JP5149134B2 - Superconducting magnet device - Google Patents

Description

  The present invention relates to a superconducting magnet apparatus using a superconducting coil, and more particularly to a superconducting magnet apparatus which is suitable for a magnetic resonance imaging (hereinafter referred to as MRI) apparatus and has improved operational stability and an MRI apparatus using the same.

  Conventionally, the mainstream of MRI devices is a magnet device for generating a static magnetic field that uses a slender cylindrical solenoid coil. Recently, however, open MRI devices have been developed that open up examination spaces where patients can lie down. . The open MRI system has a structure in which magnets for generating a static magnetic field are arranged above and below the examination space, enabling interventional procedures, that is, performing surgery, endoscopy, etc. while performing MRI examinations. Yes. The initial version of the open-type MRI system was for low and medium magnetic fields that adopted a permanent magnet as a magnet. However, in recent years, superconducting magnets have also been introduced in the open-type MRI system for higher image quality and higher functionality. Is being measured.

  In order to realize high image quality and high functionality of the MRI system, not only a magnet that generates a high magnetic field strength is used as a magnet for generating a static magnetic field, but also a high-speed imaging method and high-performance and high-speed operation. The gradient magnetic field generating means, the high frequency magnetic field generating means for exciting the nuclear spin at the examination site of the subject in a short time, and the high frequency coil (RF coil) for detecting the NMR signal with high sensitivity are also necessary components. Accordingly, such high-performance gradient magnetic field coils, high-frequency coils, and the like have been mounted on open-type MRI apparatuses using superconducting magnets.

  By the way, in general, in a magnet device using a superconducting magnet, a superconducting coil that generates a magnetic field is installed in a cryostat filled with liquid helium, and the superconducting coil kept below the critical temperature by liquid helium is excited, After a predetermined permanent current value is achieved, the permanent current switch (PCS) is turned on so that the permanent current flows to the superconducting coil. In such an MRI apparatus using a superconducting coil, once the state of the permanent current is destroyed due to a change in the temperature of the environment where the superconducting coil is placed, not only imaging becomes impossible, but a great deal of recovery is required. It will take time and effort. On the other hand, there may be situations where the static magnetic field strength must be rapidly broken even during imaging due to sudden circumstances such as changes in the patient's condition. For this reason, in an MRI apparatus using a superconducting coil, a monitor circuit that monitors the amount of liquid helium in the cryostat or an emergency reduction that stops the operation of the magnet device by demagnetizing the superconducting coil by raising the temperature of the superconducting coil above the critical temperature in an emergency. An apparatus including a magnetic unit has been developed (for example, Patent Document 1). Patent Document 2 describes a technique for reducing noise generated by an excitation power source when switching a superconducting coil to permanent current mode operation.

Japanese Patent Application No. 2001-75814 Japanese Patent Laid-Open No. 2001-110626

  In the MRI apparatus using the above-described superconducting magnet, it has been found that the following problems arise when an open type superconducting magnet is employed and the above-described enhancement in function and image quality is realized. That is, in a unit that generates a strong high-frequency magnetic field in a short time, or a unit that switches at high speed and generates a high gradient magnetic field strength, the capacity of the power source that drives them inevitably increases. Induces noise due to electromagnetic interference in surrounding electrical circuits. In the open MRI system, the shape of the RF coil that generates a high-frequency magnetic field and the gradient magnetic field coil that generates a gradient magnetic field are also flat. Similar to the increase in capacity, it causes noise due to electromagnetic interference in the MRI apparatus itself and in the surrounding electric circuit.

  Therefore, the present invention eliminates the influence on the superconducting coil circuit due to the change in magnetic flux due to the gradient magnetic field and the high frequency magnetic field accompanying the MRI scan, and uses the superconducting magnet capable of reliably and stably operating the superconducting magnet. The purpose is to provide an MRI apparatus.

  In order to achieve the above object, the present inventors have examined in detail the peripheral electric circuit for the possibility of affecting the superconducting coil circuit in the MRI apparatus. As a result, a sensor element for measuring the environment in the container installed in the container for storing the superconducting coil, a heater for emergency demagnetization, etc., an external control circuit or an external monitor circuit connected to them, and a superconducting coil circuit A closed loop circuit due to electromagnetic coupling, which could not be expected with conventional devices, in particular, in a device in which a pair of superconducting magnets are arranged across a measurement space and connected via a connecting pipe When the electromagnetic coupling is large, and the magnetic flux change due to the gradient magnetic field or the high frequency magnetic field passes through the closed loop circuit due to the MRI scan, the control circuit or the monitor circuit malfunctions, thereby destroying the permanent current state. The present inventors have found that this can be done, and have arrived at the present invention.

