The present application claims priority from Japanese patent application JP 2019-105932 filed on Jun. 6, 2019, the content of which is hereby incorporated by reference into this application.
The present disclosure relates to a method for manufacturing an alloy ribbon piece obtained by crystallizing an amorphous alloy ribbon piece.
Conventionally, amorphous alloy ribbon pieces processed from a continuous amorphous alloy ribbon manufactured by a method such as a single roll method and a twin roll method are used for, for example, a motor core. Since a nanocrystalline alloy ribbon piece obtained by crystallizing the amorphous alloy ribbon piece is a soft magnetic material that can provide a high saturation magnetic flux density and a low coercivity at the same time, recently, the nanocrystalline alloy ribbon piece has been used for those cores.
The nanocrystalline alloy ribbon piece is manufactured by heating the amorphous alloy ribbon piece to a temperature at which the amorphous alloy is crystallized. For example, JP 2018-50053 A discloses a method of crystallizing an amorphous alloy ribbon piece through a heating process of heating the amorphous alloy ribbon piece to the temperature of 390° C. or more and 480° C. or less as a method for manufacturing an alloy ribbon piece obtained by crystallizing the amorphous alloy ribbon piece through heating.
However, in the method for manufacturing alloy ribbon piece obtained by crystallizing the amorphous alloy ribbon piece through heating, when the temperature is simultaneously increased at the whole amorphous alloy ribbon piece to a temperature at which the crystallization of the amorphous alloy is completed in a wide area of the alloy ribbon piece, a problem possibly arises in that, for example, self-heating due to the crystallization simultaneously occurs in the wide area of the amorphous alloy ribbon piece to cause excessive temperature increase on the amorphous alloy ribbon piece, resulting in burning of the alloy ribbon piece. Therefore, a method for easily manufacturing the nanocrystalline alloy ribbon piece having excellent soft magnetic properties without causing such a problem is desired.
The present disclosure has been made in view of such an aspect, and provides a method for manufacturing an alloy ribbon piece that ensures easily manufacturing the alloy ribbon piece having excellent soft magnetic properties.
To solve the above-described problem, a method for manufacturing an alloy ribbon piece according to the present disclosure is a method for manufacturing an alloy ribbon piece obtained by crystallizing an amorphous alloy ribbon piece. The method includes: preparing an amorphous alloy ribbon piece; increasing a temperature of the amorphous alloy ribbon piece to a crystallization starting temperature; and increasing the temperature of the amorphous alloy ribbon piece from the crystallization starting temperature to a crystallization process termination temperature equal to or less than a crystallization completion temperature. A temperature increase rate of the amorphous alloy ribbon piece in the increasing of the temperature of the amorphous alloy ribbon piece from the crystallization starting temperature to the crystallization process termination temperature satisfies a formula (1) below where a self-heating amount of the amorphous alloy ribbon piece per unit time is ΔQself, a heat discharge amount of the amorphous alloy ribbon piece per unit time is ΔQout, a mass and a specific heat of the amorphous alloy ribbon piece are m and c, respectively, and a temperature increase width of the amorphous alloy ribbon piece per unit time is ΔT.
ΔQself≤ΔQout+mcΔT (1)
The present disclosure ensures facilitated manufacturing of the alloy ribbon pieces having excellent soft magnetic properties.
The following describes an embodiment of a method for manufacturing an alloy ribbon piece according to the present disclosure.
The method for manufacturing alloy ribbon piece according to the embodiment is a method for manufacturing an alloy ribbon piece obtained by crystallizing an amorphous alloy ribbon piece. The method includes: a preparation step of preparing the amorphous alloy ribbon piece; a first temperature increasing step of increasing a temperature of the amorphous alloy ribbon piece to a crystallization starting temperature; and a second temperature increasing step of increasing the temperature of the amorphous alloy ribbon piece from the crystallization starting temperature to a crystallization process termination temperature equal to or less than a crystallization completion temperature. A temperature increase rate of the amorphous alloy ribbon piece in the second temperature increasing step satisfies a formula (1) below where a self-heating amount of the amorphous alloy ribbon piece per unit time is ΔQself, a heat discharge amount of the amorphous alloy ribbon piece per unit time is ΔQout, a mass and a specific heat of the amorphous alloy ribbon piece are m and c, respectively, and a temperature increase width of the amorphous alloy ribbon piece per unit time is ΔT.
