WO2015199211A1 - 電磁鋼板 - Google Patents
電磁鋼板 Download PDFInfo
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- WO2015199211A1 WO2015199211A1 PCT/JP2015/068497 JP2015068497W WO2015199211A1 WO 2015199211 A1 WO2015199211 A1 WO 2015199211A1 JP 2015068497 W JP2015068497 W JP 2015068497W WO 2015199211 A1 WO2015199211 A1 WO 2015199211A1
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- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
- C22C38/18—Ferrous alloys, e.g. steel alloys containing chromium
- C22C38/34—Ferrous alloys, e.g. steel alloys containing chromium with more than 1.5% by weight of silicon
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
- H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
- H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
- H01F1/12—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
- H01F1/14—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
- H01F1/147—Alloys characterised by their composition
- H01F1/14708—Fe-Ni based alloys
- H01F1/14716—Fe-Ni based alloys in the form of sheets
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- C—CHEMISTRY; METALLURGY
- C21—METALLURGY OF IRON
- C21D—MODIFYING THE PHYSICAL STRUCTURE OF FERROUS METALS; GENERAL DEVICES FOR HEAT TREATMENT OF FERROUS OR NON-FERROUS METALS OR ALLOYS; MAKING METAL MALLEABLE, e.g. BY DECARBURISATION OR TEMPERING
- C21D8/00—Modifying the physical properties by deformation combined with, or followed by, heat treatment
- C21D8/12—Modifying the physical properties by deformation combined with, or followed by, heat treatment during manufacturing of articles with special electromagnetic properties
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- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
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- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
- C22C38/001—Ferrous alloys, e.g. steel alloys containing N
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- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
- C22C38/002—Ferrous alloys, e.g. steel alloys containing In, Mg, or other elements not provided for in one single group C22C38/001 - C22C38/60
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- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
- C22C38/008—Ferrous alloys, e.g. steel alloys containing tin
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- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
- C22C38/02—Ferrous alloys, e.g. steel alloys containing silicon
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- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
- C22C38/04—Ferrous alloys, e.g. steel alloys containing manganese
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- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
- C22C38/06—Ferrous alloys, e.g. steel alloys containing aluminium
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- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
- C22C38/18—Ferrous alloys, e.g. steel alloys containing chromium
- C22C38/40—Ferrous alloys, e.g. steel alloys containing chromium with nickel
- C22C38/42—Ferrous alloys, e.g. steel alloys containing chromium with nickel with copper
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- C—CHEMISTRY; METALLURGY
- C22—METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
- C22C—ALLOYS
- C22C38/00—Ferrous alloys, e.g. steel alloys
- C22C38/60—Ferrous alloys, e.g. steel alloys containing lead, selenium, tellurium, or antimony, or more than 0.04% by weight of sulfur
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
- H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
- H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
- H01F1/12—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
- H01F1/14—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
- H01F1/147—Alloys characterised by their composition
- H01F1/14766—Fe-Si based alloys
- H01F1/14775—Fe-Si based alloys in the form of sheets
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
- H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
- H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
- H01F1/12—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
- H01F1/14—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
- H01F1/147—Alloys characterised by their composition
- H01F1/14766—Fe-Si based alloys
- H01F1/14791—Fe-Si-Al based alloys, e.g. Sendust
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
- H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
- H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
- H01F1/12—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
- H01F1/14—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
- H01F1/16—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys in the form of sheets
Definitions
- the present invention relates to an electromagnetic steel sheet.
- split iron cores that are advantageous in terms of winding design and yield are increasingly used for motor stators.
- the divided iron core is often fixed to the case by shrink fitting, and when compressive stress acts on the electromagnetic steel sheet by shrink fitting, the magnetic properties of the electromagnetic steel sheet are deteriorated.
- Conventionally, research for suppressing such a decrease in magnetic properties has been conducted.
- An object of the present invention is to provide an electrical steel sheet that can exhibit excellent magnetic properties even when compressive stress is applied.
- the present inventors have intensively studied to clarify the reason why excellent magnetic properties cannot be obtained when a conventional magnetic steel sheet is used for a split iron core. As a result, it became clear that the relationship between the direction in which the compressive stress acts and the crystal orientation of the electrical steel sheet is important.
- the compressive stress acting on the electromagnetic steel sheet will be described. Since the drive motor of a hybrid vehicle and the compressor motor of an air conditioner are multipolar, the direction of the magnetic flux flowing through the teeth portion of the stator is usually matched with the rolling direction of the electrical steel sheet (hereinafter sometimes referred to as “L direction”). Thus, the direction of the magnetic flux flowing through the yoke portion is made to coincide with the direction orthogonal to the rolling direction and the plate thickness direction (hereinafter also referred to as “C direction”).
- the compressive stress in the C direction acts on the electromagnetic steel plate in the yoke portion, while no stress acts on the magnetic steel plate in the tooth portion. Therefore, it is desired that the magnetic steel sheet used for the split iron core can exhibit excellent magnetic properties in the C direction under compressive stress acting in the C direction while exhibiting excellent magnetic properties in the L direction under no stress. .
- the inventors of the present invention have made further studies to clarify a configuration that can exhibit such magnetic characteristics.
- the crystal grains in the Goss orientation are not easily affected by the compressive stress in the C direction, and even if the compressive stress in the C direction is applied, the magnetic properties in the C direction are not easily lowered. It has been found that the magnetic properties in the C direction are likely to be deteriorated when the C direction compressive stress is applied. It was revealed that excellent magnetic properties can be obtained by appropriately controlling the integration degree in the (001) [100] orientation and the integration degree in the (011) [100] orientation.
