SOFT MAGNETIC ALLOY POWDER AND PRODUCTION METHOD THEREFOR

20240271259 ยท 2024-08-15

    Inventors

    Cpc classification

    International classification

    Abstract

    An FeCrSi-based soft magnetic alloy powder is provided in which the Cr weight ratio of Cr contained in the alloy powder gradually decreases from the surface of the alloy powder to a predetermined depth in the depth direction, the amount contained of Si is in the range of 3 to 6.5% by weight, the amount contained of Cr may be in the range of 1 to 5% by weight, at least one of Mn, P, S, and O may be further contained, the weight ratio of Cr oxide/metal Cr may gradually decrease from the surface of the alloy powder in the depth direction, and loss in the soft magnetic alloy powder used in a dust core is reduced so as to be able to cope with higher frequencies and larger currents.

    Claims

    1-9. (canceled)

    10. A soft magnetic alloy powder that is an FeCrSi-based soft magnetic alloy powder in which a weight ratio of Cr contained in the soft magnetic alloy powder gradually decreases from a surface of the alloy powder to a predetermined depth in a depth direction.

    11. The soft magnetic alloy powder according to claim 10, wherein an amount contained of Si is in a range of 3 to 6.5% by weight, and an amount contained of Cr is in a range of 1 to 5% by weight.

    12. The soft magnetic alloy powder according to claim 10, further comprising at least one of Mn, P, S, and O.

    13. The soft magnetic alloy powder according to claim 10, wherein a weight ratio of Cr oxide/metal Cr gradually decreases from the surface of the alloy powder in the depth direction.

    14. A production method for an FeCrSi-based soft magnetic alloy powder, the method comprising: heating an alloy in a crucible to form a molten metal; and blowing a fluid onto a stream of the molten metal guided to fall from the crucible, to crush and solidify the molten metal and form an alloy powder, wherein a portion of Cr contained in the alloy powder is oxidized in forming the alloy powder from the molten metal.

    15. The production method according to claim 14, wherein oxidization is performed such that a weight ratio of Cr oxide/metal Cr of the Cr contained in the alloy powder gradually decreases from a surface of the alloy powder in a depth direction.

    16. The production method according to claim 14, wherein a weight ratio of the Cr contained in the alloy powder gradually decreases from a surface of the alloy powder to a predetermined depth in a depth direction.

    17. The production method according to claim 14, wherein in the alloy formed into the molten metal, an amount contained of Si is in a range of 3 to 6.5% by weight, and an amount contained of Cr is in a range of 1 to 5% by weight.

    18. The production method according to claim 17, wherein the alloy further contains at least one of Mn, P, S, and O.

    19. The soft magnetic alloy powder according to claim 11, further comprising at least one of Mn, P, S, and O.

    20. The soft magnetic alloy powder according to claim 11, wherein a weight ratio of Cr oxide/metal Cr gradually decreases from the surface of the alloy powder in the depth direction.

    21. The soft magnetic alloy powder according to claim 12, wherein a weight ratio of Cr oxide/metal Cr gradually decreases from the surface of the alloy powder in the depth direction.

    22. The soft magnetic alloy powder according to claim 19, wherein a weight ratio of Cr oxide/metal Cr gradually decreases from the surface of the alloy powder in the depth direction.

    23. The production method according to claim 15, wherein a weight ratio of the Cr contained in the alloy powder gradually decreases from a surface of the alloy powder to a predetermined depth in a depth direction.

    24. The production method according to claim 15, wherein in the alloy formed into the molten metal, an amount contained of Si is in a range of 3 to 6.5% by weight, and an amount contained of Cr is in a range of 1 to 5% by weight.

    25. The production method according to claim 16, wherein in the alloy formed into the molten metal, an amount contained of Si is in a range of 3 to 6.5% by weight, and an amount contained of Cr is in a range of 1 to 5% by weight.

    26. The production method according to claim 23, wherein in the alloy formed into the molten metal, an amount contained of Si is in a range of 3 to 6.5% by weight, and an amount contained of Cr is in a range of 1 to 5% by weight.

