Magnetic image sensor using Matteucci effect

Abstract: A magnetic image sensor comprises at least one magnetic wire (1), means (4, 59) for providing circumferential magnetization thereto, means (55, C1-C6) for generating a plurality of A.C. magnetic fields along a length direction of the magnetic wire, an A.C. power supply source (57), switch means (56) for supplying a current from said constant power supply source to said field generation means sequentially one after another, means (5, 7, 19-21, 23, 25-27) for detecting a Matteucci-effect voltage, developed across said magnetic wire by mutual reaction between the magnetic wire, said A.C. field generation means and a static magnetic field to be detected; and means (61) for forming an image of the static magnetic field.

Description: The present invention relates to a magnetic image sensor using Matteucci effect. When circumferential magnetization is provided to the interior of a single magnetic wire and external A.C. magnetic field is applied to the wire in the transverse direction thereof, a pulsative voltage is developed across the wire, that is, a so-called Matteucci effect takes place. Such Matteucci effect is known but substantially no application techniques are known. Further, as a digitizer or a coordinate input device for inputting handwritten letters, such a prior art device as shown in JP-A-61-70628 is known, but such a coordinate input device based on the aforementioned Matteucci effect is not known so far. Meanwhile, a prior art magnetic image sensor for detecting magnetic data on a multi-track of a magnetic card or the like or a magnetic field caused by a magnetic material film uses a gap type magnetic head of multi-channel, a magnetic resistive element array, a Hall-effect element array, or the like. Thus, the prior art magnetic image sensor has been defective in that the magnetic image sensor is expensive and requires the number of detection circuits corresponding to the multi-channel and thus its necessary circuit is increased in size. Citation "Large Barkhausen and Matteucci Effects in (...) Amorphous Wires" by K. Mohri and others in IEEE Transactions on Magnetics, September 1990, pages 1789-1791, discloses a magnetic wire being twisted in order to provide circumferential magnetization, a vertical magnetizing coil to provide an ac magnetic field in the vicinity of the magnetic wire, an ac power supply source for the magnetic wire, and means for detecting a Matteucci effect voltage across said magnetic wire. It is therefore an object of the present invention to provide a magnetic image sensor based on Matteucci effect. A plurality of magnetic wires circumferentially magnetized are arranged to form a wire array. When a coordinate designator for generating an A.C. magnetic field is moved close to the wire array, a coordinate position of the designator on the wire array is calculated and found on the basis of a mutual relationship between pulse voltages developed across the respective magnetic wires. In a magnetic image sensor of the present invention, a plurality of exciting coils for generating a predetermined A.C. magnetic field are arranged along a magnetic wire circumferentially magnetized therein and a static magnetic field to be image-detected is positioned along the wire, so that its magnetic image is detected on the basis of the magnitude of a pulse voltage developed across the wire when the exciting coils are sequentially excited one after another. Fig. 1 is a schematic block diagram of a signal detector which forms a major part of a coordinate input device of related art; Fig. 2 conceptionally shows a principle on how a pulse voltage is developed across a magnetic wire circumferentially magnetized therein; Figs. 3A and 3B are waveforms of an A.C. magnetic field and a pulse voltage generated on the above principle respectively; Fig. 4 shows a concept of a coordinate input device of related art; Fig. 5 shows a conceptional basic arrangement of another embodiment of related art for explaining its coordinate detecting operation; Fig. 6 is a diagram for explaining how the circumferential magnetization of a magnetic wire is rotated by an external magnetic field; Fig. 7 is a diagram showing how magnetic materials are fixed onto a substrate; Fig. 8 shows the concept of a high-sensitivity sensor for measuring a vertical distance between an electromagnet and a magnetic wire pattern; Fig. 9 is a block diagram of a general arrangement of a coordinate input device of related art; Fig. 10 is a cross-sectional view of a coordinate detector showing the structure of an array of magnetic wires arranged in X and Y directions; Fig. 