JP6155840B2 - Magnetic air conditioner - Google Patents

Description

  The present invention relates to a magnetic air conditioner, and more particularly, to a magnetic air conditioner that can maximize the magnetocaloric effect of a magnetic material.

  Most of refrigerators such as refrigerators, freezers, and air conditioners that are conventionally used at room temperature range use the phase change of a gaseous refrigerant such as chlorofluorocarbon gas or alternative chlorofluorocarbon gas. Recently, the problem of ozone depletion due to the emission of chlorofluorocarbons has been exposed, and there is also concern about the impact on global warming caused by the emission of alternative chlorofluorocarbons. For this reason, there is a strong demand for the development of an innovative refrigerator that is clean and has a high heat transport capability, replacing the refrigerator that uses a gaseous refrigerant such as CFC and CFC.

  Against this background, the refrigeration technology that has recently attracted attention is the magnetic refrigeration technology. Some magnetic materials exhibit a so-called magnetocaloric effect that changes their temperature according to the change of the magnitude of the magnetic field applied to the magnetic material. A refrigeration technique that transports heat using a magnetic material that exhibits this magnetocaloric effect is a magnetic refrigeration technique.

  As a refrigerator using the magnetic refrigeration technology, for example, there is a magnetic refrigerator that transports heat by utilizing the heat conduction of a solid substance as described in Patent Document 1 below.

International Publication No. 2012/150681 Pamphlet

  However, in the case of the invention described in Patent Document 1, as shown in FIG. 23, the magnet M1A facing the magnetic body MC1, the magnet M2A facing the magnetic body MC2, and the magnet M3A facing the magnetic body MC3 are: The magnetic bodies MC1, MC2, and MC3 are all arranged so that the N poles with the same polarity are opposed to each other. Similarly, the magnet M1B that faces the magnetic body MC1, the magnet M2B that faces the magnetic body MC2, and the magnet M3B that faces the magnetic body MC3 have the same S poles facing the magnetic bodies MC1, MC2, and MC3. Are arranged as follows. A magnetic body MC4 is disposed between the magnetic body MC1 and the magnetic body MC2, a magnetic body MC5 is disposed between the magnetic body MC2 and the magnetic body MC3, and a magnetic body MC6 is disposed adjacent to the magnetic body MC3. ing. Each of magnetic body MC4, magnetic body MC5, and magnetic body MC6 is not sandwiched by any of magnet M1A, magnet M2A, magnet M3A and magnet M1B, magnet M2B, and magnet M3B.

  Thus, when the magnets M1A, M2A, M3A, M1B, M2B, and M3B are arranged so that the magnets facing the magnetic bodies MC1, MC2, and MC3 have the same polarity between adjacent magnets, as shown in FIG. In addition, the direction of the magnetic field formed by the magnets M1A, M2A, M3A, M1B, M2B, and M3B is the same direction (see the white arrow in the figure).

  However, when the magnets M1A, M2A, M3A, M1B, M2B, and M3B are arranged as shown in FIG. However, since the leakage magnetic flux exists, the leakage magnetic flux indirectly acts on the magnetic bodies MC4, MC5, and MC6. Although indirect, a relatively strong magnetic field is applied to the magnetic bodies MC4, MC5, and MC6. Therefore, the magnetic flux applied to the magnetic bodies MC1, MC2, and MC3 to which a magnetic field needs to be applied. The difference between the density and the magnetic flux density of the magnetic flux applied to the magnetic bodies MC4, MC5, and MC6 for which the magnetic field is not desired is small. For this reason, it has been clarified by experiments that a sufficient magnetocaloric effect cannot be extracted in the magnetic material. Therefore, if a desired amount of heat is generated by the magnetocaloric effect, the amount of magnet used must be increased, which increases the volume of the magnetic air conditioner.

  The reason why the magnetocaloric effect cannot be sufficiently extracted is considered to be that the number of magnetic fluxes passing through the magnetic material to which a magnetic field is not applied is increased because the magnetic field lines from adjacent magnets interfere with each other. .

  The present invention has been made to alleviate the conventional problems as described above, and an object of the present invention is to provide a magnetic air conditioner that can maximize the magnetocaloric effect of a magnetic material.

  In order to achieve the above object, a magnetic air conditioner according to the present invention includes a heat transport unit, a magnetic unit, and a motor.

  The heat transport unit arranges a plurality of heat transporters arranged in parallel at intervals to alternately arrange a magnetic body having a magnetocaloric effect and a heat conducting section for transporting heat of the magnetic body. The magnetic unit is provided with a plurality of magnets that confront each magnetic body of the heat transport unit and selectively apply and remove magnetism to each magnetic body. The motor relatively moves at least one of the heat transport unit and the magnetic unit disposed to face each other in the heat transporter arrangement direction. Between the heat transporter and the heat transporter of the heat transport unit, a magnetically permeable heat insulating portion having a magnetic permeability equivalent to that of the magnetic material and blocking heat conduction is formed. The magnetization directions of the magnets arranged in the magnetic unit are opposite to each other between adjacent magnets.

  According to the magnetic air conditioner according to the present invention, the magnetization directions of the magnets arranged in the magnetic unit are opposite to each other between the adjacent magnets, so that the magnetocaloric effect of the magnetic material can be maximized. Moreover, since the fluctuation | variation of the driving force of a heat transport unit or a magnetic unit can be made small, the motor for driving a magnetic air conditioning apparatus can be reduced in size, and the power consumption of a motor can be made small. Therefore, coupled with the increase in the magnetocaloric effect of the magnetic material, the energy efficiency of the magnetic air conditioner can be increased, and the noise and vibration of the magnetic air conditioner can be reduced.

It is a figure where it uses for description of the operating principle of the magnetic air conditioning apparatus which concerns on this invention, and is a figure which shows the structure of the heat transport unit which has arrange | positioned several heat transporters. It is a figure which uses for description of the operating principle of the magnetic air conditioning apparatus which concerns on this invention, and is a figure which shows the structure of the upper magnetic unit which has arrange | positioned the several magnetic application removal part. It is a figure which uses for description of the operating principle of the magnetic air conditioning apparatus which concerns on this invention, and is a figure which shows the structure of the lower magnetic unit which has arrange | positioned the several magnetic application removal part. It is a figure where it uses for operation | movement description of the magnetic air conditioning apparatus which concerns on this invention. It is a figure where it uses for operation | movement description of the magnetic air conditioning apparatus which concerns on this invention. It is a figure where it uses for description of a mode that heat moves in the magnetic air conditioning apparatus which concerns on this invention. It is a graph which shows the effect of the magnetic air conditioning apparatus which concerns on this invention. It is a block diagram of the heat transport unit of the magnetic air conditioning apparatus which concerns on Embodiment 1. FIG. FIG. 9 is a configuration diagram of an upper magnetic unit that sandwiches the heat transport unit of FIG. 8. It is a block diagram of the lower magnetic unit which pinches | interposes the heat transport unit of FIG. It is sectional drawing of the magnetic air conditioning apparatus which concerns on Embodiment 1. FIG. It is sectional drawing of the heat transport unit and both magnetic units of the magnetic air conditioning apparatus of FIG. It is a figure which shows arrangement | positioning of the magnet of the magnetic unit which concerns on Embodiment 1. FIG. It is a figure which shows the modification of arrangement | positioning of the magnet of the magnetic unit which concerns on Embodiment 1. FIG. It is a figure where it uses for description of the effect produced by the difference in arrangement | positioning of a magnet. It is the figure which visualized the magnetic force line of the magnetic unit which concerns on Embodiment 1. FIG. It is a figure where it uses for description of the effect of the magnetic permeability heat insulation part provided in the heat transport unit. It is a block diagram of the control system of the magnetic air conditioning apparatus which concerns on Embodiment 1. FIG. It is a block diagram of the more concrete control system of the air-conditioning control part of FIG. 18, and an air-conditioning information input part. It is an operation | movement flowchart of the magnetic air conditioning apparatus of FIG. It is a block diagram of the heat transport unit of the magnetic air conditioning apparatus which concerns on Embodiment 2. FIG. It is a figure where it uses for description of the effect at the time of arrange | positioning each heat transport unit with a phase difference in the lamination direction. It is a figure which shows arrangement | positioning of the magnet in the conventional magnetic unit. It is the figure which visualized the magnetic force line in the conventional magnetic unit.

Before explaining each embodiment, the principle of operation of the magnetic air conditioner according to the present invention will be explained.
(Operation principle of magnetic air conditioner)
<Configuration of heat transport unit>
FIG. 1 is a diagram showing a configuration of a heat transport unit in which a plurality of heat transporters are arranged. The circular heat transport unit has four heat transporters 1-4 divided by separation parts 130A-130D. Each heat transporter conducts heat from the low temperature side heat exchange section 400A to the high temperature side heat exchange section 400B. Each heat transporter is formed by alternately arranging magnetic bodies and heat conducting portions. As the magnetic material, a positive magnetic material is used as a magnetic material of the same material having the same type of magnetocaloric effect. For the heat conduction part, a material having a characteristic that the heat conductivity changes greatly by applying and removing voltage is used. When the voltage is applied (ON), the thermal conductivity increases in the thermal conductivity, and when the voltage is removed (OFF), the thermal conductivity decreases. For this reason, the heat conduction part can prevent the magnetic body from conducting heat by controlling the application and removal of the voltage, and can efficiently transfer the heat toward the direction in which the magnetic bodies are arranged. Can do.

  For example, in the heat transporter 1, the magnetic bodies 100A-100E and the heat conducting units 300A-300G are alternately arranged. Specifically, from the low temperature side heat exchanging section 400A to the heat conducting section 300A-the magnetic body 100A-the heat conducting section 300B-the magnetic body 100B-the heat conducting section 300C-the magnetic body 100C-the heat conducting section 300D-the magnetic body 100D-the heat conducting. 300E-magnetic body 100E-heat conduction part 300F-magnetic body 100F-heat conduction part 300G are arranged in this order to reach the high temperature side heat exchange part 400B. The low temperature side heat exchange part 400A and the heat conduction part 300A, each heat conduction part and the magnetic body from the heat conduction part 300A to the heat conduction part 300G, and the heat conduction part 300G and the high temperature side heat exchange part 400B are connected without gaps. is there. The configuration of the heat transporter 2-4 is the same as that of the heat transporter 1.

<Configuration of magnetic unit>
The magnetic unit shown in FIGS. 2 and 3 sandwiches the heat transport unit shown in FIG. 1 with a certain gap from both sides in the vertical direction. The configuration of the magnetic unit is as follows.

