Torque detecting apparatus with abnormality signal

Abstract: A torque detecting apparatus comprises a first magnetic angular sensor (3A, 4A) outputting a sine-wave output (E A1 ) and a cosine-wave output (E B1 ) corresponding to positions of rotation of a rotary drum (2A) being fitted a rotating drive shaft (1). A second magnetic angular sensor (3B, 4B) outputs a sine-wave output (E A2 ) and a cosine-wave output (E B2 ) corresponding to positions of rotation of another rotary drum (2B) being fitted on the rotating drive shaft (1). In case of the respective other output of the sine-wave output or the cosine-wave output of the first or the second magnetic angular sensor is varied while one output of the sine-wave output or the cosine-wave output in the first or the second magnetic angular sensor is not varied, the one output cosine-wave output or the sine-wave output of the first or the second magnetic angular sensor is determined to be faulty and an abnormality signal is delivered by a judging means.

Description: The present invention relates to a torque detecting apparatus of the kind referred to in the precharacterizing portion of patent claim 1. Such an apparatus is known from US-A-4 660 671. Conventional torque detecting apparatuses are so constructed that the outputs are obtained from each of the magnetic sensors respectively corresponding to the angles of rotation of the rotary drums fitted to the opposite ends of the rotating drive shaft and the phase difference signals from these magnetic sensors are executed to determine a torque by an executing circuit, as shown in JP-A-239031/1987 for example. In the prior art stated above, no consideration is given about a method of detecting a torque when the rotating drive shaft stops, and further no consideration is given at all to the fault of the magnetic sensors itself such as wire break-down and short circuit and others such as break-down and short circuit in wiring, which produces a problem that the fault cannot be detected. US-A-4 660 671 discloses a torque detecting apparatus comprising a first rotary body being fitted on a drive side on a rotating drive shaft, a second rotary body being fitted on a load side rotating drive shaft, a first position detecting means being disposed oppositely and facing said first rotary body, a second position detecting means being disposed oppositely and facing said second rotary body, said first position detecting means generates a first output and a second output corresponding to positions of rotation of said first rotary body, said second position detecting means generates a third output and a fourth ouput corresponding to positions of rotation of said second rotary body, and a torque computing means deriving a first rotational angle from said first output of said first position detecting means and said second output of said first position detecting means and deriving a second rotational angle from said third output of said second position detecting means and said fourth output of said second position detecting means and further computing a torque from a phase difference between said first angle and second rotational angle. An object of the present invention is to provide a torque detecting apparatus wherein a fault of a position detecting means itself such as a magnetic angular sensor can be detected easily. Another object of the present invention is to provide a torque detecting apparatus wherein a fault of an electric wiring of a position detecting means such as a magnetic angular sensor can be detected easily. A further object of the present invention is to provide a torque detecting apparatus wherein an abnormality signal of a position detecting means such as a magnetic angular sensor can be sent to a system so as to protect the torque detecting apparatus. A further object of the present invention is to provide a torque detecting apparatus wherein an abnormality signal of a position detecting means such as a magnetic angular sensor can be sent to a system such as an electric driven power steering assist construction so as to protect the system. A further object of the present invention is to provide a torque detecting apparatus wherein an abnormality signal of a position detecting means such as a magnetic angular sensor can be sent to a system such as an electric driven power steering assist construction so as to prevent an unexpected or undesirable operation of the system. In accordance with the present invention, these objects are accomplished with a torque detecting apparatus as claimed. Dependent claims are directed on features of preferred embodiments of the invention. According to the present invention, any fault of a torque detecting apparatus can be detected easily. Therefore, since any abnormality and fault in the torque detecting apparatus can be detected, an unexpected or an undesirable operation of the torque detecting apparatus is prevented, thus