- the texture is the electrical steel sheet according to (1), wherein the texture satisfies Formula 4, Formula 5, and Formula 6.
- Formula 4 Formula 5
- Formula 6 Formula 6
- FIG. 1 is a diagram showing the relationship between the degree of integration obtained in the first test and the iron loss W15 / 400L.
- FIG. 2 is a diagram showing the relationship between the degree of integration obtained in the first test and the iron loss W15 / 400C.
- FIG. 3 is a diagram illustrating the distribution of the degree of integration in the first test.
- FIG. 4 is a diagram showing the distribution of magnetic flux density in the first test.
- the electrical steel sheet according to the embodiment of the present invention has a degree of integration of (001) [100] orientation (hereinafter sometimes referred to as “Cube orientation”) with I Cube , (011) [100] orientation (hereinafter referred to as “Goss orientation”). ) Is expressed as I Goss, and it has a texture satisfying the formula 1, the formula 2 and the formula 3.
- the degree of integration in a certain direction means a ratio (random ratio) of intensity in the direction to random intensity, and is an index usually used when displaying a texture.
- the crystal grains in the Goss orientation contribute to the improvement of the magnetic properties in the L direction.
- Cube-oriented crystal grains contribute to the improvement of the magnetic properties in the L direction and the magnetic properties in the C direction.
- the crystal grains in the Goss orientation are not easily influenced by the compressive stress in the C direction, and even when the compressive stress in the C direction is applied, the magnetic properties in the C direction are not easily lowered. Further, it has been clarified that the crystal grains having the Cube orientation are easily affected by the compressive stress in the C direction, and that the magnetic properties in the C direction are easily lowered when the compressive stress in the C direction is applied.
- the value of “I Goss + I Cube ” is less than 10.5, sufficient magnetic properties in the L direction cannot be obtained under no stress. Therefore, the relationship of Formula 1 needs to be satisfied.
- the value of “I Goss + I Cube ” is preferably 10.7 or more, more preferably 11.0 or more.
- the value of “I Goss / I Cube ” is less than 0.50, sufficient C-direction magnetic properties cannot be obtained when compressive stress in the C-direction is applied. Therefore, the relationship of Formula 2 needs to be satisfied.
- the value of “I Goss / I Cube ” is preferably 0.52 or more, and more preferably 0.55 or more. The relationship between the value of “I Goss / I Cube ” and the magnetic properties in the C direction under the compressive stress in the C direction is not clear, but is considered as follows.
- the magnetic properties are more likely to deteriorate than when compressive stress acts parallel to the ⁇ 110> direction.
- the C direction of the (001) [100] orientation (Cube orientation) crystal grain corresponds to the [010] direction
- the (011) [100] orientation (Goss orientation) crystal grain C direction is the [01-1] direction. It corresponds to. Accordingly, the lower the value of “I Goss / I Cube ”, that is, the higher the ratio of crystal grains in the Cube orientation, the higher the ratio of crystal grains whose ⁇ 100> direction is parallel to the C direction, and the compressive stress in the C direction. Therefore, it is considered that the magnetic properties of the electromagnetic steel sheet are likely to deteriorate.
- the value of “I Cube ” is preferably 2.7 or more, and more preferably 3.0 or more.
- Equation 2 Even if the relationship of Equation 2 is satisfied, if the relationship of Equation 3 is not satisfied, the magnetic properties in the C direction are not easily lowered by the compressive stress in the C direction, but sufficient magnetic properties in the C direction are obtained under no stress. Since it cannot be obtained, the magnetic properties in the C direction under the compressive stress in the C direction are not sufficient. If the relationship of Equations 2 and 3 is not satisfied, sufficient C direction magnetic properties cannot be obtained under no stress, and the C direction magnetic properties are reduced by the C direction compressive stress. The magnetic properties in the C direction below are not sufficient.
- Equation 3 If the relationship of Equation 3 is satisfied but the relationship of Equation 2 is not satisfied, sufficient C-direction magnetic properties can be obtained under no stress, but the C-direction magnetic properties are reduced by compressive stress in the C-direction. Therefore, the magnetic properties in the C direction under the compressive stress in the C direction are not sufficient.
- the relationship of Equations 2 and 3 When the relationship of Equations 2 and 3 is satisfied, sufficient C-direction magnetic properties can be obtained under no stress, and the C-direction magnetic properties are not easily degraded by the C-direction compressive stress. Excellent magnetic properties in the C direction can be obtained below.
- the integration degree I Goss and the integration degree I Cube can be measured as follows. First, the (110), (200) and (211) pole figures of the electrical steel sheet to be measured are measured by the Schulz method of X-ray diffraction. At this time, the position to be measured is a position where the depth from the surface of the electromagnetic steel sheet is 1/4 of the thickness (hereinafter sometimes referred to as “1/4 position”) and a position where the depth is 1/2 (hereinafter referred to as “1/4 position”). , Sometimes referred to as “1/2 position”). Next, a three-dimensional orientation analysis is performed by a series expansion method using the pole figure.
- the texture preferably satisfies the relationships of Formula 4, Formula 5, and Formula 6.
- Formula 5 I Cube ⁇ 2.7
- B50C the magnetic flux density in the direction orthogonal to the plate thickness direction (plate width direction)
- B50C it preferably has magnetic characteristics satisfying the relationship of Equation 7 and Equation 8.
- the value of “B50C / Bs” is more preferably 0.795 or more, and further preferably 0.800 or more.