  FIG. 2 is a diagram illustrating a configuration of an upper magnetic unit in which a plurality of magnetic application removing units are arranged. The circular upper magnetic unit has four magnetic application removal units 1U-4U divided by separation units 200AU-200DU. The upper magnetic unit shown in FIG. 2 is positioned clockwise so that the front side of the figure faces the front side of the heat transport unit shown in FIG. 1, and the center of the upper magnetic unit coincides with the center of the heat transport unit. Support for rotation. FIG. 2 shows a state where the upper magnetic unit positioned facing the heat transport unit is seen through from the top toward the heat transport unit.

  At time T1 when the magnetic application removal unit 1U faces the heat transporter 1, the magnetic application removal unit 1U is applied to the permanent magnet 210A and the magnetic body 100C facing the magnetic body 100A from the outer periphery to the inner periphery of the magnetic unit. The permanent magnet 210 </ b> C and the permanent magnet 210 </ b> E facing the magnetic body 100 </ b> E are opposed to each other.

  At time T2 when the magnetic application removal unit 2U faces the heat transporter 1, the magnetic application removal unit 2U moves from the outer circumference to the inner circumference of the magnetic unit toward the permanent magnet 220B and the magnetic body 100D facing the magnetic body 100B. It has permanent magnet 220F which opposes permanent magnet 220D which opposes, and the magnetic body 100F.

  Since the magnetic application removal unit 3U and the magnetic application removal unit 4U are point-symmetric with respect to the center of the upper magnetic unit, the arrangement of the permanent magnets is the same as the magnetic application removal unit 1U and the magnetic application removal unit 2U. The magnetic application removal unit 3U faces the heat transporter 1 at time T3, and the magnetic application removal unit 4U faces the heat transporter 1 at time T4.

  FIG. 3 is a diagram illustrating a configuration of a lower magnetic unit in which a plurality of magnetic application removing units are arranged. The lower circular magnetic unit has four magnetic application removal units 1D-4D divided by separation units 200AD-200DD. The lower magnetic unit shown in FIG. 3 is positioned so that the front side of the figure faces the back side of the heat transport unit shown in FIG. 1, and the center of the lower magnetic unit coincides with the center of the heat transport unit. Supports rotation around. FIG. 3 shows a state in which the lower magnetic unit positioned facing the heat transport unit is viewed from the heat transport unit side.

  At time T1 when the magnetic application removal unit 1D faces the heat transporter 1, the magnetic application removal unit 1D applies the permanent magnet 260A and the magnetic body 100C facing the magnetic body 100A from the outer periphery to the inner periphery of the magnetic unit. The permanent magnet 260 </ b> C and the permanent magnet 260 </ b> E facing the magnetic body 100 </ b> E are opposed to each other.

  At time T2 when the magnetic application removal unit 2D is opposed to the heat transporter 1, the magnetic application removal unit 2D is disposed on the permanent magnet 270B and the magnetic body 100D facing the magnetic body 100B from the outer periphery toward the inner periphery. It has permanent magnet 270F which opposes permanent magnet 270D and magnetic body 100F which oppose.

  Since the magnetic application removal unit 3D and the magnetic application removal unit 4D are point-symmetric with respect to the center of the lower magnetic unit, the arrangement of the permanent magnets is the same as the magnetic application removal unit 1D and the magnetic application removal unit 2D. The magnetic application removal unit 3D faces the heat transporter 1 at time T3, and the magnetic application removal unit 4D faces the heat transporter 1 at time T4.

  The magnetic application removal units 1U-4U of the upper magnetic unit and the magnetic application removal units 1D-4D of the lower magnetic unit face each other in the vertical direction via the heat transporters 1-4 of the heat transport unit. The upper magnetic unit and the lower magnetic unit are synchronized without changing their relative positions so that the upper magnetic unit separation unit 200AU-200DU and the lower magnetic unit separation unit 200AD-200DD always face each other. Then rotate.

<Principle of heat transport>
4 and 5 are diagrams for explaining the operation of the magnetic air conditioner according to the present invention. FIG. 4 shows two states, time T1 and time T2. The state at time T1 is a state in which the AA line of the heat transport unit in FIG. 1 coincides with the AA lines of the upper and lower magnetic units in FIGS. In other words, the heat transporter 1 of the heat transport unit faces the magnetic application removal unit 1U of the upper magnetic unit and the magnetic application removal unit 1D of the lower magnetic unit. The state at time T2 is a state in which the heat transporter 1 of the heat transport unit faces the magnetic application removal unit 2U of the upper magnetic unit and the magnetic application removal unit 2D of the lower magnetic unit. FIG. 5 shows two states at time T3 and time T4. The state at time T3 is a state in which the heat transporter 1 of the heat transport unit faces the magnetic application removal unit 3U of the upper magnetic unit and the magnetic application removal unit 3D of the lower magnetic unit. The state at time T4 is a state in which the heat transporter 1 of the heat transport unit faces the magnetic application removal unit 4U of the upper magnetic unit and the magnetic application removal unit 4D of the lower magnetic unit.

  At time T1, as shown in FIG. 4, the permanent magnets 210A and 260A are positioned on the magnetic body 100A. Further, permanent magnets 210C and 260C are located on the magnetic body 100C. Further, permanent magnets 210E and 260E are located on the magnetic body 100E. At time T1, a voltage is applied to the heat conducting units 300B, 300D, and 300F so that heat can be conducted between the adjacent magnetic bodies 100A-100B, 100C-100D, and 100E-100F.

  At time T2, since the upper and lower magnetic units rotate 90 degrees clockwise from time T1, permanent magnets 220B and 270B are positioned on the magnetic body 100B as shown in FIG. Further, the permanent magnets 220D and 270D are located on the magnetic body 100D. In addition, permanent magnets 220F and 270F are positioned on the magnetic body 100F. At time T2, a voltage is applied to the heat conducting units 300A, 300C, 300E, and 300G, and the low temperature side heat conducting unit 400A and the magnetic body 100A, the magnetic bodies 100B-100C, 100D-100E, the magnetic body 100F, and the high temperature side heat conduction. Heat conduction can be performed between the portions 400B.

  At time T3, the upper and lower magnetic units rotate 90 degrees clockwise from time T2, so that permanent magnets 230A and 280A are located on magnetic body 100A as shown in FIG. Further, permanent magnets 230C and 280C are located on the magnetic body 100C. Further, permanent magnets 230E and 280E are located on the magnetic body 100E. At time T3, similarly to time T1, a voltage is applied to the heat conducting units 300B, 300D, and 300F so that heat conduction can be performed between the adjacent magnetic bodies 100A-100B, 100C-100D, and 100E-100F.

  At time T4, the upper and lower magnetic units rotate 90 degrees clockwise from time T3, so that permanent magnets 240B and 290B are positioned on magnetic body 100B as shown in FIG. In addition, permanent magnets 240D and 290D are positioned on the magnetic body 100D. In addition, permanent magnets 240F and 290F are positioned on the magnetic body 100F. At time T4, similarly to time T2, a voltage is applied to the heat conducting units 300A, 300C, 300E, and 300G, and the low temperature side heat conducting unit 400A, the magnetic body 100A, the magnetic bodies 100B-100C, 100D-100E, and the magnetic body 100F. And high temperature side heat conduction part 400B.

  As described above, when the positional relationship of the permanent magnet is followed, the same positional relationship among the permanent magnet, the magnetic body, and the heat conducting unit at the times T1 and T2 is repeated twice during the transition from the time T1 to the time T4.

  As described above, since a positive magnetic material is used for each magnetic material, heat is generated when magnetism is applied, and heat is absorbed when magnetism is removed. In addition, since a material whose thermal conductivity is changed by applying and removing magnetism is used for the heat conducting portion, the thermal conductivity becomes relatively large when magnetism is applied, and the thermal conductivity when removing magnetism. Becomes relatively small.

  Therefore, as the time shifts from time T1 to T4, heat moves from the low temperature side heat exchange unit 400A toward the high temperature side heat exchange unit 400B, and between the low temperature side heat exchange unit 400A and the high temperature side heat exchange unit 400B. There is a temperature difference. The principle of creating a temperature difference is as follows.

  FIG. 6 is a diagram for explaining how heat moves in the magnetic air conditioner according to the present invention. The manner in which heat moves will be described with reference to FIGS.

  First, as a premise, a case is assumed in which all magnetic bodies are formed of the same material, and all the magnetic bodies have the same type of magnetocaloric effect and have a temperature change of 5 ° C. Specifically, it is assumed that all the magnetic materials have a characteristic that the temperature increases by 5 ° C. when magnetism is applied and the temperature decreases by 5 ° C. when the magnetism is removed. Further, it is assumed that all the heat conducting members have the same characteristic that the thermal conductivity increases and decreases in the same manner by applying and removing voltage.

  First, in the initial state of time T1, all the magnetic bodies 100A-100F and the heat conducting units 300A-300G are at room temperature of 20 ° C. Between the low temperature side heat exchange part 400A and the high temperature side heat exchange part 400B, the magnetic bodies and the heat conduction parts arranged alternately form a heat transporter.

  Next, when the state transitions to the state at time T2, the positional relationship between the permanent magnet, the magnetic body, and the heat conducting portion changes from the state shown at time T1 in FIG. 4 to the state shown at time T2. At time T2, a voltage is applied to the heat conducting units 300A, 300C, 300E, and 300G. As a result, as shown in FIG. 6, the temperature of the magnetic body 100A drops by 5 ° C., heat conduction by the heat conducting unit 300A becomes possible, and heat moves from the low temperature side heat exchange unit 400A to the magnetic body 100A. Further, the temperature of the magnetic bodies 100B and 100D increases by 5 ° C., the temperature of the magnetic bodies 100C and 100E decreases by 5 ° C., and heat conduction by the heat conducting portions 300C and 300E becomes possible. In addition, heat is transferred from the magnetic body 100D to the magnetic body 100E. Further, the temperature of the magnetic body 100F increases by 5 ° C., heat conduction by the heat conducting unit 300G becomes possible, and heat moves from the magnetic body 100F to the high temperature side heat exchanging unit 400B.

  In the state at time T2, the temperatures of the magnetic bodies 100A, 100C, and 100E from which magnetism has been removed drop to 15 ° C., and the temperatures of the magnetic bodies 100B, 100D, and 100F to which magnetism has been applied rise to 25 ° C. For this reason, as shown in FIG. 6, heat moves from the higher temperature side to the lower temperature side through the heat conducting portions 300A, 300C, 300E, and 300G.

  Due to this heat transfer, the temperature of the magnetic body 100A and the low temperature side heat exchange section 400A becomes 17.5 ° C. as shown in the state of T2 ′ in FIG. 6, and the temperature of the magnetic body 100F and the high temperature side heat exchange section 400B. Becomes 22.5 ° C.

