1. Field of the Invention
The present invention relates generally to superconducting magnet apparatuses each equipped with a superconducting coil, and more particularly to protection of a superconducting coil during a quench.
2. Description of the Related Art
Superconducting magnet apparatuses are each equipped with, for example, a superconducting coil, an excitation power supply that supplies current to the superconducting coil, and a persistent current switch that forms a closed circuit for supplying a persistent current. Once a portion of the superconducting coil being energized with the persistent current has suffered a transition into a normal conducting state and developed resistance, the resulting occurrence of joule heat will convert stored magnetic energy into heat energy and increase the temperature of the superconducting coil portion which has transitioned into normal electrical conduction. The periphery of the superconducting coil section which has entered the normal conducting state will also suffer a temperature rise due to heat conduction and make a transition from superconductivity into normal electrical conduction. This transition into normal conduction may eventually extend to the entire superconducting coil in rapid sequence, thus resulting in a so-called quench occurring. When the persistent current is flowing through the superconducting coil and this superconducting coil is holding a large volume of stored magnetic energy, if the large volume of stored magnetic energy is converted into heat energy by the quench, a possible excessive increase in the temperature of the superconducting coil might result in thermal damage to the coil.
Consider a case in which the superconducting coil is a high-temperature superconducting coil constructed of a high-temperature superconductor having a critical temperature exceeding 18 K, such as magnesium diboride (MgB2), iron-based superconductor, or oxide superconductor. The critical temperatures of high-temperature superconductors lie in a region that these superconductors have specific heat capacities at least 10 times as great as those of niobium titanium (NbTi), niobium tin (Nb3Sn), and other low-temperature superconductors having critical temperatures below 18 K. Heat conduction due to a quench causes a delay in the propagation of a normal-conducting region. The quench in a high-temperature superconducting coil, therefore, causes a more significant temperature rise than in low-temperature superconducting coils, since stored magnetic energy is consumed locally.
For this reason, JP-1993-190325-A and other related technical documents propose methods of protecting a superconducting coil. In these methods, a protective resistor that receives a supply of current upon a quench event and consumes stored magnetic energy is provided to suppress the consumption of the stored magnetic energy in the superconducting coil. Since the amount of energy that the protective resistor consumes is proportional to the square of the value of the current flowing through the resistor, applying a higher current to the protective resistor yields a greater suppression effect against the temperature rise due to the quench in the superconducting coil. JP-1991-278504-A and other related technical documents propose methods of supplying a high current to a protective resistor. That is to say, the protective resistor and a persistent current switch are each connected in parallel to and across a superconducting coil so that when a quench occurs, a section of a closed circuit composed of the protective resistor and the persistent current switch, this section not being a closed circuit composed of the protective resistor and the superconducting coil, will be electrically disconnected. By so doing, the current that has been supplied to the persistent current switch can be bypassed and induced into the protective resistor. In addition, when a superconducting magnet apparatus is to be operated on a persistent current, a current lead needs to be disconnected from the internal superconducting circuit of a cryostat for suppressed entry of heat into the cryostat, so a protective resistor cannot be connected to the outside of the cryostat. In this case, therefore, the protective resistor is to be connected to the inside of the cryostat and this connection makes it necessary to provide large enough an installation space inside the cryostat. JP-1986-20303-A and the like, for example, propose methods in which a normal-conducting wire to perform the function of a protective resistor is wound around a superconducting coil in order to save the space required for protective resistor connection.
To induce a high current into a protective resistor so that stored magnetic energy is consumed therein, a heat capacity large enough to avoid thermal damage due to the induction of the high current needs to be imparted to the protective resistor. To this end, a large installation space needs to be provided for the protective resistor. According to JP-1986-20303-A and the like, since a section for supporting the protective resistor can be imparted to the superconducting coil, an installation space for the support section can be saved and that of the protective resistor can be correspondingly increased. Even so, the installation space for the protective resistor is required and the need to provide a large installation space for the resistor remains to be met. It is considered useful if the installation space for the protective resistor can be reduced while at the same time assigning it the function that consumes the stored magnetic energy without causing thermal damage.
Accordingly an object of the present invention is to provide a superconducting magnet apparatus adapted to consume stored magnetic energy without causing thermal damage to a protective resistor, even if an installation space for the protective resistor is reduced.
In order to solve the foregoing problems, a superconducting magnet apparatus according to an aspect of the present invention includes: a bobbin around which a superconducting coil is wound, the bobbin serving as a protective resistor; a persistent current switch for supplying a persistent current to the superconducting coil; a first closed circuit with the superconducting coil and the persistent current switch connected to each other in series; and a second closed circuit with the superconducting coil and the bobbin connected to each other in series.