That is, the superconducting magnet device of the present invention is a superconducting magnet device comprising a superconducting coil, a superconducting coil circuit having a permanent current switch in the superconducting coil, and a container for storing the superconducting coil at a temperature for maintaining the superconducting coil in a superconducting state. The superconducting magnet is characterized in that means for electromagnetically shielding the superconducting coil circuit from the outside of the superconducting coil circuit is provided.

  The superconducting magnet apparatus according to the present invention further includes a superconducting coil circuit having a superconducting coil and a permanent current switch for passing a permanent current through the superconducting coil, and a container for storing the superconducting coil at a temperature that maintains the superconducting state. In the magnet device, the container includes a terminal portion for connecting an element installed in the container to an external circuit, and the terminal portion includes an outer wall of the container and a grounding point provided on the outer wall. A means for forming a closed loop circuit is provided.

  The MRI apparatus of the present invention is equipped with such a superconducting magnet device as a static magnetic field generator, for example, a superconducting coil circuit having a superconducting coil and a permanent current switch for passing a permanent current through the superconducting coil, A control circuit comprising a superconducting magnet having an element for controlling demagnetization of a superconducting coil or measuring the amount of liquid helium contained in a helium vessel, and a control circuit or a monitor circuit electrically connected to the element. Alternatively, the monitor circuit is provided with means for blocking the formation of a closed loop circuit with respect to the superconducting coil circuit.

  In the MRI apparatus of the present invention, for example, a filtering circuit unit or a switch circuit can be adopted as the blocking means, and such blocking means is connected between the element and the control circuit or monitor circuit. The filtering circuit unit may include, for example, an outer case and a filter element accommodated in the outer case, and in this case, a conductor connected to the outer case forms a closed loop circuit with a control circuit or a monitor circuit.

  According to the superconducting magnet apparatus and the MRI apparatus of the present invention, the closed loop circuit generated by the coupling of the control circuit, the monitor circuit, and the superconducting coil circuit can be substantially cut off. Even if electromagnetic interference occurs due to, the induced current does not flow to the superconducting coil circuit, and stable operation of the superconducting coil circuit can be ensured.

  The MRI apparatus of the present invention also includes a superconducting coil circuit having a superconducting coil and a permanent current switch for passing a permanent current through the superconducting coil, and an element for controlling the demagnetization of the superconducting coil or measuring the amount of liquid helium. A superconducting magnet housed in a container; a control circuit or a monitor circuit electrically connected to the element; and a gradient magnetic field generating means for generating a gradient magnetic field that gives a magnetic field gradient to a static magnetic field generated by the superconducting magnet; A high-frequency magnetic field generating means for generating a high-frequency magnetic field to be applied to the subject, and a means for blocking the control circuit or the monitor circuit from forming a closed loop circuit with respect to the superconducting coil circuit.

  In this MRI apparatus, preferably, the blocking means is a filtering circuit that cuts at least a signal of a driving frequency of the gradient magnetic field generating means and a frequency band of a high frequency magnetic field.

  The present invention can be suitably applied to an MRI apparatus in which a pair of superconducting coils of a superconducting magnet is disposed across a measurement space in which a subject is placed. Further, the gradient magnetic field generating means and the high-frequency magnetic field generating means can be suitably applied to an MRI apparatus in which flat coils are respectively arranged across a measurement space where a subject is placed. In these MRI apparatuses, particularly good effects can be obtained.

  According to the present invention, it is possible to eliminate the influence on the superconducting coil circuit caused by the change in magnetic flux due to the gradient magnetic field and the high-frequency magnetic field accompanying the MRI scan, and to reliably operate the MRI apparatus stably.

  Hereinafter, embodiments of the present invention will be described with reference to the drawings.

  FIG. 1 is an overall configuration diagram of an MRI apparatus to which the present invention is applied. This MRI apparatus includes a pair of static magnetic field generating magnets 102 arranged so as to sandwich an examination space where the subject 101 is placed, a gradient magnetic field coil 103 arranged on the examination space side of each of the static magnetic field generating magnets 102, and A high-frequency coil 105 disposed inside thereof, a detection coil 107 for detecting an NMR signal generated from the subject 101, and a transfer table 114 for arranging the subject 101 in the central space of the static magnetic field generating magnet 102 are provided. Yes. The gradient magnetic field coil 103 and the high frequency coil 105 have a pair of upper and lower plate-like structures so as not to disturb the advantages of the open magnet. In the figure, the high frequency coil 105 and the detection coil 107 are shown as separate coils, but one high frequency coil may serve both for high frequency magnetic field irradiation and detection.