  Next, when the state transitions from the state at time T2 ′ to the state at T3, the positional relationship between the permanent magnet, the magnetic body, and the heat conducting portion changes from the state at time T2 in FIGS. 4 and 5 to the state at time T3. Become. At time T3, a voltage is applied to the heat conducting units 300B, 300D, and 300F. As a result, the temperature of the magnetic bodies 100A, 100C, and 100E increases by 5 ° C., the temperature of the magnetic bodies 100B, 100D, and 100F decreases by 5 ° C., and heat conduction by the heat conducting units 300B, 300D, and 300F becomes possible. Heat is transferred from the magnetic body 100A to the magnetic body 100B, from the magnetic body 100C to the magnetic body 100D, and from the magnetic body 100E to the magnetic body 100F.

  In the state at time T3, the temperature of the magnetic bodies 100A, 100C, 100E to which magnetism is applied rises to 22.5 ° C. or 25 ° C., and the temperature of the magnetic bodies 100B, 100D, 100F from which magnetism has been removed is 15 ° C. The temperature falls to 17.5 ° C. For this reason, as shown in FIG. 6, heat moves from the higher temperature side to the lower temperature side through the heat conducting portions 300B, 300D, and 300F.

  Due to this heat transfer, the temperature of the low temperature side heat exchanging section 400A becomes 17.5 ° C., and the temperature of the magnetic bodies 100A and 100B becomes 18.75 ° C., as indicated by T3 ′ in FIG. The temperature of the magnetic bodies 100C and 100D is 20 ° C., and the temperature of the magnetic bodies 100E and 100F is 21.25 ° C. The temperature of the high temperature side heat exchange section 40B remains at 22.5 ° C.

  Next, when the state transitions from the state at time T3 ′ to the state at T4, the positional relationship among the permanent magnet, the magnetic body, and the heat conducting portion becomes the same as the state shown at time T2 in FIG. At time T4, a voltage is applied to the heat conducting units 300A, 300C, 300E, and 300G, as with time T2. As a result, a state as shown in T2. T4 of FIG. 6 is obtained, and heat is transferred from the low temperature side heat exchanging section 400A to the magnetic body 100A, from the magnetic body 100B to the magnetic body 100C, and from the magnetic body 100D to the magnetic body 100E. The heat moves to the high temperature side heat exchange section 400B from the magnetic body 100F.

  As described above, every time the upper magnetic unit and the lower magnetic unit make one rotation in synchronization, the state from time T1 to time T4 is repeated, and the low temperature side heat exchange unit 400A to the high temperature side heat exchange unit Heat moves to 400B. As time elapses, as shown in FIG. 7, the temperature difference between the low temperature side heat exchange section 400A and the high temperature side heat exchange section 400B increases. Eventually, the temperature difference between the low temperature side heat exchange section 400A and the high temperature side heat exchange section 400B is stabilized. In this state, for example, the indoor temperature can be lowered using the heat of the low temperature side heat exchange unit 400A, and the indoor temperature can be increased, for example, using the heat of the high temperature side heat exchange unit 400B.

  The description of FIG. 1 to FIG. 7 is applicable when a positive magnetic material is used as a magnetic material of the same material having the same type of magnetocaloric effect. When a negative magnetic material is used as a magnetic material of the same material having the same type of magnetocaloric effect, the direction of heat transfer is opposite to the direction shown in FIGS. Therefore, when a negative magnetic material is used, the positions of the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B are opposite to those in FIGS.

  Next, an embodiment of the magnetic air-conditioning apparatus according to the present invention will be described by dividing it into [Embodiment 1] and [Embodiment 2]. The magnetic cooling / heating apparatus according to [Embodiment 1] forms a magnetically permeable heat insulating portion that reduces the driving force of the magnetic unit between the heat transporter and the heat transporter of the heat transport unit. In the magnetic air conditioner according to [Embodiment 2], a plurality of heat transport units are arranged with a slight shift in the rotational direction, respectively, in order to reduce the driving force of the magnetic units.

[Embodiment 1]
Next, the configuration of the magnetic air conditioner according to the first embodiment will be described with reference to FIGS. The principle of operation of the magnetic air conditioner according to Embodiment 1 described below is the same as the principle of heat transport described above. FIG. 8 is a configuration diagram of a heat transport unit of the magnetic air conditioner according to the first embodiment. FIG. 9 is a configuration diagram of the upper magnetic unit sandwiching the heat transport unit of FIG. FIG. 10 is a configuration diagram of the lower magnetic unit sandwiching the heat transport unit of FIG. FIG. 11 is a cross-sectional view of the magnetic air conditioner according to the first embodiment. FIG. 12 is a cross-sectional view of the heat transport unit and both magnetic units of the magnetic air conditioner of FIG.

(Configuration of magnetic air conditioner)
<Configuration of heat transport unit>
As shown in FIG. 8, the heat transport unit 1000A of the magnetic air conditioner is formed in a hollow circular shape. A cylindrical high temperature side heat exchange unit 40B is disposed in the hollow portion of the heat transport unit 1000A, and the low temperature side heat exchange unit 40A is provided so as to surround the high temperature side heat exchange unit 40B. The heat transporter arrangement plate 150 (see FIG. 12) having a thickness of about 1 mm is fitted into the space between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B, and the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit are inserted. Fix with 40B. A rotor 310 is rotatably mounted via a bearing 45 in the high temperature side heat exchange section 40B.

  As shown in FIGS. 8 and 12, heat conduction for transporting the heat of the magnetic bodies 10A to 10F having the magnetocaloric effect in a fan-shaped space having a central angle of 30 degrees on the heat transporter arrangement plate 150. The parts 30A-30G are alternately arranged. One heat transporter 50-1 is constituted by the magnetic bodies 10A-10F and the heat conducting portions 30A-30G arranged alternately. As shown in FIG. 8, in a fan-shaped space having a central angle of 30 degrees adjacent to the heat transporter 50-1, a magnetic body 11A-11F having a magnetocaloric effect and a heat conducting part 31A for transporting the heat of these magnetic bodies -31G are alternately arranged. One heat transporter 50-2 is constituted by the magnetic bodies 11A-11F and the heat conducting portions 31A-31G arranged alternately. The heat transporters 50-1, 50-2,... A heat transport unit 1000 is formed by arranging the heat transporters 50-1, 50-2,...

  As shown in FIGS. 8 and 12, a total of twelve heat transporters 50-1, 50-2,... Are arranged in parallel on the heat transporter arrangement plate 150 every 30 degrees of the central angle. In addition, each of the twelve heat transporters 50-1, 50-2,... Between the adjacent heat transporter 50-1 and heat transporter 50-2, the penetration of the magnetic bodies 10A-10F and 11A-11F of the heat transporters 50-1, the heat transporter 50-2. A magnetically permeable heat insulating portion 60 having a magnetic permeability equivalent to the magnetic permeability and capable of blocking heat conduction between the adjacent heat transporter 50-1 and heat transporter 50-2 is formed. When heat conduction between the heat transporter 50-1 and the heat transporter 50-2 is blocked by the magnetically permeable heat insulating portion 60, the amount of heat released that does not contribute to air conditioning is reduced, and the thermal efficiency of the magnetic air conditioner is improved.

  The magnetically permeable heat insulating portion 60 is formed so as to fill the space between the magnetic bodies 10A-10F and 11A-11F of the adjacent heat transporters 50-1 and 50-2. The magnetically permeable heat insulating portion 60 enters between the magnetic bodies 10A-10F and 11A-11F of the adjacent heat transporters 50-1 and 50-2, and the magnetic bodies 10A-10F and 11A-. There is no gap between 11F, and the peak of the driving force of the magnetic unit is leveled. The reason for leveling will be described in detail later. The magnetic permeable heat insulating portion 60 is formed by mixing a metal powder having a high magnetic permeability such as iron in a material having a heat insulating property such as a heat insulating resin so that the heat insulating property is not hindered. When the magnetic permeable heat insulating part 60 is formed by blending a plurality of materials, the thermal conductivity and the magnetic permeability can be brought close to target values, and the magnetic permeable heat insulating part 60 can be easily created.

  The heat transporter arrangement plate 150 is formed of a material having high heat insulation so as not to take away the heat transported by the heat transporter 50-1, the heat transporter 50-2,. Moreover, since the heat transporter arrangement | positioning board 150 must not reduce the magnetic flux applied to a magnetic body, it is preferable to form with the material which makes a magnetic flux pass easily. The heat transporters 50-1, 50-2,... Are provided on the upper side of the heat transporter arrangement plate 150, but may be provided on the lower side of the heat transporter arrangement plate 150. Further, the heat transporters 50-1, 50-2,... May be provided so as to be sandwiched between the upper and lower heat transporter arrangement plates 150.

  Refrigerant passages 41 and 42 (see FIGS. 8 and 11) for circulating a refrigerant for heat exchange are formed in the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B. The refrigerant flowing through the refrigerant passages 41 and 42 may be liquid or gas. In this embodiment, air is used as the refrigerant. Cooled air is sucked into the refrigerant passage 41 of the low temperature side heat exchanging section 40A in the direction indicated by the arrow, and the cooled air is discharged in the direction indicated by the arrow. The taken-in air is warmed into the refrigerant passage 42 of the high temperature side heat exchanging section 40B and discharged from the back side in FIG. 8 in the front direction (the arrow direction in FIG. 11).

<Magnetic material>
In this embodiment, the magnetic bodies 10A-10F, the magnetic bodies 11A-11F,... Are made of the same material, and positive magnetic bodies are used as the same material. A positive magnetic substance is in a paramagnetic state (magnetic spin is in a disordered state) when no magnetism is applied, and in a paramagnetic state (magnetic spin is aligned in one direction) when magnetism is applied. Manufactured using a material that reversibly produces a ferromagnetic state.

  The positive magnetic material is an alloy based on Gd or Gd, such as Gd-Y, Gd-Dy, Gd-Er, Gd-Ho, La (Fe, Si) 13, or La (Fe). , Al) 13 or other magnetic material can be used.

  On the other hand, although not used in the present embodiment, a negative magnetic material can be used as the same material for the magnetic bodies 10A-10F, the magnetic bodies 11A-11F,. As the negative magnetic material, a magnetic material such as an FeRh alloy, CoMnSiGe system, or NiMnSn system can be used.

  Generally, positive and negative magnetic materials generate heat or absorb heat opposite to the application of magnetism, so the magnetocaloric effect of positive and negative magnetic materials The magnitude of the temperature change is different. Therefore, when one of the positive and negative magnetic bodies is used as in this embodiment, the magnitude of the temperature change due to the magnetocaloric effect of all the magnetic bodies is the same. Therefore, stable heat transfer characteristics can be obtained as a whole of the magnetic air conditioner and the heat transport efficiency can be improved. Further, since the magnetocaloric effect of the negative magnetic material is smaller than the magnetocaloric effect of the positive magnetic material, it is preferable to use the positive magnetic material in consideration of heat transport efficiency. In addition, since a negative magnetic material is rarer than a positive magnetic material, it is preferable to use a positive magnetic material in terms of cost.

