JP5729050B2 - Magnetic refrigerator and magnetic refrigeration method - Google Patents

Description

  The present invention relates to a magnetic refrigerator and a magnetic refrigeration method, and in particular, applies a magnetism to a plurality of magnetic bodies of the same type individually by a magnetic circuit to develop a magnetocaloric effect, and uses heat conduction of a solid substance. The present invention relates to a magnetic refrigerator and a magnetic refrigeration method for transporting heat.

  Most of the refrigerators in the room temperature range conventionally used, for example, refrigerators such as a refrigerator, a freezer, and an air conditioner, use the heat conduction of a gaseous refrigerant such as chlorofluorocarbon gas or chlorofluorocarbon alternative 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.

  For example, there exists a magnetic refrigerator as described in the following patent document 1 which transports heat using the heat conduction of a solid substance. This magnetic refrigerator conducts heat by the following configuration.

  Positive magnetic bodies that increase in temperature when magnetism is applied and negative magnetic bodies that decrease in temperature when magnetism is applied are alternately arranged at predetermined intervals. One magnetic body block is formed by a pair of positive and negative magnetic bodies. A plurality of magnetic blocks are arranged in a ring shape to form a magnetic unit. A heat conducting member inserted and removed between the positive and negative magnetic bodies arranged in the magnetic unit is arranged between the positive and negative magnetic bodies. A permanent magnet is arranged on a hub-like rotating body that is concentric with the magnetic body unit and has substantially the same inner diameter and outer shape to form a magnetic circuit. And the rotary body in which the permanent magnet is arrange | positioned is arrange | positioned so as to oppose a magnetic body unit, and it rotates relatively with respect to a magnetic body unit. By the rotation of the rotating body, magnetism is simultaneously applied to and removed from the positive and negative magnetic bodies. Along with the rotation of the rotating body, the heat conducting member is inserted and removed between the positive and negative magnetic bodies at a constant timing. The heat generated by the magnetic body due to the magnetocaloric effect is transported in one direction in which the magnetic body is disposed via the heat conducting member.

JP 2007-147209 A

  However, in the case of a magnetic refrigerator that transports heat using the heat conduction of a solid material as in the invention of Cited Document 1, it is necessary to use two different magnetic materials, positive and negative, as magnetic materials that exhibit a magnetocaloric effect. is there. In addition, a magnetic circuit is required for applying and removing magnetism simultaneously to two positive and negative magnetic bodies.

  In general, the magnitude of the magnetocaloric effect between the positive magnetic material and the negative magnetic material is different. Specifically, the magnetocaloric effect of the negative magnetic material is smaller than the magnetocaloric effect of the positive magnetic material. For this reason, in the case of a magnetic refrigerator using two different positive and negative magnetic bodies, a uniform magnetocaloric effect cannot be obtained, so that the heat transport efficiency of the entire magnetic refrigerator is inferior. If a uniform magnetocaloric effect can be obtained, the heat transport efficiency can be increased, so there is room for improvement in this respect. In addition, since the negative magnetic material is rarer than the positive magnetic material, the magnetic refrigerator is expensive.

  Furthermore, since the magnetic circuit that applies and removes magnetism to the two positive and negative magnetic bodies simultaneously becomes large, it becomes a heavy and large magnetic refrigerator. If the weight of the magnetic circuit can be reduced, the magnetic refrigerator can be reduced in size, weight and cost, so there is room for improvement in this respect.

  The present invention has been made to solve the above-described problems, and provides a magnetic refrigerator and a magnetic refrigeration method that can improve heat transport capability and heat transport efficiency, and can be reduced in size, weight, and cost. With the goal.

  In order to achieve the above object, a magnetic refrigerator according to the present invention includes a magnetic body unit, a low temperature side heat exchange unit, a high temperature side heat exchange unit, a heat conduction unit, a magnetic application unit, and a control unit.

In the magnetic unit, three or more magnetic bodies having the same type of magnetocaloric effect to be expressed are arranged at intervals in a row. The low temperature side heat exchange part is adjacent to the magnetic body located at one end of the magnetic body unit with a gap, and the high temperature side heat exchange part is adjacent to the magnetic body located at the other end of the magnetic body unit. . The heat conduction part is heat conduction between adjacent magnetic bodies in the magnetic body unit, or between the magnetic body located at one end of the magnetic body unit and the low temperature side heat exchange section and at the other end of the magnetic body unit. Any one of the heat conduction between the magnetic body located and the high-temperature side heat exchanging portion is alternately performed via the solid heat conduction member. The magnetism applying unit alternately applies magnetism to either the magnetic body located at one end of the magnetic body unit or the magnetic body located at the other end of the magnetic body unit. The control unit controls the operation of the heat conduction unit and the magnetic application unit, and when the magnetic application unit applies magnetism to the magnetic body located at one end of the magnetic unit, the heat conduction unit is in the magnetic unit. Heat is conducted between adjacent magnetic materials. On the other hand, when the magnetism applying unit applies magnetism to the magnetic body located at the other end of the magnetic unit, the heat conducting unit is located at both ends of the magnetic unit, the low temperature side heat exchange unit, and the high temperature side heat exchange. Heat is transferred between parts.

  In order to achieve the above object, another magnetic refrigerator according to the present invention includes a magnetic body unit, a low temperature side heat exchange section, a high temperature side heat exchange section, a heat conduction section, a magnetic application section, and a control section.

In the magnetic body unit, magnetic blocks in which three or more magnetic bodies having the same type of magnetocaloric effect to be expressed are arranged at intervals in a row are arranged in a plurality of rows at intervals. The low temperature side heat exchange part is adjacent to the magnetic body located at one end of the magnetic body unit with a gap, and the high temperature side heat exchange part is adjacent to the magnetic body located at the other end of the magnetic body unit. . The heat conduction part is a heat conduction between adjacent magnetic bodies in the magnetic body block, or between the adjacent magnetic body of the adjacent magnetic body block and at one end of the magnetic body unit and the low temperature side. The heat conduction between the heat exchange part and the heat conduction between the magnetic body located at the other end of the magnetic body unit and the high temperature side heat exchange part is alternately performed via the solid heat conduction member. The magnetism application unit alternately applies magnetism to either the magnetic body located at one end of the magnetic body block or the magnetic body located at the other end of the magnetic body block for each magnetic body block. To do. The control unit controls the operation of the heat conduction unit and the magnetic application unit, and when the magnetic application unit applies magnetism to the magnetic body located at one end of the magnetic body block, the heat conduction unit is in the magnetic body block. Heat is conducted between adjacent magnetic materials. On the other hand, when the magnetism applying unit applies magnetism to the magnetic body located at the other end of the magnetic body block, the heat conducting section conducts heat between the adjacent magnetic bodies of the adjacent magnetic body blocks and the magnetic body. Heat is conducted between the magnetic body located at both ends of the unit, the low temperature side heat exchange section, and the high temperature side heat exchange section.

  In order to achieve the above object, the magnetic refrigeration method according to the present invention includes the first to fourth steps.

In the first step, magnetism is applied to a magnetic body located at one end of a magnetic body unit in which three or more magnetic bodies having the same type of magnetocaloric effect are arranged at intervals, and the other end The magnetism is removed from the magnetic body located in the position. In the second step, heat is conducted between adjacent magnetic bodies in the magnetic unit via a solid heat conducting member. In the third step, the magnetism is removed from the magnetic body located at one end of the magnetic unit and magnetism is applied to the magnetic body located at the other end. In the fourth step, between the magnetic body located at one end of the magnetic body unit via the solid heat conducting member and the adjacent low-temperature side heat exchanging portion with an interval with respect to the magnetic body, and the other of the magnetic body unit Heat is conducted between the magnetic body located at the end and the adjacent high-temperature side heat exchanging section with an interval from the magnetic body. Then, heat is transported from the low temperature side heat exchanging portion to the high temperature side heat exchanging portion by repeating the first step to the fourth step.

  In order to achieve the above object, another magnetic refrigeration method according to the present invention includes the first to fourth steps.

In the first step, a magnetic unit in which three or more magnetic bodies having the same type of magnetocaloric effect to be expressed are arranged in rows and arranged in rows, and further arranged in a plurality of rows at intervals Is used. First, magnetism is applied to the magnetic body located at one end of each magnetic block, and the magnetism is removed from the magnetic body located at the other end. In the second step, heat is conducted between adjacent magnetic bodies in each magnetic block via a solid heat conductive member. In the third step, magnetism is removed from the magnetic body located at one end of each magnetic body block, and magnetism is applied to the magnetic body located at the other end. In the fourth step, the magnetic body located at one end of the magnetic unit and the magnetic body are adjacent to each other with an interval between the adjacent magnetic bodies of the adjacent magnetic body blocks via the solid heat conducting member. Heat is conducted between the matching low temperature side heat exchanging unit and between the magnetic body located at the other end of the magnetic unit and the adjacent high temperature side heat exchanging unit with an interval. Then, heat is transported from the low temperature side heat exchanging portion to the high temperature side heat exchanging portion by repeating the first step to the fourth step.

  According to the magnetic refrigerator and the magnetic refrigeration method according to the present invention configured as described above, the magnetism applying unit individually applies magnetism to a plurality of magnetic bodies having the same type of magnetocaloric effect to be expressed. Since the effect is expressed and the heat is transported using the solid heat conduction, the heat transport capability and the heat transport efficiency are improved, and the miniaturization, weight reduction, and cost reduction can be realized.

It is a principle figure of the magnetic refrigeration in the case of forming a magnetic unit with two magnetic bodies. It is a graph which shows the effect of magnetic refrigeration of the present invention. It is a principle figure of magnetic refrigeration in the case of forming a magnetic unit with three magnetic bodies. FIG. 4 is a principle diagram of magnetic refrigeration in the case where one magnetic block is formed by two magnetic bodies and one magnetic unit is formed by three magnetic blocks. FIG. 5 is a schematic diagram for explaining how heat moves when a magnetic circuit provided in each magnetic block is reciprocated in the left-right direction as shown in FIG. 4. It is a principle diagram of magnetic refrigeration in the case where one magnetic body block is formed by three magnetic bodies and one magnetic body unit is formed by two magnetic body blocks. FIG. 7 is a schematic diagram for explaining how heat moves when a magnetic circuit provided in each magnetic block is reciprocated in the left-right direction in the drawing as shown in FIG. 6. It is a top view which shows schematic structure of the magnetic refrigerator based on Embodiment 1. FIG. It is a front view of the magnetic refrigerator shown in FIG. It is a side view of the magnetic refrigerator shown in FIG. It is a top view which shows schematic structure of the heat transfer mechanism which manages heat transfer of the magnetic refrigerator shown in FIG. It is a front view of the heat transfer mechanism shown in FIG. It is a side view of the heat transfer mechanism shown in FIG. It is a top view which shows schematic structure of the drive mechanism which drives the magnetic application part of the magnetic refrigerator shown in FIG. It is a front view of the drive mechanism shown in FIG. It is a side view of the drive mechanism shown in FIG. 17 is an operation flowchart of the magnetic refrigerator shown in FIGS. 8 to 16. It is a figure where it uses for description of the operating temperature of a magnetic body. It is a figure which shows schematic structure of the magnetic refrigerator based on Embodiment 2. FIG. It is a figure which shows schematic structure of the magnetic refrigerator which concerns on Embodiment 3. FIG.

