A circuit apparatus for driving a magnetic head

Abstract: A circuit apparatus for driving a magnetic head to generate a magnetic field wherein a driving frequency of the magnetic head is increased and a recording density of an information recording medium is raised. In this circuit apparatus, a bridge circuit is constructed in which a chief coil for generating a magnetic field is arranged between a first connection node disposed between a serially connected first auxiliary coil and first switch element and a second connection node disposed between a serially connected second auxiliary coil and second switch element, and the magnetic field is modulated in accordance with an information signal by on-off control of the first and second switch elements to change the direction of current flowing in the chief coil. Further, third and fourth switch elements are respectively connected in parallel with the first and second switch elements so that a current path of the chief coil is separated from respective current paths of the auxiliary coils. Thus, the current path of current through the auxiliary coil is isolated. Or, there are provided circuits for respectively supplying currents to the chief coil through the first and second auxiliary coils and circuits for respectively supplying currents to the chief coil without passing through the first and second auxiliary coils.

Description: BACKGROUND OF THE INVENTION Field of the Invention The present invention relates to a circuit apparatus for driving a magnetic head to be used for magnetic modulation in a magnetic modulation type optomagnetic recording apparatus. Related Background Art Conventionally, optical modulation systems, magnetic-field modulation systems and the like are known as a recording system of an optomagnetic recording apparatus. Among them, the magnetic-field modulation system is particularly advantageous in its recording speed, for example, since new data can be directly overwritten onto old data in this modulation system. Fig. 1 illustrates a schematic structure of such a conventional magnetic-field modulation system. In Fig. 1, reference numeral 1 designates an optomagnetic disc to be used as an information recording medium, and reference numeral 2 designates an optomagnetic recording layer formed in the disc 1. In this structure, a magnetic head 6 is disposed above the optomagnetic disc 1, and an optical head 4 is disposed below the disc 1, opposite to the magnetic head 6. The optical head 4 causes a laser beam 7 from a semiconductor laser, which is arranged in the optical head 4 as a light source, to be applied onto the recording layer 2 as a minute light spot so that the temperature of a recording portion is raised to a value higher than the Curie temperature. On the other hand, the magnetic head 6 generates a bias magnetic field modulated in accordance with information to be recorded by driving a driver circuit 3, and applies this bias magnetic field to a temperature-raised portion of the recording layer 2. As a result, the orientation of magnetization in the temperature-raised portion of the recording layer 2 is changed to a direction of the bias magnetic field, and the information is recorded in the recording layer 2. As a driving apparatus for a magnetic head of a magnetic-field modulation system, an apparatus as disclosed in, for example, Japanese Patent Laid-open No. 63-94406 is known. Fig. 2 shows a circuit diagram of this driving apparatus. In Fig. 2, reference symbol L H designates a chief coil for generating a bias magnetic field, reference symbol L 1 and L 2 respectively designate auxiliary coils for speedily changing over a magnetic field, reference symbol SW 1 and SW 2 respectively designate switch elements for changing the direction of current in the chief coil L H , and reference symbol R 1 and R 2 respectively designate resistors for limiting current. Values of inductances of the auxiliary coils L 1 and L 2 are set to values larger than the inductance of the chief coil L H . In this driving apparatus, the switch elements SW 1 and SW 2 are controlled to be alternately turned on or off (closed or open), and the polarity of the generated magnetic field is switched in accordance with information to be recorded by switching the direction of current in the chief coil L H . In more detail, current paths CH 1 and CH 4 are closed or established while current paths CH 2 and CH 3 designated by dashed lines are open or nonexistent, when the switch element SW 1 is closed and the switch element SW 2 is opened. Then, since current is supplied to the chief coil L H due to the establishment of the current path CH 1 , a magnetic field in accordance with the direction of the current is generated by the chief coil L H . On the other hand, when the switch element SW 1 is opened and the switch element SW 2 is closed, the current paths CH 2 and CH 3 are closed or established while the current paths CH 1 and CH 4 are open or nonexistent. As