- the value of “B50C / Bs” is preferably 0.825 or less, more preferably 0.820 or less. More preferably, it is 0.815 or less.
- the value of “(B50L ⁇ B50C) / Bs” is less than 0.070, sufficient magnetic properties in the C direction may not be obtained under compressive stress. Therefore, it is preferable that the relationship of Formula 8 is satisfied. Since the magnetic characteristics are easily deteriorated by the compressive stress, the value of “(B50L ⁇ B50C) / Bs” is more preferably 0.075 or more, and further preferably 0.080 or more.
- the chemical composition of the electrical steel sheet and the slab used for manufacturing the electrical steel sheet according to the embodiment of the present invention will be described. Although the details will be described later, the electrical steel sheet according to the embodiment of the present invention undergoes hot rolling of a slab, hot-rolled sheet annealing, first cold rolling, intermediate annealing, second cold rolling, finish annealing, and the like. Manufactured. Therefore, the chemical composition of the electrical steel sheet and slab takes into account not only the properties of the electrical steel sheet but also these treatments.
- “%”, which is a unit of content of each element contained in the electrical steel sheet means “mass%” unless otherwise specified.
- the electrical steel sheet according to the present embodiment has C: 0.010% or less, Si: 1.30% to 3.50%, Al: 0.0000% to 1.6000%, Mn: 0.01% to 3. 00%, S: 0.0100% or less, N: 0.010% or less, P: 0.000% to 0.150%, Sn: 0.000% to 0.150%, Sb: 0.000% to 0.150%, Cr: 0.000% to 1.000%, Cu: 0.000% to 1.000%, Ni: 0.000% to 1.000%, Ti: 0.010% or less, V : 0.010% or less, Nb: 0.010% or less, and the balance: chemical composition represented by Fe and impurities.
- the impurities include those contained in raw materials such as ore and scrap and those contained in the manufacturing process.
- Si is an element effective for increasing the specific resistance and reducing the iron loss.
- the Si content is preferably 1.60% or more, more preferably 1.90% or more.
- the Si content is 3.50% or less.
- Si content becomes like this.
- it is 3.30% or less, More preferably, it is 3.10% or less.
- Al is an element that lowers the saturation magnetic flux density. If the Al content exceeds 1.6000%, a desired texture cannot be obtained, and a desired magnetic flux density cannot be obtained. Therefore, the Al content is 1.6000% or less. Al content becomes like this. Preferably it is 1.4000% or less, More preferably, it is 1.2000% or less, More preferably, it is 0.8000% or less. As a reason why a desired texture cannot be obtained when the Al content exceeds 1.6000%, it is considered that a change in deformation behavior in cold rolling accompanying an increase in the Al content occurs.
- the lower limit of the Al content is not particularly limited. Al has an effect of increasing specific resistance and reducing iron loss. In order to obtain this effect, the Al content is preferably 0.0001% or more, more preferably 0.0003% or more. .
- Mn is an element effective for increasing the specific resistance and reducing the iron loss. By making the Mn content 0.01% or more, it is possible to obtain the effect of improving specific resistance more reliably. Therefore, the Mn content is 0.01% or more.
- the Mn content is preferably 0.03% or more, and more preferably 0.05% or more.
- Mn content is 3.00% or less.
- the Mn content is preferably 2.70% or less, more preferably 2.50% or less, and still more preferably 2.40% or less.
- C (C: 0.010% or less) C is not an essential element but is contained as an impurity in steel, for example.
- C is an element that degrades magnetic properties by magnetic aging. Therefore, the lower the C content, the better. Such deterioration of the magnetic characteristics is remarkable when the C content exceeds 0.010%. For this reason, C content shall be 0.010% or less.
- the C content is preferably 0.008% or less, and more preferably 0.005% or less.
- S is not an essential element but is contained as an impurity in steel, for example.
- S combines with Mn in steel to form fine MnS, inhibits grain growth during finish annealing, and degrades magnetic properties. Therefore, the lower the S content, the better.
- Such deterioration of the magnetic characteristics is significant when the S content exceeds 0.0100%.
- S content shall be 0.0100% or less.
- S content becomes like this.
- it is 0.0080% or less, More preferably, it is 0.0050% or less.
- S contributes to the improvement of the magnetic flux density. In order to obtain this effect, 0.0005% or more of S may be contained. As a reason why S contributes to the improvement of the magnetic flux density, it is conceivable that grain growth in an orientation that is disadvantageous to magnetic properties is inhibited by S.
- N is not an essential element but is contained as an impurity in steel, for example. N combines with Al in steel to form fine AlN, inhibits grain growth during finish annealing, and degrades magnetic properties. Therefore, the lower the N content, the better. Such deterioration of the magnetic characteristics is remarkable when the N content exceeds 0.010%. For this reason, N content shall be 0.010% or less.
- the N content is preferably 0.008% or less, and more preferably 0.005% or less.
- P, Sn, Sb, Cr, Cu, and Ni are not essential elements, but are optional elements that may be appropriately contained within a predetermined amount in the electromagnetic steel sheet.
- P, Sn, and Sb have the effect of improving the magnetic properties by improving the texture of the electrical steel sheet. Therefore, P, Sn, or Sb, or any combination thereof may be contained. In order to sufficiently obtain this effect, preferably, P: 0.001% or more, Sn: 0.001% or more, or Sb: 0.001% or more, or any combination thereof, more preferably P : 0.003% or more, Sn: 0.003% or more, or Sb: 0.003% or more, or any combination thereof. However, excess P, Sn, and Sb segregate in the crystal grain size to reduce the ductility of the steel sheet, making cold rolling difficult.