Embodiments of a magnetic refrigerator and a magnetic refrigeration method according to the present invention will be described below. First, the principle of magnetic refrigeration applied to the present invention will be described in detail with reference to the drawings.
(Principle of magnetic refrigeration)
<When a magnetic unit is formed of two magnetic bodies>
FIG. 1 is a principle diagram of magnetic refrigeration when a magnetic unit is formed of two magnetic bodies.

  In this case, the magnetic refrigeration uses a plurality of magnetic bodies 10A and 10B having the same type of magnetocaloric effect, and the magnetic circuits 20A and 20B individually apply magnetism to the magnetic bodies 10A and 10B. There are characteristics in three points, that is, heat is conducted by the solid heat conducting members 30A, 30B, and 30C.

  Here, for the magnetic bodies 10A and 10B having the same type of magnetocaloric effect, a positive magnetic body that generates heat when heat is applied by the magnetic circuits 20A and 20B and absorbs heat when removed is used, or the magnetic circuit 20A. 20B, only one of the negative magnetic materials that absorbs heat when it is applied and generates heat when it is removed is used. A positive magnetic body and a negative magnetic body have opposite magneto-caloric effects, and the types of magneto-caloric effects are different. In the case of FIG. 1, a positive magnetic material that is less expensive than a negative magnetic material is used. This is because a negative magnetic material has to be manufactured from a rare magnetic material, which increases the cost, and the magnitude of the magnetocaloric effect of the negative magnetic material is smaller than that of the positive magnetic material. . In the case of FIG. 1, the magnetic body unit 200 is formed of two magnetic bodies, that is, the magnetic bodies 10A and 10B.

  The magnetic circuits 20A and 20B are provided with permanent magnets (not shown). The magnetic circuits 20A and 20B are integrated to reciprocate in the horizontal direction in the figure, thereby applying magnetism individually to the magnetic body 10A or the magnetic body 10B.

  The heat conducting members 30A, 30B, and 30C conduct the heat generated by the magnetic bodies 10A and 10B due to the magnetocaloric effect from the low temperature side heat exchange unit 40A to the high temperature side heat exchange unit 40B. The heat conducting member 30B is inserted and removed between the magnetic bodies 10A and 10B to mechanically connect the two. On the other hand, the heat conducting member 30A is inserted and removed between the low temperature side heat exchanging portion 40A and the adjacent magnetic body 10A to mechanically connect them. Similarly, the heat conducting member 30C is inserted and removed between the high temperature side heat exchanging portion 40B and the adjacent magnetic body 10B to mechanically connect the two. The heat conducting members 30A and 30C are inserted and removed at the same timing between the magnetic body 10A and the low temperature side heat exchange unit 40A, and between the magnetic body 10B and the high temperature side heat exchange unit 40B.

  As shown in FIG. 1A, when the magnetic circuits 20A and 20B are positioned on the magnetic body 10A, magnetism is applied to the magnetic body 10A, and no magnetism is applied to the magnetic body 10B and the magnetism is removed. . At this time, the magnetic body 10A generates heat and the magnetic body 10B absorbs heat. At the same time, the heat conducting member 30B is inserted between the magnetic bodies 10A and 10B to conduct heat conduction between the two magnetic bodies. That is, the heat generated by the magnetic body 10A due to the magnetocaloric effect is transferred to the magnetic body 10B. At this time, the heat conducting members 30A and 30C are not inserted between the low temperature side heat exchange unit 40A and the magnetic body 10A and between the high temperature side heat exchange unit 40B and the magnetic body 10B.

  On the other hand, as shown in FIG. 1B, when the magnetic circuits 20A and 20B move from the position of the magnetic body 10A and are positioned on the magnetic body 10B, magnetism is applied to the magnetic body 10B, and magnetism is generated from the magnetic body 10A. Removed. At this time, the magnetic body 10B generates heat and the magnetic body 10A absorbs heat. At the same time, the heat conducting members 30A and 30C are inserted between the low temperature side heat exchanging portion 40A and the magnetic body 10A and between the high temperature side heat exchanging portion 40B and the magnetic body 10B to conduct heat conduction therebetween. . That is, since the magnetic body 10A absorbs heat due to the magnetocaloric effect, heat is transferred from the low temperature side heat exchange part 40A to the magnetic body 10A, and the magnetic body 10B generates heat due to the magnetocaloric effect, so that the magnetic body 10B generates heat from the high temperature side heat exchange part. Heat moves to 40B. At this time, the heat conducting member 30B is not inserted between the magnetic bodies 10A and 10B.

  As described above, the magnetic circuits 20A and 20B are reciprocated in the left-right direction in the figure, and the application and removal of magnetism are repeated alternately on the magnetic bodies 10A and 10B. Furthermore, by interlocking with this reciprocating motion, by repeatedly inserting and removing between the heat conduction members 30A, 30B, 30C between the low temperature side heat exchange part 40A, the magnetic bodies 10A, 10B, and the high temperature side heat exchange part 40B, The heat obtained by the magnetocaloric effect moves from the low temperature side heat exchange unit 40A to the high temperature side heat exchange unit 40B.

  FIG. 2 is a graph showing the effect of the magnetic refrigeration of the present invention. As shown in this graph, the temperature difference between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B is small at a relatively initial time after the operation of the magnetic refrigerator. As time passes, the temperature difference between the low temperature side heat exchange section 40A and the high temperature side heat exchange section 40B gradually increases, and finally, as shown by the straight line after a long time has passed, The temperature difference between the heat exchange unit 40A and the high temperature side heat exchange unit 40B is maximized. In this state, for example, the indoor temperature can be lowered using the heat of the low temperature side heat exchange unit 40A, and the indoor temperature can be increased, for example, using the heat of the high temperature side heat exchange unit 40B.

  As described above, when a magnetic body unit is formed by two magnetic bodies, magnetic refrigeration can be performed with a minimum number of magnetic bodies and magnetic circuits. Therefore, the magnetic refrigerator can be reduced in size, weight, and cost.

<When a magnetic unit is formed of three magnetic bodies>
FIG. 3 is a principle diagram of magnetic refrigeration when a magnetic unit is formed of three magnetic bodies.

  In this case, the magnetic refrigeration uses a plurality of magnetic bodies 10A, 10B, and 10C that have the same type of magnetocaloric effect. The magnetic circuits 20A and 20B individually apply magnetism to the magnetic bodies 10A and 10C. There are characteristics in three points, that is, heat is conducted by the solid heat conducting members 30A, 30B, 30C, and 30D.

  When the magnetic body unit 200 is formed by three magnetic bodies, the magnetic body 10B located in the middle of the magnetic body unit simply acts as a heat accumulator for conducting heat to the adjacent magnetic body 10C and holding the heat. In the case of FIG. 3 as well, the magnetic bodies 10A, 10B, and 10C are arranged in a row at intervals, and positive magnetic bodies are used for these magnetic bodies. The configurations of the heat conducting members 30A, 30B, 30C, and 30D, the low temperature side heat exchange unit 40A, and the high temperature side heat exchange unit 40B are the same as those in FIG.

  When a magnetic unit is formed by three magnetic bodies, the magnetic circuits 20A and 20B are integrated and reciprocate in the left-right direction in the figure, and magnetism is individually applied to the magnetic body 10A or the magnetic body 10C. Therefore, the magnetic circuits 20A and 20B pass through the magnetic body 10B without stopping. That is, the magnetic circuits 20A and 20B alternately apply magnetism to either the magnetic body 10A located at one end of the magnetic body unit 200 or the magnetic body 10C located at the other end of the magnetic body unit 200. .

  The heat conducting members 30A, 30B, 30C, and 30D conduct the heat generated by the magnetic bodies 10A and 10C due to the magnetocaloric effect from the low temperature side heat exchange unit 40A toward the high temperature side heat exchange unit 40B. The heat conducting members 30B and 30C are inserted and removed between the magnetic bodies 10A, 10B, and 10C and mechanically connect them. On the other hand, the heat conducting member 30A is inserted and removed between the low temperature side heat exchanging portion 40A and the adjacent magnetic body 10A to mechanically connect them. Similarly, the heat conducting member 30D is inserted and removed between the high temperature side heat exchanging portion 40B and the adjacent magnetic body 10C to mechanically connect the two. The heat conducting members 30B and 30C are inserted / removed between the magnetic bodies 10A, 10B, and 10C at the same timing, and the heat conducting members 30A and 30D are magnetic between the magnetic body 10A and the low temperature side heat exchanging portion 40A. It is inserted and removed at the same timing between the body 10C and the high temperature side heat exchange part 40B.

  As shown in FIG. 3A, when the magnetic circuits 20A and 20B are positioned on the magnetic body 10A, magnetism is applied to the magnetic body 10A, and no magnetism is applied to the magnetic bodies 10B and 10C, and the magnetism is removed. ing. At this time, the magnetic body 10A generates heat and the magnetic body 10C absorbs heat. At the same time, the heat conducting members 30B and 30C are inserted between the magnetic bodies 10A and 10B and between the magnetic bodies 10B and 10C, and heat is transferred between the magnetic bodies. That is, heat conduction is performed between adjacent magnetic bodies 10A, 10B, and 10C in the magnetic body unit 200. Thereby, the heat generated by the magnetic body 10A due to the magnetocaloric effect is transferred to the magnetic body 10B, and further, the heat is transferred from the magnetic body 10B to 10C. At this time, the heat conducting members 30A and 30D are not inserted between the low temperature side heat exchange unit 40A and the magnetic body 10A and between the high temperature side heat exchange unit 40B and the magnetic body 10C.

  On the other hand, as shown in FIG. 3B, when the magnetic circuits 20A and 20B move from the position of the magnetic body 10A and are positioned on the magnetic body 10C, magnetism is applied to the magnetic body 10C, and magnetism is generated from the magnetic body 10A. Removed. At this time, the magnetic body 10C generates heat and the magnetic body 10A absorbs heat. The magnetic circuits 20A and 20B pass through the magnetic body 10B while moving from the position of the magnetic body 10A to the position of the magnetic body 10C. At this time, the magnetic body 10B generates heat and endotherm in an instant, but since the temperature changes of the heat generation and endotherm are the same, the temperature of the magnetic body 10B remains the original temperature.

  Simultaneously with the heat generation of the magnetic body 10C, the heat conducting members 30A and 30D are inserted between the low temperature side heat exchange section 40A and the magnetic body 10A and between the high temperature side heat exchange section 40B and the magnetic body 10C. Heat conduction takes place. That is, heat between the magnetic body 10A located at one end of the magnetic body unit 200 and the low temperature side heat exchange unit 40A and between the magnetic body 10C located at the other end of the magnetic body unit 200 and the high temperature side heat exchange unit 40B. Conduction takes place. Since the magnetic body 10A absorbs heat due to the magnetocaloric effect, heat is transferred from the low temperature side heat exchange part 40A to the magnetic body 10A, and the magnetic body 10C generates heat due to the magnetocaloric effect, so that the magnetic body 10C changes to the high temperature side heat exchange part 40B. Heat moves. At this time, the heat conducting members 30B, 30C are not inserted between the magnetic bodies 10A, 10B, 10C.

