Patent Application
20130234815
This application claims the benefit of Korean Patent Application No. 10-2012-0025224, filed on Mar. 12, 2012, in the Korean Intellectual Property Office, the disclosure of which is incorporated herein in its entirety by reference.
1. Field
Systems, apparatuses, and methods consistent with exemplary embodiments relate to a persistent switch control system, a superconducting magnet apparatus employing the persistent switch control system, and a method of controlling a persistent switch.
2. Description of the Related Art
A superconducting apparatus such as a magnetic resonance imaging (MRI) apparatus or a nuclear magnetic resonance (NMR) apparatus uses a superconducting magnet. The superconducting magnet operates when a current is applied to a superconducting coil cooled at an ultralow temperature, such as 4.2K, so that a superconducting phenomenon is generated. The superconducting magnet operates often in a persistent mode and includes a persistent switch to enter the persistent mode. The persistent mode is for allowing a current to flow through a closed loop in a superconducting magnet, and the persistent switch is used to block a current flow to a current lead between a superconducting magnet at a low temperature and a magnet power source at a normal temperature. Such persistent switch provides high field stability in application devices such as NMR apparatuses and MRI apparatuses, and can reduce a low temperature heat load for increasing a liquid helium retention time of a cryostat.
Generally, the persistent switch includes a superconducting wire and a switch heater. As heat is applied from the switch heater to the superconducting wire, the superconducting wire has resistivity since the temperature thereof rises above a superconducting transition temperature. When the persistent switch is designed appropriately, the persistent switch has a relatively high resistance. A high resistance of the persistent switch in an open state allows the superconducting magnet to be charged. The conducting wire is cooled and restores superconductivity when the charge is completed, and thus, the persistent switch is closed.
Applying heat to a persistent switch to open it causes a heat load on a cooling system of a superconducting magnet apparatus. For example, applying heat to a persistent switch to open it causes consumption of liquid helium. Furthermore, consumption of liquid helium is additionally increased due to heat dispersed from the persistent switch, which is caused by a ramp voltage that is applied to the persistent switch when the superconducting magnet is charged.
An aspect of an exemplary embodiment provides a persistent switch control system for reducing a heat load that is generated when a superconducting magnet is charged.
An aspect of an exemplary embodiment also provides a superconducting magnet apparatus employing the persistent switch control system.
Another aspect of an exemplary embodiment also provides a method of controlling a persistent switch.
According to an aspect of an exemplary embodiment, there is provided a persistent switch control system including: a persistent switch which switches between an open state and a closed state of a superconducting coil; and a persistent switch controller which controls the persistent switch, wherein, during a charging mode, a resistance state of the persistent switch is maintained by a ramp heat load that is generated by a ramp voltage applied to the persistent switch.
The persistent switch may include: a superconducting wire which constitutes a portion of a superconducting coil; and a switch heater which applies heat to the superconducting wire, wherein the persistent switch controller may supply a power supply voltage to the switch heater when the charging mode starts and may block the power supply voltage supplied to the switch heater when a current is supplied to the superconducting coil.
In the charging mode, a ramping rate of the current that is supplied to the superconducting coil may be set so that the ramp heat load, which is generated by the ramp voltage applied between ends of the superconducting wire, maintains a resistance state of the superconducting wire.
The supply of current to the superconducting coil may be stopped when the current that is supplied to the superconducting coil reaches a target current. The current that is supplied to the superconducting coil may be adjusted when it is substantially close to the target current. The persistent switch controller may turn on the switch heater before adjusting the current that is supplied to the superconducting coil, and may turn off the switch heater after adjusting the current that is supplied to the superconducting coil.
According to another aspect of an exemplary embodiment, there is provided a superconducting magnet apparatus including: a superconducting coil; a power source for a superconducting coil, which supplies a current to the superconducting coil; and a persistent switch control system, which controls an open state and a closed state of the superconducting coil. The persistent switch control system comprises: a persistent switch which switches between the open state and the closed state of the superconducting coil; and a persistent switch controller which controls the persistent switch, wherein, during a charging mode, a resistance state of the persistent switch is maintained by a ramp heat load that is generated by a ramp voltage applied to the persistent switch.
The superconducting magnet apparatus may be a magnetic resonance imaging (MRI) apparatus, a nuclear magnetic resonance (NMR) apparatus, or a superconducting magnet apparatus for a maglev car.
According to another aspect of an exemplary embodiment, there is provided a method of controlling a persistent switch for switching between an open state and a closed state of a superconducting coil, the method including maintaining a resistance state of the persistent switch by a ramp heat load that is generated by a ramp voltage that is applied to the persistent switch during a charging mode.
