This nonprovisional application claims priority under 35 U.S.C. §119(a) on Patent Applications Nos. 2005-41944 and 2005-256334, filed in Japan on Feb. 18, 2005 and Sep. 5, 2005 respectively. The entirety of each of the above documents is incorporated herein by reference.
1. Field of the Invention
The present invention relates to an induction heating apparatus for a metal plate such as a steel plate or an aluminum plate. The present invention particularly relates to an induction heating apparatus that heats a metal plate by generating an induced current therein using an induction coil surrounding the metal plate. The present invention also relates to an induction heating apparatus, which is capable of heating a metal plate with high efficiency irrespective of a thickness of the metal plate and irrespective of whether the metal plate is magnetic or non-magnetic. The present invention is further related to an induction heating apparatus, which can control a temperature distribution in the lateral (width) direction of the metal plate irrespective of a preexisting temperature distribution before heating to form a metal plate with a more uniform temperature distribution after heating.
2. Description of the Related Art
An indirect heating apparatus using gas or electricity, or a direct heating apparatus using induction heating has been used for heating a metal plate to control the quality of the metal material in the heat-treatment process. Since a direct heating apparatus has no thermal inertia, unlike an indirect heating apparatus, a direct heating apparatus can save the time which is required by an indirect heating apparatus to reach a stable furnace temperature, and can easily control the heating rate, for example, when a thickness of plate is changed. Therefore, a direct heating apparatus does not require changing of the metal plate transportation speed, which prevents productivity from being lowered.
There are two types of induction heating apparatus for a metal plate. One type is an LF type (Longitudinal Flux type), in which a metal plate is heated by generating a circular induced current therein in the cross-section using an induction coil, where an alternate current with a frequency ranging normally from 1 KHz to 500 KHz is applied, surrounding the metal plate.
In TF type heating, the induced current concentrates on a lateral end area of the metal plate and at the same time the current density in the vicinity of the end area is lowered, which easily causes a non-uniform temperature distribution in a lateral direction after heating. In particular, it becomes more difficult to provide a uniform heating when the positional relationship between the core of the induction coil and the metal plate is changed by shifting a width of the metal plate or by a snaking of the metal plate. In the background art, a technology that uses a rhombus-shaped coil was proposed so that the flux can always penetrate over an entire width of the plate by tilting the rhombus-shaped coil when the width of the metal plate is changed. However, because this technology uses leakage flux from the induction coil, it requires the metal plate and the induction coil to be close to each other. In addition, installation of a rotation mechanism on the induction heating apparatus where a large amount of current is supplied increases the difficulty in carrying out the technology on industrial scale.
The LF type heating is a method for heating a metal plate surrounded by an induction coil, which can make sure that a circular induced current is generated in the metal plate so as to heat the plate. An induced current that is generated in the cross-section of the metal plate in an LF type is concentrated at the depth “d” expressed in the following expression:
d[mm]=5.03×10+5×(ρ/μRF)0.5 (1)
where d is the induced current penetration depth [mm], ρ is the specific resistance [Ωm], μr is the relative magnetic permeability, and f is the frequency [Hz] for heating.
An induced current penetration depth increases as a temperature of the metal increases because the specific resistance increases when the temperature of the metal increases. The relative magnetic permeability of ferromagnetic material or paramagnetic material decreases as the temperature becomes closer to the Curie point, and finally becomes 1 at a temperature above the Curie point. This means that the induced current penetration depth increases as the temperature increases. Since the relative magnetic permeability of a non-magnetic material is 1, its induced current penetration depth is larger compared to that of a magnetic material.
In LF type induction heating, if the induced current penetration depth is large and yet a thickness of the metal plate is thin, the induced current generated in an upper portion of the metal and the induced current generated in a lower portion of the metal cancel each other. This leads to heating that has a low efficiency.
For example, if a heating frequency of 10 KHz is used, the induced current penetration depth at room temperature is about 1 mm with aluminum of non-magnetic material, about 4.4 mm with stainless steel 304 (SUS304) and about 0.2 mm with steel of magnetic material. The current penetration depth of steel at temperature above the Curie point (at about 750° C.) is about 5 mm. Most steel plates for automobiles and home electric appliances, which are major commercial products that use metal plates, have a thickness of not more than 2 mm. Therefore, it is usually difficult to heat such metal plate with high efficiency without the induced currents in the upper and lower portions of the metal plate being canceled as mentioned above. It could be thought to increase the frequency of the AC current supplied to the LF type induction heating apparatus to several hundred KHz in order to make the depth of the induced current penetration shallower, so that canceling the induced currents can be avoided; however, it is not very practical to use a large current power source with such a high frequency on an industrial scale.