  As described above, the magnetic circuits 20A and 20B are reciprocated in the left-right direction in the figure, and the application and removal of magnetism are repeated alternately on the magnetic bodies 10A and 10C. Further, in conjunction with this reciprocation, the heat conducting members 30A, 30B, 30C, 30D are inserted into and removed from the low temperature side heat exchange unit 40A, the magnetic bodies 10A, 10B, 10C, and the high temperature side heat exchange unit 40B. By repeating, the heat obtained by the magnetocaloric effect moves from the low temperature side heat exchange unit 40A to the high temperature side heat exchange unit 40B. As a result, as shown in the graph of FIG. 2, the temperature difference between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B increases as time elapses. The temperature difference between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B becomes constant.

  As described above, when a magnetic body unit is formed of three magnetic bodies, one magnetic body can act as a heat accumulator. For this reason, the heat transport capability of the magnetic refrigerator can be improved. Moreover, magnetic refrigeration can be performed with a small number of magnetic bodies and magnetic circuits. Therefore, the magnetic refrigerator can be reduced in size, weight, and cost.

  In addition, as described above, when the magnetic unit is formed of two or three magnetic bodies, the magnetic refrigerator can be reduced in size, weight, and cost.

<When a magnetic unit is formed with three magnetic blocks (two magnetic bodies)>
FIG. 4 is a principle diagram of magnetic refrigeration in the case where one magnetic body block is formed by two magnetic bodies and one magnetic body unit is formed by three magnetic body blocks.

  The magnetic refrigeration in this case is characterized in that all the magnetic bodies forming the magnetic body unit 200 use the same type of magnetocaloric effect that is expressed. Further, the magnetic circuits 20A and 20B have the magnetic bodies 10A and 10B of the magnetic body block 100A, the magnetic circuits 20C and 20D have the magnetic bodies 10C and 10D, and the magnetic circuits 20E and 20F have the magnetic body 100C magnetic. It is characterized in that magnetism is individually applied to the bodies 10E and 10F. Moreover, the heat conduction member 30A-30G is characterized in that heat is conducted.

  In the case of FIG. 4, the configuration of each of the magnetic blocks 100A, 100B, and 100C is the same as that in FIG. 1 differs from the case of FIG. 1 in that each magnetic circuit arranged in each magnetic block can reciprocate in conjunction with the horizontal direction in the figure, and heat conduction is performed between the magnetic blocks. This is the point.

  As shown in FIG. 4A, the magnetic circuits 20A and 20B are the magnetic body 10A of the magnetic block 100A, the magnetic circuits 20C and 20D are the magnetic body 10C of the magnetic block 100B, and the magnetic circuits 20E and 20F are the magnetic body 10E of the magnetic block 100C. Respectively. At this time, magnetism is applied to the magnetic bodies 10A, 10C, and 10E, and no magnetism is applied to the magnetic bodies 10B, 10D, and 10F, and the magnetism is removed. At this time, the magnetic bodies 10A, 10C, and 10E generate heat. At the same time, the heat conducting member 30B is inserted between the magnetic bodies 10A and 10B, the heat conducting member 30D is inserted between the magnetic bodies 10C and 10D, and the heat conducting member 30F is inserted between the magnetic bodies 10E and 10F. Is done. For this reason, heat conduction is performed between adjacent magnetic bodies in each magnetic body block. That is, the heat generated by the magnetic bodies 10A, 10C, and 10E due to the magnetocaloric effect is transferred to the magnetic bodies 10B, 10D, and 10F, respectively. At this time, the heat conducting members 30A and 30G are not inserted between the low temperature side heat exchange unit 40A and the magnetic body 10A and between the high temperature side heat exchange unit 40B and the magnetic body 10F. Further, the heat conducting members 30C and 30E that conduct heat between the blocks are not inserted between the magnetic bodies 10B and 10C and between the magnetic bodies 10D and 10E.

  Next, as shown in FIG. 4B, the magnetic circuits 20A and 20B are the magnetic body 10B of the magnetic block 100A, the magnetic circuits 20C and 20D are the magnetic body 10D of the magnetic block 100B, and the magnetic circuits 20E and 20F are the magnetic block 100C. It is located on each of the magnetic bodies 10F. At this time, magnetism is applied to the magnetic bodies 10B, 10D, and 10F, and no magnetism is applied to the magnetic bodies 10A, 10C, and 10E, and the magnetism is removed. At this time, the magnetic bodies 10B, 10D, and 10F generate heat. At the same time, the heat conducting members 30A and 30G are inserted between the low temperature side heat exchanging portion 40A and the magnetic body 10A and between the high temperature side heat exchanging portion 40B and the magnetic body 10F to conduct heat conduction therebetween. . In addition, the heat conducting member 30C is inserted between the magnetic bodies 10B and 10C, and the heat conducting member 30E is inserted between the magnetic bodies 10D and 10E, respectively. Heat conduction is performed. That is, the magnetic bodies 10A, 10C, and 10E absorb heat by the magnetocaloric effect, and the magnetic bodies 10B, 10D, and 10F generate heat by the magnetocaloric effect. For this reason, heat moves from the low temperature side heat exchange section 40A to the magnetic body 10A, from the magnetic body 10B to the magnetic body 10C, from the magnetic body 10D to the magnetic body 10E, and from the magnetic body 10F to the high temperature side heat exchange section 40B. At this time, the heat conducting members 30B, 30D, and 30F are not inserted between the magnetic bodies in the magnetic block.

  As described above, the magnetic circuit provided in each magnetic block 100A-100C is reciprocated in the left-right direction in the figure to alternately apply and remove magnetism to the magnetic bodies located at both ends of each magnetic block 100A-100C. repeat. Further, in conjunction with this reciprocating motion, the insertion / removal of the heat conducting members 30A-30G between the low temperature side heat exchange part 40A, the magnetic bodies 10A-10F, and the high temperature side heat exchange part 40B is repeated. Thereby, the heat obtained by the magnetocaloric effect moves from the low temperature side heat exchange unit 40A to the high temperature side heat exchange unit 40B. As a result, as shown in the graph of FIG. 2, the temperature difference between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B increases as time elapses. Eventually, the temperature difference between the low temperature side heat exchange part 40A and the high temperature side heat exchange part 40B becomes constant.

  Next, referring to the schematic diagram of FIG. 5, a description will be given of how heat moves when the magnetic circuit provided in each magnetic block is reciprocated in conjunction with the horizontal direction in the figure as shown in FIG.

  First, it is assumed that all the magnetic bodies forming the magnetic body unit 200 have the same magnetocaloric effect and have a temperature change amount of 5 ° C. Specifically, it is assumed that the temperature of 5 ° C. rises when magnetism is applied to all the magnetic materials, and the temperature decreases by 5 ° C. when the magnetism is removed.

  First, as shown in (1) of FIG. 5, in the initial state, all the magnetic bodies are at room temperature of 20 ° C.

  Next, as shown in FIG. 5 (2), in this state, the magnetic circuit is moved to the right, the magnetism is removed from the magnetic body located at one end of each magnetic block 100A-100C, and the magnetic circuit is located at the other end. Magnetism is applied to the magnetic material. At the same time, between the adjacent magnetic bodies of the adjacent magnetic body blocks 100A to 100C, between the magnetic body positioned at one end of the magnetic body unit 200 and the low temperature side heat exchange unit 40A, and the other end of the magnetic body unit 200. A heat conducting member is inserted so that heat conduction between the magnetic body located at the high temperature side and the high temperature side heat exchanging portion 40B is possible.

  In the state of (2) in FIG. 5, the temperature of the magnetic body from which magnetism has been removed decreases to 15 ° C., and the temperature of the magnetic body to which magnetism has been applied increases to 25 ° C. For this reason, as shown in the figure, heat moves from the higher temperature side to the lower temperature side through the heat conducting member.

  Due to this heat transfer, the temperature of the magnetic body located at one end of the magnetic body unit 200 and the low temperature side heat exchanging section 40A becomes 18 ° C. as shown in FIG. The temperature of the magnetic body located at the end and the high temperature side heat exchange section 40B becomes 22 ° C.

  Next, as shown in FIG. 5 (3), in this state, the magnetic circuit is moved to the left side to remove the magnetism from the magnetic body located at the other end of each magnetic block 100A-100C, and the magnet located at one end. Apply magnetism to the body. At the same time, a heat conducting member is inserted so that heat conduction between adjacent magnetic bodies in each magnetic body block 100A-100C is possible.

  In the state of (3) of FIG. 5, the temperature of the magnetic body to which magnetism is applied rises to 5 ° C. from the temperature of the state of (2) ′ of FIG. The temperature is lowered by 5 ° C. from the temperature in the state (2) ′. For this reason, as shown in the figure, in each of the magnetic body blocks 100A to 100C, heat moves from the higher temperature to the lower temperature through the heat conducting member.

  Due to this heat transfer, the temperature of the low temperature side heat exchanging portion 40A becomes 18 ° C. and the temperature of the magnetic body of the magnetic block 100A becomes 19 ° C. as shown in FIG. Further, the temperature of the magnetic body of the magnetic block 100B is 20 ° C., and the temperature of the magnetic body of the magnetic block 100C is 21 ° C. And the temperature of the high temperature side heat exchange part 40B will be 22 degreeC.

  As described above, by reciprocating the magnetic circuit in the left-right direction in the drawing, and inserting and removing the heat conducting member in synchronization with this reciprocating movement, heat is transferred from the low temperature side heat exchange unit 40A to the high temperature side heat exchange unit 40B. Move. As time elapses, the temperature difference between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B increases. Eventually, the temperature difference between the low temperature side heat exchange part 40A and the high temperature side heat exchange part 40B becomes constant. In this state, for example, the indoor temperature can be lowered using the heat of the low temperature side heat exchange unit 40A, and the indoor temperature can be increased, for example, using the heat of the high temperature side heat exchange unit 40B.

  As described above, when a magnetic unit is formed by three magnetic blocks (two magnetic bodies), a plurality of magnetic blocks and magnetic circuits are connected in series. For this reason, the heat transport capability of the magnetic refrigerator can be improved, and a large temperature difference can be obtained between the low temperature side heat exchange part and the high temperature side heat exchange part. Therefore, the heat transport capacity and heat transport efficiency of the magnetic refrigerator can be improved. In addition, the magnetic refrigerator can be reduced in size, weight, and cost.

<When a magnetic unit is formed with two magnetic blocks (three magnetic bodies)>
FIG. 6 is a principle diagram of magnetic refrigeration in the case where one magnetic block is formed by three magnetic bodies and one magnetic unit is formed by two magnetic blocks.