11 is a characteristic diagram showing relationships between Matteucci-effect voltages developed across adjacent wires and distances from the centers of the respective wires; Fig. 12 is a characteristic diagram showing a relationship between the distance and a ratio between voltages detected across the adjacent wires; Fig. 13 is a flowchart showing the coordinate calculation procedure of the coordinate input device; Fig. 14 is an arrangement of a magnetic image sensor in accordance with the present invention; Fig. 15 conceptionally shows a detection unit of the magnetic image sensor; and Fig. 16 is a timing chart showing the timing of exciting signals and A-B detection signal in the magnetic image sensor. Referring to Fig. 1, there is shown a signal detecting section of a coordinate input device of related art, wherein a magnetic wire 1 is used as a coordinate detector and an A.C. magnetic field is applied to a coordinate designator through the magnetic wire 1 and an electromagnet 2 for coordinate designation (or coordinate designator 2). A D.C. bias circuit 4 is provided to pass a D.C. current through the magnetic wire 1 to provide a circumferential magnetization therein. When the D.C. bias circuit 4 is connected to the magnetic wire 1 through a wiring line, this causes the impedance of the magnetic wire 1 at its both ends to be reduced, thus reducing a pulse voltage to be developed in the magnetic wire 1. For the purpose of avoiding such impedance reduction, an A.C. high impedance circuit 3 is provided to at least one end of the magnetic wire 1. The pulse voltage thus developed in the magnetic wire 1 appears at both ends P and Q of the magnetic wire 1. The pulse voltage is detected by a double-frequency detecting circuit 5 with respect to its 2f component. The double-frequency detecting circuit 5 may comprise an ordinary resonance circuit, filter circuit or synchronous detector circuit. A control circuit 6 functions to supply an exciting current having a fundamental frequency 1f to the electromagnet 2 for coordination designation and also to supply a control signal having a fundamental frequency 2f to the double-frequency detecting circuit 5 as necessary. Fig. 2 shows a pulse-voltage generating principle for explaining how to generate the pulse voltage when the circumferentially-magnetized magnetic wire 1 is subjected to an A.C. magnetic field. The circumferential magnetization of the magnetic wire 1 is repetitively subjected to partial inverting and restoring movements under the influence of the alternating magnetic field of the coordiante designating electromagnet 2. The magnetic field of the electromagnet and the pulse voltage developed across the magnetic wire are shown in Figs. 3A and 3B. More specifically, the number of inversions in the magnetization varies depending on the composite value of the magnetic field generated by the electromagnet and the magnetic field based on terrestrial magnetism. The frequency components of the voltage developed across the magnetic wire include composite values of the respective frequency components of 1f, 2f, 3f, ... where f denotes a frequency at which the electromagnet is excited. Among these frequency components, the 1f component varies largely with the alternating magnetic field, but the 2f component less varies, since the 2f component is derived from pulses having the same waveform as will be appreciated from Fig. 3B. For this reason, it is effective to detect the 2f component by the pulse voltage occurring in the magnetic wire and therefore the double-frequency detecting circuit 5 in Fig. 1 is arranged to detect the 2f component. In order to provide a circumferential magnetization to the magnetic wire, there is employed a method of supplying a D.C. current to the magnetic wire to provide thereto a magnetization caused by a magnetic field based on the right-hand rule because of its ease. To this end, the D.C. bias circuit 4 is used. The circuit 4 can control of the quantity of the aforementioned D.C. current. Further, by increasing the current supplied to the magnetic wire, the influence of the external magnetic field such as terrestrial magnetism can be made less. Conceptionally shown in Fig. 4 is a coordinate input device wherein the detection section of Fig. 1 is arranged in the form of an X-Y matrix. More in detail, in order to detect a position of the coordinate designating electromagnet 2, a plurality of the magnetic wires 1 are provided in X and Y directions. Though only a Y-direction voltage detector for the magnetic wire 1 has been illustrated in Fig. 4, an X-direction voltage detector having the same function as the Y-direction