It has been proposed to use an induction heating apparatus that uses an induction coil surrounding a metal plate, which is capable of heating a metal plate with high efficiency even if the metal plate is at a high temperature and/or is a thin metal plate. In such induction heating apparatus, an induction coil located above the metal plate (upper induction coil) and another induction coil located below the metal plate (lower induction coil) are arranged parallel to each other, so as to be set respectively in different positions in a longitudinal direction of the metal plate. In other words, two projected images of the upper induction coil and the lower induction coil, which are respectively formed by vertically projecting the two induction coils onto the metal plate, are parallel to each other and in a different position in the longitudinal direction of the metal plate.
However, in the use of such an induction heating apparatus where the upper and lower induction coils are set in different positions in the longitudinal direction of the metal plate, an edge area of the metal plate in the width direction can become overheated compared to a central area of the metal plate in the width direction. This can result in a non-uniform temperature distribution as a finishing temperature in the transverse direction of the metal plate.
This phenomenon is experienced because a width of the induced current path in the edge area of the metal plate (corresponding to “d2” in
In the use of such an induction heating apparatus where upper and lower induction coils are set in different positions in a longitudinal direction of the metal plate, if the temperature at the edge area is lower than that, of the central area of the metal plate before starting the induction heating, non-uniformity in the temperature distribution can be reduced after the induction heating. However, if the temperature distribution is uniform or the temperature at the edge area is higher than that of the central area because of a previous process, a non-uniform temperature distribution in the width direction will be obtained after the induction heating.
An object of the present invention is to solve some or all of the problems of the conventional induction heating apparatus mentioned above. An embodiment of the present invention is capable of heating a metal plate with high efficiency, even where the temperature of the metal plate is high above the Curie point, the metal plate is thin and/or the metal plate is made of a non-magnetic, non-ferrous metal with a low specific resistance such as aluminum or copper. In addition, an embodiment of the present invention is capable of providing a metal plate with a more uniform temperature distribution in the width direction, independent of the temperature distribution provided by a previous process. An embodiment of the present invention can make it easier to realize a desired temperature distribution, even when the width of the metal plate to be heated is changed, without preparing a plurality of induction coils to cope with the change in the width of the metal plate. An embodiment of the present invention can also improve a non-uniform temperature distribution caused by snaking of the metal plate. Another embodiment of the present invention provides a technology that has a great flexibility in the distance between the upper and lower induction coils, the width of the induction coils and the heat release value in the longitudinal direction of a metal plate.
The above objects of the present invention can be accomplished by an induction heating apparatus for heating a traveling metal plate, comprising: an induction coil for surrounding the metal plate, said induction coil including an upper portion for being located above the metal plate and a lower portion for being located below the metal plate, said upper and lower portions of the induction coil being spaced from each other in a longitudinal direction of the metal plate at least at one position in a transverse direction of the metal plate, wherein a distance in the longitudinal direction of the metal plate between the upper portion and the lower portion of the induction coil varies across a transverse direction of the metal plate.
The above objects of the present invention can also be accomplished by an induction heating apparatus for heating a traveling metal plate, comprising: an induction coil having an upper portion for being located above the metal plate and a lower portion for being located below the metal plate, said upper and lower portions of the induction coil being spaced from each other in a longitudinal direction of the metal plate at least at one position in a transverse direction of the metal plate; and an AC power source, each of the upper and lower portions of the induction coil being connected at one end thereof to the AC power source, wherein a distance in the longitudinal direction of the metal plate between the upper portion and the lower portion of the induction coil varies across a transverse direction of the metal plate.
In the present invention, the meaning of a traveling metal plate is not limited to a metal plate traveling in one direction, but includes a reciprocating movement of the metal plate.
In the present invention, an induction coil is a collective term that includes a coil formed by a tube, a wire, a plate or the like of an electric conductive material surrounding a metal plate by a single turn or more. In addition, surrounding of the metal plate is not limited to a specific form such as circular or square. With regard to the materials for the electric conductor, non-magnetic and low resistance materials such as copper, copper alloy or aluminum are preferable.