  The magnetic refrigeration in this case is characterized in that all of the magnetic bodies forming the magnetic unit use the same type of magnetocaloric effect. Further, the magnetic circuits 20A and 20B individually apply magnetism to the magnetic bodies 10A and 10C of the magnetic body block 100A, and the magnetic circuits 20C and 20D individually apply magnetism to the magnetic bodies 10D and 10F of the magnetic body block 100B. There is. Moreover, the heat conduction member 30A-30G is characterized in that heat is conducted.

  In the case of FIG. 6, the configuration of the magnetic blocks 100A and 100B is the same as that of FIG. 3 is different from the case of FIG. 3 in that each magnetic circuit arranged in each magnetic block can reciprocate in conjunction with the horizontal direction in the figure, and heat conduction is performed between the magnetic blocks. This is the point.

  When the magnetic blocks 100A and 100B are formed by three magnetic bodies, the heat storage for the magnetic bodies 10B and 10E located in the middle of the magnetic blocks 100A and 100B to simply conduct heat to the adjacent magnetic bodies and hold the heat. Acts as a vessel. Accordingly, each magnetic circuit passes through the magnetic bodies other than the magnetic bodies located at both ends of the magnetic blocks 100A and 100B without stopping.

  As shown in FIG. 6A, the magnetic circuits 20A and 20B are located in the magnetic body 10A of the magnetic block 100A, and the magnetic circuits 20C and 20D are located in the magnetic body 10D of the magnetic block 100B. At this time, magnetism is applied to the magnetic bodies 10A and 10D, and no magnetism is applied to the magnetic bodies 10B, 10C, 10E, and 10F, and the magnetism is removed. At this time, the magnetic bodies 10A and 10D generate heat. At the same time, the heat conduction member 30B is between the magnetic bodies 10A and 10B, the heat conduction member 30C is between the magnetic bodies 10B and 10C, and the heat conduction member 30E is between the magnetic bodies 10D and 10E. The members 30F are respectively inserted between the magnetic bodies 10E and 10F. Thereby, heat conduction is performed between adjacent magnetic bodies in each magnetic body block. That is, the heat generated by the magnetic bodies 10A and 10D due to the magnetocaloric effect is transferred to the magnetic bodies 10B and 10C and the magnetic bodies 10E and 10F, respectively. At this time, the heat conducting members 30A and 30G are not inserted between the low temperature side heat exchange unit 40A and the magnetic body 10A and between the high temperature side heat exchange unit 40B and the magnetic body 10F. Further, the heat conducting member 30D that conducts heat between the blocks is not inserted between the magnetic bodies 10C and 10D.

  Next, as shown in FIG. 6B, the magnetic circuits 20A and 20B are positioned on the magnetic body 10C of the magnetic block 100A, and the magnetic circuits 20C and 20D are positioned on the magnetic body 10F of the magnetic block 100B. At this time, magnetism is applied to the magnetic bodies 10C and 10F, and no magnetism is applied to the magnetic bodies 10A, 10B, 10D, and 10E, and the magnetism is removed. At this time, the magnetic bodies 10C and 10F generate heat. The magnetic circuits 20A and 20B pass through the magnetic body 10B while moving from the position of the magnetic body 10A to the position of the magnetic body 10C, and the magnetic circuits 20C and 20D move from the position of the magnetic body 10D to the position of the magnetic body 10F. The magnetic body 10E is passed through during the movement. At this time, the magnetic body 10B and the magnetic body 10E generate heat and endotherm in an instant, but since the temperature changes of the heat generation and endotherm are the same, the temperatures of the magnetic body 10B and the magnetic body 10E remain at their original temperatures. Simultaneously with the heat generation of the magnetic bodies 10C and 10F, the heat conducting members 30A and 30G are inserted between the low temperature side heat exchange section 40A and the magnetic body 10A and between the high temperature side heat exchange section 40B and the magnetic body 10F, respectively. Heat conduction takes place between the two. Further, the heat conducting member 30D is inserted between the magnetic bodies 10C and 10D, and heat conduction is performed between the adjacent magnetic bodies of the adjacent magnetic body blocks. That is, the magnetic bodies 10A and 10D are absorbed by the magnetocaloric effect, and the magnetic bodies 10C and 10F generate heat by the magnetocaloric effect, so that the low temperature side heat exchange section 40A changes from the magnetic body 10C to the magnetic body 10D. Heat moves from the magnetic body 10F to the high temperature side heat exchange section 40B. At this time, the heat conducting members 30B, 30C, 30E, and 30F are not inserted between the magnetic bodies in the magnetic block.

  As described above, the magnetic circuit provided in each of the magnetic blocks 100A and 100B is reciprocated in conjunction with the horizontal direction in the figure to alternately apply and remove magnetism to the magnetic bodies located at both ends of each of the magnetic blocks 100A and 100B. repeat. In conjunction with this reciprocating motion, the insertion / removal of the heat conducting members 30A-30G between the low temperature side heat exchange part 40A, the magnetic bodies 10A-10F, and the high temperature side heat exchange part 40B is repeated. Thereby, the heat obtained by the magnetocaloric effect moves from the low temperature side heat exchange unit 40A to the high temperature side heat exchange unit 40B. As a result, as shown in the graph of FIG. 2, the temperature difference between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B increases as time elapses. Eventually, the temperature difference between the low temperature side heat exchange part 40A and the high temperature side heat exchange part 40B becomes constant.

  Next, a state in which heat moves when the magnetic circuit provided in each magnetic block as shown in FIG. 6 is reciprocated in the left-right direction in the figure will be described based on the schematic diagram of FIG.

  First, it is assumed that all the magnetic bodies forming the magnetic body unit 200 have the same magnetocaloric effect and have a temperature change amount of 5 ° C. Specifically, it is assumed that the temperature of 5 ° C. rises when magnetism is applied to all the magnetic materials, and the temperature decreases by 5 ° C. when the magnetism is removed.

  First, as shown in (1) of FIG. 7, in the initial state, all the magnetic bodies are at room temperature of 20 ° C.

  Next, as shown in FIG. 7 (2), the magnetic circuit is moved to the right in this state, the magnetism is removed from the magnetic body located at one end of each magnetic block 100A, 100B, and the other is located at the other end. Magnetism is applied to the magnetic material. At the same time, between the adjacent magnetic bodies of the adjacent magnetic body blocks 100A and 100B, between the magnetic body positioned at one end of the magnetic body unit 200 and the low-temperature side heat exchange unit 40A, and the other end of the magnetic body unit 200. A heat conducting member is inserted so that heat conduction between the magnetic body located at the high temperature side and the high temperature side heat exchanging portion 40B is possible.

  In the state of (2) in FIG. 7, the temperature of the magnetic body from which magnetism has been removed decreases to 15 ° C., and the temperature of the magnetic body to which magnetism has been applied increases to 25 ° C. For this reason, as shown in the figure, heat moves from the higher temperature side to the lower temperature side through the heat conducting member.

  Due to this heat transfer, the temperature of the magnetic body located at one end of the magnetic body unit 200 and the low-temperature side heat exchanging portion 40A becomes 18 ° C. as shown in FIG. The temperature of the magnetic body located at the end and the high temperature side heat exchange section 40B becomes 22 ° C.

  Next, as shown in FIG. 7 (3), in this state, the magnetic circuit is moved to the left side to remove the magnetism from the magnetic body located at the other end of each magnetic block 100A, 100B, and the magnetic located at one end. Apply magnetism to the body. At the same time, the heat conducting member is inserted so that heat conduction between adjacent magnetic bodies of each of the magnetic body blocks 100A and 100B is possible.

  In the state of (3) of FIG. 7, the temperature of the magnetic material to which magnetism is applied rises to 5 ° C. from the temperature of the state of (2) ′ of FIG. The temperature is lowered by 5 ° C. from the temperature in the state (2) ′. For this reason, as shown in the figure, heat moves from the higher temperature to the lower temperature through the heat conducting member in each of the magnetic body blocks 100A and 100B.

  Due to this heat transfer, as shown in FIG. 7 (3) ′, the temperature of the low-temperature side heat exchanging portion 40A becomes 18 ° C., and the temperature of the magnetic body of the magnetic block 100A becomes 19.3 ° C. In addition, the temperature of the magnetic body of the magnetic block 100B is 20.7 ° C., and the temperature of the high temperature side heat exchange unit 40B is 22 ° C.

  As described above, by reciprocating the magnetic circuit in the left-right direction in the drawing, and inserting and removing the heat conducting member in synchronization with this reciprocating movement, heat is transferred from the low temperature side heat exchange unit 40A to the high temperature side heat exchange unit 40B. Move. As time elapses, the temperature difference between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B increases. Eventually, the temperature difference between the low temperature side heat exchange part 40A and the high temperature side heat exchange part 40B becomes constant. In this state, for example, the indoor temperature can be lowered using the heat of the low temperature side heat exchange unit 40A, and the indoor temperature can be increased, for example, using the heat of the high temperature side heat exchange unit 40B.

  The above is the principle of magnetic refrigeration in the present invention. In the above, the most basic form in which a magnetic unit is formed by two or three magnetic bodies, or a magnetic block is formed by two or three magnetic bodies, and a plurality of these magnetic blocks are arranged to provide magnetic properties. Four types of forms for forming body units have been described. However, the present invention is not limited to these forms, and can also be applied to those in which a larger number of magnetic bodies are arranged to form a magnetic body block and a magnetic body unit.

  As described above, when a magnetic unit is formed by two magnetic blocks (three magnetic bodies), a plurality of magnetic blocks and magnetic circuits are connected in series. In addition, one magnetic body in the magnetic block can act as a heat accumulator. For this reason, the heat transport capability and heat transport efficiency of the magnetic refrigerator can be improved, and a large temperature difference can be obtained between the low temperature side heat exchange section and the high temperature side heat exchange section. Therefore, the magnetic refrigerator can be reduced in size, weight, and cost.

  As described above, when the magnetic unit is formed of a plurality of magnetic blocks (two or three magnetic bodies), the magnetic refrigerator can be reduced in size, weight, and cost.

Next, an embodiment of a magnetic refrigerator using the above principle will be described separately from [Embodiment 1] to [Embodiment 3]. In the magnetic refrigerator according to [Embodiment 1], a plurality of magnetic bodies constituting a magnetic unit are arranged in a straight line. In the magnetic refrigerator according to [Embodiment 2], the moving direction of the magnetic application unit is different from that in Embodiment 1. In the magnetic refrigerator according to [Embodiment 3], a plurality of magnetic bodies constituting a magnetic unit are arranged in a ring shape.
[Embodiment 1]
A specific configuration of the magnetic refrigerator according to the first embodiment using the above principle will be described with reference to FIGS.
(Configuration of magnetic refrigerator)
FIG. 8 is a top view illustrating a schematic configuration of the magnetic refrigerator according to the first embodiment. 9 is a front view of the magnetic refrigerator shown in FIG. 8, and FIG. 10 is a side view of the magnetic refrigerator shown in FIG. Further, FIG. 11 is a top view showing a schematic configuration of a heat transfer mechanism that controls heat transfer of the magnetic refrigerator shown in FIG. 12 is a front view of the heat transfer mechanism shown in FIG. 11, and FIG. 13 is a side view of the heat transfer mechanism shown in FIG. Further, FIG. 14 is a top view showing a schematic configuration of a drive mechanism for driving the magnetic application unit of the magnetic refrigerator shown in FIG. 15 is a front view of the drive mechanism shown in FIG. 14, and FIG. 16 is a side view of the drive mechanism shown in FIG.