  Further, a positive or negative magnetic material is used for the magnetic materials 10A-10F, 11A-11F,..., And the operating temperatures of these magnetic materials 10A-10F, 11A-11F,. can do. However, the present invention is not limited to this, and magnetic materials having different operating temperatures can be arranged. For example, a magnetic body having a low operating temperature can be arranged stepwise from the magnetic body 10F adjacent to the high temperature side heat exchange unit 40B toward the magnetic body 10A adjacent to the low temperature side heat exchange unit 40A. Here, the difference between a magnetic material having a high operating temperature and a magnetic material having a low operating temperature is that the temperature range in which the magnetocaloric effect is exhibited is a high temperature or a low temperature.

  As described above, when the optimum operating temperature is selected in accordance with the position of the magnetic body in the heat transporter 50-1, the heat transporter 50-2,..., The heat transporter using the magnetic body having a uniform operating temperature. 50-1, the heat transporter 50-2,..., A larger temperature difference can be obtained between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B, and the heat transport capacity and heat transport efficiency can be obtained. Can be improved.

<Heat conduction part>
As illustrated in FIGS. 8 and 12, in the magnetic air conditioner according to the present embodiment, in the heat transporter 50-1, the heat conducting unit 30A is connected between the low temperature side heat exchanging unit 40B and the magnetic body 10A. . The heat conducting portions 30B-30F are connected between the magnetic bodies 10A-10F. The heat conducting unit 30G is connected between the magnetic body 10F and the high temperature side heat exchanging unit 40B. In the heat transporter 50-2, the heat conducting unit 31A is connected between the low temperature side heat exchanging unit 40B and the magnetic body 11A. The heat conducting portions 31B-31F are connected between the magnetic bodies of the magnetic bodies 11A-11F. The heat conducting unit 31G is connected between the magnetic body 11F and the high temperature side heat exchanging unit 40B. The configuration of other heat transporters is the same as that of the heat transporter 50-1 and the heat transporter 50-2.

  The heat conducting units 30A-30G, 31A-31G,... According to the present embodiment are configured by a metal / insulating phase transition body. The heat conducting portions 30A-30G, the heat conducting portions 31A-31G,... And the magnetic bodies 10A-10F, 11A-11F,. Therefore, the heat transporter 50-1, the heat transporter 50-2,... Are integrated.

  The metal / insulating phase transition body has the property that when a voltage is applied, the phase transition from the insulator to the metal increases the thermal conductivity. On the other hand, when the voltage is cut off, the phase transition from metal to insulator causes the thermal conductivity to decrease. Insulators that exhibit a phase transition between a metal and an insulator include inorganic oxide mott insulators or organic mott insulators. The inorganic oxide Mott insulator includes at least a transition metal element. As the Mott insulator, LaTiO3, SrRuO4, and BEDT-TTF (TCNQ) are known. Currently known devices capable of phase transition between metal and insulator include a ZnO single crystal thin film electric double layer FET and a TMTSF / TCNQ stacked FET element. Heat can be transferred by thermionic and lattice crystals. The ZnO single crystal thin film electric double layer FET and the TMTSF / TCNQ multilayer FET element utilize the property that the thermoelectrons move actively when a voltage is applied. In the present embodiment, the metal / insulating phase transition body includes an inorganic oxide Mott insulator, an organic Mott insulator, a ZnO single crystal thin film electric double layer FET, a TMTSF / TCNQ multilayer FET element, etc., which contain at least a transition metal element. A material whose thermal conductivity is greatly changed by application and removal of is used.

  When a DC voltage V is applied to both opposing surfaces of the metal / insulating phase transition body, the thermal conductivity of the metal / insulating phase transition body becomes relatively large, and heat transfer occurs between the magnetic bodies. On the other hand, when the DC voltage V is removed, the thermal conductivity of the metal / insulating phase transition body becomes relatively small, and heat transfer between the magnetic bodies is prevented. Therefore, the heat conducting portions 30A-30G, the heat conducting portions 31A-31G,... Become thermal switches that control the movement of heat by applying and removing voltage.

  Since the conduction of heat conduction of the heat conduction parts 30A-30G, 31A-31G,... Can be controlled by applying and removing voltage, heat can be transported without sliding the heat conduction part between the magnetic bodies. Can do. For this reason, it is not necessary to give the heat conducting portion sliding durability, and the reliability of the heat conducting portion is improved. Moreover, the mechanical loss by friction can be eliminated and the loss for driving a heat conductive part can be reduced. In addition, the heat conduction part can transport heat only in the direction of alignment with the magnetic material, and the heat conductivity of the heat conduction part can be increased compared to the sliding type, so thermal loss is reduced during heat transfer. it can. In addition, since the heat conducting unit can connect between the magnetic bodies using all the contact surfaces in accordance with the application and removal of voltage, the heat transport capability and the heat transport efficiency can be improved.

  A voltage can be easily applied to the metal / insulating phase transition body by providing an electrode in each of the heat conducting portions 30A-30G, 31A-31G,. Further, when an inorganic oxide Mott insulator, an organic Mott insulator, a ZnO single crystal thin film electric double layer FET, or a TMTSF / TCNQ stacked FET element containing at least a transition metal element is used as a metal / insulating phase transition body, heat conduction Responsiveness of rate change is improved.

  In the present embodiment, the heat conducting part using the metal / insulating phase transition body whose thermal conductivity changes with application and removal of voltage is exemplified. However, the heat conduction part can be used in any configuration as long as it has a property of increasing the thermal conductivity by applying a voltage and decreasing the thermal conductivity by cutting off the voltage. In the present embodiment, the magnetic bodies 10A-10F, the magnetic bodies 11A-11F,..., And the heat conducting portions 30A-30G, the heat conducting portions 31A-31G,. The shape was as follows. However, other shapes such as a spherical shape, an ellipsoidal shape, a cubic shape, a cylindrical shape, and an elliptical column shape may be employed.

<Configuration of magnetic unit>
The magnetic units shown in FIGS. 9 and 10 sandwich the heat transport unit 1000A shown in FIG. 8 with a certain gap from both sides in the vertical direction. The configuration of the magnetic unit is as follows.

  The circular upper magnetic unit 2000A is positioned so that the front side of FIG. 9 faces the front side of the heat transport unit 1000A shown in FIG. 8, and the center of the upper magnetic unit 2000A coincides with the center of the heat transport unit 1000A. , Supports clockwise rotation. FIG. 9 shows a state where the upper magnetic unit 2000A positioned facing the heat transport unit 1000A is seen through from the top toward the heat transport unit 1000A.

  The magnetic application removing unit 1U shown in FIG. 9 faces the heat transporter 50-1 shown in FIG. 8 at a certain time. At that time, from the outer periphery to the inner periphery of the magnetic unit 2000A, there are a permanent magnet 21A facing the magnetic body 10A, a permanent magnet 21C facing the magnetic body 10C, and a permanent magnet 21E facing the magnetic body 10E.

  The magnetic application removing unit 2U shown in FIG. 9 faces the heat transporter 50-2 shown in FIG. 8 at the same time as described above. At that time, from the outer periphery to the inner periphery of the magnetic unit 2000A, there are a permanent magnet 22B facing the magnetic body 11B, a permanent magnet 22D facing the magnetic body 11D, and a permanent magnet 22F facing the magnetic body 11F.

  Since the other magnetic application removal units present in the magnetic unit 2000A are point-symmetric with respect to the center of the magnetic unit 2000A, the arrangement of the permanent magnets is the same as the magnetic application removal unit 1U or the magnetic application removal unit 2U.

  The circular lower magnetic unit 2000B is positioned so that the front side of FIG. 10 faces the back side of the heat transport unit 1000A shown in FIG. 8, and the center of the lower magnetic unit 2000B coincides with the center of the heat transport unit 1000A. And support it so that it can rotate clockwise. FIG. 10 shows a state in which the lower magnetic unit 2000B positioned facing the heat transport unit 1000A is viewed from the heat transport unit 1000 side.

  The magnetic application removing unit 1D shown in FIG. 10 faces the heat transporter 50-1 shown in FIG. 8 at the same time as described above. At that time, from the outer periphery to the inner periphery of the magnetic unit 2000B, there are a permanent magnet 26A facing the magnetic body 10A, a permanent magnet 26C facing the magnetic body 10C, and a permanent magnet 26E facing the magnetic body 10E.

  The magnetic application removing unit 2D shown in FIG. 10 faces the heat transporter 50-2 shown in FIG. 8 at the same time as described above. At that time, from the outer periphery to the inner periphery of the magnetic unit 2000B, there are a permanent magnet 27B facing the magnetic body 11B, a permanent magnet 27D facing the magnetic body 11D, and a permanent magnet 27F facing the magnetic body 11F.

  Since the other magnetic application removal units existing in the magnetic unit 2000B are point-symmetric with respect to the center of the magnetic unit 2000B, the arrangement of the permanent magnets is the same as the magnetic application removal unit 1D or the magnetic application removal unit 2D.

  The magnetic application removal units 1U, 2U,... Of the upper magnetic unit 2000A and the magnetic application removal units 1D, 2D,... Of the lower magnetic unit 2000B are the heat transporters 50-1, 50- of the heat transport unit 1000. It opposes in the up-down direction via 2 .... The upper magnetic unit 2000A and the lower magnetic unit 2000B rotate synchronously without changing their relative positions in a state where the magnetic application removal unit 1U and the magnetic application removal unit 1D are opposed to each other.

  The magnetic units 2000A and 2000B are formed in a hollow circular shape, and a fan 210 for circulating air through a refrigerant passage 42 (FIGS. 8 and 12) formed inside the high-temperature side heat exchange unit 40B on the inner periphery thereof. Is provided. The refrigerant passage 42 is a cylindrical passage communicating in the stacking direction of the heat transport unit 1000A and the magnetic units 2000A and 2000B. The inner peripheral surface of the fan 210 is fixed to the rotor (rotating shaft) 310 of the outer rotor motor 350 (see FIG. 11). Therefore, when the rotor 310 rotates, the magnetic units 2000A and 2000B rotate, and air is circulated from the bottom of the refrigerant passage 42 upward by the fan 210. The blade 212 of the fan 210 is bent at an optimum angle with respect to the horizontal so that an air flow is generated by the rotation of the magnetic units 2000A and 2000B. By using the outer rotor motor 350, the magnetic air conditioner can be miniaturized.