high safety in the torque detecting apparatus can be secured. Further, any fault in a torque controlling apparatus for an electric power assist construction is detected easily when an assist torque means such an electric motor is cut off from a rotating drive shaft. Therefore, an unexpected or an undesirable operation of the torque controlling apparatus is prevented, thus high safety in the torque controlling apparatus can be secured. Brief Description of the Drawings: Fig. 1 is a schematic structural view of one embodiment of a torque detecting apparatus according to the present invention; Fig. 2 is a detailed view of a rotary drum and a magnetic angular sensor constituting a torque detecting apparatus; Fig. 3A is a developed view of a magnetic substance of a rotary drum; Fig. 3B is a plan view of a magnetic angular sensor in relation to a magnetic substance of a rotary drum; Fig. 4 is an illustration of magnetic poles recorded on a magnetic substance of a rotary drum and of outputs of the torque sensor; Fig. 5 is a connection diagram of a three-terminal contact of magnetro-resistance effect elements; Fig. 6A is a diagram of output waveforms obtained from a middle point of a three-terminal contact; Fig. 6B is a diagram of output waveforms obtained from a middle point of a three-terminal contact; Fig. 7A is diagrams for a method of detecting a load torque on the basis of the same output waveforms obtained from a magnetic angular sensor; Fig. 7B is diagrams for a method of detecting a load torque on the basis of the same output waveforms obtained form a magnetic angular sensor; Fig. 8A is diagrams of one embodiment of a magnetic angular sensor of the present invention for obtaining sine-wave outputs; Fig. 8B is a connection diagram of magnetro-resistance effect elements; Fig. 9 is a developed view of a rotary drum and a magnetic angular sensor of another embodiment of the present invention; Fig. 10 is a connection diagram of the magnetic angular sensor of Fig. 9; Fig. 11 is a circuit construction diagram for an electric driven power steering construction according to the present invention; Fig. 12 is a flow-chart for calculating a torque according to the present invention; Fig. 13 is an illustration for explaining an operation for an electric driven power steering construction according to the present invention; Fig. 14 is a flow-chart of detection of a speed and a position of the other embodiment for an electric driven power steering construction according to the present invention; Fig. 15 is a structural view of a torque controlling apparatus using the torque sensor according to the present invention; Fig. 16 is a schematic structural view another embodiment of an electric driven power steering assisting apparatus for an automobile according to the present invention; Fig. 17 is diagrams of detection of a fault according to the present invention; Fig. 18 is a flow-chart of detection of a fault according to the present invention; Fig. 19 is a flow-chart of one embodiment of a countermeasure to noise according to the present invention; Fig. 20 is a flow-chart of a normal operation of one embodiment of assist for an electric driven power steering construction of an automobile; Fig. 21 is a flow-chart of an abnormality processing of one embodiment of assist for an electric driven power steering construction of the automobile; Fig. 22 is a flow-chart of another embodiment covering a procedure from judgment of a fault to the abnormality processing according to the present invention; and Fig. 23 is a schematic structural view of still another embodiment of a torque detecting apparatus according to the present invention. Description of the Invention: One embodiment of a torque detecting apparatus will be explained according to the present invention. In Fig. 1, a rotating drive shaft 1 has rotary drums 2A and 2B at both end portion. The rotating drive shaft 1 serves also as a drive shaft. The rotary drums 2A and 2B have magnetic substances 3A and 3B whereon magnetic signals N - S are recorded are fixed separately by a gap L on the rotating drive shaft 1. Magnetic angular sensors 4A and 4B are constructed of magneto-resistance effect elements (hereinafter called as MR elements). These magnetic angular sensors 4A and 4B face the rotary drums 2A and 2B respectively and are disposed with a small gap therefrom. A description will be made hereupon in respect to the operations of the rotary drums 2A and 2B and the magnetic angular sensors 4A and 4B by using Fig. 2. Fig. 2 shows the rotary drum 2A and the magnetic angular sensor 4A taken out for explaining the operations. As mentioned above, the magnetic signals of N and S are recorded on the whole circumference of the magnetic substance 3A of the rotary drum 2A, and the magnetic angular sensor 4A constructed of MR elements R₁, R₂, R₃ and R4 is disposed oppositely thereto with the small gap ℓ therefrom. Fig. 3A and