<Overall configuration>
The magnetic refrigerator shown in FIG. 8 uses the same principle as the magnetic refrigerator shown in FIG. Specifically, two magnetic bodies are arranged in a row to form one magnetic block, and two magnetic blocks are arranged in a row to form a magnetic unit. A total of two magnetic application units (magnetic circuits) for applying magnetism to the magnetic material are provided for each magnetic material block. The two magnetic application units reciprocate in the direction in which the magnetic bodies are arranged. The heat conducting members responsible for heat conduction between the magnetic bodies and between the magnetic body and the low temperature side heat exchanging section and between the magnetic body and the high temperature side heat exchanging section are divided into two groups, and are alternately inserted and removed for each group.

  As shown in FIGS. 8 to 13, the magnetic refrigerator 500 illustrates a heat transfer mechanism on the base plate 520 supported by a plurality of support columns 510A-501F and 510A′-501F ′, and magnetic application units 530A and 530B. And a drive mechanism for reciprocating in the left-right direction. The plurality of support columns are provided in two rows in the depth direction (direction perpendicular to the longitudinal direction) of the base plate 520 as shown in FIG.

<Configuration of heat transfer mechanism>
As shown in FIGS. 8 to 13, the low temperature side heat exchange unit 40 </ b> A and the high temperature side heat exchange unit 40 </ b> B are attached to both ends of the base plate 520 in the longitudinal direction. As shown in FIG. 11, the magnetic bodies 10A, 10B, 10C, and 10D are arranged in a straight line between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B of the base plate 520, as shown in FIG. . A magnetic body block 100A is formed by the magnetic bodies 10A and 10B, and a magnetic body block 100B is formed by the magnetic bodies 10C and 10D. Further, the magnetic body unit 100 is formed by the magnetic body blocks 100A and 100B. When the magnetic bodies are arranged in a straight line, the heat transfer mechanism can be configured in an elongated space, and a narrow space can be used effectively.

  The magnetic bodies 10A, 10B, 10C, and 10D may be directly joined on the base plate 520. However, in order to make effective use of the magnetocaloric effect, the base plate 520 is made of a material having a large thermal resistance. It is desirable to do. This is because if the thermal resistance is small, the heat generated in the magnetic bodies 10A, 10B, 10C, and 10D is radiated through the base plate 520. In order to increase the thermal resistance, the magnetic bodies 10A, 10B, 10C, and 10D are not directly joined on the base plate 520, but between the magnetic bodies 10A, 10B, 10C, and 10D and the base plate 520. A heat insulating film or a heat insulating layer may be provided.

  In addition, the magnetic bodies 10A, 10B, 10C, and 10D may be integrally formed on the base plate 520 as the magnetic body unit 200 through a heat insulating film or a heat insulating layer. Alternatively, the magnetic blocks 100A and 100B may be divided and formed via a heat insulating film or a heat insulating layer and arranged on the base plate 520.

  As the magnetic bodies 10A, 10B, 10C, and 10D, positive magnetic bodies are used in the present embodiment as described above. 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.

  As the material of the positive magnetic body, Gd-Y series, Gd-Dy series, Gd-Er series, Gd-Ho series, La (Fe, Si) 13 and La (which are alloys based on Gd and Gd) are used. Magnetic materials such as Fe, Al) 13 can be used.

  On the other hand, although not used in this embodiment, the magnetic bodies 10A, 10B, 10C, and 10D can be formed of a negative magnetic material. A negative magnetic material is in a ferromagnetic state (a state in which magnetic spins are aligned in one direction) when no magnetism is applied, and a paramagnetic state (a state in which magnetic spins are disordered) when magnetism is applied. Manufactured using a material that reversibly produces a paramagnetic state.

  As the negative magnetic material, a magnetic material such as an FeRh alloy, CoMnSiGe system, or NiMnSn system can be used.

  8 to 13 exemplify magnetic bodies 10A, 10B, 10C, and 10D having a rectangular parallelepiped shape, but other shapes such as a spherical shape, an elliptical shape, a cubic shape, a cylindrical shape, an elliptical column shape, and the like. The shape may also be

  Moreover, positive or negative magnetic bodies can be used for the magnetic bodies 10A, 10B, 10C, and 10D, and the operating temperatures of these magnetic bodies can all be the same. 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 lower operating temperature can be arranged stepwise from the magnetic body 10D 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.

  FIG. 18 is a diagram for explaining the difference in operating temperature of the magnetic body. This figure specifically shows the relationship between the amount of magnetic entropy change (vertical axis) and temperature (horizontal axis) of the LaCeFeCoSi system. When the amount of Co is increased, the temperature at which the magnetocaloric effect is maximized changes to 225K, 250K, 270K, and 290K as shown in the figure. As for other materials, changing the composition ratio can change the temperature region in which the magnetocaloric effect is manifested.

  Therefore, as shown in FIG. 18, the magnetic body that exhibits the magnetocaloric effect in the high temperature range stepwise from the magnetic body adjacent to the high temperature side heat exchange section 40B toward the magnetic body adjacent to the low temperature side heat exchange section 40A. When arranged in the order of (for high temperature), a magnetic body that exhibits a magnetocaloric effect in a medium temperature range (for medium temperature), and a magnetic body that exhibits a magnetocaloric effect in a low temperature range (for low temperature), The temperature difference with the low temperature side heat exchange part 40A can be further increased.

  For magnetic materials having different operating temperatures, the magnetic materials may be formed of magnetic materials having different temperature regions that exhibit the magnetocaloric effect, or by changing the material composition ratio of one type of magnetic material. You may form the magnetic body from which the temperature range which expresses a calorie | heat amount effect differs, respectively.

  Generally, positive and negative magnetic materials generate heat or absorb heat opposite to the application of a magnetic field, 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 are obtained as the heat transfer mechanism, and the heat transport efficiency of the entire magnetic refrigerator is improved. In addition, since the magnetocaloric effect of the negative magnetic material is smaller than the magnetocaloric effect of the positive magnetic material, considering the heat transport efficiency, it is possible to configure the heat transfer mechanism using the positive magnetic material. preferable. Further, since the negative magnetic material is rarer than the positive magnetic material, it is preferable to configure the heat transfer mechanism using the positive magnetic material in terms of cost.

  As described above, when the optimum operating temperature is selected in the magnetic unit 200 in accordance with the position of the magnetic body, the lower temperature side heat exchanging unit 40A and the higher temperature side heat than the magnetic unit 200 using the uniform operating temperature are selected. A larger temperature difference can be obtained with the exchange unit 40B.

  Between the low temperature side heat exchange part 40A and the magnetic body 10A, between the magnetic bodies 10A and 10B, between the magnetic bodies 10B and 10C, between the magnetic bodies 10C and 10D, and between the magnetic body 10D and the high temperature side heat exchange section Heat conduction members 30A-30E are detachably disposed between 40B. As shown in FIGS. 8 to 13, heat conductive member driving units 550 </ b> A and 550 </ b> B that move the heat conductive members 30 </ b> A to 30 </ b> E in a direction intersecting the longitudinal direction of the base plate 520 are attached to the base plate 520.

  The heat conducting member drive unit 550A drives the drive shaft 560A to insert / remove the heat conducting members 30B and 30D constituting one group in conjunction with each other. The heat conduction member drive unit 550B drives the drive shaft 560B to insert / remove the heat conduction members 30A, 30C, and 30E constituting another group in conjunction with each other. The heat conduction member drive unit 550A, the heat conduction member drive unit 550B, and the heat conduction members 30A-30E constitute a heat conduction unit. Although the operations of the heat conducting member driving unit 550A and the heat conducting member driving unit 550B are contradictory to each other, they are performed synchronously.

  8 and 11 show a state in which the heat conducting member driving unit 550A is not operating, and a state in which the heat conducting member driving unit 550B is operating. In the state shown in FIGS. 8 and 11, the heat conducting member 30A is inserted between the low temperature side heat exchange part 40A and the magnetic body 10A, and the low temperature side heat exchange part 40A and the magnetic body 10A are mechanically connected. Heat conduction between the two becomes possible. Heat conduction between the magnetic bodies 10B and 10C and between the magnetic body 10D and the high temperature side heat exchanging section 40B is also possible via the heat conducting members 30C and 30E. On the other hand, since the heat conducting members 30B and 30D are not inserted between the magnetic bodies 10B and 10C and between the magnetic bodies 10C and 10D, heat conduction between them is not performed.

  Any conventionally known mechanism may be used for the heat conduction member driving units 550A and 550B as long as the heat conduction member 30A-30E can be inserted and removed. As the power source, a small motor or a piezoelectric actuator can be used, and the heat conducting member 30A-30E may be inserted and removed using a cam mechanism.

  The heat conducting members 30A-30E are made of a solid high heat conducting material that easily conducts heat. As the high thermal conductive material, Cu and Al are desirable. The portions where the heat conducting members 30A-30E are in contact with the magnetic bodies 10A, 10B, 10C, 10D, the low temperature side heat exchanging portion 40A, and the high temperature side heat exchanging portion 40B are coated with high thermal conductivity and high thermal wear. It may be formed, or a lubricant having high thermal conductivity may be interposed. For example, it is desirable to improve wear resistance and thermal conductivity by attaching carbon nanotubes to the surfaces of the thermal conductive members 30A-30E.

  The heat conducting members 30A and 30E may be made of materials and structures different from those of the heat conducting members 30B, 30C, and 30D that conduct heat to the magnetic bodies 10A to 10D.

  The base plate 520 is made of a low thermal conductive material having a large thermal resistance so that the heat generated in the magnetic bodies 10A, 10B, 10C, and 10D and the heat conducted through the thermal conductive members 30A-30E are not released. Is preferred.

  The low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B include a mechanism capable of exchanging heat with an external environment such as indoor air. For example, a mechanism may be adopted in which a refrigerant is supplied from the outside and heat exchange with the external environment can be performed via the refrigerant.

<Configuration of drive mechanism>
Magnetic application units (magnetic circuits) 530A and 530B are attached to a slider 540 that reciprocally moves the magnetic application units 530A and 530B. The slider 540 reciprocates along the longitudinal direction of the base plate 520 as shown in FIGS. 8 to 10 and FIGS. 14 to 16. The slider 540 is attached to the slide guide 580. The slide guide 580 is supported by the fixing portions 570A and 570B.

  The fixing portions 570A and 570B are located at both lower ends of the base plate 520 and support the slide guide 580. The slider 540 is attached to a linear movement mechanism 585 such as a ball screw or a linear slider, and reciprocates linearly along the slide guide 580. The linear moving mechanism 585 is driven by a magnetic circuit driving unit 590. The magnetic circuit drive unit 590 can use a cam mechanism that changes the rotation of the motor into a linear motion, a linear motor, or a piezoelectric actuator.