a result, current opposite in direction to the above-mentioned current (i.e., a reverse current) flows through the chief coil L H due to the establishment of the current path CH 2 , and a magnetic field whose polarity is reversed is generated. Here, since the inductances of the auxiliary coils L 1 and L 2 are larger than the inductance of the chief coil L H , the flowing currents are respectively maintained at approximately constant values, while the current path is changed from CH 1 to CH 3 , and from CH 4 to CH 2 as the switch elements SW 1 and SW 2 are changed over. Therefore, if the on-off time of the switch elements SW 1 and SW 2 is made sufficiently short, the direction of the current flowing through the chief coil L H can be reversed in a very short time without increasing the voltage of a DC source V. This is effective for preventing mistakes in recording information signals in order to achieve a desired signal recording. However, when the switch element is, for example, a field effect transistor, a stray capacitance between drain and source appears even if the switch element is actually open. As a result, as shown in Fig. 3, a vibration phenomenon due to such stray capacitance and the inductance component of the chief coil L H occurs, and the time required for reversing the current of the chief coil L H is determined by a period of this vibration. Therefore, in order to shorten the reversal time, a switch element having a speedy switching time and a small stray capacitance should be used. Further, the vibration is gradually attenuated as its energy is consumed, but in order to prompt this attenuation, a resistor (not shown) should be used to consume the vibration energy. Thus, current shown in Fig. 3 is supplied to the chief coil L H by alternate on-off control of the switch elements SW 1 and SW 2 , and a magnetic field corresponding to the direction of this current is generated. In Fig. 3, a dashed line indicates a vibration wave shape due to the inductance and the stray capacitance, and a solid line indicates a current wave shape in a case where the vibration is speedily attenuated using the resistor and the like. In the prior art magnetic head driving apparatus, however, most of the magnetic energy (1/2·LI 2 ; L is an inductance of the chief coil L H and I is the current passing through it) stored in the chief coil L H is consumed in the resistor and so forth in a process of the vibration phenomenon, and at this time energy of 1/2·LI 2 is momentarily supplied from the auxiliary coil to the chief coil L H as current in an opposite direction, thereby reversing the current through the chief coil L H . Therefore, the reduced energy of 1/2·LI 2 must be supplied to the auxiliary coil from the DC source V by the next current reversal. Generally, when a current supply is performed from a source having a voltage of V to an auxiliary coil having an inductance of L A , the rate of change Δi/Δt of the current relative to time is V/L A , and hence the energy supply from the DC source having a low voltage to the auxiliary coil having a large inductance takes a considerable time. Therefore, in a case where the current reversal is conducted at a high repetitive frequency, current supplied to the chief coil is reduced since the current reversal is performed in a state in which the energy supply to the auxiliary coil is inadequate. Thus, a normal recording of information becomes impossible. Actually, when the voltage of the source V is 5V, the inductance of the chief coil L H is 1 µH and the current supplied to the chief coil is 0.2A, an upper limit of the driving frequency is about 5MHz. As this frequency increases, the current decreases and information recording degradation occurs. EP-A-0365891 discloses a circuit arrangement for the magnetooptical recording of data on a magnetooptic recording layer, the circuit arrangement including a main coil for applying a modulated magnetic field to the magnetooptic recording layer. First and second auxiliary coils are connected to the coil so as to apply current in opposite directions through the chief coil dependent on the positions of two switches. A parallel circuit comprising a Zener diode and a capacitance are arranged to limit the induction voltage arising when the switches are opened. SUMMARY OF THE INVENTION It is an object of the present invention to provide a circuit apparatus for driving a magnetic head in which a driving frequency of the magnetic head can be greatly increased and a recording speed can be increased likewise. The present invention provides a circuit apparatus as set out in claim 1. These advantages and others will be more readily understood in connection with the following detailed description of the preferred embodiments in conjunction with the drawings. