ELECTROMAGNETIC INDUCTION HEATING DEVICE
20200396804 ยท 2020-12-17
Inventors
Cpc classification
International classification
Abstract
An electromagnetic induction heating device includes a rotator in which a plurality of magnets is arranged in a manner that the same poles are positioned on a side of an object to be heated, and a rotation drive part for rotating the rotator, and heats the object to be heated by an induction current which is generated by rotating the rotator, wherein magnets adjacent in a direction in which the rotator is rotated are arranged with an interval of 10 mm or more. Thereby, heating efficiency by electromagnetic induction is improved, and the object to be heated such as an aluminium material or the like can be brought to a predetermined temperature in a short time.
Claims
1. An electromagnetic induction heating device, comprising a rotator in which a plurality of magnets is arranged in a manner that the same poles are positioned on a side of an object to be heated, and a rotation drive part for rotating the rotator, and heating the object to be heated by an induction current which is generated by rotating the rotator by a rotation number at which the induction current is generated in the object to be heated with rotation, wherein an interval between the magnets adjacent in a direction in which the rotator is rotated is 20 mm or more and 45 mm or less, a distance from the object to be heated to the magnets of the rotator is 12 mm or less in the heating, the object to be heated is made of a material which generates an eddy current by changing a magnetic field, the plurality of magnets has a cylindrical shape in which a diameter is 5 mm or more and 25 mm or less and a height is 10 mm or more and 40 mm or less, a height of 0.5 time or more and 2 times or less of the diameter, and a magnetic flux density of 400 mT or more and 600 mT or less, and the plurality of magnets is mounted to the rotator via a height adjustment part for adjusting errors of height of the magnets to uniformize the heights of the magnets on the magnet surface.
2. (canceled)
3. The electromagnetic induction heating device according to claim 1, wherein the plurality of magnets is arranged concentrically taking a rotation center of the rotator as a center.
4. The electromagnetic induction heating device according to claim 1, wherein the plurality of magnets is arranged concentrically taking a rotation center of the rotator as a center, the plurality of magnets arranged along each concentric circle is arranged at equal intervals.
5. The electromagnetic induction heating device according to claim 4, wherein. the concentric circles are arranged at equal intervals, and differences between diameters of the adjacent concentric circles are 40 mm or more and 60 mm or less.
6-9. (canceled)
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0018]
[0019]
[0020]
[0021]
[0022]
[0023]
[0024]
[0025]
[0026]
DESCRIPTION OF THE EMBODIMENTS
[0027] Embodiments of the present invention are described below with reference to the drawings.
[0028]
[0029]
[0030] In
[0031] The plurality of magnets 21 arranged along the circle C1, the circle C2 and the circle C3 indicated by the dashed-dotted lines in
[0032] As shown in
[0033] From the viewpoint of improving the heating efficiency of the object to be heated 8, the interval L1 between the adjacent magnets 21 is preferably 10 mm or more, more preferably 20 mm or more, and further preferably 30 mm or more. In addition, from the same viewpoint, the interval L1 between the magnets 21 is preferably 50 mm or less, more preferably 45 mm or less, and further preferably 40 mm or less. By setting the interval L1 within the above ranges, a magnetic flux density near the magnet surface of the rotator 2 on which the plurality of magnets 21 is arranged increases. Therefore, an induction current generated in the object to be heated 8 along with the rotation of the rotator 2 can effectively heat the object to be heated 8.
[0034] Arranging the adjacent magnets 21 on the circles C at the interval L1 means arranging in a manner that the distance with the adjacent magnets 21 is within the range of the interval L1. The interval L1 is not one specified distance, but means a distance range. Therefore, the present invention is not limited to a configuration in which the intervals between the adjacent magnets 21 are all equally arranged to be the same distance, and even if the distances between the adjacent magnets 21 are different, it is sufficient that each distance is within the range of the interval L1. However, from the viewpoint of improving the heating efficiency of the object to be heated 8, a configuration is preferable in which the plurality of magnets 21 arranged along each of the circles C is arranged at equal intervals.