  In this embodiment, the linear movement mechanism 585 adopts the configuration shown in FIGS. 8 to 10 and FIGS. 14 to 16 to reciprocate the magnetic application units 530A and 530B. Not only the configuration but also various known mechanisms can be used.

  As shown in FIGS. 9, 10, 15, and 16, the magnetic application unit 530 </ b> A is formed of yokes 25 </ b> A and 25 </ b> B and permanent magnets 535 </ b> A that are made of a metal material such as iron that has a high magnetic permeability that allows magnetism to pass well. The magnetic application unit 530B is formed by yokes 25C and 25D and a permanent magnet 535B. The magnetism applying units 530A and 530B used permanent magnets 535A and 535B as means for generating magnetism. Although a superconducting magnet or an electromagnet can be used in place of the permanent magnet, it is desirable to use a permanent magnet from the viewpoint of energy saving and practicality.

  As shown in FIGS. 10 and 16, the magnetic application portions 530 </ b> A and 530 </ b> B have a U-shaped cross-section when viewed from the direction in which the magnetic application portions 530 </ b> A and 530 </ b> B reciprocate. This is because the two surfaces of the magnetic bodies 10A to 10D that are opposed to each other in the vertical direction in the figure are sandwiched together with the base plate 520 in the U-shaped gap portion. The magnetic application units 530A and 530B face each of the magnetic bodies 10A to 10D so that a strong magnetism can be applied to each of the magnetic bodies 10A to 10D. It has an area.

  In this embodiment, the configuration of the magnetic application units 530A and 530B is configured such that the yokes 25A and 25B sandwich the permanent magnet 535A at the intermediate portion as shown in FIGS. 10 and 16, but for example, the magnetic body 10A A configuration may be adopted in which permanent magnets are arranged on a portion facing one surface of −10D and the others are used as yokes.

  As described above, when the magnetic circuit is composed of permanent magnets, the magnetic circuit can be simplified in structure as compared with the case where an electromagnet is used. Moreover, magnetism can be efficiently applied with respect to a magnetic body by making a magnetic circuit the structure which pinches | interposes two surfaces which a magnetic body opposes via a gap.

  If the magnetic circuit is composed of an electromagnet, the magnitude of the magnetism applied to the magnetic material can be changed within a certain range, so that the magnetism applying unit can have versatility.

The overall operation of the magnetic refrigerator 500 is controlled by the control unit 600 shown in FIG. Specifically, the control unit 600 controls the heat conducting member driving units 550A and 550B and the magnetic circuit driving unit 590 in conjunction with each other. The control unit 600 is configured by an electronic circuit or a microcomputer. A specific operation of the control unit 600 will be described based on an operation flowchart of FIG.
(Operation of magnetic refrigerator (control unit))
FIG. 17 is an operation flowchart of the magnetic refrigerator 500 shown in FIGS. In addition, this operation | movement flowchart also shows the procedure of the magnetic refrigeration method based on this invention.

  The controller 600 determines whether a magnetic refrigeration start signal is input (S1). If the magnetic refrigeration start signal is not input (S1: NO), control unit 600 waits for input, and if input (S1: YES), proceeds to the next step.

  When the magnetic refrigeration start signal is input, the control unit 600 operates the magnetic circuit drive unit 590 to move the magnetic application units 530A and 530B. For example, as shown in FIGS. 8 and 9, the magnetic application units 530A and 530B are moved from the positions of the magnetic bodies 10A and 10C to the positions of the magnetic bodies 10B and 10D. At this time, the magnetic bodies 10A and 10C absorb heat, and the magnetic bodies 10B and 10D generate heat (S2).

  Next, as shown in FIGS. 8 and 9, the control unit 600 deactivates the heat conducting member driving unit 550 </ b> A and operates the heat conducting member driving unit 550 </ b> B. Accordingly, each of the heat conducting members 30A-30F is inserted / removed between the low temperature side heat exchange part 40A and the magnetic body 10A, between the magnetic bodies 10A-10D, and between the magnetic body 10D and the high temperature side heat exchange part 40B. Let For example, as shown in FIG. 8 and FIG. 11, the heat conduction member drive unit 550A is deactivated, so that the heat conduction member 30B, between the magnetic bodies 10B and 10C and between the magnetic bodies 10C and 10D, 30D is pulled out. On the other hand, when the heat conducting member driving unit 550B operates, the heat conducting member 30A is inserted between the low temperature side heat exchanging unit 40A and the magnetic body 10A, and the heat conducting member 30C is interposed between the magnetic bodies 10B and 10C. The heat conducting member 30E is inserted between the magnetic body 10D and the high temperature side heat exchange part 40B (S3).

  And the control part 600 judges whether the completion | finish signal of magnetic refrigeration was input (S4). If the magnetic refrigeration end signal is not input (S4: NO), control unit 600 returns to the process of step 2. That is, the control unit 600 operates the magnetic circuit driving unit 590 to move the magnetic application units 530A and 530B. At this time, the magnetic application units 530A and 530B are moved from the positions of the magnetic bodies 10B and 10D to the positions of the magnetic bodies 10A and 10C. At this time, the magnetic bodies 10B and 10D absorb heat, and the magnetic bodies 10A and 10C generate heat (S2).

  Then, the control unit 600 operates the heat conducting member driving unit 550A and deactivates the heat conducting member driving unit 550B. Accordingly, each of the heat conducting members 30A-30F is inserted / removed between the low temperature side heat exchange part 40A and the magnetic body 10A, between the magnetic bodies 10A-10D, and between the magnetic body 10D and the high temperature side heat exchange part 40B. Let At this time, the heat conducting member driving unit 550B is deactivated, whereby the heat conducting member 30A is pulled out from between the low temperature side heat exchanging unit 40A and the magnetic body 10A, and the heat conducting member 30C is removed from the magnetic bodies 10B and 10C. The heat conducting member 30E is drawn from between the magnetic body 10D and the high temperature side heat exchanging portion 40B. On the other hand, when the heat conducting member driving unit 550A operates, the heat conducting members 30B and 30D are inserted between the magnetic bodies 10B and 10C and between the magnetic bodies 10C and 10D (S3).

  Control unit 600 repeats the operations of steps S2 and S3 described above unless a magnetic refrigeration end signal is input. If the magnetic refrigeration end signal is input (S4: YES), the process is ended and the operation of the magnetic refrigerator 500 is ended.

  By moving the magnetic application parts 530A and 530B and inserting / removing each of the heat conducting members 30A-30F as described above, the temperature of the low-temperature side heat exchange part 40A is lowered as shown in the graph of FIG. The temperature of the heat exchange unit 40B can be raised, and a temperature difference can be generated between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B.

  In addition, the principle by which the temperature difference between the low temperature side heat exchange part 40A and the high temperature side heat exchange part 40B is expanded by the above operation is the same as the principle described based on FIG. 4 and FIG. Explanation here is omitted.

  When actually configuring a magnetic refrigerator having a large refrigerating capacity, the number of magnetic blocks arranged in series is increased, and a large number of them are arranged in parallel, so that the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B are arranged. Connect to. By increasing the number of magnetic blocks arranged in series, the temperature difference between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B can be further increased. Moreover, the refrigerating capacity can be further improved by arranging many magnetic blocks in parallel.

The magnetic refrigerator of this embodiment can be applied to an air conditioner that performs indoor air conditioning, a refrigerator, an air conditioner that performs air conditioning in a vehicle interior, a vehicle refrigeration apparatus, and the like.
[Embodiment 2]
Next, a specific configuration of the magnetic refrigerator according to the second embodiment will be described with reference to FIG. FIG. 19 is a diagram illustrating a schematic configuration of a magnetic refrigerator according to the second embodiment.

The magnetic refrigerator shown in FIG. 19 is different from the first embodiment in the following parts. First, in the case of the first embodiment, only one row of magnetic body blocks in which four magnetic bodies are arranged in a row is provided, but in the case of this embodiment, two rows of magnetic body blocks are provided in parallel. Further, in the case of the first embodiment, the magnetic application unit (magnetic circuit) for applying magnetism to the magnetic material is reciprocated in the direction in which the magnetic materials are arranged. Is moved in a direction crossing the direction in which the magnetic bodies are arranged.
(Configuration of magnetic refrigerator)
<Configuration of heat transfer mechanism>
As shown in FIG. 19, the low-temperature side heat exchange unit 40A and the high-temperature side heat exchange unit 40B are attached to both ends of the base plate 520 in the longitudinal direction. Between the low temperature side heat exchange part 40A and the high temperature side heat exchange part 40B of the base plate 520, as shown in the figure, the magnetic bodies 10A, 10B, 10C, 10D are arranged in a straight line, and In parallel, magnetic bodies 10E, 10F, 10G, and 10H are arranged in a straight line at intervals. A magnetic body block 100A is formed by the magnetic bodies 10A and 10B, and a magnetic body block 100B is formed by the magnetic bodies 10C and 10D. The magnetic bodies 10E and 10F form the magnetic body block 100C, and the magnetic bodies 10G and 10H form the magnetic body block 100D. The magnetic body unit 200A is formed by the magnetic body blocks 100A and 100B. Further, the magnetic body unit 200B is formed by the magnetic body blocks 100C and 100D.

  Between the low temperature side heat exchange part 40A and the magnetic body 10A, between the magnetic bodies 10A and 10B, between the magnetic bodies 10B and 10C, between the magnetic bodies 10C and 10D, and between the magnetic body 10D and the high temperature side heat exchange section Heat conduction members 30A-30E are detachably disposed between 40B. Further, between the low temperature side heat exchange section 40A and the magnetic body 10E, between the magnetic bodies 10E and 10F, between the magnetic bodies 10F and 10G, between the magnetic bodies 10G and 10H, and between the magnetic body 10H and the high temperature side heat. The heat conducting member 30F-30J is detachably disposed between the exchange unit 40B.

  The base plate 520 is attached with heat conduction member driving units 550A and 550B that move the heat conduction members 30A-30E in a direction intersecting the longitudinal direction of the base plate 520. In addition, heat conduction member drive units 550C and 550D that move the heat conduction member 30F-30J in a direction intersecting the longitudinal direction of the base plate 520 are attached.

  The heat conducting member drive unit 550A drives the drive shaft 560A to insert / remove the heat conducting members 30B and 30D constituting one group in conjunction with each other. The heat conduction member drive unit 550B drives the drive shaft 560B to insert / remove the heat conduction members 30A, 30C, and 30E constituting another group in conjunction with each other. Further, the heat conducting member driving unit 550C drives the drive shaft 560C to insert / remove the heat conducting members 30G and 30I constituting one group in conjunction with each other. The heat conducting member drive unit 550D drives the drive shaft 560D to insert / remove the heat conducting members 30F, 30H, and 30J constituting another group in conjunction with each other.

  The heat conducting member driving units 550A to 550D and the heat conducting members 30A to 30J constitute a heat conducting unit. The operations of the heat conducting member driving units 550A and 550C and the heat conducting member driving units 550B and 550D are performed in synchronism with each other, but are performed synchronously, and when one operates, the other does not operate.