  On the outer periphery of the magnetic units 2000A and 2000B, a fan 215 for circulating air through the refrigerant passage 41 formed in the low temperature side heat exchange unit 40A is provided. The refrigerant passage 41 is a passage through which the refrigerant passages individually formed on the outer peripheral portions of the heat transport unit 1000A and the magnetic unit 2000A are connected in series and the refrigerant flowing through the refrigerant passage is circulated in the stacking direction. A large number of blades 214 are formed on the fan 215. Therefore, when the rotor 310 rotates, the magnetic units 2000A and 2000B rotate, and the air in the refrigerant passage 41 is circulated along the outer periphery of the heat transport unit 1000A by the blades 214. The blade 214 is bent at right angles to the horizontal so that the air in the refrigerant passage 41 is efficiently moved by the rotation of the magnetic units 2000A and 2000B. As described above, when the fans 210 and 215 are provided on the inner and outer peripheral portions of the magnetic units 2000A and 2000B, the magnetic units 2000A and 2000B are not only used for applying and removing magnetism, but also for circulating the refrigerant. It can also play a role as a fan. Further, the refrigerant can be efficiently circulated by the refrigerant passages 41 and 42.

  In the present embodiment, as shown in FIG. 12, a reference position detection sensor 250 for detecting the reference position of the magnetic unit 2000A is provided. Further, a rotational position detection sensor for detecting the rotational position of the outer rotor motor 350 shown in FIG. 11 is built in the outer rotor motor 350.

  As shown in FIG. 9, FIG. 10 and FIG. 12, magnets are arranged annularly and radially on both surfaces of the magnetic units 2000A, 2000B. As shown in FIG. 12, the magnets arranged in the magnetic unit 2000A are arranged in consideration of the polarity so that the N pole and the S pole face each other.

  FIG. 13 is a diagram showing the arrangement of the magnets of the magnetic units 2000A, 2000B... According to the present embodiment. In the present embodiment, the magnetization directions of the magnets 21A, 21C, and 21E disposed in the magnetic unit 2000A and the magnets 26A, 26C, and 26E disposed in the magnetic unit 2000B are opposite to each other between adjacent magnets. The magnetization directions of adjacent magnets are opposite to each other. By making the directions opposite to each other, the direction of the leakage magnetic field between the magnets can be reversed. Therefore, the leakage magnetic field in the space between the magnets can be reversed. This is because the size is reduced by the interference effect.

  In the magnetic unit 2000A, the magnetization direction of the magnet 21C adjacent to the magnet 21A is reversed, the N pole of the magnet 21A is opposed to the magnetic body 10A of the heat transport unit 1000A, and the magnet 21C is opposed to the magnetic body 10C. Is the opposite of the S pole. Also, the magnetization direction of the magnet 21E adjacent to the magnet 21C is reversed, and the magnet 21C is opposed to the south pole with respect to the magnetic body 10C of the heat transport unit 1000A, and the magnet 21E is opposite to the magnetic body 10E. Confront. A magnetic body 10B is positioned between the magnetic bodies 10A and 10C, a magnetic body 10D is positioned between the magnetic bodies 10C and 10E, and a magnetic body 10F is positioned adjacent to the magnetic body 10E. The magnets 21A, 21C, and 21E do not face the magnetic bodies 10B, 10D, and 10F.

  In the magnetic unit 2000B, the magnetization direction of the magnet 26C adjacent to the magnet 26A is reversed, the S pole of the magnet 26A faces the magnetic body 10A of the heat transport unit 1000A, and the magnet 26C faces the magnetic body 10C. Is the opposite of the N pole. In addition, the magnetization direction of the magnet 26E adjacent to the magnet 26C is reversed, and the N pole of the magnet 26C is opposed to the magnetic body 10C of the heat transport unit 1000A, and the magnet 26E is the S pole of the magnetic body 10E. Confront. As with the magnetic unit 2000A, the magnets 26A, 26C, and 26E do not face the magnetic bodies 10B, 10D, and 10F.

  As described above, when magnets are arranged so that the magnetization directions of the adjacent magnets are opposite to each other, the directions of the magnetic fields generated by the adjacent magnets are reversed. For this reason, the magnetic field lines from adjacent magnets interfere with each other and cancel each other, and the leakage magnetic field with respect to the magnetic bodies (magnetic bodies 10B, 10D, 10F) that are located between the magnets and do not want to apply a magnetic field can be reduced. Therefore, the magnetic flux density applied to the magnetic body (magnetic bodies 10A, 10C, 10E) to which a magnetic field needs to be applied and the magnetic bodies (magnetic bodies 10B, 10D, 10F) that do not want to apply the magnetic field On the other hand, the difference between the applied magnetic flux and the magnetic flux density can be increased, and the magnetocaloric effect of the magnetic material can be maximized. Moreover, since the magnet and the magnetic body are alternately overlapped, the amount of the magnet and the yoke used can be suppressed.

  Moreover, FIG. 14 is a figure which shows the modification of arrangement | positioning of the magnet of magnetic unit 2000A, 2000B ... which concerns on this embodiment. In this modification, a first magnet that faces one surface of the heat transport unit 1000A and a second magnet that faces the other surface are separately arranged on the magnetic units 2000A, 2000B,. Further, the magnetization directions of the first magnet and the second magnet arranged in the magnetic units 2000A, 2000B,.

  In the magnetic unit 2000A, instead of one magnet as shown in FIG. 13, the first magnet 21Aa facing one surface of the heat transport unit and the second magnet 21Ab facing the other surface are separately arranged. Further, the first magnet 21Ca and the second magnet 21Cb are arranged adjacent to the first magnet 21Aa and the second magnet 21Ab. Further, a first magnet 21Ea and a second magnet 21Eb are arranged adjacent to the first magnet 21Ca and the second magnet 21Cb.

  The magnetization directions of the first magnet 21Aa and the second magnet 21Ab are the same, and the magnetization direction is the direction from the N pole of the second magnet 21Ab toward the S pole of the first magnet 21Aa. The magnetization directions of the first magnet 21Ca and the second magnet 21Cb are the same, and the magnetization direction is a direction from the N pole of the first magnet 21Ca toward the S pole of the second magnet 21Cb. Furthermore, the magnetization directions of the first magnet 21Ea and the second magnet 21Eb are the same, and the magnetization direction is a direction from the N pole of the second magnet 21Eb toward the S pole of the first magnet 21Ea.

  In the magnetic unit 2000B, similarly to the magnetic unit 2000A, the first magnet 26Aa facing one surface of the heat transport unit and the second magnet 26Ab facing the other surface are separately arranged. Further, a first magnet 26Ca and a second magnet 26Cb are arranged adjacent to the first magnet 26Aa and the second magnet 26Ab. Further, a first magnet 26Ea and a second magnet 26Eb are disposed adjacent to the first magnet 26Ca and the second magnet 26Cb.

  The magnetization directions of the first magnet 26Aa and the second magnet 26Ab are the same, and the magnetization direction is the direction from the N pole of the second magnet 26Ab toward the S pole of the first magnet 26Aa. The magnetization directions of the first magnet 26Ca and the second magnet 26Cb are the same, and the magnetization direction is a direction from the N pole of the first magnet 26Ca toward the S pole of the second magnet 26Cb. Furthermore, the magnetization directions of the first magnet 26Ea and the second magnet 26Eb are the same, and the magnetization direction is a direction from the N pole of the second magnet 26Eb toward the S pole of the first magnet 26Ea.

  In the magnetic unit 2000A, the magnetization direction of the first magnet 21Ca adjacent to the first magnet 21Aa is reversed. Moreover, the magnetization direction of the first magnet 21Ea adjacent to the first magnet 21Ca is reversed.

  Further, in the magnetic unit 2000A, the magnetization direction of the second magnet 21Cb adjacent to the second magnet 21Ab is reversed, and the N pole of the second magnet 21Ab is opposed to the magnetic body 10A of the heat transport unit 1000A. The second magnet 21Cb is opposed to the south pole with respect to the magnetic body 10C. Further, the magnetization direction of the second magnet 21Eb adjacent to the second magnet 21Cb is reversed, and the second magnet 21Cb faces the magnetic body 10C of the heat transport unit 1000A, and the S pole of the second magnet 21Cb faces the magnetic body 10E. Thus, the N pole faces the second magnet 21Eb. A magnetic body 10B is positioned between the magnetic bodies 10A and 10C, a magnetic body 10D is positioned between the magnetic bodies 10C and 10E, and a magnetic body 10F is positioned adjacent to the magnetic body 10E. Magnets 21Ab, 21Cb, and 21Eb do not face magnetic bodies 10B, 10D, and 10F.

  In the magnetic unit 2000B, the magnetization direction of the first magnet 26Ca adjacent to the first magnet 26Aa is reversed, and the S pole of the first magnet 26Aa is opposed to the magnetic body 10A of the heat transport unit 1000A. The N pole of the first magnet 26Ca is opposed to the magnetic body 10C. Further, the magnetization direction of the first magnet 26Ea adjacent to the first magnet 26Ca is reversed, and the N pole of the first magnet 26Ca is opposed to the magnetic body 10C of the heat transport unit 1000A, and the magnetic body 10E is opposed to the magnetic body 10E. The first magnet 26Ea faces the south pole. As with the magnetic unit 2000A, the magnets 26Aa, 26Ca, and 26Ea do not face the magnetic bodies 10B, 10D, and 10F.

  In the magnetic unit 2000B, the magnetization direction of the second magnet 26Cb adjacent to the second magnet 21Ab is reversed. The magnetization direction of the second magnet 26Eb adjacent to the second magnet 26Cb is reversed.

  As described above, when the magnetization directions of the first magnet and the second magnet are the same, and the magnets are arranged so that the magnetization directions are opposite to each other between the adjacent first magnets and the second magnets, they are adjacent to each other. The direction of the magnetic field generated by the magnet is reversed. For this reason, the magnetic field lines from adjacent magnets interfere with each other and cancel each other, and the leakage magnetic field with respect to the magnetic bodies (magnetic bodies 10B, 10D, 10F) that are located between the magnets and do not want to apply a magnetic field can be reduced. Therefore, the magnetic flux density applied to the magnetic body (magnetic bodies 10A, 10C, 10E) to which a magnetic field needs to be applied and the magnetic bodies (magnetic bodies 10B, 10D, 10F) that do not want to apply the magnetic field On the other hand, the difference between the applied magnetic flux and the magnetic flux density can be increased, and the magnetocaloric effect of the magnetic material can be maximized. Moreover, since the magnet and the magnetic body are alternately overlapped, the amount of the magnet and the yoke used can be suppressed. Furthermore, in the case of FIG. 13, since the magnet is also present in the yoke portion, the amount of the magnet used is increased. However, in the case of FIG. 14, the magnet present in the yoke portion is small. Compared with the case of FIG. 13, the amount of magnets used can be reduced.