In accordance with the present invention, since the protective resistor also serves as the bobbin for the superconducting coil, providing a space for the superconducting coil bobbin makes it unnecessary to provide an independent space for the protective resistor. This means that substantially the space provided for the protective resistor separately from the space for the bobbin can be reduced. In other words, a superconducting magnet apparatus adapted to consume stored magnetic energy without causing thermal damage to a protective resistor, even if an installation space for the protective resistor is reduced, can be supplied in accordance with the present invention. Further objects, configurational aspects, and advantages of the invention will be apparent from the detailed description of embodiments that follows.
Other objects and advantages of the invention will become apparent from the following description of embodiments with reference to the accompanying drawings in which:
The following describes embodiments of the present invention in detail referring to the accompanying drawings as appropriate. Elements common to each drawing are each assigned the same reference number or symbol, and overlapped description is omitted herein.
The superconducting coil 3 is provided in singularity or plurality (in an example of
As with the superconducting coil 3, the persistent current switch 6 uses a high-temperature superconductor having a critical temperature exceeding 18 K. The persistent current switch 6 includes a superconducting wire and a heater. As in the superconducting coil 3, in the superconducting wire, a peripheral region of one or a plurality of superconducting filaments is shrouded with a cryogenic stabilizer, spatial gaps between the plurality of superconducting filaments are filled in with the cryogenic stabilizer, and the superconducting filaments are bundled together in the cryogenic stabilizer. The heater and superconducting wire of the persistent current switch 6 are thermally connected to each other. When the heater generates heat, the heater heats the superconducting wire and thus enables the superconducting wire to make a transition from a superconducting state into a normal conducting state. The transition of the superconducting wire into the normal conducting state opens (turns off) the persistent current switch 6. Conversely, stopping the generation of heat in the heater provides cooling by a heat transfer element 2d described later herein, hence allows the superconducting wire to return to the superconducting state, and closes (turns back on) the persistent current switch 6. The cryogenic stabilizer is a metal, such as a copper-nickel alloy or gold-silver alloy, that has higher electrical resistivity than the cryogenic stabilizer (e.g., silver and oxygen-free copper) of the superconducting coils 3 (3a, 3b). In addition, since heating due to magnetic field fluctuations during a quench is likely to make the persistent current switch 6 suffer a transition into normal conduction, in order to prevent thermal damage to the persistent current switch 6, a resistance value of the protective resistor and a circuit composition are appropriately designed for a sufficient reduction in the amount of energy consumed. The persistent current switch 6, the fuse 4, and the superconducting coils 3a and 3b are interconnected in series, these elements composing a first closed circuit C1. Turning on the persistent current switch 6 supplies a persistent current Ip to the first closed circuit C1, especially the superconducting coils 3.
As with the superconducting coils 3, the fuse 4 uses a high-temperature superconductor having a critical temperature exceeding 18 K. The fuse 4 includes a superconducting wire. As in the superconducting coils 3, in the superconducting wire, a peripheral region of one or a plurality of superconducting filaments is shrouded with a cryogenic stabilizer, spatial gaps between the plurality of superconducting filaments are filled in with the cryogenic stabilizer, and the superconducting filaments are bundled together in the cryogenic stabilizer. The fuse 4 and the superconducting coils 3a and 3b are interconnected in series. Connection terminals (connections) 14c and 14d are provided at the opposite ends of the fuse 4.
The bobbin (protective resistor) 5 uses a non-magnetic material, a normal conducting material (electric conductor), and a member having sufficient strength to operate as one element of the bobbin 5. More specifically, the bobbin (protective resistor) 5 uses a member of aluminum, copper, stainless steel, or the like. The bobbin (protective resistor) 5, the persistent current switch 6, and the superconducting coils 3a and 3b are interconnected in series, these elements composing a second closed circuit C2. Connection terminals (connections) 14a and 14b are provided at two places each distant from the bobbin (protective resistor) 5. The connection terminal 14a connects to the connection terminal 14d of the fuse 4 via a superconducting wire 15a. The connection terminal 14b connects to the connection terminal 14c of the fuse 4 via a superconducting wire 15b. Superconducting wires 15a, 15b may instead be superconductive wiring. The bobbin (protective resistor) 5, the connection terminal 14a, the superconducting wire 15a, the connection terminal 14d, the fuse 4, the connection terminal 14c, the superconducting wire 15b, and the connection terminal 14b also compose a closed circuit independent of the first closed circuit C1 and the second closed circuit C2.