  The static magnetic field generating magnet 102, the gradient magnetic field coil 103, the high frequency coil 105, the detection coil 107, and the transfer table 114 are installed in a shield inspection chamber 115 that is shielded from electromagnetic waves. Electromagnetic shielding prevents foreign electromagnetic waves from flying into the detection coil 107, and has an attenuation factor of, for example, about 70 dB in the resonance frequency band of the nucleus used for inspection (usually 42 megahertz for hydrogen nuclei used). ing.

  Outside the shield examination room 115, there are a gradient magnetic field power source 104 for driving the gradient magnetic field coil 103, a high frequency power amplifier 106 for driving the high frequency coil 105, a receiver 108 for receiving a signal detected by the detection coil 107, and the operation of each coil. A sequencer 109 for controlling the timing and a computer 110 for controlling the apparatus and processing and imaging the NMR signal are provided.

  The power supply and control equipment installed outside the shield inspection room 115 are connected to various coils, the static magnetic field generating magnet 102, and the transfer table 114 in the shield inspection room 115 through a filter circuit 116 grounded to the shield inspection room 115. Or connected by a coaxial cable whose outer part is covered with a shield layer (the distinction between coaxial cables is not shown in the figure). This prevents external noise from being drawn into the shield inspection room 115.

  In the illustrated embodiment, the static magnetic field generating magnet 102 constitutes a magnetic circuit for a pair of cryostats 117 divided into upper and lower parts, a superconducting coil incorporated in each cryostat 117, and a magnetic flux generated by the superconducting coil. It consists of an iron yoke (not shown). The superconducting coil generates a static magnetic field having a uniform strength in the space in which the subject 101 is disposed. The magnetic field strength is, for example, 1.0 Tesla, the direction of magnetic flux is from the floor to the ceiling, and the magnetic field uniformity is adjusted to be about 5 ppm or less in a spherical space with a diameter of 40 centimeters where the subject 101 is disposed. Has been. The magnetic field uniformity is adjusted by passive shimming or active shimming. In passive shimming, for example, a plurality of small magnetic pieces (not shown) are attached to the surfaces of a pair of cryostats 117.

  Further, although not shown in FIG. 1, the static magnetic field generating magnet 102 includes an internal circuit such as a power source for excitation and a permanent current switch (PCS) for maintaining a permanent current, and controls its operation. An emergency demagnetizing unit 120 that quickly attenuates the magnetic field generated by the static magnetic field generating magnet 102 in an emergency situation and a measurement unit 121 that monitors internal information of the pair of cryostats 117 are connected. The measurement unit 121 is connected to the computer 110 via the filter circuit 116, and sends the measured internal information to the computer 110 as an electrical signal. In the illustrated example, the emergency demagnetization unit 120 is attached to the wall surface of the shield inspection chamber 115, and the measurement unit 121 is attached to the rear of the transfer table 114. The signal cables of the emergency demagnetization unit 120 and the measurement unit 121 are connected to a heater, a measurement element, and the like installed inside the cryostat 117 via the filter circuit 122.

  The gradient magnetic field coil 103 is composed of three sets of coils wound so as to change the magnetic flux density in three axial directions of x, y, and z orthogonal to each other, each connected to the gradient magnetic field power source 104, and the gradient magnetic field generating means Configure. The gradient magnetic field power supply 104 is driven in accordance with a control signal from the sequencer 109 to change the current value flowing through the gradient magnetic field coil 103, thereby changing the gradient magnetic fields Gx, Gy, and Gz consisting of three axes into the static magnetic field in the installation space of the subject 101. It is designed to be superimposed on. This gradient magnetic field is used to identify the spatial distribution of NMR signals obtained from the examination site of the subject 101.

  The high-frequency coil 105 is connected to a high-frequency power amplifier 106 for causing a high-frequency current to flow through the high-frequency coil 105, and generates a high-frequency magnetic field of, for example, 42 megahertz for resonance excitation of hydrogen nuclei at the examination site of the subject 101. The high frequency power amplifier 106 is also controlled by the control signal of the sequencer 109.