Fig. 3B are enlarged developed views showing the relationship in disposition between the magnetic substance 3A on the rotary drum 2A and the magnetic angular sensor 4A, which are shown in Fig. 2. In Fig. 3B, the MR elements R₁, R₃, R₂ and R₄ are disposed separately by λ/4 in relation to a magnetic recording wavelength (a gap between an N-pole and an S-pole) λ. Fig. 4 shows the operating waveforms of the MR elements. In Fig. 4, the magnetic substance 3A of the rotary drum 2A moves as indicated by an arrow mark shown in the figure, with the rotation of the rotary drum 2A. On the other hand, the MR elements R₁ and R₂ have a characteristic that the resistance value thereof lowers when either one signal of magnetic flux variation of the N-pole and the S-pole of the magnetic signals is applied thereto, as is known well. When the magnetic substance 3A moves as indicated by the arrow mark, therefore, the changes of resistances of the MR elements R₁ and R₂ are obtained in accordance with the recording wavelength λ, and the change of resistance of each MR element has a waveform shifted in phase by λ/2 from that of the other. The MR elements R₁ and R₂ are connected in series as shown in Fig. 5, and an output terminal E A1 is taken out from the middle point of the MR elements and connected to three-terminals including the output terminal E A1 . When a voltage V is applied to the opposite both ends, a voltage obtained then from the output terminal E A1 has a waveform as shown in Fig. 6A, and thus an output E A1 corresponding to the magnetic signal recorded on the magnetic substance 3A can be obtained. The MR elements R₃ and R₄ are shifted by λ/4 from the MR elements R₁ and R₂, and therefore an output E B1 being different in phase by 90 degrees from the output E A1 is obtained likewise from the MR elements R₃ and R₄. Besides, waveforms or outputs E A2 and E B2 shown in Fig. 6B are obtained likewise from the rotary drum 2B and the magnetic angular sensor 4B of Fig. 1 by the same operation. When a motor is fitted on the drive side of the rotating drive shaft 1 and a load on the load side thereof, for instance, in the torque detecting apparatus of Fig. 1, the rotating drive shaft 1 is twisted by an angle ϑ in proportion to a load torque given thereto. This relationship is expressed by the following equation. Herein mark ϑ denotes a torsion angle (rad), G a shear coefficient (kg/cm²) of the rotating drive shaft 1, L a distance (cm) between the rotary drums 2A and 2B, and D the diameter (cm) of the rotating drive shaft 1. The shear coefficient G is determined by the material of the rotating drive shaft 1, and so a torque T in relation to the torsion angle ϑ is found when the distance L between the rotating drums 2A and 2B and the diameter D of the rotary drive shaft 1 are set. Accordingly, the measurement of the torque is enabled by detecting the torsion angle ϑ of the rotating drive shaft 1. One example of a method for measuring the torsion angle ϑ of the rotating drive shaft 1 is shown in Fig. 7A and Fig. 7B. In Fig. 7A, the torsion ϑ of the rotating drive shaft 1 is found by measuring a phase difference (ϑ₂ - ϑ₁) at the zero cross of the magnetic angular sensor 4A and the output E A2 obtained from the rotary drum 2B and the magnetic angular sensor 4B. As shown in Fig. 7A, in other words, the amount of the torsion of the rotating drive shaft 1 is small when the load torque is small, and therefore a phase difference ϑ s at the zero cross of the outputs E A1 and E A2 turns to be small as well. In the case when the load torque is large as shown in Fig. 7B, to the contrary, the amount of the torsion of the rotating drive shaft 1 is also increased, and therefore a phase difference ϑ m at the zero cross turns to be large. Accordingly, the amplitude of the torque can be detected by measuring this phase difference ϑ s or ϑ m . While the phase difference at the zero cross of the signals of the outputs E A1 and E A2 of the magnetic angular sensors 4A and 4B is determined in the example of Fig. 7, the torque can be detected also in a place other than the zero cross. When the outputs E A1 and E B1 , and the outputs E A2 and E B2 are sine waves, the angles of the magnetic drums can be measured from the amplitudes of the sine waves respectively, and therefore the torque can be measured with high resolution by finding the difference between the angles of the rotary drums 4A and 4B. Fig. 8A and Fig. 8B are illustrations of the principle on the basis of which sine waves are obtained by the magnetic angular sensor 4A of MR elements. Magneto-resistance effect elements (MR elements) R₁₁ and R₁₅, and MR elements R₁₂ and R₁₆ of the magnetic sensor 4 are disposed separately by λ/2 in relation to a recording wave λ, while the MR elements R₁₁ and R₁₂, and the MR elements R₁₅ and R₁₆, are disposed separately by λ/6 from each other, respectively. Since the MR elements R₁₁, R₁₂, R₁₅ and R₁₆ are