The excitation power supply 10 is a direct-current source for supplying a direct current to each superconducting coil 3. The circuit breaker 11 lets the direct current flow from the excitation power supply 10 into the superconducting coil 3 or interrupts the flow of the direct current. The circuit breaker 11 is connected in series to the excitation power supply 10. The circuit breaker 11, the excitation power supply 10, and the persistent current switch 6 are further interconnected in series, these elements composing a third closed circuit C3. In addition, the circuit breaker 11, the excitation power supply 10, the superconducting coil 3, and the fuse 4 are interconnected in series to compose a further, closed circuit, thus enabling magnetic energy to be stored into the superconducting coil 3. The circuit breaker 11 and the excitation power supply 10 are arranged outside a cryostat 2, and can be removed from a main body of the superconducting magnet apparatus 1.
The superconducting magnet apparatus 1 additionally includes a quench detector 7, heater 9, and a current source (direct-current source) 8. The quench detector 7 detects the normal conducting state that may occur in part of the superconducting coil 3 (3a, 3b). The quench detector 7 can detect the occurrence of the normal conducting state in part of the superconducting coil 3 (3a, 3b), as, for example a change in differential potential across the superconducting coil 3 (3a, 3b). The quench detector 7, upon detecting the occurrence of the normal conducting state in part of the superconducting coil 3 (3a, 3b), generates an output of a quench detection signal “Sq” and transmits the signal to the current source 8. The current source 8 is a direct-current source, and upon receiving the quench detection signal “Sq”, supplies a direct current to a heater 9 to energize this heater.
The heater 9 is thermally connected to the fuse 4. In addition, the heater 9 is preferably in contact with the fuse 4. A flow of the direct current into the heater 9 activates the heater 9 to generate heat, which in turn heats the fuse 4. The fuse 4 then rises in temperature and experiences a transition from superconductivity into normal conduction. When the persistent current Ip through the first closed circuit C1 flows into the fuse 4 which has transitioned into normal conduction, the fuse 4 generates joule heat to heat itself and blow. This opens the first closed circuit C1 and allows the persistent current Ip to continue to flow, with the result that the persistent current Ip flows through the second closed circuit C2 into the bobbin (protective resistor) 5. The bobbin (protective resistor) 5 generates joule heat to heat itself and attenuate the persistent current Ip. When the persistent current Ip is still flowing through the first closed circuit C1, the persistent current switch 6 as well as the fuse 4 may transition into normal conduction. The fuse 4 is desirably designed so that even in this case, a temperature of the fuse 4 will readily increase above that of the persistent current switch 6 to heat the fuse to such an extent that it blows.
The superconducting magnet apparatus 1 further includes a cryostat 2. The cryostat 2 includes a refrigerator 2c that cools the superconducting coil 3 and the like by depriving these elements of heat, a heat transfer element 2d that conducts heat from the superconducting coil 3 and the like to the refrigerator 2c, a vacuum vessel 2a that accommodates the heat transfer element 2d and the like and conducts heat insulation under a vacuum, and a radiation shield 2b that accommodates the heat transfer element 2d and the like and suppresses entry of radiant heat. The radiation shield 2b is included in the vacuum vessel 2a, and the heat transfer element 2d is included in the radiation shield 2b. The refrigerator 2c includes a first stage and a second stage, each of which can be cooled down to a different temperature. The second stage, which is able to be cooled down to a temperature lower than that of the first stage, can be cooled down to a level below a critical temperature of a high-temperature superconductor. The second stage is thermally connected to the heat transfer element 2d, and the heat transfer element 2d is cooled below the critical temperature of a high-temperature superconductor. The first stage is thermally connected to the radiation shield 2b. The first stage cools the radiation shield 2b, whereby the radiant heat that the radiation shield 2b has absorbed can be released from the first stage.
The heat transfer element 2d, thermally connected to the superconducting coil 3 (3a, 3b), the fuse 4, the persistent current switch 6, and the superconducting wires that connect these elements, transfers (releases) heat to cool them below the critical temperature of a high-temperature superconductor. Thus the superconducting coil 3 (3a, 3b), the fuse 4, the persistent current switch 6, and the superconducting wires that connect these elements can be maintained in a superconducting condition.
The fuse 4, if it blows out, will be replaced with a new fuse 4. This replacement can be easily performed by disconnecting the connections (terminals) 14c, 14d from the blown fuse 4 and then removing the fuse 4, along with the heater 9 and the heat insulator 12, from the heat transfer element 2d. In order to allow for such a blowout, the fuse 4 is placed at a position that enables one to easily access a non-blown fuse, for example at an end of the heat transfer element 2d.