  The detection coil 107 is connected to the receiver 108 and constitutes a means for detecting the NMR signal. The receiver 108 amplifies and detects the NMR signal detected by the detection coil 107 and converts it to a digital signal that can be processed by the computer 110. The operation timing of the receiver 108 is also controlled by the sequencer 109.

  The computer 110 performs operations such as image reconstruction and spectrum calculation using the NMR signal converted into a digital quantity, and controls the operation of each unit of the MRI apparatus via the sequencer 109 at a predetermined timing. The computer 110, the display device 111 that displays the processed data, and the console 112 that performs operation input constitute an arithmetic processing system.

  The details of the static magnetic field generating magnet 102 which is a magnetic field generator will be further described. As shown in FIG. 2, a pair of cryostats 117 are connected by a connecting pipe 201, and the static magnetic field generating magnet 102 is arranged above and below a space 118 in which a subject is arranged. The inside of the pair of cryostats 117 is maintained at a high vacuum, and an upper helium tank 202 and a lower helium tank 203 filled with liquid helium are incorporated therein. A pair of superconducting coils 204 is housed in the upper helium tank 202 and the lower helium tank 203, and this superconducting coil 204 is maintained at a low temperature of 4.2 degrees Kelvin by liquid helium, and is supplied to the superconducting coil 204, for example, 400 amperes. A permanent electric current of 1.0 Tesla is generated in the space 118. FIG. 2 shows a pair of superconducting coils 204. However, in order to set the magnetic field strength, the magnetic field uniformity, or the leakage magnetic field strength to a predetermined value, a plurality of superconducting coils having different sizes and winding numbers may be accommodated.

  A heat shield 205 is provided between the cryostat 117 and the upper helium tank 202 and the lower helium tank 203 so as to surround the helium tank. Although only one layer is shown in the figure, the heat shield 205 may be two or more layers, and is made of, for example, an aluminum plate having a thickness of 1 mm. The heat shield 205 is thermally connected to the helium refrigerator 206 at a contact point 207, and is maintained at a low temperature of 20 degrees Kelvin, for example. Covering the upper helium tank 202 and the lower helium tank 203 with the low-temperature heat shield 205 in this way prevents direct radiant heat from room temperature (300 degrees Kelvin), thereby minimizing the evaporation of liquid helium. it can. The upper helium tank 202, the lower helium tank 203, the heat shield 205, and the pair of cryostats 117 are connected at the connecting pipe 201 so that the temperatures in the upper and lower helium tanks are the same.

  In the upper helium tank 202 and the lower helium tank 203, in addition to the superconducting coil 204, a permanent current switch (PCS) 208, a heater element 209 for emergency demagnetization, a sensor element 210 for measuring the level of liquid helium, and a protective element for the superconducting coil ( (Not shown in the figure). The heater element 209 and sensor element 210 are connected to a control circuit (emergency demagnetization unit 120, measurement unit 121) installed outside the superconducting magnet 102 via a connector 211. The lead wires 212 connecting the elements in the upper helium tank 202 and the lower helium tank 203 and the pair of superconducting coils 204 are bundled and assembled together in the connecting pipe 201.

  FIG. 3 shows an equivalent circuit of the superconducting coil circuit of the static magnetic field generating magnet 102 and the external control circuit.

  The superconducting coil circuit includes a pair of superconducting coils 204 connected in series, a permanent current switch PCS208 connected in parallel at both ends thereof, an excitation power source 303a for exciting the superconducting coil, and a heater 306 built in the PCS208. The superconducting coil 204 and the PCS 208 are in a cryostat 117 indicated by a dotted line in the figure, and are connected to an external excitation power source 303a and a heater power source 303b by terminals 301, 302, 304, and 305, respectively. Yes. The cryostat 117 is connected to the ground point 123 of the filter box, which is the system ground, and is maintained at the ground potential.

  Although not shown, a protection diode element for protecting and checking the superconducting coil 204 and a lead wire for measuring the voltage and resistance at each point in the closed loop are connected. These lead wires and the superconducting wires connecting the superconducting coil 204 and the PCS 208 to the terminals are bundled and passed through the connecting pipe 201.