connected in such a disposition as shown in Fig. 8B, an output e a obtained from the MR elements R₁₁ and R₁₅ turns to be one as indicated by a solid line e a of Fig. 8A when the rotary drum 2A rotates. This waveform distortion occurs because the change of resistance of the MR element is saturated in relation to a magnetic field. Therefore the main component of this distorted wave is a tertiary harmonic, and the wave can be separated into a fundamental wave e a1 and the tertiary harmonic e a3 as indicated by broken lines in Fig. 8A. An output e b obtained from the MR elements R₁₆ and R₁₂ is turned also into a fundamental wave e b1 and a tertiary harmonic e b3 . When a bridge output (e a + e b ) i.e., the output E A1 , shown in a connection diagram is considered, the tertiary harmonics e a3 and e b3 are reverse in phase to each other and canceled by each other consequently, and thus only the fundamental wave is obtained. Fig. 9 is a developed view of a magnetic substance of a rotary drum and a magnetic angular sensor of one embodiment wherein the magnetic angular sensor outputting a sine wave is employed for the torque sensor. A base 41 is formed of a glass material or the like and bearing MR elements. A rotary drum 21 on the drive side is provided with a magnetic track 311 of a magnetic substance, whereon magnetic signals of N-S are recorded successively at a recording pitch λ. There are two magnetic tracks 321 and 322 on a rotary drum 22 on the load side, and magnetic signals of the recording pitch λ are recorded on magnetic track 321 successively in the same way as on the magnetic track 311 of the rotary drum 21. On the magnetic track 322, only one magnetic signal of the recording pitch λ is recorded. On a magnetic angular sensor 4 facing the rotary drums 21 and 22, MR elements R₁₁-R₁₈ and R₂₁-R₂₈ are disposed as shown in the figure. Namely, for the rotary drum 21, MR elements R₁₁-R₁₈ are disposed for the rotary track 321, and MR elements R₂₁-R₂₈ are disposed for the magnetic track 321 of the rotary drum 22. Moreover, MR elements R₃₁ and R₃₂ are disposed for the magnetic track 322. Besides, the MR elements R₁₁ and R₁₂, R₁₃ and R₁₄, R₁₅ and R₁₆, R₁₇ and R₁₈, R₂₁ and R₂₂, R₂₃ and R₂₄, R₂₅ and R₂₆, and R₂₇ and R₂₈, are disposed separately by λ/6 from each other, respectively, while the MR elements R₁₁, R₁₃, R₁₅, R₁₇, and R₂₁, R₂₃, R₂₅, R₂₇, and further R₃₁, R₃₂, are disposed separately by λ/4 from each other, respectively. The magnetic angular sensor has at least four sets of a first MR element array having MR elements and a second MR element array having MR elements disposed separately by an electrical angle of n ± λ/6 (n:an integer) from each other respectively, and a third MR element array having MR elements delivering a reference signal. The respective two sets of the first MR element array and the second MR element array are disposed separately by an electric angle of n ± λ/6 from each other. The two sets of the first MR element array and the second MR element array are disposed separately by each other by n ± λ/6 from each other being spaced by an electrical angle of n ± λ/6 from the other two sets of MR element arrays. These MR elements are connected in such a manner as shown in Fig. 10, so as to obtain outputs e₀-e₈ therefrom. The outputs e₁-e₂, e₃-e₄, e₅-e₆ and e₇-e₈ of bridges formed by the MR elements R₁₁, R₁₂, R₁₅ and R₁₆, R₁₃, R₁₄, R₁₇ and R₁₈, R₂₁, R₂₂, R₂₅ and R₂₆, and R₂₃, R₂₄, R₂₇ and R₁₆, have the same constructions as that in Fig. 8, and sine-wave outputs are obtained therefrom. The output formed by the MR elements R₃₁ and R₃₂ is provided for obtaining an output of one pulse in one rotation, which is used as a reference position signal. These outputs e₀-e₈ are amplified by processing circuits shown in Fig. 11, subjected to analog-digital conversion and taken in a microcomputer (MC) so as to perform the computation of a torque. Fig. 11 shows a construction wherein differential amplification is conducted by fixed resistors R₀₁-R₀₄ and an amplifier AMP₁, and an output thereof is inputted to an analog-digital converter ADC₁. Four sets of the same constructions are employed and four kinds of voltages e₁-e₂, e₃-e₄, e₅-e₆ and e₇-e₈ being equivalent to the output voltages E A1 , E B1 , E A2 and E B2 of Fig. 6 are inputted to the respective inputs thereof, while outputs A₁, B₁, A₂ and B₂ are delivered therefrom. Four sets of signals A₁, B₁, A₂ and B₂ converted by ADC₁-ADC₄ are inputted to the microcomputer (MC) respectively. The reference signal e₀ of one rotation is passed through a comparator (CM₁) and an output pulse thereof is inputted to the microcomputer (MC). A position information, a speed information, a torque output, etc., which are computed on the basis of the reference position signal in the microcomputer (MC), are outputted respectively from output terminals 12, 13 and 14 to send the signals to a system. Moreover, an abnormality