[0035] The circle C1, the circle C2 and the circle C3 which are concentrically arranged may be large enough to arrange the magnets 21 side by side. For example, when the magnets 21 have a cylindrical shape with a cross-sectional diameter of 20 mm, differences D1 (=R1R2) and D2 (=R3R2) between diameters of adjacent concentric circles are preferably 40 mm or more and 60 mm or less, and more preferably 45 mm or more and 55 mm or less. A configuration may be employed in which the circle C1, the circle C2 and the circle C3 which are concentrically arranged are respectively arranged at equal intervals (D1=D2).
[0036] The rotator 2 is connected to the rotation drive motor 3 via a rotation shaft 22 at a position of a center of the concentric circles of the magnets 21 on a surface opposite the magnet surface (see
[0037] Ferrite magnets, rare earth magnets such as samarium-cobalt magnets (SmCo magnets), neodymium magnets (NdFeB magnets) and the like, alnico magnets (AlNiCo magnets), and the like can be used as the magnets 21. From the viewpoint of efficiently heating the object to be heated 8, magnets such as rare earth magnets or the like which have a strong magnetic force are preferable.
[0038]
[0039] From the viewpoint of improving the heating efficiency of the object to be heated 8, a magnetic flux density on surfaces of the magnets 21 is preferably 350 mT or more, more preferably 400 mT or more, and further preferably 450 mT or more. An upper limit of the magnetic flux density is not particularly limited and is, for example, 600 mT or less.
[0040]
[0041] As shown in
[0042] In the embodiment, a configuration in which the rotator 2 is rotated in order to generate an induction current in the object to be heated 8 is shown. However, a configuration in which the rotator 2 is fixed and the object to be heated 8 is rotated to generate the induction current may also be employed. However, an effect that the magnets 21 are cooled by air is obtained by rotating the rotator 2, and thus when rare earth magnets with a relatively low Curie point are used as the magnets 21, a configuration of rotating the rotator 2 is preferable. The electromagnetic induction heating device 1 may cool the magnets 21 using a cooling part such as a cooling fan or the like.
[0043] The rotation drive motor 3 (see
[0044] The distance measurement part 4 measure the distance X between an end on the object to be heated 8 side of the magnet 21 of the rotator 2 and the object to be heated 8. The distance measurement part 4 may be, for example, a part for detecting change in capacitance between the magnets 21 of the rotator 2 and the object to be heated 8, or change in laser light passing through a gap between the magnets 21 of the rotator 2 and the object to be heated 8.
[0045]
[0046] The temperature measurement part 5 measures a temperature of the object to be heated 8 and outputs a result to the control part 7. A known temperature sensor such as a thermocouple can be used as the temperature measurement part 5. The temperature of the object to be heated 8 may be measured in one place as shown in
[0047] The motor for movement 6 moves the rotation drive motor 3 in a direction parallel to the rotation shaft 22 and changes the distance X between the rotator 2 and the object to be heated 8. For example, when it is detected by the distance measurement part 4 that the object to be heated 8 is thermally expanded and the distance X is reduced, the rotation drive motor 3 is moved in a direction separated from the object to be heated 8, and the distance X can be maintained in a range where the heating efficiency is good.
[0048] In
[0049] The control part 7 is electrically connected in a wired or wireless manner to the rotation drive motor 3, the distance measurement part 4, the temperature measurement part 5 and the motor for movement 6 that are described above and controls each of them, and can be configured using, for example, a computer or the like.
[0050] The control part 7 controls the rotation drive motor 3 or the motor for movement 6 using the distance X measured by the distance measurement part 4. When it is detected that the object to be heated 8 is expanded and deformed by heating, the rotation drive motor 3 is stopped or the rotator 2 is moved by the motor for movement 6. Thereby, contact between the rotator 2 and the object to be heated 8 can be prevented. For example, when the distance X between the rotator 2 and the object to be heated 8 is so small that there is a risk of contact, the rotator 2 is moved in the direction separated from the object to be heated 8. At this time, if the distance X is maintained in the range where the heating efficiency is good, the heating efficiency can be improved.