  When exciting the superconducting coil 204, connect the heater power supply 303b to the terminals 304 and 305 of the PCS 208, and gradually increase the output from the exciting power supply 303a while keeping the superconducting coil 204 in the normal conducting state due to the heat generated by the built-in heater 306. . When the current flowing through the superconducting coil 204 reaches a desired current value, the power supply 303b of the heater 306 is turned off to form a closed loop (arrow 300) between the PCS 208 and the superconducting coil 204 so that the permanent current due to the superconducting state flows through the closed loop 300. To.

  Aside from such a drive circuit, as a control circuit and a monitor circuit for maintaining and managing the operation of the static magnetic field generating magnet 102 (hereinafter sometimes abbreviated as a control / monitor circuit), the cryostat 117 has an emergency Sometimes a heater element 209 for attenuating the magnetic field and a sensor element 210 for measuring the amount of liquid helium in the upper and lower helium tanks 202 and 203 are provided. The heater element 209 is a resistance element that generates heat when a voltage is applied from the emergency demagnetization unit 120, and is connected to the emergency demagnetization unit 120 via a terminal 211. The sensor element 210 is made of, for example, a superconducting material whose resistance value changes depending on temperature, and is installed in upper and lower helium tanks. The upper and lower sensor elements are electrically connected to each other, and the middle point of each sensor element. Are connected to the liquid helium measurement unit 121 via a terminal 211. Lead wires connecting the heater element 209 and sensor element 210 and the terminal 211 are also bundled and passed through the connecting pipe 201.

  Thus, the lead wire constituting the superconducting coil circuit and the lead wire constituting the control / monitor circuit (emergency demagnetization unit 120, liquid helium measurement unit 121) pass through the thin connecting pipe 201 connecting the upper and lower cryostats 117. Because they are threaded, they bind strongly to each other. This coupling is shown as stray capacitances 307, 308 in FIG. The value of this stray capacitance is greatly affected by the shape of the magnet, how the lead wires are bundled and how they are arranged, but in the case of the device of this embodiment, typically, it is between the superconducting coil circuit and the control / monitor circuit. It was found that the stray capacitance 307 was 0.7 nanohenry, and the stray capacitance 308 between the superconducting coil circuit and the cryostat 117 was about 6 nanohenry. As a result of such coupling, as shown in FIG. 5, the closed loop circuit from the control / monitor circuit 120, 121 through the terminal 211, the lead wire, the stray capacitance 307, the superconducting coil circuit, the stray capacitance 308, and the ground point 123 of the cryostat. 501 is formed.

  The MRI apparatus of the present embodiment is a circuit interruption means between the terminal 211 and the external control / monitor circuit in order to prevent the current from flowing through the superconducting coil circuit through the stray capacitances 307 and 308. 310 is provided. Specifically, a filter circuit, a switch circuit, or a combination of these is employed as the circuit interrupting means 310.

  An embodiment of the filter circuit is shown in FIG. The filter circuit includes a current feed type filter element 407. As shown in the figure, the current feed-through filter element 407 is a π-type filter element in which an inductance element 410 is incorporated in an exterior (outer case) made of a metal tube 408, and a feed-through capacitor 409 is configured with its input terminal and output terminal. By using such a current feed-through filter element, induction of noise voltage from the outside is avoided, and the signal voltage of the input terminal is low frequency by removing high frequency components such as induction noise (generally DC current Only the electrical signal of the sensor element is transmitted to its output terminal.

  The current feed-through filter 407 is connected to each terminal (FIG. 3, 211) on the cryostat side via the connector 401, and is connected to the measurement unit 121 and the emergency demagnetization unit 120 via the connectors 402, 403. The For example, the terminals 404A and 404B of the connector 401 are terminals for applying a voltage to both ends of a helium liquid level sensor as a sensor element, and the terminals 404C, 404D and 404E are connected to both ends and a middle point of the liquid level sensor. This is a terminal for measuring the change in resistance between the center and the middle point. The terminals 404F and 404G are connected to the heaters 209 of the upper helium tank and the lower helium tank.

  Next, the operation when such a filter circuit is provided will be described with reference to FIGS. FIG. 5 is a conventional circuit configuration diagram in which a filter circuit is not provided, and FIG.

  First, when no circuit interruption means is provided, the ground point 123 of the cryostat 117 and the liquid helium measurement circuit 121 and the liquid helium measurement circuit 121 and the emergency demagnetization unit 120 are connected to the terminal 211 as shown in FIG. A large loop circuit 501 passing through the ground point of the emergency demagnetizing unit 120 is formed. In this state, when scanning (imaging) of the MRI apparatus is started, the magnetic flux of the gradient magnetic field and high-frequency magnetic field that are pulse-driven along with imaging pass through the loop circuit 501, and several volts to several tens of volts. Inductive voltage is generated.