The persistent switch control system, the superconducting magnet apparatus employing the persistent switch control system, and the method of controlling a persistent switch may reduce a heat load, which is separately applied from the outside for operation of the persistent switch, by using the persistent switch's own ramp heat load in a charging mode.
The above and other aspects of exemplary embodiments will become more apparent with reference to the attached drawings in which:
Hereinafter, exemplary embodiments will be described in detail with reference to the attached drawings. The same reference numerals in the drawings denote the same element. In the drawings, the thicknesses of layers and regions are exaggerated for clarity.
Referring to
The persistent switch control system 120 includes a persistent switch 121 that is disposed at one side of the superconducting coil 110 and a persistent switch controller 125 that is disposed outside the cryostat 190 and controls the persistent switch 121.
The persistent switch 121 switches between an open state of the superconducting coil 110 and a closed state thereof. That is, the state of the persistent switch 121 may become a resistance state and thereby allow the superconducting coil 110 to be in the open state, and may become a superconducting state and thereby allow the superconducting coil 110 to be in the closed state. For this, the persistent switch 121 includes a superconducting wire 122 and a switch heater 123 that is disclosed adjacent to the superconducting wire 122 and may apply heat to the superconducting wire 122. It may be understood that the superconducting wire 122 is a portion of the superconducting coil 110 in a persistent mode. From the viewpoint of the power source 160 for a superconducting magnet, the superconducting wire 122 and the superconducting coil 110 are connected to each other in parallel. The superconducting wire 122 may be formed of a non-inductive coil to have a minimum inductance. The superconducting wire 122 is designed to have a ramp heat load that may maintain a temperature for maintaining the resistance state (that is, a state in which the superconducting state is broken). That is, the superconducting wire 122 is designed so that a resistance value thereof in the resistance state has a predetermined ramp heat load. The ramp heat load will be described below.
The persistent switch controller 125 may control the persistent switch 121 by controlling a power supply that is applied to the switch heater 123. In addition, the persistent switch 121 may be controlled by the ramp heat load also in the state where the switch heater 123 has been turned off, and the ramp heat load may be controlled by adjusting a ramping rate of a current that is supplied from the power source 160 for a superconducting magnet.
The superconducting coil 110 may be electrically connected to the power source 160 for a superconducting magnet, which is disposed outside the cryostat 190, through the current lead 150, and thus may receive a current from the power source 160 in a charging mode. In the superconducting magnet apparatus 100, a current supply to the superconducting coil 110 is blocked in the persistent mode, and in some cases, the current lead 150 may have a detachable and attachable structure.
The superconducting coil 110 is cooled in the superconducting state during operation of the superconducting magnet apparatus 100. The superconducting magnet apparatus 100 may have a charging mode in which a current is supplied to the superconducting coil 110 to charge it and a persistent mode in which a current flows in a closed circuit of the superconducting coil 110.
Prior to start of the charging mode, a target current and a ramping rate are set (operation S10). The target current is the amount of current that is used for determining whether charging has been completed. The ramping rate is a change of current via time, in which the current is gradually increased until the target current is reached. The ramping rate is set in consideration of a load that is generated by the inductance of the superconducting coil 110, and is set so that the superconducting wire 122 may maintain the resistance state by using a ramp heat load thereof in the charging mode.
Next, when the charging mode starts, the persistent switch controller 125 applies heat to the superconducting wire 122 to break the superconducting state thereof, by supplying a current to the switch heater 123, and changes the state of the superconducting wire 122 from the superconducting state to the resistance state (operation S20). For example, the amount Hr of heat per hour, which is generated in the switch heater 123, may be obtained according to equation 1 below.
Hr=Ih2·Rh (1)
Ir denotes a current supplied to the switch heater 123, and Rh denotes a resistance value of the switch heater 123. For example, if Rh is 100Ω and Ib is 30 mA, the amount Hr of heat per hour, which is generated in the switch heater 123, is 90 mW, and the generated heat may increase the temperature of the superconducting wire 122 to a temperature over 10K by heating the superconducting wire 122. Thus, the state of the superconducting wire 122 may be changed from the superconducting state to the resistance state. If the state of the superconducting wire 122 is changed from the superconducting state to the resistance state, it may be understood that the persistent switch 121 is substantially in an open state while the superconducting coil 110 is in the superconducting state.
