parts (T₁, T₂) of said two magnetoresistive elements of each group, voltage dividing resistive means (R₁, R₂) which are connected to the second parts (V₁, V₂) for setting a common reference voltage of each group, the intervals between the groups of magnetoresistive elements being shifted from each other so that output signals have a phase difference, characterized in that the magnetoresistive elements are such that an increase in intensity of magnetic field sensed thereby causes a decrease in their resistance, said decrease being independent of whether a N or S is being sensed, without any bias magnetic field being applied, each of said groups has only two magnetoresistive elements (R₁₁, R₁₂; R₂₁, R₂₂), all magnetoresistive elements (R₁₁, R₁₂; R₂₁, R₂₂) and the corresponding low resistivity parts (T₀; V₁, V₂; T₁, T₂) are formed integral as one piece, the magnetoresistive elements of each groups being spaced apart of an interval of P/2 or an odd integral multiple thereof in the rotation direction, in that said magnetic recording medium (4) and said magnetoresistive elements (R₁₁, R₁₂; R₂₁, R₂₂) are disposed opposite to each other with parallel directions of extension and in that all magnetoresistive elements (R₁₁, R₁₂; R₂₁, R₂₂) consists each of a single linear stripe, the low resistivity parts (T₀; V₁, V₂) constituting terminals connecting said two groups of linear stripes in series and across which a voltage is applied, respectively, are positioned adjacent on the same side of said stripes. 4. A rotation detecting means for a rotating body (1, 3) according to claim 1, 2 or 3, characterized in that said magnetoresistive elements (R11, R12; R21, R22) and said low resistive parts (C₁, C₂, C₃, C₄, T₀, T₁, T₂, V₁, V₂) are formed by the same material and the widths of those parts other than the parts for forming said magnetoresistive elements are large enough to have a low resistivity. 5. A rotation detecting means for a rotating body (1, 3) according to claim 4 in connection with claim 3, characterized in that said voltage dividing resistive means (R₁, R₂; T₀, C₃, C₄) are formed by the same material as that of said magnetoresistive elements (R11, R12; R21, R22) and disposed at positions free from the fnfluence of said magnetic poles recorded on said magnetic recording medium (4). 6. A rotation detecting means for a rotating body according to claim 3, characterized in that the magnetoresistive elements (R11, R12) of the one group and the magnetoresistive elements (R21, R22) of the other group are disposed in such a manner that the interval between said groups is equal to P/4 or an odd number multiple thereof.

Inventors: HAYASHIDA, HIROSHI, MIYASHITA, KUNIO, SEKIZAWA, SADAO, TAKAHASHI, TADASHI
Applicants: HITACHI, LTD.
Application year: 1981
Main classification: G01D5
IPC codes: G01D5, G01P13, G01P3