[0051] The control part 7 can control the rotation drive motor 3 or the motor for movement 6 using the temperature of the object to be heated 8 which is measured by the temperature measurement part 5. For example, before the object to be heated 8 reaches the predetermined temperature, the distance X and the rotation number for a high heating efficiency are maintained, and the distance X and the rotation number are changed as the target temperature is approached, and thereby the temperature of the object to be heated 8 can be precisely controlled. At the time the object to be heated 8 reaches the predetermined temperature, the rotation drive motor 3 may be stopped and the rotator 2 may be moved in the direction separated from the object to be heated 8.
[0052] When the electromagnetic induction heating device 1 includes a plurality of the distance measurement parts 4, the control part 7 may control each portion using a maximum value or a minimum value among a plurality of the detected distances X.
[0053] The object to be heated 8 is made of a material which generates an eddy current by changing the magnetic field. The object to be heated 8 may be an object made of, for example, an aluminum alloy and the like containing aluminum, specifically, may be an aluminum sash, an aluminum foil or the like. In addition, an object made of a light alloy which is an alloy mainly composed of light metals such as aluminum, magnesium, titanium and the like can also be heated as the object to be heated 8.
[0054] In
Implementation Examples
[0055] The present invention is more specifically described below by implementation examples, but the present invention is not limited to these examples.
[0056] An electromagnetic induction heating device including the following magnets is used to heat the following object to be heated, and thermocouples which are arranged at positions 100 mm and 150 mm from a center of the object to be heated are used to measure the time required from start of the heating until the temperature of the object to be heated reaches 300 C. [0057] Object to be heated (ingot) [0058] Material: aluminum alloy [0059] Shape: trapezoidal columnar shape (width 97 mm, length 600 mm) [0060] Weight: 5.0 kg [0061] Specific heat: 900 (J/Kg K) (20 C.) [0062] Thermal conductivity: 204 (W/m K) [0063] Magnets (neodymium magnets) [0064] Shape: cylinder shape [0065] Diameter: 20 mm [0066] Height: 20 mm [0067] Magnetic flux density: 560-590 mT
Implementation Example 1
[0068] The electromagnetic induction heating device 1 is used which includes the rotator 2 with a diameter of 660 mm in which a plurality of neodymium magnets is equally arranged on the magnet surface (see
[0069] On the magnet surface, along eight circles C being concentric circles with diameters of 530 mm, 480 mm, 430 mm, 380 mm, 330 mm, 280 mm, 230 mm and 180 mm, 65, 59, 54, 46, 40, 35, 28 and 22 magnets 21 are respectively arranged in this order at equal intervals along the same circle C.
[0070] In the implementation example, the interval L1 between adjacent magnets 21 in the rotation direction is set to 5-6 mm (a distance (a pitch) between centers of the magnets 21 is set to 25-26 mm), and the interval D between adjacent concentric circles is set to 50 mm.
[0071] An inverter setting frequency is set to 90 Hz, and the time required for the temperature of the object to be heated to reach 300 C. from the start of the heating is measured.
Implementation Example 2
[0072] An electromagnetic induction heating device 1 is used which is only different from the electromagnetic induction heating device 1 of implementation example 1 in terms of a configuration that the numbers of the magnets 21 which are equally arranged along eight circles being concentric circles arranged at equal intervals on the magnet surface with diameters of 530 mm, 480 mm, 430 mm, 380 mm, 330 mm, 280 mm, 230 mm and 180 mm are 33, 30, 27, 23, 20, 17, 14 and 11.
[0073] The same as in implementation example 1, the distance X from the object to be heated 8 to the magnets 21 of the rotator 2 is set to 0.45 mm.
[0074] In the implementation example, because the numbers of the magnets 21 arranged in the rotator 2 are approximately half of the numbers in implementation example 1, the interval L1 between adjacent magnets 21 in the rotation direction is set to 30-32 mm (the distance (the pitch) between centers of the magnets 21 is set to 50-52 mm), and the interval D between adjacent concentric circles is set to an equal interval (50 mm).