If the state of the persistent switch 121 is changed to the open state, the power source 160 for a superconducting magnet supplies a current to the superconducting coil 110 through the current lead 150 (operation S30). Since the superconducting wire 122 is in the resistance state in the charging mode, most of the current flows to the superconducting coil 110 that substantially has no resistance, and thus, the superconducting coil 110 is charged. In this case, the power source 160 for a superconducting magnet slowly increases a current (that is, ramps up a current), which is supplied to the superconducting coil 110, in consideration of the inductance of the superconducting coil 110. If a voltage Vr is applied through the current lead 150 from the power source 160 for a superconducting magnet, the increase amount dI/dt of current that is supplied to the superconducting coil 110 may be obtained by the following equation 2.
L denotes the inductance of the superconducting coil 110. The increase amount dI/dt of current is referred to as a ramping rate, and the voltage Vr that is applied to the superconducting coil 110 is referred to as a ramp voltage.
Referring to equation 2, it may be understood that a current flowing through the superconducting coil 110 increases by the ramping rate Vr/L if the ramp voltage Vr is applied to the superconducting coil 110.
Since the superconducting wire 122 is connected in parallel to the superconducting coil 110, the ramp voltage Vr supplied from the power source 160 for a superconducting magnet is applied also between ends of the superconducting wire 122. Since the superconducting wire 122 is in the resistance state in the charging mode, the superconducting wire 122 generates Joule's heat due to the ramp voltage Vr. A heat load Hr of the superconducting wire 122 (hereinafter, referred to as a ramp heat load), which is generated due to the ramp voltage Vr, may be obtained according to equation 3 below.
Rs denotes the resistance of the superconducting wire 122 in the resistance state.
Referring to
When or immediately after the power source 160 for a superconducting magnet applies the ramp voltage Vr to the superconducting coil 110, the persistent switch controller 125 blocks a current, which is applied to the switch heater 123, to change the state of the switch heater 123 to a turn-off state (operation of S40). Since the resistance and the ramping rate (or the ramping voltage) of the superconducting wire 122 according to the current exemplary embodiment is designed to have a ramp heat load Hr so that the resistance state may be maintained in the charging mode, the superconducting wire 122 may maintain the resistance state due to heat, which is generated by the superconducting wire 122 itself, although the state of the switch heater 123 is changed to the turn-off state. Thus, since the persistent switch 121 is still in the open state, the superconducting coil 110 is charged by a current that is supplied from the power source 160 for a superconducting magnet.
Next, after a predetermined time has elapsed, the power source 160 for a superconducting magnet determines whether the charging of the superconducting coil 110 has been completed (operation S50). For example, it is possible to determine whether the charging has been completed by determining whether a current that is supplied from the power source 160 for a superconducting magnet has reached a target current. Until a current that is supplied from the power source 160 for a superconducting magnet is close to the target current, the turn-off state of the switch heater 123 and the charging state are maintained. In this case, a heat load that is generated in the switch heater 123 may be minimized since the switch heater 123 is in the turn-off state, and thus, a heat load that is applied to the cryostat 190 may be reduced.
If a current that is supplied from the power source 160 for a superconducting magnet reaches a target current, the power source 160 for a superconducting magnet stops the supply of current. A ramp heat load that is generated in the superconducting wire 122 is also reduced when the supply of current from the power source 160 is stopped, and thus, the superconducting wire 122 may be automatically cooled and then may return to the superconducting state. If the superconducting wire 122 returns to the superconducting state, the persistent switch 121 is closed and a current flowing through the superconducting coil 110 is turned toward the persistent switch 121 constituting a closed loop, and thus, the charging mode is ended.
Operation S60 of minutely adjusting a current may be further performed in the operation of stopping the supply of current from the power source 160 for a superconducting magnet.
Since, as stated above, the superconducting magnet apparatus 100 according to the current exemplary embodiment places the switch heater 123 in the turn-off state except in the charging process and the minute current adjustment process, the superconducting magnet apparatus 100 may minimize a heat load that is generated in the switch heater 123, may reduce a heat load that is applied to a cooler of the superconducting magnet apparatus 100, and may improve heat efficiency.
The superconducting magnet apparatus 100 according to the current exemplary embodiment may be a magnetic resonance imaging (MRI) apparatus, a nuclear magnetic resonance (NMR) apparatus, a superconducting magnet apparatus for a maglev car, or the like. For example, if the superconducting magnet apparatus 100 is an MRI apparatus, the superconducting magnet apparatus 100 may further include a gradient coil or a radio frequency (RF) coil.
While exemplary embodiments have been particularly shown and described, it will be understood by those of ordinary skill in the art that various changes in form and details may be made therein without departing from the spirit and scope of the present invention as defined by the following claims.
| Number | Date | Country | Kind |
|---|---|---|---|
| 10-2012-0025224 | Mar 2012 | KR | national |