voltage detector is also provided in actual applications. A detection-side terminating circuit 7, which has the same function as the A.C. high impedance circuit 3 in Fig. 1, including a signal multiplexing circuit for sequentially guiding pulse signals from the respective Y-direction magnetic wires 1 to the detection circuit as well as the double-frequency detecting circuit. A drive-side terminating circuit 8 includes such a D.C. current bias circuit 4 and an A.C. high impedance circuit 3 connected to the circuit 4 as necessary as shown in Fig. 4. A coordinate detection control circuit 9 acts to excite the electromagnet 2 for coordinate designation and also to generate a timing signal for controlling the function of the double-frequency detecting circuit and the function of the multiplexing circuit. The structures of these circuits will be detailed later. As has been explained above, the coordinate input device detects voltages developed (when the circumferential magnetization of the magnetic wires is inverted) in one of the circumferentially-magnetized magnetic wires when the coordinate designator excited with an A.C. current approaches thereto. Such a coordiante input device is effective because it is based on a new detection principle that the magnetic wires as coordinate detectors require no windings or the like for voltage generation. However, since a voltage is developed between both ends of the magnetic wire, when a multiplicity of magnetic wires for coordinate detection are arranged in the form of an array, the both ends of each magnetic wire is spaced by a relatively long distance. For this reason, a signal return path for connecting the both ends of the magnetic wire is necessary. When the signal return path is provided in an outer frame part, electromagnetic coupling between the external magnetic field and a loop coil comprising the magnetic wire and the return path causes generation of a coupling signal, in addition to the original coordiante detection signal caused by the inversion in the magnetization of the magnetic wire. In the event where the magnetic wire is made thin, the coupling signal becomes larger than the voltage component caused by the inversion in the circumferential magnetization of the magnetic wire, which results in reduction of S/N ratio of the coordinate detection signal. In order to minimize the electromagnetic coupling of the loop coil of the coordinate detector and the return path with the external magnetic field, a method for making small the area of the loop coil is effectively employed. This enables reduction of the noise in the detection voltage caused by the electromagnetic coupling. Further, when the return path is also made in the form of the same magnetic wire, the magnetization reversal signal is added to the voltages generated by the magnetic wires of the go and return paths on the detection principle of the circumferentially magnetized magnetic wire, whereby the detection voltage can be obtained which corresponds to twice the detection voltage obtained when the go path is made in the form of a magnetic wire and the return path is made in the form of an ordinary conductor. This case will be detailed in connection with Figs. 5 and 6. In Fig. 5, the magnetic wire 1 as a go path is connected at a fixed turn point lR to a magnetic wire 1' as a return path. The D.C. bias circuit 4 is used to provide circumferential magnetization to the both wires. The coordinate designator 2 excited by an A.C. signal source 2S applies an A.C. magnetic field to the both magnetic wires. The operational principle of the coordinate detector is shown in Fig. 6, wherein a bias current shown by arrows causes such circumferential magnetization as shown in Fig. 6 to be developed in the interiors of the magnetic wires 1 and 1' of the go and return paths. When the magnetic field generated by the coordinate designator 2 causes rotation of the magnetization direction of the wires, a voltage is developed by a change in the magnetic flux of the rotary magnetization part of each wire with such polarities as shown in Fig. 6. Thus, the voltages developed in the respective wires are added together and therefore a generation voltage is doubled when compared to the case of use of the single magnetic wire. Since the turn path lR between the magnetic wires 1 and 1' of the go and return paths are minimized to dispose the wires as close to each other as possible, the area of a loop coil constituted of the both wires can be made small. For this reason, a voltage caused by electromagnetic coupling other than the detection voltage caused by the rotary magnetization can be suppressed down to a