- P: more than 0.150%, Sn: more than 0.150%, or Sb: more than 0.150%, or any combination thereof P: 0.150% or less, Sn: 0.150% or less, and Sb: 0.150% or less.
- P: 0.100% or less, Sn: 0.100% or less, or Sb: 0.100% or less, or any combination thereof more preferably P: 0.050% or less, Sn : 0.050% or less, or Sb: 0.050% or less, or any combination thereof. That is, P: 0.001% to 0.150%, Sn: 0.001% to 0.150%, or Sb: 0.001% to 0.150%, or any combination thereof may be satisfied. preferable.
- Cr, Cu and Ni are effective elements for increasing the specific resistance and reducing the iron loss. Therefore, Cr, Cu, or Ni, or any combination thereof may be contained. In order to sufficiently obtain this effect, preferably, Cr: 0.005% or more, Cu: 0.005% or more, or Ni: 0.005% or more, or any combination thereof, more preferably Cr : 0.010% or more, Cu: 0.010% or more, Ni: 0.010% or more, or any combination thereof. However, excess Cr, Cu and Ni degrade the magnetic flux density.
- Cr 1.000% or less, Cu: 1.000% or less, and Ni: 1.000% or less.
- Cr 0.500% or less, Cu: 0.500% or less, or Ni: 0.500% or less, or any combination thereof, more preferably Cr: 0.300% or less, Cu : 0.300% or less, or Ni: 0.300% or less, or any combination thereof. That is, Cr: 0.005% to 1.000%, Cu: 0.005% to 1.000%, or Ni: 0.005% to 1.000%, or any combination thereof may be satisfied. preferable.
- Ti, V, and Nb are not essential elements but are contained as impurities in, for example, steel.
- Ti, V, and Nb combine with C, N, Mn, and the like to form inclusions, inhibit growth of crystal grains during annealing, and deteriorate magnetic properties. Therefore, the lower the Ti content, the V content, and the Nb content, the better.
- Such deterioration of the magnetic properties is significant when Ti is more than 0.010%, V is more than 0.010%, or Nb is more than 0.010%, or any combination thereof. Therefore, Ti: 0.010% or less, V: 0.010% or less, and Nb: 0.010% or less.
- Ti 0.007% or less, V: 0.007% or less, or Nb: 0.007% or less, or any combination thereof, more preferably Ti: 0.004% or less, V : 0.004% or less, or Nb: 0.004% or less, or any combination thereof.
- the average crystal grain size of the electrical steel sheet according to the embodiment of the present invention will be described. Even if the average crystal grain size is too large or too small, the iron loss is deteriorated. Such deterioration of the iron loss is remarkable when the average crystal grain size is less than 20 ⁇ m or exceeds 300 ⁇ m. Accordingly, the average crystal grain size is 20 ⁇ m or more and 300 ⁇ m or less.
- the lower limit of the average crystal grain size is preferably 30 ⁇ m, and more preferably 40 ⁇ m.
- the upper limit of the average crystal grain size is preferably 250 ⁇ m, more preferably 200 ⁇ m.
- an average value of crystal grain sizes measured by a cutting method in the plate thickness direction and the rolling direction in the longitudinal cross-sectional structure photograph parallel to the plate thickness direction and the rolling direction can be used.
- an optical microscope photograph can be used. For example, a photograph taken at a magnification of 50 times can be used.
- the plate thickness is preferably 0.10 mm or more.
- the thickness of the electromagnetic steel sheet is more preferably 0.15 mm or more, and still more preferably 0.20 mm or more.
- the plate thickness is preferably 0.50 mm or less.
- the thickness of the electromagnetic steel sheet is more preferably 0.35 mm or less, and still more preferably 0.30 mm or less.
- slab hot rolling, hot rolled sheet annealing, first cold rolling, intermediate annealing, second cold rolling, and finish annealing are performed.
- hot rolling for example, a slab having the above chemical composition is charged into a heating furnace and hot rolled.
- hot rolling may be started without charging the heating furnace.
- the slab can be obtained, for example, by continuous casting of steel, or obtained by performing ingot rolling on a steel ingot.
- hot rolled sheet annealing After hot rolling, the hot rolled steel sheet obtained by hot rolling is annealed (hot rolled sheet annealing).
- Hot-rolled sheet annealing may be performed using a box furnace, or continuous annealing may be performed as hot-rolled sheet annealing.
- box-type annealing annealing using a box furnace.
- the holding temperature in the case of performing box-type annealing is more preferably 730 ° C. or more, and further preferably 750 ° C. or more.
- the holding temperature in the case of performing box-type annealing is more preferably 1050 ° C. or less, and further preferably 1000 ° C. or less.
- the holding time when performing box-type annealing is more preferably 2 hours or more, and further preferably 3 hours or more.
- the holding time when performing box-type annealing is more preferably 150 hours or less, and even more preferably 100 hours or less.
- the holding temperature in the case of performing the continuous annealing is more preferably 780 ° C. or more, further preferably 800 ° C. or more.
- the holding temperature in continuous annealing is more preferably 1220 ° C. or lower, and further preferably 1200 ° C. or lower.
- the holding time in the case of continuous annealing is more preferably 3 seconds or more, and further preferably 5 seconds or more.
- the holding time for continuous annealing is more preferably 500 seconds or less, and still more preferably 400 seconds or less.