  When the pulsed induced voltage is applied to the terminal 211 in this way, an induced current flows through the closed loop circuit 300 through which a permanent current flows from the sensor element circuit via the stray capacitance 307 as indicated by an arrow in the figure. The inductance of the superconducting coil 204 is extremely high, and, for example, 36 Henry is shown in this embodiment. For this reason, most of the pulsed induced current flows from the circuit on the PCS 208 side having a resistance value of zero to the ground of the cryostat 117. Since this current is pulse-like induced noise, it may flow locally, such as the superconducting skin of PCS208, and may exceed the intrinsic critical current of the superconducting wire. When the critical current is exceeded for a moment, the PCS 208 transitions to the normal conducting state, and the current 400 amperes of the closed loop circuit 300 is consumed as thermal energy by the normal conducting resistance of the PCS 208, a quench phenomenon occurs in the magnet, and the magnetic field disappears.

  On the other hand, as shown in FIG. 6, when the filter circuit 400 is incorporated between the terminal 211 and the external control circuit, the outer case of the cryostat 117, the ground point 123, and the outer case of the filter circuit 400 The liquid helium measurement circuit 121 and the connection cable of the emergency demagnetization unit 120 form a closed loop (arrow 601 in the figure). In this state, when a gradient magnetic field or a high-frequency magnetic field is pulse-driven and the magnetic flux passes through the loop circuit 601, an induced voltage of several volts to several tens of volts is generated. Here, the inside of the cryostat 117 has the same circuit constant as in the case of FIG. 5, but the impedance of the terminal 211 becomes a very high value due to the presence of the filter circuit 400. Although this impedance value depends on the frequency of the passing current, since the magnetic flux change of the gradient magnetic field and the high frequency magnetic field pulse-driven according to the imaging sequence is several hundred kilohertz or more, the impedance value is a value of several mega ohms. On the other hand, the impedance value between the input terminal 409 of the filter circuit 400 and the ground is several ohms or less. As a result, the pulsed induced current flows directly through the outer case of the filter circuit 400 to the case of the cryostat 117 and does not flow into the cryostat 117. That is, the filter circuit 400 can block the formation of a substantial loop circuit (501 in FIG. 5) between the internal circuit of the cryostat 117 and the connection cable of the liquid helium measurement circuit 121 and the emergency demagnetization unit 120. it can.

  In this way, by providing the filter circuit 400 as a cutoff circuit in the terminal 211 portion connecting the internal circuit of the cryostat 117 and the outside, it is possible to suppress the inductive current from flowing into the internal circuit due to the MRI scan, and a stable superconducting magnet The operation of the device can be ensured.

  A more specific structure of the filter circuit 400 is shown in FIG. In FIG. 7, the elements corresponding to the elements shown in FIG. 4 are denoted by the same reference numerals.

  In this structure, the current feed type filter element 407 is firmly fixed to the copper plate 701, one side is connected to the connector 401 via the lead wire, and the other side is the connector 402 of the measuring unit 121, the emergency demagnetizing unit. It is connected to 120 connectors 403. Although only two filter elements 407 are shown in the figure, actually, as many filter elements as the terminals of the connector 401 are provided as shown in FIG. The connector 401 is composed of a metal shell and has a structure in which external noise is not induced in the core wire. The copper plate 701 that fixes the metal shell of the connector 401 and the current feed filter element 407 is electrically connected by a shield copper net 702. Further, the outer periphery of the metal shell of the connector 401 and the terminal portion 211 of the cryostat 117 are wound with a shield copper wire 703, and the shield copper wire 703 is firmly fixed with a reinforcing band 704. Thus, the metal shell of the connector 401 is configured to be reliably connected to the ground potential of the ground point 123 of the outer case of the cryostat 117.

  As described above, the embodiment in which the filter circuit is employed as the circuit interruption means has been described. According to the present embodiment, only the induced current of the cryostat is obtained by using the frequency difference of the current component induced by the gradient magnetic field or the high frequency magnetic field and the frequency difference of the superconducting magnet control / monitor circuit that handles the DC current level. The effect can be completely removed by flowing on the metal surface.

  Next, as another embodiment of the MRI apparatus of the present invention, an apparatus provided with a switch circuit as a circuit interruption means will be described. FIG. 8 is a diagram showing an overall outline of the apparatus, and the same components as those in FIG. 1 are denoted by the same reference numerals. In FIG. 8, the power supply and control equipment installed outside the shield inspection room 115 are omitted, but these are the same as those in FIG.