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a schematic view showing a prior art magnetic-field modulation system. Fig. 2 is a circuit diagram showing a magnetic head driving apparatus of the prior art magnetic-field modulation system. Fig. 3 is a view showing a vibration phenomenon of current flowing through a chief coil L H shown in Fig. 2. Fig. 4 is a circuit diagram showing a magnetic lead driving apparatus. Fig. 5 is a view showing a vibration phenomenon of current flowing through a chief coil L H shown in Fig. 4. Fig. 6 is a circuit diagram showing a magnetic head driving apparatus of a first preferred embodiment of the present invention. Fig. 7 is a circuit diagram showing a magnetic head driving apparatus of a second preferred embodiment of the present invention. DESCRIPTION OF THE PREFERRED EMBODIMENT Fig. 4 is a circuit diagram showing a magnetic head driving apparatus. In Fig. 4, the same portions as those shown in the prior art apparatus of Fig. 2 are designated by the same reference symbols as those in Fig. 2. In Fig. 4, reference symbol L H designates a chief coil of a magnetic head wound around a magnetic core (not shown), and reference symbols L 1 and L 2 respectively designate auxiliary coils. The inductances of the auxiliary coils L 1 and L 2 are set to values larger than the inductance of the chief coil L H . Further, reference symbols SW 1 -SW 4 respectively designate switch elements such as field effect transistors, reference symbols D 1 and D 2 designate rectification elements (connection elements) such as semiconductor diodes, and reference symbols R 1 and R 2 designate resistors for current limitation. In this embodiment, pairs of the switch elements SW 1 and SW 3 and the switch elements SW 2 and SW 4 respectively operate at the same time as a pair, and the switch elements SW 1 , and SW 3 and the switch elements SW 2 and SW 4 are alternately on-off controlled by a control means CM. Initially, in a state wherein the switch elements SW 2 and SW 4 are closed and the switch elements SW 1 and SW 3 are open, current paths CH 1 and CH 4 indicated by solid lines are established or closed and currents are respectively supplied to the chief coil L H and the auxiliary coil L 1 through path CH 1 and to the auxiliary coil L 2 through path CH 4 . In this case, the current of the chief coil L H is approximately equal to that of the auxiliary coil L 1 , and the current of the current path CH 1 through the chief coil L H would not flow into the current path CH 4 since it is stopped by the rectification element D 2 . Further, since the rectification element D 2 has a potential difference, the current of the current path CH 4 would not flow into the current path CH 1 . Next, when the switch elements SW 1 and SW 3 are closed and the switch elements SW 2 and SW 4 are opened, current paths CH 2 and CH 3 indicated by dashed lines are closed and currents are respectively supplied to the chief coil L H and the auxiliary coil L 2 through path CH 2 and to the auxiliary coil L 1 through path CH 3 . The direction of current through the chief coil L H is reversed, and the current of the chief coil L H is approximately equal to that of the auxiliary coil L 2 . Further, the current of the current path CH 2 would not flow into the current path CH 3 and the current of the current path CH 3 would not flow into the current path CH 2 for the same reason as stated above, i.e., due to the rectification element D 1 . As has been described in the foregoing, in a circuit apparatus for driving a magnetic head, a bridge circuit is constructed in which a chief coil for generating a magnetic field is arranged between a first connection node disposed between a serially connected first auxiliary coil and first switch element and a second connection node disposed between a serially connected second auxiliary coil and second switch element, and the magnetic field is modulated in accordance with an information signal by on-off control of the first and second switch elements to change the direction of current flowing in the chief coil. Further, third and fourth switch elements are respectively connected in parallel with the first and second switch elements so that a current path of the chief coil is separated from respective current paths of the auxiliary coils by using respective rectification elements for preventing a reverse current from the chief coil. Thus, the current path of current through the auxiliary coil can be isolated. The time required for reversing the current of the chief coil L H is approximately determined by a period of the vibration caused by a stray capacitance (a capacitance between a drain and a source when the switch element is a field effect transistor) of the switch element and the inductance of the chief coil L H , as described above. In this case, but for the rectification elements D 1 and D 2 , a configuration in which two switch elements are connected in parallel would appear to double its stray capacitance and the reversal time of the supply curent in the chief coil L H would be prolonged. In this apparatus, however, since the rectification elements D 