low level. In Fig. 7, magnetic materials 14 each in the form of a thin magnetic wire pattern are bonded or deposited as fixed onto the front and back surfaces of a substrate 13. A through hole 15 made in the substrate 13 is for interconnection between the patterns provided on the front and back sides of the substrate. When it is desired to form very thin magnetic patterns, this can be realized by depositing a magnetic film on each of the entire front and back sides of the substrate and then etching the substrate to leave the thin magnetic patterns 14 thereon. When it is desired to provide such magnetic patterns both in X and Y directions, this can be realized by constructing the substrate in the form of a multiple layer. Fig. 8 shows that the magnetic material 41 is made in the form of a thin magnetic pattern of repetitive magnetic lines to add together detection voltages developed in the magnetic lines to obtain a high total detection voltage and thus a high sensitivity. With such an arrangement, there can be realized a proximity sensor which detects a vertical distance with respect to the coordinate designator 2 with a high sensitivity. It goes without saying that such a thin magnetic pattern 14 of repetitive magnetic lines as shown in Fig. 8 may be replaced by a single wire as necessary to form the proximity sensor. The magnetic wire or magnetic material mentioned above may be made of preferably material having a negative magnetostrictive coefficient such as amorphous material. Detailed explanation will next be made as to the coordinate input device by referring to a block diagram of Fig. 9. In the drawing, reference numeral 18 denotes a matrix of repetitively turned magnetic wires arranged as equi-spaced in X and Y directions. One ends of all the magnetic wires are connected through a line 19 to the D.C. bias circuit 4 which supplies a constant current; while the other ends of all the magnetic wires are connected to collectors of switching transistors of X- and Y-decoders 20 and 21. The switching transistors are also connected at their emitters to a common circuit part. A wire selection circuit 23 supplies a switching signal to the bases of the switching transistors of the X- and Y- decoders 20 and 21 to sequentially turn ON the transistors one after another and to sequentially switch ON the wires one after another to sequentially supply a bias current thereto. A coordinate detection control circuit 9 supplies a timing pulse for wire selection to the wire selection circuit 23 and also supplies an A.C. current to the coordinate designator 2 to generate an A.C. magnetic field therein. When the coordinate designator 2 is approached to the matrix 18 and when one of the magnetic wires close to the coordinate designator 2 is supplied with the bias current via the decoder, such a pulse voltage as shown in Fig. 3B appears on the line 19. The pulse voltage is sent through a resistor/capacitor coupling circuit 25 to a detection circuit 26 to be detected thereat. Subsequently, the pulse voltage is sample-held at a sample/hold circuit 27, converted into a digital signal at an A/D covnerter 28, subjected to a signal processing at a CPU 29, and then transmitted to a host computer (not shown) as a coordinate data. The wire matrix, more in detail, is constructed so that, as shown in Fig. 10, magnetic wires lX and lX' for detection of X-direction coordinate magnetic wires lY and lY' for detection of Y-direction coordinate are arranged at regular intervals on a panel 30 which acts to stabilize a vertical distance between the coordinate designator 2 and the magnetic wires and also to fixedly mount the magnetic wires thereto. The wires lX, lX' and lY, lY' are arranged as bent or turned as shown in Figs. 5 and 6 respectively, and an insulator 31 is disposed between the associated wires to avoid any short-circuiting of the generation voltage caused by the rotary magnetization. Further, another insulator 31 is disposed between the X- and Y-direction wires. With the present coordinate input device, a multiplicity of magnetic wires are arranged in the X and Y directions to generate detection outputs indicative of a distance between the coordinate designator and ones of the wires close to the designator, so that the detection outputs of the associated magnetic wires made high when subjected to the A.C. magnetic field of the coordinate designator are used to carry out a coordinate estimation computation. Thus, even when the X- and Y-direction coordinate detectors are arranged at intervals of, for example, 10 mm, the coordinate input device can have a resolution of 0.1 mm. This computation is carried out in the