  In this apparatus, unlike the apparatus of FIG. 1, the signal cables of the emergency demagnetizing unit 801 and the measuring unit 802 are connected to the internal circuit of the static magnetic field generating magnet 102 without passing through a filter circuit or the like. Further, the emergency demagnetization unit 801 and the measurement unit 802 are incorporated with a switch circuit so that induction noise is not induced in the signal cable in accordance with the pulse drive of the gradient magnetic field or the high frequency magnetic field.

  As shown in FIG. 9, the emergency demagnetization unit 801 is connected to a commercial power source 901, and transforms a commercial power source voltage (100 to 120V) to a desired voltage, a rectifying diode 903, a transformer 902, and the like. A secondary battery 904 functioning as a power source during a power failure, a current drive circuit 905, and a switch circuit 906 provided between the current drive circuit 905 and the connector 907. The power cable connected to the commercial power source is a three-phase cable, and one wire is a ground cable connected to the unit ground including the case of the emergency demagnetizing unit 801 in accordance with the electrical safety standard.

  The connector 907 is connected to the terminal 211 of the cryostat 117 and is connected to the emergency demagnetization heater 209 in the cryostat 117. The switch circuit 906 operates by pressing an external button (not shown), and cuts off both the line connected to the ground potential and the line to which the voltage is applied. By blocking both lines in this way, the closed loop circuit (FIG. 5, 501) formed through the ground potential can be completely blocked. In this case, the switch circuit 906 and the connector 907 are covered with an insulating case to ensure safety.

  In such a configuration, the operator presses the external button of the emergency demagnetizing unit 801 to operate the switch circuit 906 when emergency demagnetization is necessary. In this state, the voltage from the commercial power supply is transformed by the transformer 902, then rectified by the rectifier circuit of the diode 903, charges the storage battery 904, and is input to the current drive circuit 905. The output of the current drive circuit 905 is transmitted via a switch circuit 906 to a connector 907 connected to the heater element. As a result, the heater element generates heat, the superconducting state is destroyed, and the superconducting coil becomes a normal conducting state and rapidly demagnetizes.

  On the other hand, when the switch circuit 906 is in a shut-off state in a normal state, a closed circuit including a heater element is not formed. Therefore, a closed loop as shown in FIG. 5 is formed between the emergency demagnetizing unit and the internal circuit of the cryostat. The circuit 501 is not formed.

  As shown in FIG. 10, the measurement unit 802 applies a predetermined voltage to the interface circuit 1001 for exchanging data signals and control signals with the computer 110 (FIG. 1) of the MRI apparatus, and the liquid level sensor. A helium measurement circuit 1002 that calculates the amount of liquid helium from the measured measurement value, a switch circuit 1003 provided between the helium measurement circuit 1002 and the connector 1005 connected to the liquid level sensor, and an interface A control circuit 1004 for controlling the operation of the helium measurement circuit 1002 and the switch circuit 1003 based on a control signal from the circuit 1001 is provided. Here again, the switch circuit 1003 uses a switch for intermittently connecting both plus and minus. As in the case of the emergency demagnetizing unit 801, the switch circuit 1003 and the connector 1005 are covered with an insulating case.

  In such a configuration, when a command for measuring the amount of helium is input from an input device (for example, the console 112) provided in the computer 110 of the MRI apparatus, the signal is input to the control circuit 1004 via the interface circuit 1001. As a result, the switch circuit 1003 is closed and the helium measurement circuit 1002 starts operating. For example, the helium measurement circuit 1002 applies a current of 400 milliamperes to the liquid level sensor 210 for about 10 seconds, and measures the resistance value of the liquid level sensor element when the current is applied. As already described, the liquid level sensor element is made of a material whose resistance value varies depending on the temperature, and the current of the sensor element rises by passing a current of 400 milliamperes. However, since the temperature of the portion immersed in liquid helium does not increase, the resistance value is proportional to the length of the portion above the helium liquid surface. Therefore, the decrease in the liquid amount can be obtained by measuring the change in the resistance value. The liquid amount measured by the helium measurement circuit 1002 is input as a data signal to the computer 110 of the MRI apparatus via the interface circuit 1001 and displayed on the display 111.