signal is outputted from an output terminal 15 in the case of the torque sensor being faulty, on which a description will be made later. In the microcomputer (MC), an arithmetic operation is executed in conformity with a flow-chart to be shown in Fig. 12, and an output being proportional to a torque is presented to the output terminal 14. According to the flow-chart of Fig. 12, first the outputs of the magnetic angular sensors 4A, 4B are amplified and then subjected to A/D conversion, and digital values A₁, B₁, A₂, B₂ thus obtained are read in. Next, such a execution as expressed by the following equation is executed by using A₁ and B₁, so as to find an angle ϑ₁ of the rotary drum 2A. The plus and minus of A₁ and B₁ are discriminated herein, the mode thereof is determined, and the value of ϑ₁ is decided. The angle ϑ₂ of the rotary drum 2B is calculated likewise on the basis of the inputs A₂ and B₂ by the following equation. Next, an angular difference between the rotary drums 2A and 2B, i.e. a torsional angle ϑ₀, is calculated from the difference between the angles ϑ₁ and ϑ₂, and a torque T is calculated by the following equation obtained by transformation of the equation (1). Then, the torque T is outputted and a return is made to the initial state. Herein the value ϑ₁ of the equation (2) can be calculated by using only A₁ or B₁, as expressed by an equation (5). The outputs A₁ and B₂ are varied simultaneously, ϑ₁ = sin⁻¹(A₁) = cos⁻¹(B₁) (5) however, when the outputs of the magnetic angular sensors 4A and 4B are varied due to a change in a small gap (spacing) between the rotary drum 2A or 2B and the magnetic angular sensor 4A or 4B, or the like, and therefore the accuracy can be made higher by such a division of A₁ by B₁ as expressed in the equation (2). Fig. 13 shows an operation according to the flow-chart of Fig. 12. The signals A₁ and B₁, which are obtained from the MR elements R₁₁-R₁₈ constituting the first magnetic angular sensor and are inputted to the microcomputer (MC), are a sine wave and a cosine wave as shown in Fig. 13. When the plus and minus of signal A₁ and signal B₁ are determined, first, they are divided as indicated by signal A 1F and signal B 1F . If signal A 1F and signal B 1F are regarded as signals of 2 bits, they can be divided into four modes shown in Fig. 13. Besides, the relationship between a value D obtained by dividing the sine wave A₁ by the cosine wave B₁ and the angle ϑ₁ is as shown in Fig. 13, and the value thereof turns to be ∞ at each angle of ± 90 degrees and each angle 180 degrees. Regarding the signals A₂ and B₂ obtained from the MR elements R₂₁-R₂₈ constituting the second magnetic sensor, such a relationship between the angle ϑ₂ and the value D as shown in Fig. 13 can be obtained also just in the same way. Although the value D of A₁/B₁ is the same at two points between 0° and 360°, the angle thereof can be discriminated because of a difference in a mode. Now, when the angles ϑ₁ and ϑ₂ are determined from the outputs of the first and second magnetic sensors at a point (a), ϑ₁ = 0 and ϑ₂ = -30 degrees, and accordingly the angular difference between them is (ϑ₁ - ϑ₂) = 30 degrees. A torque corresponding thereto can be calculated from the equation (4). When the angles are measured likewise at a point (b) after a certain time passes from the point (a), ϑ₁ = 60 degrees and ϑ₂ = 30 degrees, thus the angular difference (ϑ₁ - ϑ₂) turning to be 30 degrees. Accordingly, the same torque can be detected at any points on condition that the torque is fixed. Fig. 14 is a flow-chart for detecting a rotational position and a rotational speed. First the digital inputs A₁ and B₁ of sine waves are taken in, a time t of a timer for measuring a speed is read and stored temporarily, and then the timer is re-started. Next, the minute angle ϑ₁ within one cycle is obtained by the calculation according to the equation (2) in the same way as in the detection of torque. Then, a minute angle ϑ n-1 obtained previously is read out of a memory, a difference between this angle and the present angle ϑ n is calculated to find a change (ϑ n-1 - ϑ n ) in the angle, value thus found is divided by the time difference t between the previous and present angles stored temporarily before, so as to calculate a speed v , and this is outputted to an output terminal 13. As for the calculation of a position, the cumulation ϑ Σn-1 of angles obtained till the preceding time is added to the difference between the present minute angle ϑ n and the previous minute angle ϑ n-1 , so as to calculate the current angle ϑ Σn . Next, the reference position signal is taken in, and when there comes any signal, the current angle ϑ n is altered to ϑ Σn so as to be matched with a reference value. Then, the value ϑ Σn is outputted to an output terminal 12. Subsequently the present minute position ϑ n is put in the memory of ϑ n-1 , while the current angle ϑ n is put in the previous