[0075] The same as in implementation example 1, the inverter setting frequency is set to 90 Hz, and the time required for the temperature of the object to be heated to reach 300 C. from the start of the heating is measured.
[0076] Measurement results of implementation examples 1 and 2 are shown in table 1.
TABLE-US-00001 TABLE 1 Implementation Implementation example 1 example 2 Position (A) (B) (C) (A) (B) (C) Reaching 11 5 6 3 2 2 time minutes minutes minutes minutes minutes minutes and 33 and 16 and 26 and 11 and 1 seconds seconds seconds seconds second
[0077] It is known from the results shown in table 1 that by reducing the number of the magnets in half, the distance (the pitch) between each magnet increases, and the time for the object to be heated to reach 300 C. can be shortened.
[0078] In addition, it is known that by arranging the object to be heated shifted from the rotation center of the rotator 2, the heating efficiency is improved compared with arranging in a manner of overlapping the rotation center of the rotator 2.
[0079] It is known from the results shown in table 1 that as the number of the magnets which are arranged at equal intervals along the circles becomes greater, the object to be heated cannot be heated more efficiently, and the heating efficiency of the object to be heated is greatly affected by the distance between the magnets adjacent in the rotation direction of the rotator 2. Thus, in order to examine the effect of the distance between the magnets on the magnetic flux density, the magnetic fields at positions 12 mm away from a surface of each magnet 21 on the side of the object to be heated are measured for implementation example 1 in which 65 neodymium magnets are arranged along the circle with the diameter of 530 mm, and for implementation example 2 in which 33 neodymium magnets are arranged along the same circle. The measurement results are shown in table 2.
TABLE-US-00002 TABLE 2 Implementation Implementation example 1 example 2 Diameter of circle (mm) 530 530 Number of magnets 65 33 Diameter of magnets (mm) 20 20 Distance (mm) 6 30 Pitch (mm) 26 50 Peak value of magnetic flux density 55-94.2 78-109.2 (mT)
[0080] As shown in table 2, it is known that the magnetic flux density on the side of the object to be heated is higher in implementation example 2 having a relatively sparse arrangement of the magnets than in implementation example 1 having a relatively dense arrangement of the magnets. From this result, it can be stated that the reason for the improvement of the heating efficiency by arranging a reduced number of the magnets is that the magnetic flux density is increased.
Implementation Examples 3-5
[0081] Except that the inverter setting frequency is changed from 90 Hz to 60-80 Hz, the time required for heating the object to be heated to reach 300 C. is measured in the same way as implementation example 2. Measurement results of implementation examples 1 to 5 are shown in table 3.
TABLE-US-00003 TABLE 3 Implemen- Implemen- Implemen- Implemen- Implemen- tation tation tation tation tation example 1 example 2 example 3 example 4 example 5 Position (B) (B) (B) (B) (B) Distance 5-6 30-32 30-32 30-32 30-32 (mm) Frequency 90 90 60 70 80 (Hz) Reaching 5 minutes 2 minutes 3 minutes 2 minutes 2 minutes time and 16 and 0 and 14 and 43 and 21 seconds second seconds seconds seconds
[0082] As shown in implementation examples 2-5, it is known that the heating efficiency of the object to be heated is affected by a rotation speed (a frequency) of the rotator in which the magnets are arranged. However, in implementation example 3 in which the frequency is set to 60 Hz and the distance is set to 30-32 mm, the object to be heated can reach 300 C. in a time about 40% shorter than the time of implementation example 1 in which the frequency is set to 90 Hz and the distance is set to 5-6 mm. From this result, it can be stated that the interval L1 between the magnets 21 adjacent in the rotation direction affects the heating efficiency more greatly than the rotation speed of the rotator.