The fuse 4 is a so-called superconducting wire, and as shown in
Connection terminals 14a and 14b are provided at two places that are distant from each other on one of the paired flanges 5b. The connection terminals 14a and 14b are provided on outer circumferential sections of the paired flanges 5b. The connection terminals 14a and 14b are positioned across the central axis 5c of the bobbin (protective resistor) 5 (flange 5b). The connection terminals 14a and 14b are positioned at where a line segment (line) connecting the connection terminals 14a and 14b intersects with the central axis 5c of the bobbin (protective resistor) 5 (flange 5b). The superconducting wire 15a connecting to the persistent current switch 6 and forming a part of the first closed circuit C1 (see
Next, operation of the superconducting magnet apparatus 1 is described below. First, as shown in
Next after the persistent current switch 6 has been opened (turned off) for normal conduction, the circuit breaker 11 is closed (turned on) and the current is supplied from the excitation power supply 10 to the superconducting coils 3 (3a, 3b). After this, the persistent current switch 6 is closed (turned on) for superconductivity, the current from the excitation power supply 10 is turned off, and then the circuit breaker 11 is opened (turned off). At this time, although the supply of the current from the excitation power supply 10 to the superconducting coils 3 (3a, 3b) is stopped, current attenuation in the first closed circuit C1 having the superconducting coils 3 (3a, 3b), fuse 4, and closed (activated) persistent current switch 6 connected in series, becomes very small, which then resumes the flow of the persistent current Ip and places the superconducting magnet apparatus 1 in persistent-current operation. During persistent-current operation, the superconducting magnet apparatus 1 can form/hold the magnetic fields over extended periods of time, even without power being supplied from the excitation power supply 10. Since the bobbin (protective resistor) 5 has finite electrical resistance, substantially no current flows into the bobbin (protective resistor) 5 (second closed circuit C2) during persistent-current operation.
A description is given below of a case in which, during the persistent-current operation of the superconducting magnet apparatus 1, part of the superconducting coil 3a of the two superconducting coils 3 (3a, 3b) undergoes a transition into the normal conducting state and this normal conduction expands to the peripheral region of that part, that is, the quench event occurs. First, if a normal-conduction transition occurs in part of the superconducting coil 3a, the quench detector 7, upon determining that for example, the differential potential across the superconducting coil 3a has exceeded a predetermined value, detects the partial normal-conduction transition of the superconducting coil 3a and transmits the quench detection signal “Sq” to the direct-current power supply 8. After receiving the quench detection signal “Sq”, the direct-current power supply 8 supplies the direct current to a heater 13 in contact with the fuse 4. The heater 13 then heats the fuse 4, whereby the fuse 4 transitions from the superconducting state into the normal-conducting state and generates joule heat in itself to blow. The cryogenic stabilizer 4b (see
When the fuse 4 blows, this section exhibits a very high resistance value and the persistent current Ip is rerouted to the bobbin (protective resistor) 5 having a lower resistance value. A consequential flow of a larger persistent current Ip into the bobbin (protective resistor) 5 correspondingly increases the volume of stored magnetic energy consumed, and the generation of heat in the superconducting coils 3 (3a, 3b) is suppressed, that is, the superconducting coils 3 (3a, 3b) are lowered in maximum temperature. This avoids thermal damage to the superconducting coils 3 (3a, 3b). Additionally, since the fuse 4 is placed at a position readily accessible for replacement, the fuse can be replaced after the attenuation of the persistent current Ip, so the superconducting magnet apparatus 1 can be energized once again.
As described above, in accordance with the first embodiment, since the bobbin (protective resistor) 5 of the superconducting coils 3 also serves as a protective resistor, if the space for the bobbin 5 of the superconducting coils 3 is provided, a space independent of that space does not need to be provided for the protective resistor (5). This means that the installation space provided for the protective resistor (5) separately from the space for the bobbin 5 in conventional technology has been reduced. Briefly, in accordance with the embodiment is provided the superconducting magnet apparatus 1 adapted to consume stored magnetic energy without thermally damaging the protective resistor (5), even if the installation space for the protective resistor (5) is reduced.