angle ϑ n-1 , and a return is made to the start. The foregoing description relates to an example wherein the minute angle ϑ n and the previous minute angle ϑ n-1 are found within one cycle, and when the angle is varied beyond one cycle, calculation is conducted by using the cumulation of angles. Fig. 15 shows a torque controlling apparatus wherein the present torque sensor is employed. A comparison is made between a torque instruction value (CM) and an output of a torque sensor (TS), and an electric current applied to a motor (M) and the direction of rotation thereof are controlled by a control circuit (CC) in accordance with a value obtained from the comparison. This is one example wherein an output of the motor (M) is detected by the torque sensor (TS) and checked and compared with the torque instruction value (CM). Fig. 16 shows a driving force assisting apparatus using the torque sensor (TS), which is an electric drive power assist steering construction an automobile, in the concrete. The electric driven power assist steering construction has a construction wherein the torque sensor (TS) of Fig. 1 is fitted to a steering wheel shaft (HS), which is the shaft of a steering wheel (SW), the steering wheel (SW) is provided as the drive side while the torque of the motor (M) is transmitted onto the load side, and a wheel (W) is steered through the intermediary of a pinion gear (PI) and a rack gear (LA) provided in the fore end of the steering wheel shaft (HS). When a driver operates the steering wheel (SW) and thereby a torque is given to the torque sensor (TS), this torque is detected according to an instruction, and a current or a direction of rotation matched with the torque is outputted by a control circuit (CC) so as to drive the motor (M). The torque of the motor (M) is transmitted for steering through the pinion gear (PI) and the rack gear (LA), so as to compensate the power of the driver. As is seen from these examples of employment, any fault of the torque sensor (TS) causes a false operation of the driving force assisting apparatus, thus bringing forth a great danger. Fig. 17 shows an example of fault judgment for judging the fault of the torque sensor (TS) to take a step for safety quickly. This figure shows the waveforms of the signals A₁ and B₁ of Fig. 11. The signals A₁ and B₁ appear normally between the times t₁ and t₂ and the signal B₁ turns faulty due to a fault at the time t₂ in this example. Values of the output are varied from (a) to (n) according to the cause of abnormality, and the output ceases to vary when the abnormality occurs. In contrast, the signal A₁ continues to give a normal output. Accordingly, the occurrence of the fault can be detected by checking that the signal B₁ is not varied while the signal is varied. The same can be detected also by checking a state of variation of the signal A₁ while the signal B₁ is varied. Fig. 18 is a flow-chart for detecting abnormality. First the signals A₁ and B₁ are taken in, and a mode is determined from each signal. Next, values A 1(n-1) and B 1(n-1) of the previous signals stored in a memory are compared sequentially with the present values. Judgment of being normal is made when both signals are varied or when neither of them is varied, and the calculation of a normal torque is conducted so as to execute normal driving. When the comparison of the signals A₁ and B₁ with the previous values shows that one of them is varied while the other is not varied, either one of the signals is judged to be abnormal, and a processing to cope with the abnormality is executed. The same operation is conducted also with regard to the signals A₂ and B₂. Fig. 19 is a flow-chart for preventing the judgment of abnormality due to electric noise. According to this flow-chart, the signal A₁ or B₁ is read twice at a certain short time interval, and the judgment of being abnormal is made when the values thereof are equal substantially, while the judgment of being affected by noise is made when the values are different in a large degree. In the latter case, the judgment of being abnormal is not made and a return is made to the start. Fig. 20 shows a sequence of normal operations in the case when it is applied to the driving force assisting apparatus shown in Fig. 16, that is, to the assistance of steering of an automobile. In the normal operations, the torque of a motor is decided and the direction of rotation of the motor is determined in accordance with an output of the torque sensor, and subsequently a current made to flow through the motor and the direction of rotation are outputted. Fig. 21 shows one example of a processing in abnormality in the case when it is used for a steering force assisting control apparatus of the same automobile. First an abnormality signal and an alarm are outputted. Then, driving f the motor is stopped, and simultaneously a clutch fitted onto the load side is released so that the