With regard to the metal plate of the present invention, a magnetic material such as steel, non-magnetic materials such as aluminum or copper and steel in a non-magnetic state at a temperature above the Curie point can be used.
In the present invention, the traverse direction of the metal plate means a direction perpendicular to a traveling direction of the metal plate, and the longitudinal direction of the metal plate means the traveling direction of the metal plate.
In the present invention, an edge of the metal plate is an end of the metal plate in a transverse direction. An edge area of the metal plate is the upper (top) of lower (bottom) surface of the metal plate close to or in the vicinity of the edge of the metal plate.
In the present invention, the width of an induction coil means a width of the induction coil in the longitudinal direction of the metal plate.
In the present invention, a distance in the longitudinal direction between the induction coil located above the metal plate and the induction coil located below the metal plate is defined as a distance between the two projected images of the induction coil located above and located below the metal plate, which are respectively formed by vertically projecting each induction coil onto the metal plate.
Hereinafter “an induction coil located above the metal plate” may be referred to as an “upper portion of the induction coil” or simply an “upper induction coil,” and “an induction coil located below the metal plate” may be referred to as a “lower portion of the induction coil” or simply a “lower induction coil.”
A distance in the longitudinal direction between the upper and lower induction coils is defined as “L” in
In the case where a width of the upper induction coil and a width of the lower induction coil are different, a starting point to determine the distance “L” is an edge (end) of the vertically projected image of the wider induction coil.
Further scope of applicability of the present invention will become apparent from the detailed description given hereinafter. However, it should be understood that the detailed description and specific examples, while indicating preferred embodiments of the invention, are given by way of illustration only, since various changes and modifications within the spirit and scope of the invention will become apparent to those skilled in the art from this detailed description.
The present invention will become more fully understood from the detailed description given hereinbelow and the accompanying drawings which are given by way of illustration only, and thus are not limitative of the present invention, and wherein:
The present invention will now be described with reference to the accompanying drawings. All of the drawings illustrate a single turn of the induction coil surrounding a metal plate. However, the number of turns of the induction coil in the present invention is not limited to specific number.
When the upper induction coil and the lower induction coil are located so as to be away from each other in the longitudinal direction of the metal plate, in particular at the central area shown in
A maximum distance between the upper and lower induction coils (In
When an appropriate distance is set in the central area in the transverse direction of the metal plate, the central area of the metal plate can be effectively heated. However, if the same distance is set at the edge area of the metal plate, the edge area of the metal plate is overheated as previously mentioned, forming a non-uniform temperature distribution in the transverse direction of the metal plate.
In the example shown in
In
The induced current passing near the edge of the metal plate tends to follow a flow path closer to the central area of the metal plate so that the inductance between the induced current and the primary current running through the induction coil located at the edge of the metal plate can be reduced. In other words, an upper induced current induced by the upper induction coil and a lower induced current induced by the lower induction coil tend to connect to each other along the shortest path. This provides a relatively wider passage of induced current flow near the edge of the metal plate to restrain the increase of current density near the edge. Thus, when the upper and the lower induction coils have a portion that extends oblique to the transverse direction at edge area, overheating at the edge area can be effectively restrained relative to an induction coil without such an oblique portion.
While keeping the distance between the upper and lower induction coils provides the central area of the metal plate with an efficient heating, a relatively smaller distance and oblique arrangement of the induction coil at the edge area of the metal plate restrains overheating at the edge area. As a result, in the example of
An optimum distance between the upper and lower induction coils at different positions in the transverse direction should be determined after taking into consideration a preexisting temperature distribution of the metal plate to be heated. It is possible to have three different representative preexisting temperature distribution patterns in a metal plate, for example, a metal plate that has a flat temperature distribution (the same temperature at the central area and the edge area), a metal plate, that has a temperature distribution that is slightly lower at the edge area relative to the central area, or a metal plate that has a temperature distribution that is slightly higher at the edge area relative to the temperature in the central area.