  Such a measurement of the amount of helium may be performed once, for example, at a regular inspection or startup of the apparatus. In other cases, the monitor circuit 802 of the measurement unit 802 is cut off by the switch circuit 1003. Yes. Therefore, similarly to the emergency demagnetization unit 801, the closed loop circuit 501 as shown in FIG. 5 is not formed between the measurement unit 8 and the internal circuit of the cryostat.

  As described above, the MRI apparatus of the present embodiment in which the switch circuit is inserted as the circuit interruption means utilizes the fact that the time when the emergency demagnetization unit and the measurement unit perform their functions and the time when the subject is inspected never coincide. The switch circuit is operated so that a substantially closed loop is not formed while the gradient magnetic field or the high-frequency magnetic field is driven. Therefore, the control circuit and the monitor circuit itself are completely disconnected from the superconducting magnet 102 except in the case of an emergency or periodic inspection, so that the gradient magnetic field and the high-frequency magnetic field are driven by the scanning of the MRI apparatus. However, the induced current induced thereby flows to the ground through the outer case of the cryostat 117 and does not affect the internal circuit, as in the case of the apparatus having the filter circuit shown in FIG. . On the other hand, when the operation of the emergency demagnetization unit 801 is required, the switch circuit is connected, and the cryostat 117, the emergency demagnetization unit 801, and the connection cable form a closed loop. Originally, when the magnetic field of the superconducting magnet 102 is attenuated, there is no problem even if a closed loop is formed and induction noise is induced by driving a gradient magnetic field or a high-frequency magnetic field to cause magnetic field attenuation. The liquid helium measurement unit 802 operates when the MRI apparatus is maintained and inspected, and when the gradient magnetic field or the high frequency magnetic field is not driven. Even if a closed loop is formed, no induction noise is induced.

  As described above, as the embodiment of the present invention, the embodiment in which the filter circuit is employed as the circuit interrupting means and the embodiment in which the switch circuit is employed have been described, but both the filter circuit and the switch circuit may be provided. In the above embodiments, the MRI apparatus has been mainly described. However, the superconducting magnet apparatus of the present invention is not only applied to the MRI apparatus, but generally applied to a superconducting magnet apparatus having a terminal for connecting a superconducting coil and an external circuit. Can do.

The figure which shows one Embodiment of the MRI apparatus of this invention The figure which shows the details of the magnetic field generator which the MRI equipment of Figure 1 adopts The figure which shows the equivalent circuit of the magnetic field generator of FIG. Circuit diagram showing the filter circuit The figure explaining formation of a closed loop circuit in the conventional MRI apparatus The figure explaining the function of the circuit interruption means in the MRI apparatus of this invention Diagram showing the structure of the filter circuit The figure which shows other embodiment of the MRI apparatus of this invention Circuit diagram showing emergency demagnetization unit including switch circuit Block diagram showing helium measurement unit including switch circuit

Explanation of symbols

  102 Superconducting magnet, 103 Gradient magnetic field coil, 105 High frequency coil, 120 Emergency demagnetization unit, 121 Measurement unit, 310 Circuit breaker, 400 Filter circuit, 906, 1003 Switch circuit

Claims (3)

A superconducting coil circuit housed in a shield inspection chamber and having a superconducting coil and a permanent current switch for switching whether or not to pass a permanent current through the superconducting coil, and a container for housing the superconducting coil ,
Control means for maintaining and managing the operation of the superconducting coil circuit is connected to the inside and outside of the container via a signal cable, and the inductive noise generated in the shield inspection chamber is prevented from flowing into the superconducting coil circuit. A superconducting magnet device provided in the signal cable with a suppression means to perform,
The suppression means uses the frequency component of the induced noise induced by the gradient magnetic field or the high-frequency magnetic field and the frequency difference of the control circuit of the superconducting magnet that handles the direct current level, and only induces the induced noise on the metal surface of the cryostat. A superconducting magnet device characterized by flowing. 2. The superconducting magnet device according to claim 1, wherein the control means includes a heater element for controlling demagnetization of at least the superconducting coil housed in the container and / or a sensor element for measuring the amount of liquid helium, and the outside of the container. a provided, the superconducting magnet apparatus characterized by a heater element and electrically connected to the control circuit and / or a monitor circuit electrically connected to the sensor element. A superconducting magnet apparatus according to claim 2, wherein the suppression hand stage, connected filter between the connected filter circuit and / or the sensor element and a monitor circuit between the heater element and control circuit A superconducting magnet device characterized by being a circuit.

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