[0083] From the results of implementation examples 1-5, it is known that the magnetic flux density is increased and the heating efficiency is improved by arranging the magnets in a manner that the interval between the magnets adjacent in the direction in which the rotator is rotated becomes large, and it is known that the interval at which the magnets are arranged has a greater effect on the heating efficiency than the rotation number of the rotator. Thus, a relationship between the interval (the distance, the pitch) between the magnets and the magnetic flux density is examined as following.
Implementation Example 6
[0084]
[0085] As shown in
TABLE-US-00004 TABLE 4 Arrangement interval (mm) Peak (mT) Pitch P1 Distance L1 S N S N S N 30 10 83.2 19.6 45.5 42.3 28.8 76.0 35 15 78.7 36.9 53.4 50.6 45.5 68.3 40 20 74.7 49.2 60.6 53.4 54.1 68.1 45 25 72.6 52.2 64.9 60.9 59.4 65.3 50 30 71.7 53.2 66.8 60.7 61.1 61.7 55 35 71.7 59.1 67.4 62.7 65.1 66.9 60 40 70.7 59.7 65.5 61.3 65.9 64.3
Implementation Example 7
[0088] The following magnets are used to measure the magnetic flux density for the following magnets in the same way as implementation example 6. Results are shown in table 5. [0089] Magnets: a cylindrical shape with a diameter of 20 mma height of 20 mm, the magnetic flux density of the surface 567-598 mT (an average of 577 mT) [0090] Interval: 10-40 mm (distance L1), 30-60 mm (pitch P1)
TABLE-US-00005 TABLE 5 Arrangement interval (mm) Peak (mT) Pitch P1 Distance L1 S N S N S N 30 10 125.3 14.9 70.7 49.9 33.8 113.9 35 15 118.4 42.4 79.7 68.0 62.2 109.8 40 20 115.2 59.8 87.7 73.9 71.0 102.6 45 25 108.3 62.7 93.5 74.8 79.4 88.8 50 30 110.3 66.9 99.0 77.3 89.5 82.3 55 35 110.0 74.5 102.2 81.2 97.9 88.2 60 40 103.8 66.2 95.5 73.6 86.4 73.8
[0091] For implementation example 6 and implementation example 7, maximum flux densities of S poles and N poles for each arrangement interval are summarized and shown in table 6 and
TABLE-US-00006 TABLE 6 Maximum value of magnetic flux density (mT) Implementation Implementation Arrangement example 6 example 7 interval (mm) (20 10) (20 20) Pitch P1 Interval L1 S N S N 30 10 45.5 42.3 70.7 49.9 35 15 53.4 50.6 79.7 68.0 40 20 60.6 53.4 87.7 73.9 45 25 64.9 60.9 93.5 74.8 50 30 66.8 60.7 99.0 77.3 55 35 67.4 62.7 102.2 81.2 60 40 65.5 61.3 95.5 73.6
[0092] From the results shown in tables 4-6 and
Implementation Example 8
[0093] The following magnets are used to measure the magnetic flux density for the following magnets in the same way as implementation example 6. Results are shown in table 7. [0094] Magnets: a cylinder with a diameter of 10 mma height of 5 mm, the magnetic flux density of the surface 411-440 mT (an average of 425 mT) [0095] Interval: 27-45 mm (distance L1), 37-55 mm (pitch P1)
TABLE-US-00007 TABLE 7 Arrangement interval (mm) Peak (mT) Pitch P1 Distance L1 S N S N S N 37 27 19.9 16.4 18.9 17.8 17.2 20.2 38 28 20.4 16.5 17.7 17.5 18.5 20.7 39 29 20.2 17.9 18.8 18.2 17.5 19.5 40 30 20.2 17.4 19.0 18.0 18.2 19.0 41 31 19.7 16.7 18.5 18.4 18.4 18.8 42 32 20.0 18.0 19.2 18.4 18.4 19.4 43 33 19.2 16.7 19.7 18.2 17.7 18.1 43.4 33.4 19.9 17.5 19.1 17.3 18.1 21.0 44 34 19.8 18.2 18.9 17.7 18.1 19.2 45 35 18.9 17.1 19.5 19.0 18.2 19.7 50 40 19.9 18.5 19.4 18.7 18.7 19.6 52.4 42.4 19.6 18.4 18.6 17.9 17.7 18.6 55 45 19.4 17.8 18.6 18.1 18.0 18.4