In the present invention, an upper part of the induction coil located above the metal plate and a lower part of the induction coil located below the metal plate are arranged so as to be located respectively in different positions in the longitudinal direction of the metal plate at least at one position in the transverse direction of the metal plate, wherein a distance between the different positions varies in the transverse direction. The shape of the induction coil is not limited to the one shown in
In the example shown in
When the metal plate to be fed in an induction heating apparatus has a preexisting temperature distribution, where the edge area temperature is slightly higher than that of the central area (central area temperature is slightly lower than that of the edge area), the apparatus of
In the example shown in
Reference numerals 7, 8 and 9 represent a conductive member, an AC power supply and an induction coil located near the edge of metal plate, respectively. In the example of
In
In order to obtain a necessary heat divergence in a practical operation of the heating apparatus of the present invention, it is possible to determine the distance and/or the width of the induction coil for each position in the transverse direction in advance through an electromagnetic field analysis. However, because of a fluctuation in a previous process, a metal plate to be fed into the induction heating apparatus of the present invention may have an initial temperature variation. Therefore, the necessary heat divergence may not be obtained even if the predetermined distance and/or the width of the induction coil are adopted.
If the distance between upper and lower coils increases, it helps to avoid Cancellation of induced currents in the metal plate and an increase in the heating time, which leads to an increase in the heat divergence. In another embodiment of the present invention, where the distance is adjustable, it is possible to obtain a desired temperature independently of the preexisting temperature state given by the previous process by adjusting the distance to the temperature variation of the metal to be fed in.
As with some other examples, the upper induction coil 2a and the lower induction coil 2b in
The heat divergence is controlled by changing the amount of distance between the upper and lower induction coils as set forth above. Therefore, for example, the amount of distance can be changed according to the temperature of the metal plate measured by a thermometer located upstream of the induction heating apparatus.
In order to obtain a heat divergence needed at each position in the transverse direction, it is possible to determine the distance and/or the width of the induction coil for each position in the transverse direction in advance through electromagnetic field analysis. However, when a width of the metal plate is changed in accordance with a manufacturing lot-change, a metal plate with a uniform temperature distribution may not be obtained, even if the above predetermined amount of the distance for each position in the transverse direction of induction coil are adopted.
In
A lower induction coil includes a plurality of edge area conductors A-A′ to I-I′ and J-J′ to R-R′ each of which is insulated and independent from each other. Each of the edge area conductors A-A′ to I-I′ and J-J′ to R-R′ is selectably connected to a central area connecting conductor 9f.
As with other examples, in the embodiment of
In the embodiment shown in
In comparison with the case shown in
Thus, even when the width of the metal plate to be heated changes from a narrower one to a wider one (from the case shown in
The induction heating apparatus of the present invention can be used stand-alone, as a process set before/after preheating a furnace of an indirect heating type or as a process combined in series with a conventional LF (Longitudinal Flux) type heating apparatus so as to prevent interference between the induction coils. The induction heating apparatus of the present invention can be used with high efficiency for heating a metal plate even in the region of a large induced current penetration depth at a temperature above the Curie point, since the upper induction coil and the lower induction coil are located at a distance from each other in the longitudinal direction of the metal plate (there is a distance between the upper and lower induction coils in terms of the projected images of both coils). In view of above, the induction heating apparatus of the present invention can be used more preferably for a metal plate that has a temperature above the Curie point while a low cost indirect heating furnace can be used for a metal plate that has a temperature sufficiently lower than the Curie point.
A heating test of the present invention was carried out with a metal plate made of non-magnetic SUS304 steel plate (thickness: 0.2 mm, width: 600 mm). The test will be described with reference to
The distance at the edge area of the steel plate is adjustable by changing an oblique angle of the induction coil in the edge area. More specifically, as shown in
The steel plate is heated by the induction heating apparatus while the distance in the edge area as described above is changed, and the temperature of the steel plate at both the central area and the edge area (a position 50 mm away from edge of the steel plate) was measured at the exit of the induction heating apparatus using a two-dimensional infrared thermometer to calculate a value of {(the temperature at the edge area)−(the temperature at the central area)}. The results are shown in TABLE 1 below.
It can be found from the above results that the temperatures of the edge area and the central area can be changed (the temperature distribution can be changed) by changing the distance between the upper induction coil and the lower induction coil at the edge area. In
In
A heating test of the present invention was also carried out with respect to a cold rolled steel plate (thickness: 0.6 mm, width: 600 mm). The AC power supply (not shown) was 50 KHz, and a capacitor having a 200 KW capacitance was adjusted to match the induction coil to be used. The traveling speed of the steel plate was 2 m/min.
An induction coil shown in
The temperature of the steel plate at both the central area and the edge area (at a position 50 mm away from the edge of the steel plate) was measured at the exit of the induction coils using an infrared thermometer.