    27. The production method according to claim 24, wherein the alloy further contains at least one of Mn, P, S, and O.

    28. The production method according to claim 25, wherein the alloy further contains at least one of Mn, P, S, and O.

    29. The production method according to claim 26, wherein the alloy further contains at least one of Mn, P, S, and O.

    Description

    BRIEF DESCRIPTION OF DRAWINGS

    [0014] FIG. 1 A graph illustrating the distribution of Cr in the depth direction of soft magnetic alloy powders.

    [0015] FIG. 2 A graph illustrating the distribution of the XPS spectrum of Cr in the depth direction of soft magnetic alloy powders.

    [0016] FIG. 3 This graph is a continuation of FIG. 2.

    [0017] FIG. 4 This graph is a continuation of FIG. 3.

    [0018] FIG. 5 A graph illustrating the area circularity of soft magnetic alloy powders.

    [0019] FIG. 6 A graph illustrating the dependence of the relative magnetic permeability of soft magnetic alloy powders on the magnetic field.

    [0020] FIG. 7 A graph illustrating the dependence of the volume resistivity of soft magnetic alloy powders on a pressing force.

    DESCRIPTION OF EMBODIMENTS

    [0021] Hereinafter, an embodiment of a soft magnetic alloy powder and a production method therefor will be described in detail with reference to the drawings. In the present embodiment, an FeCrSi-based alloy is assumed as the alloy constituting the soft magnetic alloy powder. The FeCrSi-based soft magnetic alloy of the present embodiment is an alloy constituted by adding chromium (Cr) and silicon (Si) to iron (Fe) which is the main component, and the remainder of Cr and Si is composed of Fe except for additives and unavoidable impurities as noted.

    [0022] The soft magnetic alloy powder of the present embodiment (hereinafter, soft magnetic alloy powder is sometimes also referred to as alloy powder, and soft magnetic alloy is sometimes also referred to as alloy) is produced by an atomization method. First, material constituting an alloy powder is placed in a crucible and heated by a melting furnace to form a molten alloy. In an FeCrSi-based alloy, Fe is the main component and Cr and Si are added, and carbon (C), manganese (Mn), phosphorus (P), and sulfur (S) may be added. Oxygen (O) may also be added.

    [0023] In the FeCrSi-based alloy of the present embodiment, the amount contained of Si may be in the range of 3 to 6.5% by weight. The amount contained of Cr may be in the range of 1 to 5% by weight. The amount contained of C may be in the range of 0.003 to 0.02% by weight, may be in the range of 0.005 to 0.017% by weight, or may be in the range of 0.007 to 0.015% by weight. The amount contained of Mn may be in the range of 0.01 to 0.1% by weight, may be in the range of 0.015 to 0.08% by weight, or may be in the range of 0.017 to 0.07% by weight. The amount contained of P may be in the range of 0.001 to 0.009% by weight, may be in the range of 0.002 to 0.006% by weight, or may be in the range of 0.0025 to 0.005% by weight. The amount contained of S may be in the range of 0.001 to 0.009% by weight, may be in the range of 0.002 to 0.006% by weight, or may be in the range of 0.0025 to 0.005% by weight. The amount contained of O may be 2500 wt. ppm or less.

    [0024] Next, the molten alloy is guided to a nozzle from a hole formed at the bottom of the crucible, to form a stream of molten alloy falling from the nozzle. A jet flow of a fluid such as water or gas is blown onto the falling molten alloy, and the molten alloy is crushed and solidified to form an alloy powder. In the present embodiment, the alloy powder is formed from the molten alloy, and the molten alloy, which is pulverized into droplets, is oxidized. Therefore, oxygen may be contained in the fluid blown onto the stream of the falling molten alloy, or oxygen may be contained in the atmosphere in which the molten alloy falls.