  The state shown in the figure is a state in which the heat conducting member driving units 550B and 550C are not operating, and a state in which the heat conducting member driving units 550A and 550D are operating. In this state, the heat conducting member 30B is inserted between the magnetic body 10A and the magnetic body 10B, and the heat conducting member 30D is inserted between the magnetic body 10C and the magnetic body 10D, and heat conduction therebetween can be performed. . Further, the heat conducting member 30F is between the low temperature side heat exchange part 40A and the magnetic body 10E, the heat conducting member 30H is between the magnetic body 10F and the magnetic body 10G, and the heat conducting member 30J is between the magnetic body 10H and the high temperature side. It is inserted between the heat exchanging part 40B, and heat conduction between them becomes possible. On the other hand, between the low temperature side heat exchange part 40A and the magnetic body 10A, between the magnetic body 10B and the magnetic body 10C, and between the magnetic body 10D and the high temperature side heat exchange part 40B, the heat conducting members 30A, 30C, 30E. Since no is inserted, no heat conduction takes place between them. Further, since the heat conducting members 30G and 30I are not inserted between the magnetic body 10E and the magnetic body 10F and between the magnetic body 10G and the magnetic body 10H, heat conduction between them is not performed.

<Configuration of drive mechanism>
Magnetic application units (magnetic circuits) 530A-530D are attached to sliders 540A-540D that individually reciprocate magnetic application units 530A-530D in a direction orthogonal to the longitudinal direction of base plate 520. The slider 540A linearly reciprocates the magnetic application unit 530A between the magnetic body 10A and the magnetic body 10E. In the sliders 540B, 540C, and 540D, the magnetic application unit 530B is between the magnetic body 10C and the magnetic body 10G, the magnetic application unit 530C is between the magnetic body 10B and the magnetic body 10F, and the magnetic application unit 530D is the magnetic body. It is reciprocated linearly between 10D and the magnetic body 10H.

The magnetic application units 530A and 530B are driven by the magnetic circuit drive unit 590A, and the magnetic application units 530C and 530D are driven by the magnetic circuit drive unit 590B.
(Operation of magnetic refrigerator (control unit))
The operation of the magnetic refrigerator 500 according to the present embodiment configured as described above will be described in detail based on the operation flowchart of FIG. In addition, this operation | movement flowchart also shows the procedure of the magnetic refrigeration method based on this invention.

  The controller 600 determines whether a magnetic refrigeration start signal is input (S1). If the magnetic refrigeration start signal is not input (S1: NO), control unit 600 waits for input, and if input (S1: YES), proceeds to the next step.

  When the magnetic refrigeration start signal is input, the control unit 600 operates the magnetic circuit driving units 590A and 590B and moves the magnetic application units 530A to 530D. For example, as shown in FIG. 19, the magnetic application unit 530A is changed from the magnetic body 10E to the magnetic body 10A, the magnetic application unit 530B is changed from the magnetic body 10G to the magnetic body 10C, and the magnetic application unit 530C is changed from the magnetic body 10B to the magnetic body 10F. The magnetic application unit 530D is moved from the magnetic body 10D to the magnetic body 10H. At this time, the magnetic body 10A, the magnetic body 10C, the magnetic body 10F, and the magnetic body 10H generate heat, and the magnetic body 10B, the magnetic body 10D, the magnetic body 10E, and the magnetic body 10G absorb heat. (S2).

  Next, as shown in FIG. 19, the control unit 600 deactivates the heat conducting member driving units 550B and 550C and operates the heat conducting member driving units 550A and 550D. Thus, each of the heat conducting members 30A-30J is connected between the low temperature side heat exchanging portion 40A and the magnetic bodies 10A and 10E, between the magnetic bodies 10A to 10H, and between the magnetic bodies 10D and 10H and the high temperature side heat. It is inserted into and removed from the exchange unit 40B. Specifically, the heat conduction member 30B is inserted between the magnetic body 10A and the magnetic body 10B, and the heat conduction member 30D is inserted between the magnetic body 10C and the magnetic body 10D. Become. Further, the heat conducting member 30F is between the low temperature side heat exchange part 40A and the magnetic body 10E, the heat conducting member 30H is between the magnetic body 10F and the magnetic body 10G, and the heat conducting member 30J is between the magnetic body 10H and the high temperature side. It is inserted between the heat exchanging part 40B, and heat conduction between them becomes possible. On the other hand, the heat conducting members 30A, 30C, and 30E are provided between the low temperature side heat exchange unit 40A and the magnetic body 10A, between the magnetic body 10B and the magnetic body 10C, and between the magnetic body 10D and the high temperature side heat exchange unit 40B. Withdrawn, no heat conduction takes place between them. Further, the heat conducting members 30G and 30I are pulled out between the magnetic body 10E and the magnetic body 10F, and between the magnetic body 10G and the magnetic body 10H, and heat conduction therebetween is not performed (S3).

  And the control part 600 judges whether the completion | finish signal of magnetic refrigeration was input (S4). If the magnetic refrigeration end signal is not input (S4: NO), control unit 600 returns to the process of step 2. That is, the control unit 600 operates the magnetic circuit driving units 590A and 590B to move the magnetic application units 530A to 530D in the direction opposite to the previous time. For example, the magnetic application section 530A is changed from the magnetic body 10A to the magnetic body 10E, the magnetic application section 530B is changed from the magnetic body 10C to the magnetic body 10G, the magnetic application section 530C is changed from the magnetic body 10F to the magnetic body 10B, and the magnetic application section 530D is magnetic. The body 10H is moved to the magnetic body 10D. At this time, the magnetic body 10B, the magnetic body 10D, the magnetic body 10E, and the magnetic body 10G generate heat, and the magnetic body 10A, the magnetic body 10C, the magnetic body 10F, and the magnetic body 10H absorb heat (S2).

  Next, the control unit 600 operates the heat conducting member driving units 550B and 550C and deactivates the heat conducting member driving units 550A and 550D. Thereby, between the low temperature side heat exchange part 40A and the magnetic body 10A, between the magnetic body 10B and the magnetic body 10C, and between the magnetic body 10D and the high temperature side heat exchange part 40B, the heat conducting members 30A, 30C, 30E. Is inserted, allowing heat conduction between them. Further, the heat conducting members 30G and 30I are inserted between the magnetic body 10E and the magnetic body 10F, and between the magnetic body 10G and the magnetic body 10H, and heat conduction therebetween can be performed. On the other hand, the heat conducting member 30B is pulled out from between the magnetic body 10A and the magnetic body 10B, and the heat conducting member 30D is pulled out from between the magnetic body 10C and the magnetic body 10D, and heat conduction between them is not performed. Further, the heat conducting member 30F is between the low temperature side heat exchanging portion 40A and the magnetic body 10E, the heat conducting member 30H is between the magnetic body 10F and the magnetic body 10G, and the heat conducting member 30J is between the magnetic body 10H and the high temperature side. The heat exchange unit 40B is pulled out, and heat conduction between them is not performed (S3).

  Control unit 600 repeats the operations of steps S2 and S3 described above unless a magnetic refrigeration end signal is input. If the magnetic refrigeration end signal is input (S4: YES), the process is ended and the operation of the magnetic refrigerator 500 is ended.

  By moving the magnetic application units 530A-530D and inserting / removing each of the heat conducting members 30A-30J as described above, the temperature of the low-temperature side heat exchange unit 40A is lowered as shown in the graph of FIG. The temperature of the heat exchange unit 40B can be raised, and a temperature difference can be generated between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B.

  In addition, the principle by which the temperature difference between the low temperature side heat exchange part 40A and the high temperature side heat exchange part 40B is expanded by the above operation is the same as the principle described based on FIG. 4 and FIG. Explanation here is omitted.

  When actually configuring a magnetic refrigerator having a large refrigerating capacity, the number of magnetic blocks arranged in series is increased, and a large number of them are arranged in parallel as in the present embodiment. It connects to the high temperature side heat exchange part 40B. By increasing the number of magnetic blocks arranged in series, the temperature difference between the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit 40B can be further increased. Moreover, the refrigerating capacity can be further improved by arranging many magnetic blocks in parallel.

The magnetic refrigerator of this embodiment can be applied to an air conditioner that performs indoor air conditioning, a refrigerator, an air conditioner that performs air conditioning in a vehicle interior, a vehicle refrigeration apparatus, and the like.
[Embodiment 3]
Next, a specific configuration of the magnetic refrigerator according to the third embodiment will be described with reference to FIG.

  FIG. 20 is a diagram illustrating a schematic configuration of the magnetic refrigerator according to the third embodiment.

  In the magnetic refrigerator according to this embodiment, a plurality of magnetic bodies constituting the magnetic unit are not arranged linearly as in the first embodiment, but a plurality of magnetic bodies constituting the magnetic unit are arranged in an annular shape. There is a feature in the point.

  As shown in the figure, a low temperature side heat exchange unit 40A and a high temperature side heat exchange unit 40B are arranged on the upper end and lower end of a circular base plate 520A. Eight magnetic bodies 10A-10H are annularly arranged on one surface of the base plate 520A. The magnetic bodies 10A and 10B, the magnetic bodies 10C and 10D, the magnetic bodies 10E and 10F, and the magnetic bodies 10G and 10H each form a magnetic block. Further, the magnetic blocks 100A and 100B and the magnetic blocks 100C and 100D each form a pair to form one magnetic unit. When the magnetic bodies are arranged in an annular shape, it is only necessary to rotate the magnetic application unit, so that the drive mechanism of the magnetic circuit drive unit can be made simple.

  Between the low temperature side heat exchange part 40A and the magnetic bodies 10A and 10H, between the magnetic bodies of the magnetic bodies 10A to 10H, and between the high temperature side heat exchange part 40B and the magnetic bodies 10D and 10E, the heat conducting members 30A to 30H Place. Each of the heat conducting members 30A-30H is inserted and removed by a heat conducting member driving unit (not shown) that operates in the same manner as in the first embodiment.

  The magnetic application units 530A to 530E are formed at the radial tip portions of the protruding portions of the five rectangular bodies that extend radially from the rotation center of the rotating body at an equal angle. The structure of the magnetic application units 530A to 530E is the same as that shown in FIGS. 10 and 16 of the above embodiment, and the magnetic application units 530A to 530E rotate around the rotation center of the rotating body. The magnetic application units 530A to 530E rotate the low temperature side heat exchange unit 40A, the magnetic bodies 10A to 10H, and the high temperature side heat exchange unit 40B in a propeller shape so that the respective magnetic circuits sandwich the base plate 520A.

  In FIG. 20A, since the magnetic application parts 530A-530E are located in the magnetic bodies 10B, 10D, 10E, and 10G, these magnetic bodies generate heat, and the other magnetic bodies 10A, 10C, 10F, and 10H absorb heat. At this time, the heat conducting members 30A, 30C, 30E, 30F, 30H, and 30J are between the magnetic bodies 10A and 10H and the low temperature side heat exchanging portion 40A, between the magnetic bodies 10B and 10C, and between the magnetic bodies 10D and 10E. It is inserted between the high temperature side heat exchange part 40B and between the magnetic bodies 10F and 10G.