The results are shown in TABLE 2, where the combinations of the selected induction coil conductors and the resulting difference between the temperatures at the edge area and the central area, i.e., (the temperature at the edge area)-(the temperature at the central area). The upper induction coil and the lower induction coil are away from each other in the longitudinal direction of the metal plate. Therefore, heating in a non-magnetic region of 750° C. or more can be performed.
In Example F, two parallel-to-transverse-direction induction coil conductors and two oblique induction coil conductors are selected both with respect to the upper and lower induction coils, where the upper and lower oblique conductors intersect (in terms of the projected images) at a position inside the width of the steel plate. In Example G, similarly to Example F, two parallel-to-transverse-direction induction coil conductors and two oblique induction coil conductors are selected. However, the upper and lower oblique conductors intersect (in terms of the projected images) over (in the vicinity of) the edge of the steel plate. In Example H, similarly to Examples F and G, two parallel-to-transverse-direction induction coil conductors and two oblique induction coil conductors are selected. However, the upper and lower oblique conductors intersect (in terms of the projected images) outside the edge of the steel plate. In Examples F, G and H, the selection of the conductors is made so that the distance between the upper and lower coils in the edge area of the steel plate becomes larger in turn from F to H.
As can be understood from the data “(the temperature at the edge area)-(the temperature at the central area)” in TABLE 2, the temperature distribution in the transverse direction is more uniform in Example F (where the upper and lower oblique conductors intersect at the position inside the width of the steel plate) than in Example H (where the upper and lower oblique conductors intersect outside the edge of the steel plate).
In Example I, two parallel-to-transverse-direction induction coil conductors and three oblique induction coil conductors are selected with upper and lower induction coils. In Example J, three parallel-to-transverse-direction induction coil conductors and three oblique induction coil conductors are selected with upper and lower induction coils. Since the current density in the central area is higher in Example I than in Example J, the heat divergence in the central area is larger in Example I than in Example J. As a result, “(the temperature at the edge area)-(the temperature at the central area)” is smaller in Example I than in Example J. However, the temperature at the edge area is still slightly overheated.
In Example K, three parallel-to-transverse-direction induction coil conductors and two oblique induction coil conductors are selected with upper and lower induction coils. In Example L, one parallel-to-transverse-direction induction coil conductor and two oblique induction coil conductors are selected with upper and lower induction coils. Since the current density in the central area is higher in Example L than in Example K, the heat divergence in the central area is larger in Example L than in Example K. As a result, “(the temperature at the edge area)-(the temperature at the central area)” is smaller in Example L than in Example K. However, the temperature at the edge area is still slightly overheated.
As described above, various temperature distributions can be realized by selecting the conductors and the number thereof.
An induction heating apparatus as shown in
In Examples M and N, a distance between the upper and lower induction coils was set to 200 mm in the central area, and a distance at the edge area when an 800 mm steel plate was used was 170 mm in Example M (corresponding to
In Example M, since the distance at the edge area is smaller than in the central area, the temperature in the edge area can be generally lowered relative to that in the central area. In the case of the 600 mm width steel plate, the distance at the edge area (measurement point is 50 mm away from the edge of the steel plate) is relatively larger to that in the case of the 800 mm width steel plate, which leads to a longer heating time and a relative increase in temperature at the edge area. On the contrary, in Example N, where the distance at the edge area becomes larger than in the central area, the heat divergence also becomes relatively larger, which leads to a higher temperature at the edge area relative to that in the central area.
As described above, the present invention is capable of heating a metal plate with high efficiency, even where the temperature of the metal plate is high above the Curie point, the metal plate is thin and/or the metal plate is made of a non-magnetic non-ferrous metal with a low specific resistance such as aluminum or copper. Also, the present invention is capable of providing a metal plate with a flatter temperature distribution in the width direction independently of any preexisting initial temperature distribution provided by a previous process. The present invention can make it easier to control an amount of heat divergence according to an initial temperature condition of the metal plate to be heated and/or realize a desired temperature distribution even when the width of metal plate to be heated is changed.
The invention being thus described, it will be obvious that the same may be varied in many ways. Such variations are not to be regarded as a departure from the spirit and scope of the invention, and all such modifications as would be obvious to one skilled in the art are intended to be included within the scope of the following claims.
Number | Date | Country | Kind |
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2005-041944 | Feb 2005 | JP | national |
2005-256334 | Sep 2005 | JP | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/JP2006/002676 | 2/9/2006 | WO | 00 | 8/14/2007 |