    [0025] With such a production method, alloy powders were prepared from alloys of different compositions of Experimental Examples 1 to 3 as shown in Table 1 below. Note that the compositions of alloy powders of Comparative Examples 1 to 4 are also shown in Table 1. Comparative Examples 1 to 4 were prepared by a production method similar to that of the present embodiment except that droplets of molten alloy were not oxidized in the step of blowing a jet flow of a fluid onto the molten alloy falling from the nozzle to form an alloy powder.

    TABLE-US-00001 TABLE 1 C Si Mn P S Cr Fe [%] [%] [%] [%] [%] [%] [%] Experimental 0.01 3.96 0.03 0.003 0.003 4.64 Remainder Example 1 Experimental 0.01 3.88 0.04 0.003 0.003 4.63 Remainder Example 2 Experimental 0.01 4.00 0.03 0.003 0.004 4.46 Remainder Example 3 Comparative 0.01 3.91 0.07 0.004 0.007 4.33 Remainder Example 1 Comparative 0.01 4.03 0.02 0.003 0.003 4.33 Remainder Example 2 Comparative 0.01 3.91 0.03 0.005 0.005 4.54 Remainder Example 3 Comparative 0.01 2.91 0.03 0.003 0.004 4.39 Remainder Example 4

    [0026] Table 2 shows the results of measuring the concentration of O, median diameter D.sub.50, tap density, specific surface area, and coercive force of Experimental Examples 1 to 3. Table 2 also shows the measurement results for Comparative Examples 1 to 3. Here, the median diameter D.sub.50 is the diameter of the alloy powder in the center when the alloy powder is arranged in order of the size of the diameter. The tap density is the density measured by placing the alloy powder in a container and tapping the container to fill gaps within the alloy powder. The specific surface area is the surface area per weight of the alloy powder.

    TABLE-US-00002 TABLE 2 Tap Specific Coercive O D.sub.50 density surface area force Hc [ppm] [?m] [g/cm.sup.3] [m.sup.2/g] [A/m] Experimental 2300 5.6 4.15 0.33 565 Example 1 Experimental 2200 6.0 4.21 0.35 681 Example 2 Experimental 1800 11.3 4.52 0.22 481 Example 3 Comparative 2800 5.4 4.12 0.52 710 Example 1 Comparat 1600 10.8 4.60 0.32 672 Example 2 Comparative 1800 10.7 4.47 0.43 694 Example 3 Comparative 1800 10.5 4.37 0.37 714 Example 4

    [0027] Comparing Experimental Examples 1 to 3 and Comparative Examples 1 to 4 in Table 2, it is observed that the concentration of O, median diameter D50, tap density, and specific surface area have similar values. However, the coercive force Hc is in the range of 461 to 581 [A/m] in Experimental Examples 1 to 3, whereas the coercive force Hc is 672 to 714 [A/m] in Comparative Examples 1 to 4. Thus, it is observed that the coercive force Hc is notably reduced in the alloy powders prepared according to the production method of the present embodiment. Since the coercive force Hc decreases in Experimental Examples 1 to 3, the loss due to hysteresis of magnetization of the dust cores formed by the alloy powders of Experimental Examples 1 to 3 is notably reduced.

    [0028] FIG. 1 is a graph illustrating the distribution of Cr in the depth direction of the alloy powders. In FIG. 1, the distribution of the Cr amount from the surface of the alloy powder to a depth of approximately 130 nm was measured by X-ray photoelectron spectroscopy (XPS). In Experimental Examples 1 to 3, it is observed that the Cr amount gradually decreases in the depth direction from the surface of the powder, saturates when reaching a certain depth of approximately 50 to 70 nm, and thereafter transitions at a substantially constant value. In contrast, in Comparative Examples 1 to 4, it is observed that the Cr amount starts from a smaller value than in Experimental Examples 1 to 3 at the surface of the alloy powder, and gradually increases and then saturates when reaching a certain depth of approximately 50 to 70 nm and thereafter transitions at a substantially constant value, but the value at which the Cr amount transitions at a constant value is slightly smaller than the value at which the Cr amount transitions at a substantially constant value in Experimental Examples 1 to 3.