CPU 29 in Fig. 9. Fig. 11 shows Matteucci effect voltage characteristics V N-l , V N , and V N+l detected across three wires N-l, N, and N+l when the coordinate designator is positioned at points spaced by a distance S from the centers of these wires, respectively. In the illustrated example, the distance between the wires is set to be 5 mm. When the coordinate designator is located between the wires N and N+l and closer to the wire N as shown in Fig. 11, voltages V N , V N+l , and V N-l are detected across the wires N, N+L, and N-l respectively. In this case, since the voltage V N has the largest value and the voltage V N+l has the next largest value among these voltages V N , V N+l , and V N-l , these two voltages V N and V N+l are employed and the smaller voltage V N+l is divided by the larger voltage V N to obtain a value of V N+l /V N . The obtained value V N+l /V N satisfies such a characteristic with respect to a distance δ from the wire center as shown in Fig. 12. More specifically, the value V N+l /V N becomes minimum on the wire N (δ = 0) and becomes larger as the position of the coordinate designator shifts rightwardly from the wire N and when the coordinate designator reaches a point (δ = 2.5) between the wires N and N+l, the value becomes 1. The shape of the characteristic of Fig. 12 is identical or symmetrical with respect to each wire position in the left and right directions. Accordingly, when the characteristic is previously stored in a memory of the CPU 29, the position δ of the coordinate designator from the wire N producing the largest detection voltage can be calculated on the basis of the ratio ( V N+l /V N ) between the detection voltages of the wire N and adjacent wire N+l respectively having the largest and the next largest values in the detection voltages of the wires, and then a coordinate point indicate of the coordinate designator can be calculated on the basis of the position δ. The above calculation procedure will be explained by referring to a flowchart of Fig. 13. In the drawing, first, a detection signal is input from a wire in a step 40 and it is judged in a step 41 whether or not the input signal is larger than a predetermined value. Determination of NO in the step 41 causes control to proceed to a step 43. Determination of YES in the step 41 causes control to go to a step 42 where the coordinate valus of the wire and the size of the detection signal are recorded in the memory and control goes to the step 43. In the step 43, it is judged whether or not detection of all the wires has been completed. Determination of NO in the step 43 causes control to go back to the step 40 to input the detection signal of the next wire. Determination of YES, on the other hand, causes control to proceed to a step 44 to find detection signals V N-l , V N , V N+l , ... which have been judged as having predetermined continuous values. In a next step 45, one of these detection signals having a maximum value, for example, the signal V N is determined. Subsequently, comparison is made in a next step 46 between the detection signals V N-l and V N+l of the wires N-l and N+l adjacent to the wire N which produced the maximum detection signal. When the comparison result satisfies a relation V N-l > V N+l , control goes to a step 47 to calculate a value V N-l /V N . In a next step 48, a value δ is found by referencing a table (stored in the memory) having the characteristic as shown in Fig. 12. In a next step 49, the value δ is subtracted from the coordinate value of the wire N and then a coordinate point at which the coordinate designator is positioned is calculated. If the comparison result in the step 46 satisfies a relation V N+l > V N-l , then control proceeds to a step 50 to calculate a value V N+l /V N . In a next step 51, the value δ is found by referencing the table according to the calculated value V N+l /V N . After this, in a step 52, the value δ is added to the coordinate value of the wire N to find a coordinate point indicative of the position of the coordinate designator. In a step 53, the coordinate calculation is completed. Although the aforementioned coordinate calculation has been explained in connection with a single coordinate axis, the same explanation holds true for the coordinate calculation of the other coordinate axis with use of the similar flowchart. Explanation will be made as to yet a further embodiment. In the present embodiment, when circumferential magnetization is generated in a magnetic wire having a magnetostrictive coefficient of from zero to a negative value and when an exciting magnetic field caused by an exciting coil is applied to the magnetic