ΔQself≤ΔQout+mcΔT (1)
Here, the “crystallization starting temperature” means a temperature at which the crystallization of the amorphous alloy starts at any portion of the amorphous alloy ribbon piece when the temperature of the amorphous alloy ribbon piece increases, and the “crystallization completion temperature” means a temperature at which the crystallization of the amorphous alloy is completed at all the portions of the amorphous alloy ribbon piece when the temperature of the amorphous alloy ribbon piece increases. The crystallization of the amorphous alloy differs depending on the material and the like of the amorphous alloy, and in the case of a Fe-based amorphous alloy, the crystallization of the amorphous alloy means that, for example, a fine bccFe crystal is precipitated. The “crystallization process termination temperature” means a temperature which is equal to or less than the crystallization completion temperature and is set such that characteristic values, such as a saturation magnetic flux density and a coercivity, of the alloy ribbon piece obtained by the crystallization of the amorphous alloy ribbon piece are desired values.
The “temperature increase rate of the amorphous alloy ribbon piece in the second temperature increasing step” is a temperature increase rate of the amorphous alloy ribbon piece in the temperature increase process from the crystallization starting temperature to the crystallization process termination temperature (hereinafter simply referred to as “temperature increase process” in some cases), and means a rate of the temperature increase caused by a heat transferred from an external environment to the amorphous alloy ribbon piece. Therefore, the “temperature increase rate of the amorphous alloy ribbon piece in the second temperature increasing step” does not include a rate of the temperature increase caused by a heat generated by the self-heating due to the crystallization of the amorphous alloy ribbon piece.
Furthermore, the “self-heating amount of the amorphous alloy ribbon piece per unit time” means an amount of a heat generated by the self-heating due to the crystallization of the amorphous alloy ribbon piece per unit time in the temperature increase process. The “heat discharge amount of the amorphous alloy ribbon piece per unit time” means an amount of a heat discharged from the amorphous alloy ribbon piece to the external environment per unit time in the temperature increase process. Furthermore, the “temperature increase width of the amorphous alloy ribbon piece per unit time” means a temperature increase width when the temperature of the amorphous alloy ribbon piece is increased by the heat transferred from the external environment to the amorphous alloy ribbon piece per unit time in the temperature increase process. Therefore, the “temperature increase width of the amorphous alloy ribbon piece per unit time” does not include a temperature increase width when the temperature of the amorphous alloy ribbon piece is increased by the heat generated by the self-heating due to the crystallization of the amorphous alloy ribbon piece per unit time in the temperature increase process.
First, the method for manufacturing alloy ribbon piece of the embodiment will be described with an example.
Here,
In the example of the embodiment, first, as illustrated in
Next, as illustrated in
Next, as illustrated in
Next, as illustrated in
For one amorphous alloy ribbon piece, the temperature at which the amorphous alloy crystallizes is different for each portion. That is, one amorphous alloy ribbon piece has a portion where the amorphous alloy crystallizes at a relatively low temperature and a portion where the amorphous alloy crystallizes at a relatively high temperature. Accordingly, during the temperature increase of the amorphous alloy ribbon piece 1, as seen from the DSC curve illustrated in
On the premise of the characteristic of crystallization reaction of amorphous alloy ribbon piece, since the heat is sufficiently discharged by the clearance S for each of the amorphous alloy ribbon pieces 2A, the temperature increase rate of the amorphous alloy ribbon piece 2A in the second temperature increasing step satisfies the formula (1) below where a self-heating amount of the amorphous alloy ribbon piece 2A per unit time is ΔQself, a heat discharge amount of the amorphous alloy ribbon piece 2A per unit time is ΔQout, a mass and a specific heat of the amorphous alloy ribbon piece 2A are m and c, respectively, and a temperature increase width (temperature increase width of the amorphous alloy ribbon piece 2A per unit time described above) when the temperature of the amorphous alloy ribbon piece 2A is increased by the heat transferred from the external environment inside the heating furnace F to the amorphous alloy ribbon piece 2A per unit time is ΔT. Note that, the temperature increase rate of the amorphous alloy ribbon piece 2A in the second temperature increasing step is the temperature increase rate of the amorphous alloy ribbon piece 2A in the temperature increase process from 419.19° C. (crystallization starting temperature) to 460° C. (crystallization process termination temperature) in the second temperature increasing step, and means the rate of the temperature increase due to the heat transferred from the external environment inside the heating furnace F to the amorphous alloy ribbon piece 2A.