- the average crystal grain size of the annealed steel sheet obtained by hot-rolled sheet annealing is preferably 20 ⁇ m or more, more preferably 35 ⁇ m or more, and further preferably 40 ⁇ m or more.
- the cold rolling rate of the first cold rolling (hereinafter sometimes referred to as “first cold rolling rate”) is preferably 40% or more and 85% or less.
- first cold rolling rate is more preferably 45% or more, and further preferably 50% or more.
- the first cold rolling rate is more preferably 80% or less, and further preferably 75% or less.
- annealing (intermediate annealing) of the cold-rolled steel sheet obtained by the first cold rolling (hereinafter sometimes referred to as “intermediate cold-rolled steel sheet”) is performed.
- Box-type annealing may be performed as intermediate annealing, and continuous annealing may be performed as intermediate annealing.
- the temperature of the intermediate annealing is too low or when the time is too short, the crystal grains cannot be sufficiently coarsened and desired magnetic properties may not be obtained.
- the temperature of the intermediate annealing is too high or when the time is too long, the manufacturing cost increases.
- the holding temperature in the case of performing box-type annealing is more preferably 880 ° C. or more, and further preferably 900 ° C. or more.
- the holding temperature in the case of performing box-type annealing is more preferably 1050 ° C. or less, and further preferably 1000 ° C. or less.
- the holding time when performing box-type annealing is more preferably 2 hours or more, and further preferably 3 hours or more.
- the holding time when performing box-type annealing is more preferably 150 hours or less, and even more preferably 100 hours or less.
- the holding temperature in the case of performing continuous annealing is more preferably 1080 ° C. or more, and further preferably 1110 ° C. or more.
- the holding temperature in continuous annealing is more preferably 1220 ° C. or lower, and further preferably 1200 ° C. or lower.
- the holding time for continuous annealing is more preferably 2 seconds or more, and further preferably 3 seconds or more.
- the holding time for continuous annealing is more preferably 500 seconds or less, and still more preferably 400 seconds or less.
- the average crystal grain size of the intermediate annealed steel sheet obtained by the intermediate annealing is preferably 140 ⁇ m or more, more preferably 170 ⁇ m or more, and further preferably 200 ⁇ m or more.
- box-type annealing is preferable to continuous annealing.
- second cold rolling of the intermediate annealing steel plate obtained by the intermediate annealing is performed.
- the cold rolling rate of the second cold rolling (hereinafter sometimes referred to as “second cold rolling rate”) is preferably 45% or more and 85% or less.
- the second cold rolling rate is more preferably 50% or more, and further preferably 55% or more.
- the second cold rolling reduction is more preferably 80% or less, and further preferably 75% or less.
- the cold-rolled steel sheet obtained by the second cold rolling is annealed (finish annealing). If the finish annealing temperature is too low or the time is too short, an average crystal grain size of 20 ⁇ m or more cannot be obtained, and desired magnetic properties may not be obtained. On the other hand, in order to perform finish annealing above 1250 ° C., special equipment is required, which is economically disadvantageous. If the finishing temperature exceeds 600 hours, the productivity is low, which is economically disadvantageous.
- the temperature of finish annealing is preferably 700 ° C. or more and 1250 ° C. or less, and the finish annealing time is preferably 1 second or more and 600 seconds or less.
- the temperature of finish annealing is more preferably 750 ° C. or higher.
- the temperature of finish annealing is more preferably 1200 ° C. or less.
- the finish annealing time is more preferably 3 seconds or longer.
- the finish annealing time is more preferably 500 seconds or less.
- An insulating film may be formed on the surface of the electromagnetic steel sheet after the finish annealing.
- an insulating film you may form what consists only of an organic component, what consists only of an inorganic component, and what consists of an organic inorganic composite. From the viewpoint of reducing the environmental burden, an insulating coating that does not contain chromium may be formed.
- the coating may be an insulating coating that exhibits adhesive ability by heating and pressing.
- a coating material that exhibits adhesive ability for example, an acrylic resin, a phenol resin, an epoxy resin, or a melamine resin can be used.
- Such a magnetic steel sheet according to this embodiment is suitable for a high-efficiency motor iron core, particularly a high-efficiency split iron-core motor stator (stator) iron core.
- the high efficiency motor include compressor motors such as air conditioners and refrigerators, and drive motors and generator motors such as electric vehicles and hybrid vehicles.
- the cold-rolled steel sheet having a thickness of 0.30 mm was obtained by subjecting the annealed steel sheet to cold rolling twice or two times with intermediate annealing in between.
- the intermediate annealing box-type annealing held at 950 ° C. for 10 hours, or continuous annealing held at a temperature of 900 ° C. to 1100 ° C. for 30 seconds was performed.
- the grinding plate with a thickness of 3 mm was obtained by the grinding process of front and back.
- the ground plate was heated at 1150 ° C. for 30 minutes, and then subjected to one-pass finish rolling at 850 ° C. under the condition of a strain rate of 35 s ⁇ 1 to obtain a hot-rolled steel plate having a plate thickness of 1.0 mm. Then, after performing hot-rolled sheet annealing held at 1000 ° C. for 30 seconds, a cold-rolled steel sheet having a sheet thickness of 0.30 mm was obtained by cold rolling.
- the cold rolled steel sheet was subjected to finish annealing that was held at 1000 ° C. for 1 second to obtain an electromagnetic steel sheet.
- the integration degree I Cube was 0.1 or more and 10.0 or less
- the integration degree I Goss was 0.3 or more and 23.8 or less. It was.
- the average crystal grain size was 66 ⁇ m or more and 72 ⁇ m or less.