wire, a pulse voltage is generated across the wire at the time that the circumferential magnetization is inverted. At this time, if an external magnetic field other than the exciting magnetic field is present, then the pulse voltage at the time of the magnetization reversal is influenced by both of the exciting magnetic field and the external magnetic field. Thus, when the exciting magnetic field is previously set at a predetermined value, the intensity of the external magnetic field can be detected. Further, in the case where a plurality of exciting coils are arranged along a magnetic wire so that a switch enables sequential change-over of the exciting coils, an external magnetic field in the vicinity of associated one of the exciting coils can be detected, whereby a magnetic image sensor can be realized. Provision of the circumferential magnetization to a magnetic wire having a magnetostrictive coefficient of zero to a negative value can be realized by providing a suitable twist to the magnetic wire to give it a twisting stress. In the event where provision of the circumferential magnetization to a magnetic wire having a magnetostrictive coefficient of zero to a negative value is realized by providing a twist to the magnetic wire, when the external magnetic field exceeds a predetermined value, this causes inversion of the magnetization, at which time a voltage proportional to -d/dt is generated, where  denotes magnetic flux. Accordingly, an A.C. magnetic field is applied to the magnetic wire, a pulse voltage at the time of the magnetization inversion is developed across the magnetic wire. Under such a condition, if a magnetic field other than the magnetic field caused by the exciting coil in the vicinity of the magnetic wire is present, then a composite magnetic field of the both magnetic fields is applied to the magnetic wire so that the composite magnetic field causes inversion of the magnetization in the interior of the magnetic wire. In other words, the external magnetic field acts as a modulation signal when the exciting magnetic field is considered to be a carrier, and thus separate detection of the external magnetic field can be realized by processing the signal caused by the magnetization inversion. Detection of the external magnetic field can be attained with a high resolution by narrowing the range of the exciting magnetic field and this can be realized with use of a ferrite core wound by a winding. An arrangement of the magnetic image sensor in accordance with the present embodiment is shown in Fig. 14. The magnetic image sensor comprises a magnetic wire 1 as a detector, one or more exciting coils 55 for providing a local exciting magnetic field to the wire 1, a change-over switch 56 for switchingly supplying an exciting current to one of the exciting coils, and an oscillator 57 for supplying the exciting current to the switch 56. A detection unit of the magnetic image sensor of Fig. 14 is shown in Fig. 15, in which case circumferential magnetization takes place within the interior of the magnetic wire 1. In this case, the exciting magnetic field of the exciting coil 55 causes inversion of the interior magnetization direction, whereby a pulsative voltage is developed between terminals A and B of the magnetic wire 1. Pulses occur in the detection signal at a predetermined phase of the exciting current, i.e., the exciting magnetic field. Under such a condition, when an external magnetic field other than the exciting magnetic field is present, the external magnetic field causes the magnetization in the interior of the magnetic wire 1 to have been partially reversed in direction, which partial part of the magnetic wire, when subjected to application of the exciting magnetic field, does not contribute to generation of the pulse voltage between the terminals A and B. In other words, the magnitude of the detection signal is modulated by the external magnetic field. The pulse voltage is developed across the magnetic wire 1 on such a principle as mentioned above. A control circuit 60 controls the switching operation of the change-over switch 56 and also controls a magnetic image forming circuit 61 which detects the magnitude of the pulse voltage developed across the wire 1 and which forms a magnetic image. Only that part of the magnetic wire 1 excited by associated one of the respective exciting magnetic fields of the exciting coils 55 is modulated by the external magnetic field, and thus the other parts not excited by the exciting magnetic field will not affect the pulse signal at all. For this reason, when a multiplicity of such exciting coils 55 are arranged along a magnetic