  FIG. 15 is a diagram for explaining an effect caused by a difference in magnet arrangement. Specifically, as shown in FIG. 23, when the magnets are arranged so that the magnetization directions are the same, and when the magnets are arranged so that the magnetization directions are alternate as in this embodiment, It is a figure where it uses for description of the difference in an effect.

  As shown in the figure, compared to the case where the magnets are arranged so that the magnetization directions are the same, the case where the magnets are arranged so that the magnetization directions are alternating is more suitable for the magnetic material to which a magnetic field needs to be applied. It can be seen that the difference between the magnetic flux density of the magnetic flux applied to the magnetic body and the magnetic flux density of the magnetic flux applied to the magnetic body to which no magnetic field application is desired increases in any magnetic body. This is because when the magnets are arranged so that the magnetization directions are the same, leakage magnetic fields from adjacent magnets interfere with each other, so that the magnetic field applied to the magnetic material that does not need to be applied increases. is there. Therefore, the difference between the magnetic flux density when the magnetic field is applied and the magnetic flux density when no magnetic field is applied is reduced.

  FIG. 16 is a diagram visualizing lines of magnetic force of the magnetic unit (configuration of FIG. 14) according to the first embodiment. As can be seen from this figure, it can be seen that the magnetic fields formed by the magnets are alternating. In this way, when the magnetic field directions are alternately formed, the magnetic field lines from adjacent magnets interfere with each other, and the magnetic flux density of the magnetic flux applied to the magnetic material to which no magnetic field is to be applied can be reduced. It is possible to increase the difference between the magnetic flux density of the magnetic flux applied to the magnetic body that needs to be applied and the magnetic flux density of the magnetic flux applied to the magnetic body that does not want to apply the magnetic field. For this reason, the magnetocaloric effect of the magnetic material can be maximized. Moreover, since the magnet and the magnetic body are alternately overlapped, the amount of the magnet and the yoke used can be suppressed.

  According to the experiment, when the calorific values of the magnetic bodies in the configurations of FIG. 23 and FIG. 13 are compared, the configuration of FIG. 13 shows the magnetic flux density of the magnetic flux applied to the magnetic body to which the magnetic field needs to be applied The difference between the magnetic flux density applied to the magnetic material to which the magnetic field is not applied was improved by 15%, and the calorific value was also improved by 15%. Further, the configuration of FIG. 13 can increase the temperature fluctuation range of the magnetic material by 15%, so that the number of magnetic units to be stacked can be reduced by 15%, and the volume of the magnetic air conditioner can be reduced by 15%. can do. As a result, the cooling / heating capacity per unit volume of the magnetic cooling / heating device can be improved by about 30%.

  As shown in FIGS. 11 and 12, a plurality of heat transport units 1000A, 1000B,... And magnetic units 2000A, 2000B,. When a plurality of heat transport units 1000A, 1000B,... And magnetic units 2000A, 2000B,... Are stacked, the heat capacity of the magnetic air conditioner can be increased, and heat can be efficiently transferred in a small space. The heat transport unit 1000A is fixed to the rotor 310 via a bearing 45 as shown in FIG. Therefore, all the stacked heat transport units 1000A, 1000B,... Remain stationary without rotating even when the rotor 310 rotates. On the other hand, the magnetic units 2000A, 2000B,... Are attached to the rotor 310 as shown in FIGS. Therefore, all the stacked magnetic units 2000A and 2000B rotate with the rotation of the rotor 310.

  In the present embodiment, the magnetic units 2000A, 2000B,... Are rotated by the outer rotor motor 350. However, the magnetic units 2000A, 2000B,... Are fixed and the heat transport units 1000A, 1000B,. You may do it. The magnetic units 2000A, 2000B,... And the heat transport units 1000A, 1000B,. Furthermore, the heat transporters 50-1, 50-2,... May not be arranged in a ring shape as in the present embodiment, but may be arranged in parallel in a straight line on the outer peripheral surface of the cylinder. In this case, the magnetic unit 2000A has a magnet on the inner peripheral surface of a cylinder positioned outside the heat transporters 50-1, 50-2,... Concentrically with the heat transporters 50-1, 50-2,. It will be arranged. The magnets arranged in the magnetic units 2000A, 2000B,... Are preferably permanent magnets, but electromagnets may be used. When an electromagnet is used, the structure of each magnetic unit 2000A, 2000B,. This is because it is necessary to perform wiring so that power can be supplied to the electromagnet in the rotated state. Therefore, in this embodiment, a permanent magnet is used.

  When the magnetic units 2000A, 2000B,... Rotate, the magnetic bodies of the heat transporters 50-1, 50-2,... Of the heat transport units 1000A, 1000B,. Magnetism is applied to or removed from. At this time, the magnets of the magnetic units 2000A, 2000B,... Transfer from the magnetic body of one of the heat transporters 50-1, 50-2,. However, in this embodiment, since the magnetically permeable heat insulating portion 60 exists between the magnetic bodies, the fluctuation of the driving force of the magnetic units 2000A, 2000B,. The fluctuation of the driving force will be described with reference to FIG.

  FIG. 17 is a diagram for explaining the effect of the magnetically permeable heat insulating portion 60 provided in the heat transport unit 1000A. As shown in the figure, when the magnet moves in the illustrated moving direction and the magnet is in a position to sandwich the magnetic body from above and below, the magnetic lines of force of the magnet pass through the magnetic body and cause the magnetic body to generate heat. At this time, a reaction force opposite to the moving direction of the magnet as shown in the figure is applied to the magnetic units 2000A and 2000B. If the magnet continues to move and the front part of the magnet reaches the gap between the magnetic bodies (position a in the figure), the reaction force gradually increases. Without the magnetically permeable heat insulating portion 60 provided in the present embodiment, the reaction force increases to FAmax as shown in the figure. When the rear part of the magnet passes through the gap, a reverse reaction force is generated (position b in the figure). This variation in reaction force increases the required capacity of the outer rotor motor 350 that drives the magnetic units 2000A and 2000B. This is because the driving force of the outer rotor motor 350 must be at least the reaction force of FAmax or more. In addition, the reaction force fluctuation occurs every time the magnet passes between the heat transporters, and thus causes noise and vibration.

  However, in the present embodiment, since the magnetically permeable heat insulating portion 60 having the same magnetic permeability as that of the magnetic material is formed between the heat transporters, as shown in the lower diagram of FIG. Is considerably smaller. Therefore, the magnetic units 2000A and 2000B can rotate relatively smoothly, and the driving force of the outer rotor motor 350 only needs to be larger than the reaction force generated between the magnet and the magnetic body. For this reason, it is not necessary to prepare an outer rotor motor 350 that is larger than necessary, and the magnetic air conditioner can be downsized. Further, noise and vibration are extremely reduced, and a magnetic air conditioner having quietness can be realized.

  The magnetic materials of the heat transporters 50-1, 50-2,... Of the heat transport units 1000A, 1000B,... Are alternately applied or removed every other rotation. That is, in each of the heat transporters 50-1, 50-2,..., The state in which magnetism is applied to the magnetic bodies 10A, 10C, and 10E and the state in which magnetism is applied to the magnetic bodies 10B, 10D, and 10F are alternated. To happen. For this reason, every time the magnetic unit 2000A rotates 30 degrees, the magnetic bodies of the heat transporters 50-1, 50-2,... Repeatedly generate and absorb heat. The amount of heat generated per unit time of the magnetic body varies depending on the rotation speed of the magnetic unit 2000A. In order to increase the heat generation amount, the rotation speed of the magnetic units 2000A, 2000B,. If a large calorific value is not required, the rotation speed of the magnetic units 2000A, 2000B,.

  In order to transfer the heat generated when the magnetic body of each heat transporter 50-1, 50-2,... Generates heat and absorbs heat from the low temperature side heat exchanger 40A to the high temperature side heat exchanger 40B, at an optimal timing. A voltage must be applied to or removed from each heat transfer section. The control system shown in FIG. 18 and subsequent figures controls the timing for applying or removing the voltage of all the heat conducting portions.

  FIG. 18 is a block diagram of a control system of the magnetic air conditioner according to this embodiment. FIG. 19 is a block diagram of a more specific control system of the air conditioning control unit and the air conditioning information input unit of FIG.

  As shown in FIG. 18, the control system of the magnetic air conditioner according to this embodiment includes a reference position detection sensor 250, an air conditioning information input unit 460, an outer rotor motor 350, a motor control unit 380, heat conduction units 30A to 30G, a voltage An application control unit 38 and an air conditioning control unit 450 are provided. The outer rotor motor 350 includes a rotational position detection sensor 370 that detects its own rotational position.

  The reference position detection sensor 250 detects the reference position set in the magnetic unit 2000A (see FIGS. 11 and 12). The reference position is provided on the outer periphery of the magnetic unit 2000A. For example, when a reflector that reflects light is attached to the outer periphery of the magnetic unit 2000A, the attachment position of the reflector becomes the reference position. In this case, a light receiving / emitting element is used as the reference position detection sensor 250, and the reference position is detected when the reflector reflects light from the light receiving / emitting element.

  The air conditioning information input unit 460 inputs information necessary for air conditioning. Information necessary for air conditioning is a set temperature, a low temperature side heat exchange section inlet temperature, a low temperature side heat exchange section outlet temperature, a high temperature side heat exchange section inlet temperature, and a high temperature side heat exchange section outlet temperature. A specific description of the air conditioning information input unit 460 will be given based on FIG.

  The outer rotor motor 350 is a motor that drives a magnet in order to selectively apply magnetism to each magnetic body of the heat transporters 50-1, 50-2,. Specifically, the outer rotor motor 350 simultaneously rotates all the magnetic units 2000A on which magnets are arranged as shown in FIG. The outer rotor motor 350 is provided with a rotational position detection sensor 370 that detects its rotational position. The rotational position detected by the rotational position detection sensor 370 is used to control the rotational speed of the magnetic units 2000A,.

  The motor control unit 380 controls the rotation of the outer rotor motor 350 using the rotation position detected by the rotation position detection sensor 370 and the reference position detected by the reference position detection sensor 250.

  As described above, the thermal conductivity of the heat conducting units 30A to 30G increases when the voltage is applied, and decreases when the voltage is removed. The heat conduction between the magnetic bodies of the heat transporter 50-1 is interrupted.