1 and D 2 are respectively connected between the switch elements SW 1 and SW 3 and the switch elements SW 2 and SW 4 , the effect of capacitances of the newly added switch elements SW 3 and SW 4 can be lessened when the capacitance of the rectification element (a junction capacitance if the rectification element is a diode) is small. Thus, the reversal time of current in the chief coil L H will not be long. Further, in this apparatus, since currents of the chief coil and the auxiliary coil are respectively caused to flow in different current paths, the current of the switch element is half as much as that in the prior art and a switch element having a small capacitance can be used accordingly. This results in the technical advantage that the current reversal time of the chief coil is reduced because the stray capacitance of the switch element can be lowered (a drain-source capacitance is made small if the switch element is a field effect transistor). In addition, since energy consumed by the respective switch elements becomes one fourth of the energy consumed by the prior art, it is well suited to a design in which consideration of heat radiation is important at the time of packaging the switch element. In the above apparatus, while the switch elements SW 1 and SW 3 , and the switch elements SW 2 and SW 4 are respectively on-off controlled at the same time, the prior art problem that the current of the chief coil is reduced when a high driving frequency is used can be solved if the switch element SW 4 is opened a short predetermined time after the opening of the switch element SW 2 and the switch element SW 3 , is opened a short predetermined time after the opening of the switch element SW 1 . In the prior art apparatus, when the switch element is opened, the vibration phenomenon of current occurs due to the inductance of the chief coil and the capacitance of the switch element, and at the same time a necessary current is momentarily supplied from the auxiliary coil to the chief coil. At this time, the current is concentrated to the chief coil, and as a result, the energy (1/2·LI 2 ) that the chief coil originally has and that is a source of the current vibration phenomenon becomes excessive. Therefore, in order to speedily reduce the vibration, the excessive energy must be consumed by a resistor or the like, and on the other hand, the amount of reduced energy must be restored to the auxiliary coil by the next current reversal. Therefore, in this apparatus, timing is controlled so that the switch element SW 3 is opened after the switch element SW 1 is opened and the switch element SW 4 is opened after the switch element SW 2 is opened, and hence the current supply from the auxiliary coil to the chief coil is delayed. Thus, the amplitude of the current vibration is greatly reduced compared with the prior art, and the generation of excessive energy in the chief coil is suppressed. The time delay between opening of the switch elements SW 1 and SW 3 and between opening of the switch elements SW 2 and SW 4 is preferably about one half of the vibration period at which the reversed current is maximum. According to an experiment conducted under the above condition, it was confirmed that the current vibration was less than a third of that of the prior art. Fig. 5 shows a current wave shape of the chief coil obtained in that experiment, where A indicates a prior art current vibration and B indicates the current vibration obtained when the off-timing of the switch elements is shifted as discussed above. From Fig. 5, it is seen that the amplitude of the current vibration is extremely reduced as compared to the prior art. In actuality, in order to speedily reduce the current vibration as shown by C of Fig. 5, the excessive energy is consumed by the resistor or the like and the energy of the same magnitude is supplied to the auxiliary coil by the next current reversal. Since the consumption of energy accompanying one current reversal of the chief coil is lessened by shifting the off-timing of the above-mentioned pairs of the switch elements, the shortage of current in the chief coil would not occur, and hence the chief coil can be driven at a higher driving frequency. According to an experiment conducted by the applicant, an upper limit of the driving frequency was 10MHz when the voltage of a DC source V was 5V, the inductance of the chief coil L H was 1 µ H and its current was 0.2A. Thus, it was confirmed that the driving frequency was greatly increased as compared with the frequency of 5MHz that is an upper limit of the prior art driving frequency. Fig. 6 is a circuit diagram showing a first preferred embodiment of a magnetic head driving apparatus of the present invention. In Fig. 6, reference sign V 1 designates a DC source of, for example, 5V, and reference sign V 2 designates a DC source of, for example, 12V that is greater than that of the DC source V 1 . The DC source V 1 is connected to a switch