wire, a magnetic image sensor can be increased in resolution. The exciting coils 55 may be realized not only by ferrite core rods wound by windings but also by a pattern (in a helical or other shape) formed on a substrate in the form of copper-clad multi-laminates. Since the multiplicity of exciting coils 55 are arranged to be sequentially excited, that part of the wire which can detect the external magnetic field is moved along the length of the wire, whereby the magnetic image sensor can be realized. Since the design exciting current of the exciting coil is below several ten mA, an ordinary analog switch or the like may be used as the change-over switch 56. Referring to Fig. 16, there are shown operational signals of the magnetic image sensor of Fig. 14. In Fig. 16, reference symbols C1 to C4 denote exciting signals for the exciting coils C1 to C4 which signals are sequentially switched as illustrated. In the illustrated example, the detection signal is subjected to a modulation by the external magnetic field in the vicinity of the respective exciting coils and appears as such a detection signal having a modulated amplitude as an A-B detection signal in Fig. 16. In the case where the magnetic wire is made of material having a magnetostrictive coefficient of zero to a negative value, circumferential magnetization tends to easily occur and the magnetization is stabilized by applying a twist to the wire at a rate of about one turn/10 cm from a twist application means 59 as shown by an arrow C in Fig. 14. In this connection, the application of the twist to the wire may be replaced by the supply of a bias current thereto or the bias current may be supplied to the wire in addition to the twist. In accordance with the present embodiment, there can be realized a magnetic image sensor which can realize a wide range of detection with a necessary resolution while eliminating the need for precise winding operations, precise processing of magnetic cores and semiconductor techniques. Further, the structure of the present invention can be made highly simple when compared with the prior art and thus its cost can be easily reduced. In addition, since the present invention is based on the still reading principle, the invention can be independent of the moving speed of a detection medium.

Claims: A magnetic image sensor based on Matteucci effect, comprising: at least one magnetic wire (1); means (4, 59) for providing circumferential magnetization to said magnetic wire; a plurality of means (55, C1-C6) disposed along a length direction of the magnetic wire for generating a plurality of A.C. magnetic fields; constant A.C. power supply source (57); switch means (56) for supplying a current from said constant power supply source to said plurality of A.C. field generation means sequentially one after another; means (5, 7, 19-21, 23, 25-27) for detecting a Matteucci-effect voltage developed across said magnetic wire by mutual reaction between the magnetic wire, said A.C. field generation means and a static magnetic field to be detected; and means (61) for forming an image of the static magnetic field based on a modulation signal into which said Matteucci-effect voltage detected by said detection means is modulated by said static magnetic field to be detected. A magnetic image sensor according to claim 1, wherein said magnetic wire (1) is made of material having a magnetostrictive coefficient of zero to a negative value. A magnetic image sensor according to claim 2, wherein said circumferential magnetization means (4, 59) is a means (59) for applying a twist to said magnetic wire (1). A magnetic image sensor according to claim 3, wherein said twist application means (59) applies a twist to said magnetic wire at a rate of about one turn/10 cm. A magnetic image sensor according to claim 1, wherein said circumferential magnetization means (4, 59) is a means (4) for supplying a D.C. current to said magnetic wire. A magnetic image sensor according to one of the claims 1 to 5, wherein each of said plurality of A.C. magnetic field generation means (55, C1-C6) includes a ferrite core rod and a winding wound onto said ferrite core rod. A magnetic image sensor according to claim 6, wherein said winding is formed on a substrate in the form of multi-laminates.

Inventors: KANO MITSUNARI, KINO JIRO, KONISHI YOSHIHARU, MATSUDA TOSHIHIKO, MOHRI KANEO, OIZUMI JUNICHI, TAKASHI MORIHIKO, KANO, MITSUNARI, KINO, JIRO, KONISHI, YOSHIHARU, MATSUDA, TOSHIHIKO, MOHRI, KANEO, OIZUMI, JUNICHI, TAKASHI, MORIHIKO
Applicants: HITACHI LTD, HITACHI, LTD.
Application year: 1991
Main classification: G01R33
IPC codes: G06F3, G01R33, G01D5, G01B7