  The voltage application control unit 38 selectively applies a voltage to each heat conducting unit 30A-30G according to the rotational position of the outer rotor motor 350 and removes it. The rotational position of the outer rotor motor 350 can be determined by the rotational position detected by the rotational position detection sensor 370 and the reference position detected by the reference position detection sensor 250. That is, it can be recognized where the position of each magnet is with respect to the magnetic body of each heat transporter 50-1, 50-2,. When the position of each magnet becomes an optimal position with respect to the position of the magnetic body of each heat transporter 50-1, 50-2,..., The voltage application control unit 38 applies to each heat conducting unit 30A-30G. A voltage is selectively applied and removed. As described above, the voltage application control unit 38 applies and removes the voltage to each heat conduction unit in synchronization with the timing at which the magnet selectively applies and removes the magnetism to each magnetic body, thereby removing the low temperature side heat exchange unit. Heat is transported from 40A to the high temperature side heat exchange section 40B.

  The voltage application control unit 38 applies and removes a voltage to each heat conducting unit 30A-30G using the voltage application and removal timings determined for each operation condition. The voltage application / removal timing determined for each operating condition is rewritten to an optimum timing in accordance with the operation of the magnetic air conditioner. The operating condition is at least one of a required heat amount of the heat transporters 50-1, 50-2,..., A temperature difference between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B, or a magnet drive pattern. .

  The air conditioning controller 450 generally controls the operation of the magnetic air conditioner according to the present embodiment. A specific description of the air conditioning control unit 450 will be made with reference to FIG.

  As shown in FIG. 19, the air conditioning information input unit 460 includes a temperature setting unit 462, a low temperature side heat exchange unit inlet temperature sensor 464, a low temperature side heat exchange unit outlet temperature sensor 466, a high temperature side heat exchange unit inlet temperature sensor 468, and a high temperature. A side heat exchanger outlet temperature sensor 470 is provided.

  The temperature setting unit 462 is a controller that sets the temperature in the passenger compartment that is air-conditioned by the magnetic air conditioner. The low temperature side heat exchange section inlet temperature sensor 464 detects the temperature of the refrigerant supplied to the low temperature side heat exchange section 40A of the heat transport units 1000A, 1000B,... Shown in FIG. The low temperature side heat exchange section inlet temperature sensor 464 is provided at the refrigerant inlet portion of the low temperature side heat exchange section 40A.

  The low temperature side heat exchange section outlet temperature sensor 466 detects the temperature of the refrigerant discharged from the low temperature side heat exchange section 40A of the heat transport units 1000A, 1000B,... Shown in FIG. The low temperature side heat exchange section outlet temperature sensor 466 is provided at the refrigerant outlet portion of the low temperature side heat exchange section 40A. The high temperature side heat exchange section inlet temperature sensor 468 detects the temperature of the refrigerant supplied to the high temperature side heat exchange section 40B shown in FIGS. The high temperature side heat exchange section inlet temperature sensor 468 is provided at the refrigerant inlet portion of the high temperature side heat exchange section 40B. The high temperature side heat exchange section outlet temperature sensor 470 detects the temperature of the refrigerant discharged from the high temperature side heat exchange section 40B. The high temperature side heat exchange section outlet temperature sensor 470 is provided at the refrigerant outlet portion of the high temperature side heat exchange section 40B.

  The temperature setting unit 462, the low temperature side heat exchange unit inlet temperature sensor 464, the low temperature side heat exchange unit outlet temperature sensor 466, the high temperature side heat exchange unit inlet temperature sensor 468, and the high temperature side heat exchange unit outlet temperature sensor 470 are provided with heat. This is to know how much heat must be transferred from the low temperature side heat exchange section 40A to the high temperature side heat exchange section 40B in the transport units 1000A, 1000B,. If the amount of heat to be moved is known, the rotational speed of the outer rotor motor 350 and the ON / OFF timing of the voltages of the heat transfer units 30A-30G, 31A-31G,.

  The air conditioning control unit 450 includes a switching control unit 452 and a switching pattern storage unit 454. The switching control unit 452 uses the set temperature, the low-temperature side heat exchange unit inlet temperature, the low-temperature side heat exchange unit outlet temperature, the high-temperature side heat exchange unit inlet temperature, and the high-temperature side heat exchange unit outlet temperature. Controls ON / OFF switching of voltages applied to 30G, 31A-31G,. The switching pattern storage unit 454 stores ON / OFF switching patterns of voltages applied to the heat conducting units 30A-30G, 31A-31G,.

  Next, operation | movement of the magnetic air conditioning apparatus which concerns on this embodiment is demonstrated easily based on the flowchart of FIG. FIG. 20 is an operation flowchart of the magnetic air conditioner according to this embodiment.

(Operation of magnetic air conditioner)
First, the operator inputs a set temperature in the passenger compartment from the temperature setting unit 462. When the set temperature is input, the air conditioning control unit 450 inputs the required heat amount and the required temperature difference (S1). The air conditioning control unit 450 refers to the space capacity in the vehicle interior, the current temperature in the vehicle interior, and the set temperature in the vehicle interior to obtain the required heat amount necessary for setting the vehicle interior to the set temperature. Further, a temperature difference between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B is obtained. The obtained values are input as the required heat amount and the required temperature difference.

  Next, the air-conditioning control unit 450 obtains the magnetic application frequency f by collating the input required heat amount and the required temperature difference with a previously stored map, and turns on the heat conducting units 30A-30G, 31A-31G,. An OFF switching pattern is acquired from the switching pattern storage unit 454 (S2). TSs of the switching pattern is a timing for turning on the heat conducting units 30A-30G, 31A-31G,..., In other words, a timing for applying a voltage to the heat conducting units 30A-30G, 31A-31G,. On the other hand, TSe of the switching pattern is a timing at which the heat conduction by the heat conducting portions 30A-30G, 31A-31G,... Is turned off, in other words, a timing at which the voltage is removed from the heat conducting portions 30A-30G.

  The air conditioning control unit 450 operates the magnetic air conditioner (S3). That is, the air-conditioning control unit 450 issues a rotation speed instruction to the motor control unit 380 in order to realize the obtained magnetic application frequency f. The magnetic application frequency indicates how many times a magnetic substance is applied and removed per second. For example, assuming that the magnetic application frequency f is 6 Hz, in the case of the magnetic air conditioner configured as shown in FIGS. 8 to 12, when the magnetic units 2000A, 2000B,. Therefore, the rotational speed required for the magnetic units 2000A, 2000B,... Is 60 rpm. The motor control unit 380 is instructed about the number of rotations of the outer rotor motor 350 necessary for the magnetic units 2000A, 2000B,... To rotate at 60 rpm. Further, the air conditioning control unit 450 sends the switching pattern to the voltage application control unit 38 in order to reproduce the switching pattern acquired from the switching pattern storage unit 454.

  The air conditioning control unit 450 determines whether or not the operation in step S3 has been performed in a specified cycle (S4). As shown in FIG. 7, the temperature difference gradually increases between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B immediately after the operation of the magnetic cooling / heating device is started. Until this temperature difference reaches the required temperature difference, the application and removal of magnetism must be repeated for a predetermined cycle. In the case of the magnetic air conditioner of this embodiment, when the magnetic units 2000A, 2000B,... Make one rotation, the application and removal of magnetism to each heat transporter 50-1, 50-2,. Therefore, for example, if the specified cycle is set to 1200 cycles, it is determined whether or not the magnetic units 2000A, 2000B,.

  If the operation in step S3 has not reached the specified cycle (S4: NO), the air conditioning controller 450 repeats the process in step S3. On the other hand, if the operation of step S3 reaches a specified cycle (S4: YES), the process proceeds to the next step.

  Next, the air conditioning control unit 450 calculates an output heat amount and an output temperature difference (S5). The amount of output heat includes the refrigerant low temperature side heat exchange section inlet temperature Tci detected by the low temperature side heat exchange section inlet temperature sensor 464, and the low temperature side heat exchange section outlet refrigerant temperature Tco detected by the low temperature side heat exchange section outlet temperature sensor 466. Is obtained by multiplying the temperature difference by the mass mc of the refrigerant and the specific heat Cp. Further, the difference in output temperature between the refrigerant high temperature side heat exchange section outlet temperature Tho detected by the high temperature side heat exchange section outlet temperature sensor 468 and the refrigerant temperature detected by the low temperature side heat exchange section outlet temperature sensor 466 is the low temperature side heat exchange section. This is the temperature difference from the outlet Tco.

  Next, the air conditioning control unit 450 calculates the difference between the required heat amount input in step S1 and the output heat amount obtained in step S5. Further, a difference between the required temperature difference input in step S1 and the output temperature difference obtained in step S5 is calculated (S6).

  The air-conditioning control unit 450 determines whether the difference between the required heat amount and the output heat amount and the difference between the required temperature difference and the output temperature difference are within a specified range (S7).

  If the difference between the required heat amount and the output heat amount and the difference between the required temperature difference and the output temperature difference are within the specified range (S7: YES), the air conditioning controller 450 determines the magnetic application frequency f obtained in step S2, The ON / OFF switching patterns of the heat conducting units 30A-30G, 31A-31G,... Are updated and stored in the switching pattern storage unit 454. The operation of the magnetic air conditioner is continued using the magnetic application frequency f obtained in step S2 and the ON / OFF switching patterns of the heat conducting portions 30A-30G, 31A-31G,... (S8).

  If the difference between the required heat amount and the output heat amount and the difference between the required temperature difference and the output temperature difference are not within the specified range, the air conditioning control unit 450 sets the magnetic application frequency f obtained in step S2 to f + Δf, and sets the heat conduction unit. The TSs of the 30A-30G ON / OFF switching patterns are set to TSs + ΔTSs, and TSe is set to TSe + ΔTSe (S9). Then, the processing from step S3 to step S7 is repeated. In this way, when the optimum magnetic application frequency f and the optimum switching pattern are learned, it is possible to correct variations in heat generation characteristics that differ from one magnetic material to another and heat transfer characteristics that differ from one heat conduction unit to another.

  As described above, in the magnetic air conditioner according to the present embodiment, the magnetic units 2000A, 2000B,... Where the magnets are arranged are rotated, and the heat conducting units 30A-30G, 31A-31G,. Heat can be transferred from the low temperature side heat exchanger 40A to the high temperature side heat exchanger 40B simply by applying a voltage. Also, air is circulated in the magnetic unit 2000A, 2000B,... In the stacking direction through the refrigerant passage 42 of the high temperature side heat exchanger 40B by the fan 210 formed in the inner periphery of the magnetic units 2000A, 2000B,. To do. Further, the fan 215 formed on the outer periphery of the magnetic units 2000A, 2000B,... Generates cold air by circulating air in the rotation direction of the magnetic units 2000A, 2000B,. To do.

[Embodiment 2]
The configuration of the magnetic air conditioning apparatus according to the second embodiment will be described with reference to FIGS. 21 and 22. In the configuration shown in FIGS. 11 and 12, the magnetic air conditioner according to the present embodiment is arranged by slightly shifting each of the heat transport units 1000 </ b> A, 1000 </ b> B, 1000 </ b> C, and 1000 </ b> D in the rotational direction (with a phase difference). ing. The operation of the magnetic air conditioner according to the second embodiment is the same as the operation of the magnetic air conditioner according to the first embodiment.