- the magnetic flux density B50L in the L direction when magnetized with a magnetizing force of 5000 A / m and the magnetic flux density B50C in the C direction when magnetized with a magnetizing force of 5000 A / m were measured.
- the iron loss W15 / 400L and the magnetic flux density B50L were measured without applying compressive stress, and the iron loss W15 / 400C and the magnetic flux density B50C were measured in a state where a compressive stress of 40 MPa was applied in the C direction.
- the magnetic properties were measured by a 55 mm square single sheet magnetic property test method (SST) in accordance with JIS C2556. The results are shown in Table 1 and FIGS. The underline in Table 1 indicates that the numerical value is out of the range of the present invention or the preferred range.
- the saturation magnetic flux density Bs in Table 1 was obtained by the following formula.
- [Si], [Mn], and [Al] are the contents of Si, Mn, and Al, respectively.
- Bs 2.1561-0.0413 ⁇ [Si] ⁇ 0.0198 ⁇ [Mn] ⁇ 0.0604 ⁇ [Al]
- FIG. 3 shows the relationship between the degree of integration I Goss and the degree of integration I Cube of the invention example and the comparative example, and the expressions 1, 2 and 3.
- FIGS. 1, 2 and 3 when all of the relations of Expressions 1, 2 and 3 are satisfied, it is possible to obtain excellent magnetic properties in the L direction under no stress.
- excellent magnetic properties in the C direction could be obtained under compressive stress in the C direction.
- FIG. 4 shows the relationship between the ratio (B50L / Bs) of the magnetic flux density B50L to the saturation magnetic flux density Bs and the ratio (B50C / Bs) of the magnetic flux density B50C to the saturation magnetic flux density Bs.
- the inventive example satisfies the relationship of Equation 7 and Equation 8.
- the first cold rolling with a first cold rolling rate of 60% was applied to the annealed steel sheet to obtain an intermediate cold rolled steel sheet with a thickness of 1.0 mm.
- an intermediate annealed steel sheet was obtained by subjecting the intermediate cold rolled steel sheet to intermediate annealing under the conditions shown in Table 2 below. As shown in Table 2, the average grain size of the intermediate annealed steel sheet was 71 ⁇ m or more and 355 ⁇ m or less.
- the cold-rolled steel sheet having a thickness of 0.30 mm was obtained by subjecting the intermediate annealed steel sheet to second cold rolling. Thereafter, the cold-rolled steel sheet was subjected to finish annealing for 15 seconds at 1000 ° C. to obtain an electromagnetic steel sheet.
- the integration degree I Cube was 2.3 or more and 4.1 or less
- the integration degree I Goss was 6.5 or more and 24.5 or less. It was.
- the average crystal grain size was 70 ⁇ m or more and 82 ⁇ m or less.
- the first cold rolling with a first cold rolling rate of 70% was applied to the annealed steel sheet to obtain an intermediate cold-rolled steel sheet with a thickness of 0.6 mm.
- the intermediate cold-rolled steel sheet was subjected to box-type intermediate annealing that was held at 950 ° C. for 100 hours to obtain an intermediate-annealed steel sheet.
- the average grain size of the intermediate annealed steel sheet was 280 ⁇ m or more and 343 ⁇ m or less.
- the cold-rolled steel sheet having a thickness of 0.25 mm was obtained by subjecting the intermediate-annealed steel sheet to second cold rolling with a second cold rolling rate of 58%.
- the cold-rolled steel sheet was subjected to finish annealing that was held at a temperature of 1050 ° C. for 30 seconds to obtain an electromagnetic steel sheet.
- the integration degree I Cube was 1.9 or more and 3.9 or less
- the integration degree I Goss was 8.0 or more and 21.3 or less. It was.
- the average crystal grain size was 105 ⁇ m or more and 123 ⁇ m or less.
- Sample No. 31-No. 38 since the component was within the range of the present invention, a desired texture was obtained, and magnetic characteristics satisfying the relations of Expressions 7 and 8 were obtained.
- sample No. 39-No. In No. 41 since the Al content or the Si content was out of the scope of the present invention, a desired texture was not obtained, and the magnetic characteristics did not satisfy the relationship of Formula 8.
- an annealed steel sheet was obtained by subjecting the hot-rolled steel sheet to hot-rolled sheet annealing under the conditions shown in Table 5 below.
- Table 5 the average grain size of the annealed steel sheet was 24 ⁇ m or more and 135 ⁇ m or less.
- the first cold rolling rate of 35% to 75% was applied to the annealed steel sheet to obtain an intermediate cold rolled steel sheet having a thickness of 0.5 mm to 1.3 mm.
- the intermediate cold-rolled steel sheet was subjected to box-type intermediate annealing held at 950 ° C. for 10 hours to obtain an intermediate-annealed steel sheet.
- the average grain size of the intermediate annealed steel sheet was 295 ⁇ m or more and 314 ⁇ m or less.
- a cold-rolled steel sheet having a thickness of 0.15 mm or more and 0.35 mm or less was obtained by subjecting the intermediate annealed steel sheet to second cold rolling with a second cold rolling rate of 30% to 86%. . Thereafter, the cold-rolled steel sheet was subjected to finish annealing at 800 ° C. to 1120 ° C. for 15 seconds to 60 seconds to obtain a magnetic steel sheet.
- the integration degree I Cube was 1.5 or more and 3.7 or less
- the integration degree I Goss was 5.5 or more and 16.4 or less. It was.
- the average crystal grain size was 32 ⁇ m or more and 192 ⁇ m or less as shown in Table 6.