element SW 1 through a resistor R 3 and a rectification element D 3 such as a diode, and is connected to a switch element SW 2 through a resistor R 4 and a rectification element D 4 . A circuit comprising the resistor R 3 and the rectification element D 3 and a circuit comprising the resistor R 4 and the rectification element D 4 respectively change their impedances when the switch elements SW 1 and SW 2 are changed over, so that the current vibration of the chief coil L H is reduced. This will be explained in more detail below. The remaining construction is the same as that of Fig. 2, and reference symbol L H designates a chief coil wound around a magnetic core (not shown), reference symbol L 1 and L 2 designate auxiliary coils, and reference symbol SW 1 and SW 2 designate switch elements such as a field effect transistor which are alternately on-off controlled. The inductances of the auxiliary coils L 1 and L 2 are set to values larger than the inductance of the chief coil L H . The operation of this embodiment will be described. Initially, when the switch element SW 1 is closed and the switch element SW 2 is open, a path from the DC source V 1 to the current paths CH 1 and CH 5 , a path from the DC source V 1 to the current path CH 5 through the current path CH 2 and the chief coil L H , a path from the DC source V 2 to the current paths CH 3 and CH 5 and a path from the DC source V 2 to the current path CH 5 through the current path CH 4 and the chief coil L H are respectively established. At this time, it is assumed that current flowing in each of the current paths CH 1 and CH 2 is I 1 and current flowing in each of the current paths CH 3 and CH 4 is I 2 . In this state, when the switch element SW 1 is opened and the switch element SW 2 is closed, the current path CH 5 is opened and the current path CH 6 is closed. Here, since the inductance of the auxiliary coils L 1 and L 2 is large, the current of the current paths CH 3 and CH 4 remains approximately constant, but a high voltage is momentarily induced between the auxiliary coil L 1 and the chief coil L H . Therefore, a reverse bias voltage is applied to the rectification element D 3 , and hence the current path CH 1 is momentarily opened and has a high impedance. On the other hand, the current flowing in the current path CH 3 is approximately maintained at a constant value I 2 , and its flow path is changed from the current path CH 5 to the chief coil L H in a very short time. Further, since magnetic energy of 1/2·LI 2 (I=I 1 +I 2 ) is originally stored in the chief coil L H , the above-discussed vibration phenomenon of current occurs due to the inductance of the chief coil L H , the capacitance of the switch element and the like. In this case, after a time lapse of one half of a period of the current vibration, current flowing in an opposite direction through the chief coil L H reaches a maximum whose value is I 1 +I 2 -ΔI. ΔI is an amount of current reduction due to the energy loss at the time of one half of the period of the vibration, and amounts to about 20% of I 1 +I 2 . On the other hand, the constant current I 2 is momentarily supplied from the current path CH 3 to the chief coil L H , and hence current flowing into the chief coil L H at this time becomes equal to I 1 +2I 2 - ΔI. Here, if I 2 ≒ ΔI is established, current flowing into the chief coil L H becomes equal to I 1 +I 2 . This value is the same as that before the switch element SW 1 is opened and the switch element SW 2 is closed (its direction is opposite). Further, when current flowing in the chief coil L H in an opposite direction is maximum, a voltage induced between the auxiliary coil L 1 and the chief coil L H is lowered and the reverse bias voltage across the rectification element D 3 is eliminated. As a result, the momentarily opened current path CH 1 is closed and its impedance is changed from high to low. Thus, the vibration phenomenon of current flowing in the chief coil L H will not. continue any longer. Thereafter, a total current of I 1 +I 2 , from the current path CH 1 of low impedance and the current path CH 3 , respectively, is continuously supplied to the chief coil L H , and thus the reversal of current is completed. Further, in a case when the switch element SW 2 is opened and the switch element SW 1 is closed, i.e., the reverse of the operation discussed above, the operation is completely the same as above. Namely, the current vibration is suppressed due to the change of the current path CH 2 from high impedance to low impedance. As has been described in the foregoing, in a circuit apparatus for driving a magnetic head of the present invention, a bridge circuit is constructed in which a chief coil for generating a magnetic field is arranged between a first connection node disposed between a serially connected first auxiliary coil and first switch element and a second connection node disposed between a second auxiliary coil and second switch element, and