ΔQself≤ΔQout+mcΔT (1)
The second temperature increasing step provides a plurality of alloy ribbon pieces 2C where the plurality of amorphous alloy ribbon pieces 2A have been each entirely crystallized.
Next, as illustrated in
Here, conventional examples 1 to 4 will be described as examples according to the conventional method for manufacturing alloy ribbon piece.
In the conventional example 1, as indicated by the temperature history B of
In the conventional example 2, as indicated by the temperature history C of
In the conventional example 3, as indicated by the temperature history D of
In the conventional example 3, on the premise of the above-described characteristic of crystallization reaction of amorphous alloy ribbon piece, for each of the amorphous alloy ribbon pieces 2A, the temperature increase rate of the amorphous alloy ribbon piece 2A in the second temperature increasing step is high compared with the one example of the embodiment. Therefore, the formula (2) below is satisfied when the meanings of ΔQself, ΔQout, m, c, and ΔT are similar to those of the formula (1), and further, the temperature increase width of the temperature increase of the amorphous alloy ribbon piece 2A caused by the heat generated by the self-heating due to the crystallization of the amorphous alloy ribbon piece 2A per unit time is ΔTself.
ΔQself=ΔQout+mcΔTself>ΔQout+mcΔT (2)
When the temperature increase rate of the plurality of amorphous alloy ribbon pieces 2A in the second temperature increasing step satisfies the formula (2) but does not satisfy the formula (1), a difference (ΔQself−ΔQout) between the self-heating amount and the heat discharge amount of the amorphous alloy ribbon pieces 2A in the unit time becomes larger than a heat amount mcΔT necessary for the temperature increase of the amorphous alloy ribbon pieces 2A at the temperature increase width ΔT due to the heat transferred from the external environment inside the heating furnace F to the amorphous alloy ribbon pieces 2A per unit time. Therefore, the temperature of the amorphous alloy ribbon pieces 2A increases by the temperature increase width ΔTself corresponding to the difference (ΔQself−ΔQout) between the self-heating amount and the heat discharge amount that exceeds the temperature increase width ΔT by the heat transferred from the external environment to the amorphous alloy ribbon pieces 2A per unit time. Accordingly, because of the above-described characteristic of crystallization reaction of amorphous alloy ribbon piece, the self-heating due to the crystallization occurs in chain reaction at each of the plurality of amorphous alloy ribbon pieces 2A. Consequently, a problem arises in that, for example, the temperatures of the amorphous alloy ribbon pieces 2A are each excessively increased to cause the amorphous alloy ribbon pieces 2A to be burnt.
In the conventional example 4, as indicated by the temperature history E of
In contrast, in the one example of the embodiment, since the temperature increase rate of the amorphous alloy ribbon pieces 2A in the second temperature increasing step is low compared with the conventional example 3 to satisfy the formula (1), the difference (ΔQself−ΔQout) between the self-heating amount and the heat discharge amount of the amorphous alloy ribbon pieces 2A per unit time becomes equal to or less than the heat amount mcΔT necessary for the temperature increase of the amorphous alloy ribbon pieces 2A at the temperature increase width ΔT due to the heat transferred from the external environment inside the heating furnace F to the amorphous alloy ribbon pieces 2A per unit time. Therefore, unlike the conventional example 3, the temperature of the amorphous alloy ribbon pieces 2A does not increase at the temperature increase width exceeding the temperature increase width ΔT due to the heat transferred from the external environment to the amorphous alloy ribbon pieces 2A per unit time. Accordingly, the occurrence in chain reaction of the self-heating due to the crystallization at each of the plurality of amorphous alloy ribbon pieces 2A because of the characteristic of crystallization reaction of amorphous alloy ribbon piece is suppressed, thereby ensuring suppression of the excessive temperature increase of each of the amorphous alloy ribbon pieces 2A.
Furthermore, in the one example of the embodiment, unlike the conventional example 4, the temperature increasing time of the amorphous alloy ribbon pieces 2A in the second temperature increasing step is not excessively long, thereby ensuring suppression of the growth of the crystallized crystal grains for a long period of time to be coarsened. Accordingly, the nanocrystalline alloy ribbon piece 2C having excellent soft magnetic properties can be manufactured.