    [0029] As described above, in Experimental Examples 1 to 3, the droplets of the molten alloy are oxidized in the step of forming the alloy powder from the molten alloy, whereas in Comparative Examples 1 to 4, oxidization is not carried out in the step of forming the alloy powder from the alloy. Therefore, it is thought that the distribution in the depth direction of the Cr amount in the alloy powders of Experimental Examples 1 to 3, in other words, the distribution in which the Cr amount gradually decreases in the depth direction from the surface of the powder and then saturates, was formed due to the process of oxidizing the droplets of the molten alloy.

    [0030] FIGS. 2 to 4 are graphs illustrating the distribution of the XPS spectrum of Cr in the depth direction of the alloy powders. FIG. 2(a) shows the XPS spectrum of Cr at a depth of 6.5 nm, FIG. 2(b) at a depth of 13 nm, FIG. 3(c) at a depth of 19.5 nm, FIG. 3(d) at a depth of 26 nm, and FIG. 4(e) at a depth of 130 nm from the surface of the alloy powder. Note that the depth of the alloy powder is according to SiO.sub.2 conversion.

    [0031] In each graph, the binding energy of metal Cr is shown as E1 and the binding energy of Cr oxide is shown as E2. Referring to FIGS. 2(a) to 4(e), in Experimental Examples 1 to 3, at a depth of 6.5 nm in FIG. 2(a), Cr oxide is greater than metal Cr in terms of the ratio thereof in the Cr, but as the depth increases in FIGS. 2(a) to 4(e), metal Cr gradually increases in terms of the ratio thereof in the Cr. At a depth of 13 nm in FIG. 2(b), the ratio of Cr oxide is still greater than that of metal Cr, but at a depth of 19.5 nm and thereafter in FIG. 3(c), the ratio of metal Cr becomes greater than that of Cr oxide.

    [0032] In Comparative Examples 1 to 4 also, the trend of metal Cr gradually increasing in terms of the ratio thereof in the Cr as the depth increases in FIGS. 2(a) to 4(e) is similar to that in Experimental Examples 1 to 3. However, there is a difference in that the ratio of metal Cr is already greater than that of Cr oxide at a depth of 13 nm in FIG. 2(b). Compared with such Comparative Examples 1 to 4, in Experimental Examples 1 to 3, it can be said that there is advanced oxidation of Cr in a surface layer from the surface of the alloy powder to a certain depth.

    [0033] As described above, in Experimental Examples 1 to 3, the droplets of the molten alloy are oxidized in the step of forming the alloy powder from the molten alloy, while in Comparative Examples 1 to 4, the powder is not oxidized in the step of forming the alloy powder from the alloy. Therefore, in the alloy powders of Experimental Examples 1 to 3, it is thought that the oxidation of Cr proceeds from the surface in this step, and the amount of Cr oxide in the surface layer becomes greater than that in Comparative Examples 1 to 4.

    [0034] FIG. 5 is a graph illustrating the area circularity of alloy powders obtained by image analysis. Referring to FIG. 5, for an alloy powder having a diameter smaller than 5 um, it is observed that the area circularities of Experimental Examples 2 and 3 and Comparative Example 3 are similar values of approximately 9.2, but in the range where the diameter is 5 ?m or more and less than 10 ?m and the range where the diameter is 10 ?m or more, the area circularities of both Experimental Examples 2 and 3 are larger than the area circularity of Comparative Example 3. This is thought to be because, in Experimental Examples 2 and 3, alloy droplets were formed in powders having a high circularity due to the ratio of Cr oxide in the Cr in the surface layer being large and the strong bonding force of Cr oxide in the surface layer.