motor may not be a load on steering. Fig. 22 is a flow-chart of the case when the stop is not made at once even when any abnormality occurs, a torque being detected for some time only by signals of one magnetic sensor, and the processing for the abnormality being executed after some time passes. First, judgment on a fault is made by a method as shown in Fig. 18, and when the fault is judged to be present, a primary alarm is outputted. Next, the value ϑ₁ is calculated by using the signal A₁ or B₁ not being faulty. Although modes can not be discriminated due to the fault of one output and consequently two values of ϑ₁ come out, the value nearer to a value of ϑ 1(n-1) used in the preceding calculation is selected as ϑ₁. Then, ϑ₂ is calculated in the same way, the difference ϑ between the two angles ϑ₁ and ϑ₂ is calculated, and a torque is calculated therefrom. Subsequently, the number N in the preceding time is made to be (N+1), and it is checked whether N becomes a certain number N₀ or not. The abnormality processing is executed when N is N₀, while a normal operation is conducted when N is less than N₀. According to this method, the motor is not stopped immediately even when any fault occurs, and it is stopped gradually with a time for preparation secured. Therefore, it may be said that this method is a safe and practical method. Fig. 23 shows an example of employment of magnetic discs. In this example, the magnetic disks are fixed on the right and left of a shaft, and the positions of the disks are detected by two magnetic sensors facing them respectively.

Claims: A torque detecting apparatus comprising a first rotary body (2A) being fitted on a drive side on a rotating drive shaft (1), a second rotary body (2B) being fitted on a load side rotating drive shaft, a first position detecting means (3A, 4A; R₁₁-R₁₈) being disposed oppositely and facing said first rotary body, a second position detecting means (3B, 4B; R₂₁-R₂₈, R₃₁, R₃₂) being disposed oppositely and facing said second rotary body (2B), said first position detecting means (3A, 4A) generates a first output (E A1 ; e a , e₁, e₃) and a second output (E B1 ; e b , e₂, e₄) corresponding to positions of rotation of said first rotary body (2A), said second position detecting means (3B, 4B) generates a third output (E A2 ; e₅, e₆) and a fourth ouput (E B2 ; e₇, e₈) corresponding to positions of rotation of said second rotary body (2B), and a torque computing means (MC) deriving a first rotational angle from said first output of said first position detecting means and said second output of said first position detecting means and deriving a second rotational angle from said third output of said second position detecting means and said fourth output of said second position detecting means and further computing a torque from a phase difference between said first angle and second rotational angle, characterized in that said torque computing means (MC) comprises further a judging means judging whether a fault appeared and arranged to output an abnormality signal (15 in Fig. 11), when one of said first and second outputs of said first position detecting means (3A, 4A) is detected to be faulty; said abnormality signal (15) being delivered, if the respective other output of both outputs of said first position detecting means (3A, 4A) is detected to be varied while the one output of both outputs of said first position detecting means (3A, 4A) is detected to be not varied, one of said two outputs of said first position detecting means (3A, 4A) is a sine-wave-output and the respective other output is a cosine-wave output and one output of said two outputs of said second position detecting means (3B, 4B) is a sine-wave and the respective other output is a cosine-wave output. A torque detecting apparatus according to claim 1, characterized in that said judging means are judging a fault and outputting an abnormality signal, when one of said third and said fourth outputs of said second position detecting means is determined to be faulty; said abnormality signal being delivered, if the respective other output of both outputs of said second position detecting means is detected to be varied while said one of both outputs of said second position detecting means (3B, 4B) is detected to be not varied. A torque detecting apparatus according to claim 1, characterized in that for deriving the rotational angle of said first rotary body (2A) a quotient of said sine-wave output and said cosine-wave output is calculated. A torque detecting apparatus according to claim 1, characterized in that, for deriving the rotational angle of said second rotary body (2B) a quotient of said sine-wave output and said cosine-wave output is calculated. A torque detecting apparatus according to claim 1, characterized in that when one of said sine-wave output and said cosine-wave output of said first position detecting means does not change while