the magnetic field is modulated in accordance with an information signal by on-off control of the first and second switch elements to change the direction of current flowing in the chief coil. Further, circuits for respectively supplying currents to the chief coil through the first and second auxiliary coils and other circuits for respectively supplying currents to the chief coil without passing through the first and second auxiliary coils are constructed. In the other circuits, rectification elements are respectively arranged so that no current flows in an opposite direction. The other circuits constitute an impedance changing means for changing an output side impedance of the chief coil from high to low after a predetermined time from the current change-over (switch-over of the switch elements SW 1 and SW 2 ) when currents are respectively supplied to the chief coil. The impedance changing means is comprised of a rectification element whose impedance changes to a low impedance when a reverse bias voltage due to a reverse electromotive force of each of the first and second auxiliary coils is eliminated. The impedance changing means is comprised of a switch element which is controlled such that the switch is closed in a predetermined time after the direction of a current of the chief coil is changed over. The first and second auxiliary coils and the impedance changing means are driven separately by respective DC sources, and the voltage of the DC source of the first and second auxiliary coils is set to a value larger than that of the DC source of the impedance changing means. The impedance changing means changes its impedance from high to low in approximately one half of a current vibration period after the current is changed over. This period is determined by the inductance of the chief coil and the capacitance in the vicinity of the chief coil. In this embodiment, when the current of the chief coil is reversed, all of the magnetic energy originally stored in the chief coil is not consumed, but only energy corresponding to a current decrease or reduction ΔI (about 20% of I) is consumed during one half of the period of the current vibration. After that, the current vibration of the chief coil is terminated by supplying current to the chief coil from the current path whose impedance is changed to low. Thus, the energy consumption of the chief coil can be lowered. As a result, since the amount of energy supplemented by the auxiliary coil can be small, its supplement time can be short and the driving frequency can be enhanced. In this case, the voltage of the DC source V 2 of the auxiliary coils can be made high, for example, 12V (in the prior art, generally 5V) such that the energy supplementing can be quickened and the driving frequency can be further increased. Here, even if the voltage of the auxiliary coil is increased, the current I 2 supplied from the auxiliary coil is approximately equal to ΔI, i.e., 20% of I, and so a consumed power of the apparatus will not rise greatly. Further, although two sources are used in this embodiment to increase the voltage of the auxiliary coil, a single source of, for example, 5V, can adequately attain the advantage that the driving frequency can be increased. Fig. 7 is a circuit diagram showing a second preferred embodiment of a magnetic head driving apparatus of the present invention. While the rectification elements are arranged in the energy supply circuit for supplying the chief coil without including the auxiliary coil, in the embodiment of Fig 6, switch elements SW 5 and SW 6 , such as field effect transistors, are disposed in place of the rectification elements in the second embodiment. The energy supply can effectively be performed by controlling those switch elements with an appropriate timing. The basic operation of this embodiment is the same as that of the embodiment of Fig. 6. When the switch element SW 1 is closed and the switch element SW 2 is opened, the switch element SW 5 is opened and the switch element SW 6 is closed and the current path CH 1 is opened differently from the embodiment of Fig. 6. In this state, when the switch elements SW 1 and SW 6 are opened and the switch element SW 2 is closed, current is supplied to the chief coil L H from the current path CH 3 and current is supplied to the auxiliary coil L 2 by the current path CH 4 . At this time, as mentioned above, the current vibration occurs due to the magnetic energy stored in the chief coil L H , and the current flowing into the chief coil L H due to the vibration becomes maximum (I 1 +I 2 -ΔI) after one half of the vibration period. Further, since the current I 2 is supplied to the chief coil L H from the current path CH 3 , current supplied to the chief coil L H is I 1 +2I 2 -ΔI. Here, if I 2 ≒ ΔI is established, the supplied current becomes equal to I 1 +I 2 . Since the switch element SW 5 is closed at the time of that maximum value and the current path CH 1 is closed