    [0035] FIG. 6 is a graph illustrating results of measuring the DC superposition characteristics of the alloy powders. The drawing shows measurement data of Experimental Examples 2 and 3 and Comparative Example 2 used in FIG. 5. In the graph, the horizontal axis is the magnetic field, and the vertical axis is the relative magnetic permeability with 100 being when no magnetic field is applied. Referring to the drawing, it is observed that the measurement data of Experimental Examples 2 and 3 and Comparative Example 2 increases to maximum values before reaching 1000 [A/m] as the magnetic field increases, and then decreases monotonically to near 12000 [A/m]. Furthermore, it is also observed that the relative magnetic permeability of Experimental Examples 2 and 3 and Comparative Example 2 are almost equal until the magnetic field is approximately 2000 [A/m], but when approximately 2000 [A/m] is exceeded, the relative magnetic permeability of Experimental Examples 2 and 3 is larger than the magnetic permeability of Comparative Example 2 up to near 12000 [A/m], which is the upper limit of the measurement range. Therefore, it can be said that Experimental Examples 2 and 3 have favorable DC superposition characteristics in that the decrease in magnetic permeability is small regardless of an increase in the strength of the magnetic field corresponding to DC current.

    [0036] In this way, the alloy powders of Experimental Examples 2 and 3 have more favorable DC superposition characteristics than the alloy powder of Comparative Example 2. Such DC superposition characteristics of Experimental Examples 2 and 3 are thought to be due to the high circularities of the alloy powders of Experimental Examples 2 and 3 as shown in FIG. 5. A dust core formed with an alloy powder of the present embodiment, such as that of Experimental Examples 2 and 3, can ensure magnetic permeability by suppressing a decrease in magnetic permeability even when a large current is applied, and therefore loss can be reduced.

    [0037] FIG. 7 is a graph illustrating the dependence of the volume resistivity of alloy powders on a pressing force. FIG. 7 shows measurement data of typical values such as the mean value or median value and the range from the minimum value to the maximum value for Experimental Example 3 and Comparative Example 3. Referring to the drawing, it is observed that the volume resistivity gradually decreases as the pressing force increases, in the measurement data of both Experimental Example 3 and Comparative Example 3. Furthermore, it is also observed that the volume resistivity of Experimental Example 3 is approximately 10.sup.1 to 10.sup.3 higher than the volume resistivity of Comparative Example 3.

    [0038] In this way, the powder alloy of Experimental Example 3 has a higher volume resistivity than the powder alloy of Comparative Example 3. It is thought that this kind of high volume resistivity of Experimental Example 3 is due to the powder alloy of the experimental example prepared according to the production method of the present embodiment having a large ratio of Cr oxide, which has no conductivity, in the Cr of the surface layer. A dust core formed with an alloy powder of the present embodiment, such as that of Experimental Example 3, has a large volume resistivity, and therefore loss due to the generation of eddy current can be reduced.

    [0039] As described above, an alloy powder of the present embodiment is prepared while oxidizing droplets of molten alloy in a step of forming an alloy powder from a molten alloy by an atomization method in the production method of the present embodiment. The coercive force of such an alloy powder of the present embodiment is smaller than that of comparative examples that do not use the production method of the present embodiment. Furthermore, the ratio of Cr oxide in the Cr in the surface layer of the alloy powder is larger than that of metal Cr. In addition, due to the high circularity of the alloy powder, the decrease in magnetic permeability that accompanies an increase in magnetic field is small, and favorable DC superposition characteristics can be obtained. Moreover, since the ratio of Cr oxide in the Cr in the surface layer of the alloy powder is larger than that of metal Cr, high volume resistivity can be obtained.

    [0040] A dust core formed using this kind of alloy powder of the present embodiment has a small coercive force and favorable DC superposition characteristics and high magnetic permeability can be ensured, and therefore hysteresis loss can be reduced. Furthermore, since the volume resistivity of the alloy powder is high, loss due to eddy current can also be reduced. In this way, a dust core formed with an alloy powder of the present embodiment can reduce loss regardless of the higher frequencies and larger currents of choke coils, inductors, and the like, and can cope with higher frequencies and larger currents.

    INDUSTRIAL APPLICABILITY

    [0041] The alloy powder and the production method therefor of the present embodiment can be used for producing a dust core for a choke coil, inductor, or the like of an electrical device.