Accordingly, the one example of the embodiment can suppress the excessive temperature increase and the coarse crystal grains to manufacture the nanocrystalline alloy ribbon piece having excellent soft magnetic properties only by adjusting the temperature increase rate of the amorphous alloy ribbon piece 2A in the second temperature increasing step without the use of complicated heating facilities.
According to the embodiment, as the one example of the embodiment, the excessive temperature increase is suppressed only by adjusting the temperature increase rate of the amorphous alloy ribbon piece in the second temperature increasing step so as to satisfy the formula (1), thereby ensuring easily manufacturing the alloy ribbon piece having excellent soft magnetic properties. Furthermore, by adjusting the temperature increase rate of the amorphous alloy ribbon piece in the second temperature increasing step to the predetermined rate or more, the coarse crystal grains can be suppressed to easily manufacture the alloy ribbon piece having further excellent soft magnetic properties.
Subsequently, the method for manufacturing alloy ribbon piece according to the embodiment will be described in detail, mainly the conditions in respective steps.
In the preparation step, the amorphous alloy ribbon piece is prepared.
Here, the “amorphous alloy ribbon piece” means, for example, a ribbon piece, which is used for a component such as a core in a final product such as a motor, punched in a desired shape from, for example, a continuous sheet-shaped amorphous alloy ribbon manufactured by a common method such as a single roll method and a twin roll method.
While the amorphous alloy ribbon piece is not specifically limited insofar as the amorphous alloy ribbon piece is a ribbon piece punched in the desired shape, for example, a ribbon constituting a stator core or a rotor core of a motor and a ribbon obtained by further dividing the ribbon constituting the stator core in a circumferential direction are included.
While the material of the amorphous alloy ribbon piece is not specifically limited insofar as the material is the amorphous alloy, for example, a Fe-based amorphous alloy, a Ni-based amorphous alloy, and a Co-based amorphous alloy are included. Especially, the Fe-based amorphous alloy and the like is used in some embodiments. Here, the “Fe-based amorphous alloy” means an amorphous alloy that contains Fe as a main component, and contains impurities such as B. Si, C, P, Cu, Nb, and Zr. The “Ni-based amorphous alloy” means an amorphous alloy that contains Ni as a main component. The “Co-based amorphous alloy” means an amorphous alloy that contains Co as a main component.
The Fe-based amorphous alloy may have, for example, a Fe content in a range of 84 atomic percent or more, and may have a larger Fe content. This is because a magnetic flux density of the alloy ribbon piece obtained by crystallizing the amorphous alloy ribbon piece differs depending on the Fe content.
While the plane size of the amorphous alloy ribbon piece is not specifically limited, for example, general plane sizes of a ribbon constituting a stator core or a rotor core of a motor and a ribbon obtained by further dividing the ribbon constituting the stator core in a circumferential direction are included. While the thickness of the amorphous alloy ribbon piece is not specifically limited, the thickness is different depending on the material and the like of the amorphous alloy ribbon piece. When the material is the Fe-based amorphous alloy, the thickness is, for example, in a range of 10 μm or more and 100 μm or less, and is in a range of 20 μm or more and 50 μm or less in some embodiments.
In the first temperature increasing step, the temperature of the amorphous alloy ribbon piece is increased to the crystallization starting temperature.
While the crystallization starting temperature differs depending on the material and the like of the amorphous alloy ribbon piece, when the material is the Fe-based amorphous alloy, the crystallization starting temperature is, for example, in a range of 400° C. or more and 450° C. or less.
While the method for increasing the temperature of the amorphous alloy ribbon piece to the crystallization starting temperature is not specifically limited, the method includes, for example, a method where the amorphous alloy ribbon piece is moved from an inlet to a predetermined position in a continuous heating furnace (for example, a tunnel furnace) in which the temperature at a predetermined position on the inlet side inside the furnace is set to the crystallization starting temperature, the temperature near the outlet inside the furnace is set to the crystallization process termination temperature, and the temperature continuously changes from near the inlet to near the outlet inside the furnace, in addition to the method where the temperature inside the heating furnace into which the amorphous alloy ribbon piece has been moved is increased to the crystallization starting temperature as the example illustrated in
In the second temperature increasing step, the temperature of the amorphous alloy ribbon piece is increased from the crystallization starting temperature to the crystallization process termination temperature equal to or less than the crystallization completion temperature. The temperature increase rate of the amorphous alloy ribbon piece in the second temperature increasing step satisfies the formula (1) below where a self-heating amount of the amorphous alloy ribbon piece per unit time is ΔQself, a heat discharge amount of the amorphous alloy ribbon piece per unit time is ΔQout, a mass and a specific heat of the amorphous alloy ribbon piece are m and c, respectively, and a temperature increase width of the amorphous alloy ribbon piece per unit time is ΔT.