- Sample No. 51-No. In No. 53 since hot-rolled sheet annealing, first cold rolling, and second cold rolling were performed under preferable conditions, a desired texture was obtained, and magnetic characteristics satisfying the relationship of Equations 7 and 8 were obtained. It was. On the other hand, Sample No. 54-No. 57, since the conditions of hot-rolled sheet annealing, first cold rolling or second cold rolling were out of the preferred range, the desired texture could not be obtained, and the magnetic properties were the relationship of Formula 7 or Formula 8. Did not meet.
- sample no. The torque constant of the split iron motor with iron core material 3 is the same as that of sample No. under all load torques. 7, Sample No. It was superior to the torque constant of the split core motor using 8 as the core material. On the other hand, Sample No. 7 or sample no. The torque constant of the split core motor using 8 as the iron core material was low especially under low load torque conditions.
- the present invention can be used, for example, in the manufacturing industry of electromagnetic steel sheets and the industries using electromagnetic steel sheets such as motors.
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Abstract
Description
(1)
質量%で、
C :0.010%以下、
Si:1.30%~3.50%、
Al:0.0000%~1.6000%、
Mn:0.01%~3.00%、
S :0.0100%以下、
N :0.010%以下、
P :0.000%~0.150%、
Sn:0.000%~0.150%、
Sb:0.000%~0.150%、
Cr:0.000%~1.000%、
Cu:0.000%~1.000%、
Ni:0.000%~1.000%、
Ti:0.010%以下、
V :0.010%以下、
Nb:0.010%以下、かつ
残部:Fe及び不純物
で表される化学組成を有し、
結晶粒径が20μm~300μmであり、
(001)[100]方位の集積度をICube、(011)[100]方位の集積度をIGossとあらわしたとき、式1、式2及び式3の関係を満たす集合組織を有することを特徴とする電磁鋼板。
IGoss+ICube≧10.5 ・・・式1
IGoss/ICube≧0.50 ・・・式2
ICube≧2.5 ・・・式3
前記集合組織は、式4、式5及び式6を満たすことを特徴とする(1)に記載の電磁鋼板。
IGoss+ICube≧10.7 ・・・式4
IGoss/ICube≧0.52 ・・・式5
ICube≧2.7 ・・・式6
飽和磁束密度をBs、5000A/mの磁化力で磁化した際の圧延方向の磁束密度をB50L、5000A/mの磁化力で磁化した際の圧延方向及び板厚方向に直交する方向(板幅方向)の磁束密度をB50Cとあらわしたとき、式7及び式8の関係を満たす磁気特性を有することを特徴とする(1)又は(2)に記載の電磁鋼板。
B50C/Bs≧0.790 ・・・式7
(B50L-B50C)/Bs≧0.070 ・・・式8
前記磁気特性は、式9の関係を満たす磁気特性を有することを特徴とする(3)に記載の電磁鋼板。
(B50L-B50C)/Bs≧0.075 ・・・式9
前記磁気特性は、式10の関係を満たすことを特徴とする(3)又は(4)に記載の電磁鋼板。
B50C/Bs≦0.825 ・・・式10
前記化学組成において、
P :0.001%~0.150%、
Sn:0.001%~0.150%、若しくは
Sb:0.001%~0.150%、
又はこれらの任意の組み合わせが満たされることを特徴とする(1)乃至(5)のいずれかに記載の電磁鋼板。
前記化学組成において、
Cr:0.005%~1.000%、
Cu:0.005%~1.000%、
Ni:0.005%~1.000%、
又はこれらの任意の組み合わせが満たされることを特徴とする(1)乃至(6)のいずれかに記載の電磁鋼板。
厚さが0.10mm以上0.50mm以下であることを特徴とする(1)乃至(7)のいずれか1項に記載の電磁鋼板。
IGoss+ICube≧10.5 ・・・式1
IGoss/ICube≧0.50 ・・・式2
ICube≧2.5 ・・・式3
IGoss+ICube≧10.7 ・・・式4
IGoss/ICube≧0.52 ・・・式5
ICube≧2.7 ・・・式6
B50C/Bs≧0.790 ・・・式7
(B50L-B50C)/Bs≧0.070 ・・・式8
(B50L-B50C)/Bs≧0.075 ・・・式9
B50C/Bs≦0.825 ・・・式10