  FIG. 21 is a configuration diagram of a heat transport unit of the magnetic air conditioner according to the second embodiment. FIG. 22 is a diagram for explaining an effect when the arrangement of the heat transport units has a phase difference.

  Unlike the heat transport units 1000A, 1000B,... Of the first embodiment, the heat transport units 1000A-1000D shown in FIG. For this reason, a reaction force of Fmax as described in FIG. 8 is generated in each of the heat transport units 1000A to 1000D. If the heat transport units 1000 </ b> A to 1000 </ b> D are simply stacked, the sum of reaction forces generated in all the heat transport units 100 becomes large. In the present embodiment, the sum of the reaction forces is reduced.

  As shown in FIGS. 11 and 12, the heat transport units 1000A-1000D,... Are alternately stacked with the magnetic units 2000A, 2000B,. In the present embodiment, when stacking the heat transport units 1000A-1000D,..., As shown in FIG.

  As shown in FIG. 21, the first heat transport unit 1000A is disposed without shifting the phase in the rotation direction. Under the heat transport unit 1000A, the heat transport unit 1000B is arranged with a phase shifted in the direction of rotation of 7.5 degrees. Similarly, the heat transport units 1000C, 1000D,... Stacked below the heat transport unit 1000B are arranged with a phase shift of 7.5 degrees with respect to the heat transport unit directly above. As described above, when the heat transport units 1000A-1000D,... Are arranged, a plurality of sheets without overlapping the gap (see FIG. 8) between the heat transporter 50-1 and the heat transporter 50-2 in the stacking direction. Heat transport units 1000A-1000D,... Can be arranged.

  When the magnetic units 2000A, 2000B, ... rotate, the magnetic bodies 10A-10F, 11A-11F, ... of the heat transporters 50-1, 50-2, ... of the heat transport units 1000A, 1000B, 1000C, 1000D, ... Every 30 rotations, magnetism is applied or removed alternately. At this time, the magnets of the magnetic units 2000A, 2000B,... Transfer from the magnetic body of one heat transporter adjacent in the rotation direction to the magnetic body of the other heat transporter. However, in the present embodiment, the heat transport units 1000A to 1000D are arranged out of phase with each other, so that fluctuations in the driving force of the heat transport units 1000A to 1000D are dispersed. The fluctuation of the driving force will be described with reference to FIG.

  As shown in FIG. 22, when the magnet moves in the illustrated moving direction and overlaps the magnetic body, the magnetic lines of force of the magnet pass through the magnetic body and cause the magnetic body to generate heat. At this time, a reaction force opposite to the moving direction of the magnet as shown in the figure is applied to the magnetic units 2000A and 2000B. When the magnet continues to move and the front part of the magnet reaches the gap between the magnetic bodies (position a in the figure), the reaction force gradually increases and the four heat transport units 1000A-1000D As a result, the reaction force increases to FAmax (a reaction force four times as large as that in the case of a single layer). Subsequently, when the rear part of the magnet passes through the gap, a reaction force of the same magnitude is generated in the opposite direction (position b in the figure). This variation in reaction force increases the required capacity of the outer rotor motor 350 that drives the magnetic units 2000A and 2000B. This is because the driving force of the outer rotor motor 350 must be at least the reaction force of FAmax or more. In addition, the reaction force fluctuation occurs every time the magnet passes between the heat transporters 50-1 and 50-2, and thus causes noise and vibration.

  If each heat transport unit 1000A-1000D is arranged with a phase difference in the stacking direction as in this embodiment, the same reaction as in the case of a single layer is shown as shown in the lower diagram of FIG. Although there is power, each reaction force is dispersed. Therefore, the magnetic units 2000A and 2000B can rotate relatively smoothly as compared with the case where there is no phase difference, and the driving force of the outer rotor motor 350 only needs to be larger than the reaction force generated in the case of a single layer. For this reason, it is not necessary to prepare an outer rotor motor 350 that is larger than necessary, and the magnetic air conditioner can be downsized. Further, noise and vibration are extremely reduced, and a magnetic air conditioner having quietness can be realized.

  In the present embodiment, the arrangement of the heat transport units 1000A-1000D has a phase difference, but the arrangement of the magnetic units 2000A-2000D may have a phase difference. Moreover, you may give a phase difference to arrangement | positioning of both heat transport unit 1000A-1000D and magnetic unit 2000A-2000D.

  As described above, according to the magnetic air conditioner according to the present invention, fluctuations in the driving force of the magnetic units 2000A,... Can be reduced, so that the motor for driving the magnetic air conditioner can be reduced in size. Therefore, the power consumption of the motor can be reduced. Therefore, the energy efficiency of the magnetic air conditioner can be increased, and the magnetic air conditioner can be reduced in noise and vibration.

  In the above embodiment, the thing which provided the magnetic permeability interruption | blocking part 60 between the heat transporter 50-1 and the heat transporter 50-2 was illustrated separately. Those provided with the magnetic permeability blocking part 60 (Embodiment 1) are arranged without changing the phase in the stacking direction, and those without the magnetic permeability blocking part 60 (Embodiment 2) are arranged with the phase changed in the stacking direction. . However, in addition to this, it is also possible to configure a configuration in which a magnetically permeable blocking part 60 is provided between the heat transporter 50-1 and the heat transporter 50-2 and the phase is changed in the stacking direction. In this case, the power consumption of the motor can be further reduced as compared with the case of the first and second embodiments.

10A-10F, 11A-11F magnetic material,
21A-21F, 22A-22F, 26A-26F, 27A-27F Permanent magnet,
30A-30G, 31A-31G heat conduction part,
40A low temperature side heat exchange section,
40B high temperature side heat exchange section,
50-1, 50-2 heat transporter,
60 permeability blocker,
1000A-1000D heat transport unit,
2000A, 2000B magnetic unit,
210, 215 fans,
250 reference position detection sensor,
350 outer rotor motor (motor),
310 rotor (rotating shaft),
450 Air conditioning control unit.

Claims (10)

A heat transport unit that arranges a plurality of heat transporters alternately arranged in parallel, with a heat transport unit that alternately arranges a magnetic body having a magnetocaloric effect and a heat conduction part that transports heat of the magnetic body, and
A magnetic unit that disposes a plurality of magnets that confront each magnetic body of the heat transport unit and selectively apply magnetism to each magnetic body; and
A motor that relatively moves at least one of the heat transport unit and the magnetic unit disposed to face each other in the direction in which the heat transporter is disposed,
Between the heat transporter and the heat transporter of the heat transport unit, the magnetic material has a magnetic permeability equivalent to that of the magnetic material, and a magnetically permeable heat insulating portion that blocks heat conduction is formed.
The magnetic air conditioner according to claim 1, wherein the magnets arranged in the magnetic unit are magnetized in directions opposite to each other.   A plurality of the heat transport units and the magnetic units are alternately stacked at intervals, and the motor is relatively and integrally formed by at least one of the plurality of stacked heat transport units and the plurality of stacked magnetic units. The magnetic air-conditioning apparatus according to claim 1, wherein In the magnetic unit, a first magnet facing one surface of each heat transport unit and a second magnet facing the other surface are separately arranged,
The magnetic air conditioner according to claim 2, wherein the magnetization directions of the first magnet and the second magnet arranged in the magnetic unit are the same.   The magnetic air-conditioning apparatus according to any one of claims 1 to 3, wherein the magnetically permeable heat insulating portion is formed so as to fill a gap between the magnetic bodies of adjacent heat transporters.   The said magnetic permeability heat insulation part mixes and forms metal powder with a large magnetic permeability to such an extent that the heat insulation property is not inhibited in the material provided with heat insulation, It forms in any one of Claim 1 to 4 characterized by the above-mentioned. Magnetic air conditioning unit. A heat transport unit in which a magnetic body having a magnetocaloric effect and a heat conduction unit that alternately transports heat of the magnetic body are arranged with a plurality of parallel air gaps, and a heat transport unit,
A plurality of magnet units arranged to confront each magnetic body of the heat transport unit and selectively apply magnetism to each magnetic body and remove the magnet, and
A magnetic air-conditioning / heating device in which the heat transport unit and the magnetic unit are alternately stacked at intervals.
Arrange at least a part of the heat transport unit with respect to the other heat transport units in the direction of arrangement of the heat transporter, or dispose at least a part of the magnetic units with respect to the other magnetic unit Place it in the direction
Magnetization directions of magnets arranged in the magnetic unit are opposite to each other between adjacent magnets,
At least one of the plurality of stacked heat transport units and magnetic units is integrally moved with a motor and relatively moved in the arrangement direction of the heat transporter ,
In the magnetic unit, a first magnet facing one surface of each heat transport unit and a second magnet facing the other surface are separately arranged,
The magnetic air conditioner characterized by the magnetization direction of the 1st magnet and 2nd magnet which are arrange | positioned at the said magnetic unit being the same . The heat transport unit and the magnetic unit are formed in a hollow circular shape, and at least one of the heat transport unit and the magnetic unit is rotatably supported and rotated by the motor,
A low-temperature side heat exchanging part disposed through the heat conducting part at one end of the heat transporter of the heat transporting unit;
A high temperature side heat exchanging part disposed through the heat conducting part at the other end of the heat transporter;
Further comprising
A fan that supplies a refrigerant to a refrigerant passage of the low-temperature side heat exchange unit or the high-temperature side heat exchange unit is provided on an inner peripheral portion or an outer peripheral portion of the rotating heat transport unit or the magnetic unit. The magnetic air conditioning apparatus in any one of Claim 1 to 6 . Arranging the high temperature side heat exchanging portion on the inner periphery of the heat transport unit and the magnetic unit,
The low temperature side heat exchange part is arranged on the outer peripheral part of the heat transport unit and the magnetic unit,
The refrigerant passage of the high temperature side heat exchanging portion has a cylindrical shape that communicates in the stacking direction of the heat transport unit and the magnetic unit, and the refrigerant passage of the low temperature side heat exchange portion is the outer peripheral portion of the heat transport unit or the heat transport. The magnetic air conditioner according to claim 7 , wherein the magnetic air conditioner has a shape in which refrigerant passages individually formed in outer peripheral portions of the unit and the magnetic unit are connected in series. The magnetic air conditioner according to any one of claims 1 to 8 , wherein the motor is an outer rotor motor whose rotor is a rotating shaft that integrally rotates the magnetic unit. The magnetic body having the magnetocaloric effect is a positive magnetic body that generates heat when heat is applied and absorbs heat, or a negative magnetic body that generates heat when heat is applied and removed. the magnetic air conditioner according to claim 1, characterized in that 9.