ΔQself≤ΔQout+mcΔT (1)
Here, the “unit time” in the “self-heating amount of the amorphous alloy ribbon piece per unit time,” the “heat discharge amount of the amorphous alloy ribbon piece per unit time,” and the “temperature increase width of the amorphous alloy ribbon piece per unit time” means the temperature increasing time/n (n: natural number), wherein the temperature increasing time is a temperature increasing time from the crystallization starting temperature to the crystallization process termination temperature. The unit time is set to, for example, a time in a range of the temperature increasing time (a temperature increasing time from the crystallization starting temperature to the crystallization process termination temperature) or less, and especially, the unit time is set to a time in a range of one second or less in some embodiments.
The description of the crystallization starting temperature is omitted because it is similar to that of the first temperature increasing step. While the crystallization completion temperature differs depending on the material and the like of the amorphous alloy ribbon piece, when the material is the Fe-based amorphous alloy, the crystallization completion temperature is, for example, in a range of 450° C. or more and 550° C. or less. The crystallization process termination temperature is not specifically limited insofar as the crystallization process termination temperature is a temperature equal to or less than the crystallization completion temperature and is set such that characteristic values such as a saturation magnetic flux density and a coercivity, of the alloy ribbon piece obtained by the crystallization of the amorphous alloy ribbon piece become desired values. While the crystallization process termination temperature differs depending on the material and the like of the amorphous alloy ribbon piece, when the material is the Fe-based amorphous alloy, the crystallization process termination temperature is, for example, set to 460° C. as the example illustrated in
The temperature increase rate may constantly satisfy the formula (1) in the temperature increase process from the crystallization starting temperature to the crystallization process termination temperature and does not have to constantly satisfy the formula (1) in the temperature increase process insofar as the excessive temperature increase is suppressed to ensure manufacturing the alloy ribbon piece having the desired soft magnetic properties. The temperature increase rate constantly satisfies the formula (1) in the temperature increase process in some embodiments. This is because the excessive temperature increase can be effectively suppressed.
The temperature increase rate may be constant in the temperature increase process from the crystallization starting temperature to the crystallization process termination temperature, or may be changed in the temperature increase process. For example, the temperature increase rate may be relatively increased in a temperature range where the heat generation amount is relatively small on the DSC curve as illustrated in
While the average temperature increase rate of the amorphous alloy ribbon piece in the second temperature increasing step differs depending on the material and the like of the amorphous alloy ribbon piece, when the material of the amorphous alloy ribbon piece is the Fe-based amorphous alloy, the average temperature increase rate is, for example, in a range of 0.5° C./second or more and 20° C./second or less, or is in a range of 0.5° C./second or more and 10° C./second or less in some embodiments. This is because the average temperature increase rate equal to or more than the lower limits of these ranges ensures the effective suppression of the coarse crystal grains, and the average temperature increase rate equal to or less than the upper limits of these ranges ensures the effective suppression of the excessive temperature increase. Note that, the average temperature increase rate of the amorphous alloy ribbon piece in the second temperature increasing step means the average of the temperature increase rate in the temperature increase process from the crystallization starting temperature to the crystallization process termination temperature. While the average temperature increase rate differs depending on the material and the like of the amorphous alloy ribbon piece, when the material is the Fe-based amorphous alloy, the average temperature increase rate means, for example, the average of the temperature increase rate in the temperature increase process from the crystallization starting temperature in a range of 400° C. or more and 450° C. or less to the crystallization process termination temperature.