Next, a superconducting magnet apparatus 1 according to a fourth embodiment is described below. The superconducting magnet apparatus 1 according to the fourth embodiment differs from those of the first to third embodiments in that a low-temperature superconductor that exhibits superconductivity at a critical temperature equal to or less than 18 K is used in each of superconducting coils 3, a fuse 4, superconducting filaments in a superconducting wire used in a persistent current switch 6, and superconducting filaments in a superconducting wire interconnecting each of those elements. In association with this difference, a cryostat 2 has appropriate or sufficient cooling capabilities to maintain superconductivity of the low-temperature superconductor. Niobium titanium (NbTi), niobium tin (Nb3Sn), or the like can be used as the low-temperature superconductor having the critical temperature of 18 K or less. The critical temperature of the low-temperature superconductor, compared with the high-temperature superconductors having critical temperatures exceeding 18 K, lies in a region that the low-temperature superconductor has a specific heat capacity at most one-tenth as great as those of niobium titanium (NbTi), niobium tin (Nb3Sn), and other low-temperature superconductors having critical temperatures below 18 K. For this reason, heat conduction due to a quench causes a delay in the propagation of a normal-conducting region. In the superconducting coils 3, therefore, stored magnetic energy can also be consumed without causing thermal damage, so that the stored magnetic energy to be consumed in a protective resistor (5) can be lessened. Hence the installation of a protective resistor for the low-temperature superconductors does not require a space as wide as that required for high-temperature superconducting coils. In the fourth embodiment, however, since a bobbin (protective resistor) 5 for the superconducting coils 3 also serves as a protective resistor, if an appropriate space for the bobbin 5 of the superconducting coils 3 is provided, a space independent of that space does not need to be provided for the protective resistor (5). The installation space for the protective resistor (5) can be made smaller than in the first embodiment, but even so, it follows that the installation space required has been reduced. In addition, even when the installation space for the protective resistor (5) is reduced, the stored magnetic energy can be consumed without thermally damaging the protective resistor (5).
As shown in
As described above, since the current-flow route 17 is limited to the inside of the flange 5b by the presence of the insulating sheet 5e and is staggered within the flange 5b by the presence of the grooves 5f, the resistance value of the bobbin (protective resistor) 5 is high relative to that obtained in the first embodiment. A time required for the current attenuation during the quench is correspondingly reduced. A time required for the quench detector 7 to detect the quench in the superconducting coil 3, and a time required until the fuse 4 has been blown out are extended according to the particular reduction in the quench detection time required. Consequently, the quench detector 7, the fuse 4, and other members and system elements required for the circuit composition are simplified, for example, the capacity of the heater 13 is reduced.
The bobbin (protective resistor) 5 is divided into the plurality of partial bobbins 21, namely 21a, 21b, 21c, 21d, 21e (in the example of
The cutting planes between the adjacent partial bobbins 21a, 21b, 21c, 21d, 21e are in close proximity to each other via one insulating sheet 5e. A fastening portion 70 is provided on each partial bobbin 21a, 21b, 21c, 21d, 21e. Any two of the fastening portions 70 on the adjacent partial bobbins 21a, 21b, 21c, 21d, 21e face each other via one insulating sheet 5e, and are securely tightened together by a bolt 60 and a nut 61. This structure with the paired fastening portions 70 tightened together by the bolt 60 and the nut 61 can be the structure described per
The adjacent partial bobbins 21a, 21b, 21c, 21d, 21e are electrically interconnected via the electroconductive connecting portions 16a, 16b, 16c, 16d. The electroconductive connecting portions 16a, 16c are opposed to the electroconductive connecting portions 16b, 16d across the central axis 5c. The current-flow route 17 therefore extends from the connection terminal 14b through the partial bobbin 21a, the electroconductive connecting portion 16a, the partial bobbin 21b, the electroconductive connecting portion 16b, the partial bobbin 21c, the electroconductive connecting portion 16c, the partial bobbin 21d, the electroconductive connecting portion 16d, and the partial bobbin 21e, in that order, to the connection terminal 14b. In this way, while staggering, the current-flow route 17 is narrowed down and elongated, whereby the resistance value of the bobbin (protective resistor) 5 can be increased. Since the number of partial bobbins 21a, 21b, 21c, 21d, 21e into which the bobbin is divided is odd (in the example of
The present invention is not limited to the above-described first to seventh embodiments and may include various modifications. For example, the first to seventh embodiments have been described in detail only for clarity of the present invention and are not limited to apparatus configurations including all described constituent elements. In addition, part of the configurations in the first to seventh embodiments may be replaced by any one or more of the other embodiments, and conversely, any one or more of the other embodiments may be added to part of the configurations in the first to seventh embodiments. Furthermore, addition, deletion, and/or replacement of any one or more of the other embodiments may take place for part of the configurations in the first to seventh embodiments.
Number | Date | Country | Kind |
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2012-127568 | Jun 2012 | JP | national |