the respective other output is changed, said unchanged output is determined to be the faulty output and said abnormality signal is generated, while the calculation of the rotational angle is carried out only on the basis of the changing output and a value nearest to a preceding torque is used. A torque detecting apparatus according to claim 4, characterized in that, when one of said sine-wave output and said cosine-wave output of said second rotary body does not change while the respective other output is changed, said unchanged output is determined to be the faulty output and said abnormality signal is generated, while the calculation of the rotational angle is carried out only on the basis of the changing output and a value nearest to a preceding torque is used. A torque detecting apparatus according to claim 1, characterized in that said first rotary body (2A) comprises a magnetic drum or a magnetic disc (3A), and said first position detecting means (4A) comprises magnetic angular sensor for magnetically detecting an angular position of said first rotary body (2A). A torque detecting apparatus according to claim 2, characterized in that said second rotary body (2B) comprises a magnetic drum or a magnetic disc (3B), and said second position detecting means (4B) comprises a magnetic angular sensor for magnetically detecting an angular position of said second rotary body (2B). A torque detecting apparatus according to claim 1, characterized in that a step of reading said first and second outputs of said first position detecting means (3A, 4A) is repeated by the judging means after a prescribed short time and if values obtained by the repeated reading step are not substantially equal to the preceding ones, said first and second outputs are determined as a noise, while a judgment of being faulty is not made, and a read step is again repeated from the beginning. A torque detecting apparatus according to claim 2, characterized in that a step of reading said third and fourth outputs of said second position detecting means (3B, 4B) is repeated by the judging means after a prescribed short time and if values obtained by the repeated reading step are not substantially equal to the preceding ones, said third and fourth outputs are determined as a noise, while a judgment of being faulty is not made, and a read step is again repeated from the beginning. A torque detecting apparatus according to claim 1, characterized in that said torque computing means (MC) further comprises an alarm means for giving an alarm when one output of said first output and said second output is determined to be faulty. A torque detecting apparatus according to claim 2, characterized in that said torque computing means (MC) further comprises an alarm means for giving an alarm (Fig. 21) when one output of said third output and said fourth output is determined to be faulty. A torque detecting apparatus according to claim 7, characterized in that said magnetic angular sensor comprises on a common base at least four sets of a first and a second magnetro-resistance effect element arrays having magnetro-resistance effect elements (R₁₁-R₁₈) disposed separately by an electrical angle of n ± λ/6 from each other respectively and a third magnetro-resistance effect element array delivering a reference signal, the respective two sets of said first and said second magnetro-resistance effect element arrays being disposed separately by an electrical angle of n ± λ/4 from each other and the two sets of said arrays separated by n ± λ/4 from each other being spaced by an electrical angle of n ± λ/2 from the other two sets thereof, λ being the angular pitch between respective opposite magnetic poles on said magnetic drum or disc (4, Fig. 9). A torque detecting apparatus according to claim 8, characterized in that said magnetic angular sensor comprises on a common base at least four sets of a first and a second magnetro-resistance effect element arrays having magnetro-resistance effect elements (R₂₁-R₂₈) disposed separately by an electrical angle of n ± λ/6 from each other respectively and a third magnetro-resistance effect element array delivering a reference signal are borne by a base, the respective two sets of said first and said second magnetro-resistance effect element arrays being disposed separately by an electrical angle of n ± λ/4 from each other and the two sets of said arrays separated by n ± λ/4 from each other being spaced by an electrical angle of n ± λ/2 from the other two sets thereof, λ being the angular pitch between respective opposite magnetic poles on said magnetic drum or disc (4, Fig. 9).

Inventors: KAWAMATA SYOOICHI, KURIYAMA SHIGERU, MASAKI RYOOSOO, MIYASHITA KUNIO, TAKAHASHI TADASHI, KAWAMATA, SYOOICHI, KURIYAMA, SHIGERU, MASAKI, RYOOSOO, MIYASHITA, KUNIO, TAKAHASHI, TADASHI
Applicants: HITACHI LTD, HITACHI, LTD.
Application year: 1989
Main classification: G01L3
IPC codes: G01L3