While the method for increasing the temperature of the amorphous alloy ribbon piece from the crystallization starting temperature to the crystallization process termination temperature is not specifically limited, the method includes, for example, a method where the amorphous alloy ribbon piece is moved from an inlet to a predetermined position and subsequently moved from the predetermined position to an outlet in a continuous type heating furnace in which the temperature at a predetermined position on the inlet side inside the furnace is set to the crystallization starting temperature, the temperature near the outlet inside the furnace is set to the crystallization process termination temperature, and the temperature continuously changes from near the inlet to near the outlet inside the furnace, in addition to the method where the temperature inside the heating furnace into which the amorphous alloy ribbon piece has been moved is increased from the crystallization starting temperature to the crystallization process termination temperature at the desired rate as the example illustrated in
The method for manufacturing alloy ribbon piece usually includes, for example, the cooling step of cooling the temperature of the alloy ribbon piece obtained by crystallizing the amorphous alloy ribbon piece to a temperature at which the growth of the crystal grains crystallized in the alloy ribbon piece stops after the temperature increase of the amorphous alloy ribbon piece from the crystallization starting temperature to the crystallization process termination temperature in the second temperature increasing step as the example illustrated in
While the method for cooling the temperature of the alloy ribbon piece obtained by crystallizing the amorphous alloy ribbon piece to the temperature at which the growth of the crystal grains crystallized in the alloy ribbon piece stops is not specifically limited, the method includes, for example, a method for cooling the temperature to normal temperature by taking out the alloy ribbon piece obtained by crystallizing the amorphous alloy ribbon piece from the inside of the heating furnace to move it to the environment of normal temperature as the example illustrated in
While the method for manufacturing alloy ribbon piece is not specifically limited insofar as the method suppresses the excessive temperature increase to ensure manufacturing the alloy ribbon piece having the desired soft magnetic properties, the method is a method for manufacturing the nanocrystalline alloy ribbon piece having the desired soft magnetic properties in some embodiments.
Here, the “nanocrystalline alloy ribbon piece” means a nanocrystalline alloy ribbon piece that provides desired properties of soft magnetic properties such as a coercivity by precipitating fine crystal grains without substantially causing the coarse crystal grains or the precipitation of the compound phase. The material of the nanocrystalline alloy ribbon piece differs depending on the material and the like of the amorphous alloy ribbon piece, and when the material of the amorphous alloy ribbon piece is the Fe-based amorphous alloy, the material of the nanocrystalline alloy ribbon piece is, for example, a Fe-based nanocrystalline alloy having a mixed phase structure of crystal grains of Fe or Fe alloy (for example, fine bccFe crystal) and amorphous phases.
The grain diameter of the crystal grain of the nanocrystalline alloy ribbon piece is not specifically limited insofar as the desired soft magnetic properties are obtained, and differs depending on the material and the like. When the material is the Fe-based nanocrystalline alloy, for example, the grain diameter is in a range of 25 nm or less in some embodiments. This is because coarsening deteriorates the coercivity. The grain diameter of the crystal grain can be measured through, for example, a direct observation using a transmission electron microscope (TEM). The grain diameter of the crystal grain can be estimated from the coercivity or the temperature history of the nanocrystalline alloy ribbon piece.
The saturation magnetic flux density of the nanocrystalline alloy ribbon piece differs depending on the material and the like of the nanocrystalline alloy ribbon piece, and when the material is the Fe-based nanocrystalline alloy, the saturation magnetic flux density is, for example, 1.7 T or more in some embodiments. This is because, for example, the torque of the motor and the like can be increased. The coercivity of the nanocrystalline alloy ribbon piece differs depending on the material and the like of the nanocrystalline alloy ribbon piece, and when the material is the Fe-based nanocrystalline alloy, the coercivity is, for example, 20 A/m or less and is 10 A/m or less in some embodiments. This is because, thus decreasing the coercivity ensures effectively reducing, for example, a loss in the core of the motor and the like. The saturation magnetic flux density and the coercivity can be measured using, for example, a vibrating sample magnetometer (VSM).