  Accordingly, as shown in FIG. A, between the magnetic bodies 10A and 10H and the low temperature side heat exchange section 40A, between the magnetic bodies 10B and 10C, and between the magnetic bodies 10D and 10E and the high temperature side heat exchange section 40B. Then, heat conduction is performed between the magnetic bodies 10F and 10G.

  Next, as shown in FIG. B, when the magnetic application units 530A-530E are positioned on the magnetic bodies 10A, 10C, 10F, and 10H, these magnetic bodies generate heat, and the other magnetic bodies 10B, 10D, 10E, and 10G are It absorbs heat. At this time, the heat conducting members 30A, 30C, 30E, 30F, 30H, and 30J are between the magnetic bodies 10A and 10H and the low temperature side heat exchanging portion 40A, between the magnetic bodies 10B and 10C, and between the magnetic bodies 10D and 10E. It is removed from between the high temperature side heat exchange section 40B and between the magnetic bodies 10F and 10G. At the same time, the heat conducting members 30B, 30D, 30G, and 30I are located between the magnetic bodies 10A and 10B, between the magnetic bodies 10C and 10D, between the magnetic bodies 10E and 10F, and between the magnetic bodies 10G and 10H. Inserted.

  Accordingly, as shown in FIG. B, heat conduction is performed between the magnetic bodies 10A and 10B, between the magnetic bodies 10C and 10D, between the magnetic bodies 10E and 10F, and between the magnetic bodies 10G and 10H. Is called.

  Thus, if the magnetic body to which magnetism is applied is changed one after another while the magnetic application units 530A to 530E are rotationally moved, the heat generating magnetic body and the heat absorbing magnetic body are alternately switched. Further, when the heat conduction member 30A-30J is alternately switched in accordance with the rotation of the magnetic application unit 530A-530E, as shown in the graph of FIG. 2, the low temperature side heat exchange unit 40A and the high temperature side heat exchange unit A temperature difference can be produced between the temperature and 40B.

  In the case of this embodiment, the magnetic application units 530A-530E only need to be rotated using a motor that functions as a magnetic circuit drive unit, so the configuration of the drive mechanism of the magnetic application units 530A-530E can be simplified. Moreover, the refrigerating capacity of the magnetic refrigerator 500 can be easily adjusted by changing the rotational speed of the magnetic application units 530A-530E.

  The principle of magnetic refrigeration in this embodiment is the same as that shown in FIGS. 4 and 5, and the operation of magnetic refrigeration is basically the same as the flowchart shown in FIG.

  Also in this embodiment, a positive or negative magnetic body can be used for the magnetic bodies 10A-10D, 10E-10H, and the operating temperatures of these magnetic bodies can all be the same. 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 bodies 10D and 10E adjacent to the high temperature side heat exchange section 40B to the magnetic bodies 10A and 10H adjacent to the low temperature side heat exchange section 40A.

  As described above, the magnetic refrigerator according to the present invention can obtain the following effects.

  Magnetism is applied individually to the positive or negative magnetic body at the magnetic application section to develop the magnetocaloric effect, and heat is transported using the heat conduction of the solid. Improvements can be made in size, weight and cost.

  In addition, the magnetic body constituting the magnetic unit is more efficient by gradually reducing the operating temperature from the magnetic body adjacent to the high temperature side heat exchange section toward the magnetic body adjacent to the low temperature side heat exchange section. Magnetic refrigeration becomes possible, and the temperature difference between the low temperature side heat exchange part and the high temperature side heat exchange part can be further increased.

  Furthermore, when magnetic refrigeration is performed by arranging the magnetic body in an annular shape and rotating the magnetic application unit, the configuration of the drive mechanism can be simplified, and a small and lightweight magnetic refrigerator can be obtained.

10A-10H magnetic material,
30A-30J heat conduction member,
40A low temperature side heat exchange section,
40B high temperature side heat exchange section,
500 magnetic refrigerator,
530A-530D magnetic application unit,
550A-550D heat conduction member drive unit,
590, 590A, 590B magnetic circuit drive unit,
600 Control unit.

Claims (12)

A magnetic body unit in which three or more magnetic bodies having the same kind of magnetocaloric effect to be expressed are arranged in rows,
A low temperature side heat exchanging portion adjacent to the magnetic body located at one end of the magnetic body unit at a distance;
A high temperature side heat exchanging portion adjacent to the magnetic body located at the other end of the magnetic body unit with a gap therebetween;
Heat conduction between adjacent magnetic bodies in the magnetic body unit, or between the magnetic body located at one end of the magnetic body unit and the low temperature side heat exchanging unit and at the other end of the magnetic body unit Heat conduction between the magnetic body and the high temperature side heat exchanging part, alternately conducting heat conduction through a solid heat conduction member, and
A magnetic applying unit that alternately applies magnetism to any of the magnetic bodies located at one end of the magnetic body unit or the magnetic body located at the other end of the magnetic body unit;
When the operation of the heat conducting unit and the magnetic application unit is controlled so that the magnetic application unit applies magnetism to a magnetic body located at one end of the magnetic unit, the heat conducting unit is used as the magnetic unit. Heat is conducted between adjacent magnetic bodies, and when the magnetic application unit applies magnetism to a magnetic body located at the other end of the magnetic unit, the heat conduction unit A controller that conducts heat between the magnetic body located at both ends of the unit and the low temperature side heat exchange unit and the high temperature side heat exchange unit;
A magnetic refrigerator comprising: Magnetic body units in which three or more magnetic bodies having the same kind of magnetocaloric effect to be expressed are arranged in rows and arranged at intervals, and further arranged in a plurality of rows at intervals, and
A low temperature side heat exchanging portion adjacent to the magnetic body located at one end of the magnetic body unit at a distance;
A high temperature side heat exchanging portion adjacent to the magnetic body located at the other end of the magnetic body unit with a gap therebetween;
Heat conduction between adjacent magnetic bodies in the magnetic block, or between the adjacent magnetic bodies of adjacent magnetic blocks and at one end of the magnetic unit and the low-temperature side heat exchange Heat conduction between the magnetic body and the magnetic body located at the other end of the magnetic body unit and between the high temperature side heat exchanging section through the solid heat conduction member. A conduction part;
Magnetism that alternately applies magnetism to either the magnetic body located at one end of the magnetic body block or the magnetic body located at the other end of the magnetic body block for each magnetic body block An application unit;
When the operation of the heat conducting unit and the magnetic application unit is controlled so that the magnetic application unit applies magnetism to the magnetic body located at one end of the magnetic body block, the heat conducting unit is the magnetic body block. When heat is conducted between adjacent magnetic bodies, and when the magnetism applying section applies magnetism to the magnetic body located at the other end of the magnetic block, the heat conducting sections are adjacent to each other. Control that conducts heat between adjacent magnetic bodies of the body block and conducts heat between the magnetic bodies located at both ends of the magnetic body unit and the low temperature side heat exchange section and the high temperature side heat exchange section And
A magnetic refrigerator comprising:   A magnetic material that exhibits the same type of magnetocaloric effect is either a positive magnetic material that generates heat when applied with magnetism and absorbs heat when it is removed, or a negative magnetic material that generates heat when applied with magnetism and removes heat. The magnetic refrigerator according to claim 1, wherein the magnetic refrigerator is a magnetic material.   The magnetic body constituting the magnetic unit is characterized in that the operating temperature is lowered stepwise from the magnetic body adjacent to the high temperature side heat exchange section toward the magnetic body adjacent to the low temperature side heat exchange section. The magnetic refrigerator according to any one of claims 1 to 3. The heat conducting part is
A solid heat conduction member that conducts heat by mechanically connecting between the magnetic body, between the magnetic body and the low temperature side heat exchange section, and between the magnetic body and the high temperature side heat exchange section,
A heat conducting member driving unit that drives the heat conducting member to conduct the heat, and
The control unit drives the heat conducting member driving unit in conjunction with the operation in which the magnetism applying unit alternately applies magnetism to the magnetic body, and performs any one of the heat conductions via the solid heat conducting member. The magnetic refrigerator according to any one of claims 1 to 4, wherein the magnetic refrigerator is alternately performed. The magnetic application unit is
With a magnetic circuit containing a permanent magnet,
The magnetic circuit has a structure in which two opposing surfaces of the magnetic body are sandwiched through a gap with respect to a magnetic body constituting the magnetic unit. The magnetic refrigerator as described.   The magnetic refrigerator according to claim 6, wherein the plurality of magnetic bodies constituting the magnetic unit are arranged in a straight line.   The magnetic refrigerator according to claim 6, wherein the plurality of magnetic bodies constituting the magnetic unit are arranged in a ring shape. The magnetic application unit further includes a magnetic circuit driving unit that reciprocates the magnetic circuit linearly along the magnetic body,
8. The magnetic circuit according to claim 7, wherein the magnetic application to one magnetic body and the magnetic application to the other magnetic body are alternately performed among the plurality of magnetic bodies arranged in a straight line. The magnetic refrigerator as described. The magnetic application unit further includes a magnetic circuit driving unit that rotates the magnetic circuit along the arrangement of the magnetic bodies,
9. The magnetic circuit according to claim 8, wherein magnetism is alternately applied to one of the plurality of magnetic bodies arranged in an annular shape and magnetism is applied to the other magnetic body. Magnetic refrigerator. A magnetic body located at the other end by applying magnetism to a magnetic body located at one end of a magnetic body unit in which three or more magnetic bodies having the same type of magnetocaloric effect are arranged at intervals. A first step of removing magnetism from
A second step of conducting heat between adjacent magnetic bodies in the magnetic unit via a solid heat conductive member;
A third step of removing magnetism from the magnetic body located at one end of the magnetic unit and applying magnetism to the magnetic body located at the other end;
Via the solid heat conduction member, between the magnetic body located at one end of the magnetic body unit and the adjacent low-temperature side heat exchanging portion with a gap to the magnetic body, and the other end of the magnetic body unit And a fourth step of conducting heat between the magnetic body located at the high temperature side heat exchange section adjacent to the magnetic body with a gap therebetween,
A magnetic refrigeration method comprising transporting heat from the low temperature side heat exchange section to the high temperature side heat exchange section by repeating the first to fourth steps. Each magnetic body block of a magnetic body unit in which three or more magnetic bodies having the same type of magnetocaloric effect expressed are arranged in a row at intervals and arranged in a plurality of rows at intervals. A first step of applying magnetism to a magnetic body located at one end of the magnetic material and removing the magnetism from the magnetic body located at the other end;
A second step of conducting heat between adjacent magnetic bodies in each of the magnetic body blocks via a solid heat conductive member;
A third step of removing magnetism from the magnetic body located at one end of each magnetic block and applying magnetism to the magnetic body located at the other end;
The low temperature side adjacent to the magnetic body located at one end of the magnetic unit and the magnetic body between the adjacent magnetic bodies of the adjacent magnetic block via the solid heat conducting member The fourth step of conducting heat between the heat exchanger and the magnetic body located at the other end of the magnetic unit and the adjacent high temperature side heat exchanger with a gap with respect to the magnetic body And comprising
A magnetic refrigeration method comprising transporting heat from the low temperature side heat exchange section to the high temperature side heat exchange section by repeating the first to fourth steps.

Images