Implementation Example 9
[0096] The following magnets are used to measure the magnetic flux density for the following magnets in the same way as implementation example 6. Results are shown in table 8. [0097] Magnets: a cylinder with a diameter of 10 mma height of 10 mm, the magnetic flux density of the surface 507-531 mT (an average of 521 mT) [0098] Interval: 27-45 mm (distance L1), 37-55 mm (pitch P1)
TABLE-US-00008 TABLE 8 Arrangement interval (mm) Peak (mT) Pitch P1 Distance L1 S N S N S N 37 27 35.0 26.4 31.1 29.3 29.1 33.1 38 28 35.1 26.4 32.4 29.3 29.5 33.3 39 29 35.2 28.9 31.0 29.5 30.8 33.5 40 30 35.3 27.9 32.3 29.9 31.2 33.2 41 31 34.7 29.1 33.2 29.0 31.2 33.1 42 32 34.5 29.5 32.7 31.2 31.1 33.4 43 33 34.6 28.7 32.5 29.9 30.6 31.6 43.4 33.4 34.9 28.1 32.7 30.7 31.3 33.7 44 34 34.8 28.3 32.2 30.5 30.0 32.6 45 35 34.3 29.7 31.6 29.6 31.6 33.0 50 40 29.7 20.5 28.1 20.8 26.8 20.8 52.4 42.4 31.0 22.9 30.4 23.8 29.0 25.7 55 45 31.4 24.3 29.4 24.4 29.3 24.8
[0099] For implementation example 8 and implementation example 9, maximum flux densities of S poles and N poles for each arrangement interval are summarized and shown in table 9 and
TABLE-US-00009 TABLE 9 Maximum value of magnetic flux density (mT) Implementation Implementation Arrangement example 8 example 9 interval (mm) (10 10) (10 20) Pitch P1 Interval L1 S N S N 37 27 18.9 17.8 31.1 29.3 38 28 17.7 17.5 32.4 29.3 39 29 18.8 18.2 31.0 29.5 40 30 19.0 18.0 32.3 29.9 41 31 18.5 18.4 33.2 29.0 42 32 19.2 18.4 32.7 31.2 43 33 19.7 18.2 32.5 29.9 43.4 33.4 19.1 17.3 32.7 30.7 44 34 18.9 17.7 32.2 30.5 45 35 19.5 19.0 31.6 29.6 50 40 19.4 18.7 28.1 20.8 52.4 42.4 18.6 17.9 30.4 23.8 55 45 18.6 18.1 29.4 24.4
[0100] From the results shown in tables 7-9 and
[0101] From the results shown in
INDUSTRIAL APPLICABILITY
[0102] The electromagnetic induction heating device of the present invention is useful as, for example, a device which heats dies or the like used during manufacturing of a semi-finished light alloy foil or aluminum sash to get a predetermined temperature suitable for a processing step in a short time.
REFERENCE SIGNS LIST
[0103] 1 electromagnetic induction heating device [0104] 2 rotator [0105] 21 magnet [0106] 22 rotation shaft [0107] 23 height adjustment part [0108] 3 rotation drive motor (rotation drive part) [0109] 4 distance measurement part [0110] 5 temperature measurement part [0111] 6 motor for movement [0112] 7 control part [0113] 8 object to be heated [0114] X distance between magnet and object to be heated [0115] L1 distance between magnets (interval between magnets) [0116] P1 pitch (distance between centers of magnets) [0117] O rotation center (center of concentric circle) [0118] C, C1, C2, C3 concentric circle [0119] R1, R2, R3 radius of concentric circle [0120] D, D1, D2 difference between diameters of adjacent concentric circles (intervals between concentric circles) [0121] diameter of magnet [0122] H height of magnet