The method for manufacturing alloy ribbon piece is not specifically limited insofar as the method is a method for manufacturing a alloy ribbon piece obtained by crystallizing the amorphous alloy ribbon piece, the method includes the preparation step, the first temperature increasing step, and the second temperature increasing step, and the temperature increase rate of the amorphous alloy ribbon piece in the second temperature increasing step satisfies the formula (1). For example, as the example illustrated in
The clearance provided between the alloy ribbon pieces in the method where the temperature of the plurality of amorphous alloy ribbon pieces is increased in the state where the clearance is provided between the adjacent amorphous alloy ribbon pieces in the second temperature increasing step is not specifically limited insofar as the heat is sufficiently discharged by the clearance for each of the amorphous alloy ribbon pieces, thereby suppressing the excessive temperature increase for each of the amorphous alloy ribbon pieces to ensure manufacturing the plurality of alloy ribbon pieces having the desired soft magnetic properties. The clearance is, for example, 1 mm or more in some embodiments. This is because the heat is effectively discharged.
While the atmosphere to perform the steps included in the method for manufacturing alloy ribbon piece is not specifically limited, for example, the air atmosphere is included.
While the method for manufacturing alloy ribbon piece is not specifically limited insofar as the alloy ribbon piece having the desired soft magnetic properties can be manufactured, the method may be, for example, a manufacturing method where the whole of the amorphous alloy ribbon piece is crystallized to obtain a desired grain diameter of the crystal grain of the crystallized alloy ribbon piece without substantially causing the burning due to the excessive temperature increase, the coarse crystal grains, or the precipitation of the compound phase. In the method for manufacturing alloy ribbon piece, in order to crystallize the whole of the amorphous alloy ribbon piece to obtain the desired grain diameter of the crystal grain of the crystallized alloy ribbon piece without substantially causing the burning due to the excessive temperature increase, the coarse crystal grains, or the precipitation of the compound phase, other conditions may be appropriately set in addition to the above-described conditions. Not only the respective conditions are appropriately set independently, but also combinations of the respective conditions may be appropriately set.
The following further specifically describes the method for manufacturing alloy ribbon piece according to the embodiment with Example and Comparative Examples.
First, as illustrated in
Saturation Magnetic Flux Density: less than 1.7 T
Coercivity: less than 6 A/m
Next, as illustrated in
Next, as illustrated in
Next, as illustrated in
Next, as illustrated in
As indicated by the temperature history B of
As indicated by the temperature history C of
As indicated by the temperature history D of
As indicated by the temperature history E of
One alloy ribbon piece was selected from the 400 alloy ribbon pieces manufactured by each of Example, Comparative Example 1, and Comparative Example 4 where the amorphous alloy ribbon piece 2A did not burn among Example and Comparative Examples, a part of the one alloy ribbon piece was cut out, and the saturation magnetic flux density and the coercivity were measured by VSM (vibrating sample magnetometer) in the part of the one alloy ribbon piece. Table 1 below indicates the measurement values.
As indicated by Table 1 above, in Example, the saturation magnetic flux density was equal to or more than the lower limit (1.7 T) of the target range, and the coercivity was within the target range without exceeding the upper limit (10 A/m) of the target range. It is considered that the temperature increase rate of the amorphous alloy ribbon piece 2A in the second temperature increasing step satisfying the formula (1) suppressed the occurrence in chain reaction of the self-heating due to the crystallization at the amorphous alloy ribbon piece 2A, thereby suppressing the excessive temperature increase of the amorphous alloy ribbon piece 2A, and the not excessively long temperature increasing time of the amorphous alloy ribbon piece 2A in the second temperature increasing step suppressed the growth of the crystallized crystal grains for a long period of time to be coarsened.
Meanwhile, in Comparative Example 1, while the coercivity did not exceed the upper limit of the target range, the saturation magnetic flux density was less than the lower limit of the target range. It is considered that because of the temperature increase of the whole amorphous alloy ribbon piece 2A only up to 400° C., the amorphous alloy ribbon piece 2A was not entirely crystallized. In Comparative Example 4, while the saturation magnetic flux density was the lower limit or more of the target range the coercivity significantly exceeded the upper limit of the target range. It is considered that because of the excessively long temperature increasing time of the amorphous alloy ribbon piece 2A in the second temperature increasing step, the crystallized crystal grains grew for a long period of time to be coarsened.
While the embodiment of the method for manufacturing alloy ribbon piece according to the present disclosure have been described in detail above, the present disclosure is not limited thereto, and can be subjected to various kinds of changes in design without departing from the spirit of the present disclosure described in the claims.
All publications, patents and patent applications cited in the present description are herein incorporated by reference as they are.
Number | Date | Country | Kind |
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2019-105932 | Jun 2019 | JP | national |