as described above to change its impedance from high to low, the current vibration is terminated and the current I 1 is supplied from the current path CH 1 to the chief coil L H . Thus, the current I 1 and the current I 2 from the auxiliary coil L 1 are supplied to the chief coil L H , and the reversal of current is completed. The switch element SW 6 at the other side operates in the same way, and the impedance of the current path CH 2 is changed to low at the time of the current reversal of the chief coil L H . As a result, the current vibration of the chief coil L H is suppressed. Thus, in this embodiment, since the current vibration of the chief coil is suppressed by controlling the on-off state of the switch elements SW 5 and SW 6 , wasteful consumption of the magnetic energy of the chief coil can be prevented in a manner similar to the above-discussed embodiments. Therefore, the energy supplementing time of the auxiliary coil can be short, and so the driving frequency can be increased. Further, while the current path is opened only when the reverse bias voltage is applied to the rectification element in the embodiment of Fig. 6, the switch elements SW 5 and SW 6 are controlled to be closed by an external control circuit only when necessary in this embodiment. So, no wasteful current is supplied, and as a result a consumed power of the apparatus can further be reduced compared with the embodiment of Fig. 6. According to an experiment, the power reduction was 10-20% as compared with the prior art apparatus. As described in the foregoing, in the present invention, the driving frequency of a magnetic head can greatly be increased as compared with the prior art. As a result, a recording speed of information can be extremely enhanced. The individual components shown in outline or designated by blocks in the drawings are all well-known in the optomagnetic recording apparatus arts and their specific construction and operation are not critical to the operation or best mode for carrying out the invention. While there has been shown and described what are considered preferred embodiments of the present invention, it will be understood by those skilled in the art that various changes and modifications may be made therein without departing from the invention as defined by the following claims.

Claims: A circuit apparatus for generating a magnetic field for driving a magnetic head, said apparatus comprising: a chief coil (L H ) for generating the magnetic field for driving the magnetic head; and a first auxiliary coil (L 1 ) for supplying a first current (I 2 ) ; a first switch element (SW 1 ) serially connected to said first auxiliary coil (L 1 ) at a first connection node; a second auxiliary coil (L 2 ) for supplying a second current (I 2 ); a second switch element (SW 2 ) serially connected to said second auxiliary coil (L 2 ) at a second connection node; a first supply circuit (V 2 , R 1 ) for supplying current to said first auxiliary coil (L 1 ); a second supply circuit (V 2 , R 2 ) for supplying current to said second auxiliary coil (L 2 ), the circuit apparatus being characterized by: a third supply circuit (V 1 , R 3 , D 3 or SW 5 ) connected to said first switch element (SW 1 ) in parallel with said first auxiliary coil (L 1 ) for supplying a third current (I 1 ) to said chief coil (L H ); and a fourth supply circuit (V 1 , R 4 , D 4 or SW 6 ) connected to said second switch element (SW 2 ) in parallel with said second auxiliary coil (L 2 ) for supplying a fourth current (I 1 ) to said chief coil (L H ); said chief coil (L H ) being connected between the first and second connection nodes, wherein said first switch element (SW 1 ) establishes a path for the second and fourth currents through said chief coil (L H ), and said second switch element (SW 2 ) establishes a path for the first and third currents through said chief coil (L H ). A circuit apparatus according to claim 1, wherein said third supply circuit (V 1, R 3 , D 3 ) and said fourth supply circuit (V 1 , R 4 , D 4 ) each comprise a rectification element (D 3 , D 4 ). A circuit apparatus according to claim 1, wherein said third supply circuit (V 1 , R 3 , SW 5 ) and said fourth supply circuit (V 1 , R 4 , SW 6 ) each comprise a switch element (SW 5 , SW 6 ). A circuit apparatus according to any one of the preceding claims, wherein said first (V 2 , R 1 ), second (V 2 , R 2 ), third (V 1 , R 3 , D 3 ) and fourth (V 1 , R 4 , D 4 ) supply circuits include a common power source. A circuit apparatus according to any one of the claims 1 to 3, wherein said first (V 2 , R 1 ) and second (V 2 , R 2 ) supply circuits include a first power source (V 2 ) and said third (V 1 , R 3 , D 3 ) and fourth (V 1 , R 4 , D 4 ) supply circuits include a second power source (V 1 ).

Inventors: KAZUYOSHI ISHII, KAZUYOSHI, ISHII
Applicants: CANON KK, CANON KABUSHIKI KAISHA
Application year: 1992
Main classification: G11B11
IPC codes: G11B5, H03K17, G11B11