Siは、比抵抗を高めて鉄損を低減させるのに有効な元素である。Si含有量を1.30%以上とすることで、より確実にかかる比抵抗向上効果を得ることができる。従って、Si含有量は1.30%以上とする。Si含有量は、好ましくは1.60%以上であり、より好ましくは1.90%以上である。一方、Si含有量が3.50%超であると、所望の集合組織を得ることができず、所望の磁束密度が得られない。従って、Si含有量は3.50%以下とする。Si含有量は、好ましくは3.30%以下であり、より好ましくは3.10%以下である。Si含有量が3.50%超の場合に所望の集合組織を得ることができない理由として、Si含有量の増加に伴う冷間圧延での変形挙動の変化が生じていることが考えられる。
Alは、飽和磁束密度を低下させる元素である。Al含有量が1.6000%超であると、所望の集合組織を得ることができず、所望の磁束密度が得られない。従って、Al含有量は、1.6000%以下とする。Al含有量は、好ましくは1.4000%以下であり、より好ましくは1.2000%以下であり、更に好ましくは0.8000%以下である。Al含有量が1.6000%超の場合に所望の集合組織を得ることができない理由として、Al含有量の増加に伴う冷間圧延での変形挙動の変化が生じていることが考えられる。Al含有量の下限は特に限定されない。Alは、比抵抗を高めて鉄損を低減させる効果を有し、この効果を得るために、Al含有量は、好ましくは0.0001%以上であり、より好ましくは0.0003%以上である。
Mnは、比抵抗を高めて鉄損を低減させるのに有効な元素である。Mn含有量を0.01%以上とすることで、より確実にかかる比抵抗向上効果を得ることができる。従って、Mn含有量は0.01%以上とする。Mn含有量は、好ましくは0.03%以上であり、より好ましくは0.05%以上である。一方、Mnを過剰に含有させると磁束密度が低下する。このような現象は、Mn含有量が3.00%超で顕著である。従って、Mn含有量は、3.00%以下とする。Mn含有量は、好ましくは2.70%以下であり、より好ましくは2.50%以下、更に好ましくは2.40%以下である。
Cは、必須元素ではなく、例えば鋼中に不純物として含有される。Cは、磁気時効により磁気特性を劣化させる元素である。従って、C含有量は低ければ低いほどよい。このような磁気特性の劣化は、C含有量が0.010%超で顕著である。このため、C含有量は0.010%以下とする。C含有量は、好ましくは0.008%以下であり、より好ましくは、0.005%以下である。
Sは、必須元素ではなく、例えば鋼中に不純物として含有される。Sは、鋼中のMnと結合して微細なMnSを形成し、仕上焼鈍中の粒成長を阻害し、磁気特性を劣化させる。従って、S含有量は低ければ低いほどよい。このような磁気特性の劣化は、S含有量が0.0100%超で顕著である。このため、S含有量は0.0100%以下とする。S含有量は、好ましくは0.0080%以下であり、より好ましくは、0.0050%以下である。Sは磁束密度の向上に寄与する。この効果を得るために、0.0005%以上のSが含有されていてもよい。Sが磁束密度の向上に寄与する理由として、磁気特性に不利な方位の粒成長がSによって阻害されていることが考えられる。
Nは、必須元素ではなく、例えば鋼中に不純物として含有される。Nは、鋼中のAlと結合して微細なAlNを形成し、仕上焼鈍中の粒成長を阻害し、磁気特性を劣化させる。従って、N含有量は低ければ低いほどよい。このような磁気特性の劣化は、N含有量が0.010%超で顕著である。このため、N含有量は0.010%以下とする。N含有量は、好ましくは0.008%以下であり、より好ましくは、0.005%以下である。
P、Sn及びSbは、電磁鋼板の集合組織を改善して磁気特性を向上させる作用を有する。従って、P、Sn、若しくはSb、又はこれらの任意の組み合わせが含有されていてもよい。この効果を十分に得るために、好ましくは、P:0.001%以上、Sn:0.001%以上、若しくはSb:0.001%以上、又はこれらの任意の組み合わせとし、より好ましくは、P:0.003%以上、Sn:0.003%以上、若しくはSb:0.003%以上、又はこれらの任意の組み合わせとする。しかし、過剰なP、Sn及びSbは、結晶粒径に偏析して鋼板の延性が低下させ、冷間圧延を困難にする。このような延性の低下は、P:0.150%超、Sn:0.150%超、若しくはSb:0.150%超、又はこれらの任意の組み合わせで顕著である。このため、P:0.150%以下、Sn:0.150%以下、かつSb:0.150%以下とする。好ましくは、P:0.100%以下、Sn:0.100%以下、若しくはSb:0.100%以下、又はこれらの任意の組み合わせであり、より好ましくは、P:0.050%以下、Sn:0.050%以下、若しくはSb:0.050%以下、又はこれらの任意の組み合わせである。つまり、P:0.001%~0.150%、Sn:0.001%~0.150%、若しくはSb:0.001%~0.150%、又はこれらの任意の組み合わせが満たされることが好ましい。
Cr、Cu及びNiは、比抵抗を高めて鉄損を低減させるのに有効な元素である。従って、Cr、Cu、若しくはNi、又はこれらの任意の組み合わせが含有されていてもよい。この効果を十分に得るために、好ましくは、Cr:0.005%以上、Cu:0.005%以上、若しくはNi:0.005%以上、又はこれらの任意の組み合わせとし、より好ましくは、Cr:0.010%以上、Cu:0.010%以上、若しくはNi:0.010%以上、又はこれらの任意の組み合わせとする。しかし、過剰なCr、Cu及びNiは、磁束密度を劣化させる。このような磁束密度の劣化は、Cr:1.000%超、Cu:1.000%超、若しくはNi:1.000%超、又はこれらの任意の組み合わせで顕著である。このため、Cr:1.000%以下、Cu:1.000%以下、かつNi:1.000%以下とする。好ましくは、Cr:0.500%以下、Cu:0.500%以下、若しくはNi:0.500%以下、又はこれらの任意の組み合わせであり、より好ましくは、Cr:0.300%以下、Cu:0.300%以下、若しくはNi:0.300%以下、又はこれらの任意の組み合わせである。つまり、Cr:0.005%~1.000%、Cu:0.005%~1.000%、若しくはNi:0.005%~1.000%、又はこれらの任意の組み合わせが満たされることが好ましい。
Ti、V及びNbは、必須元素ではなく、例えば鋼中に不純物として含有される。Ti、V及びNbは、C、N、Mn等と結合して介在物を形成し、焼鈍中の結晶粒の成長を阻害して磁気特性を劣化させる。従って、Ti含有量、V含有量及びNb含有量は低ければ低いほどよい。このような磁気特性の劣化は、Ti:0.010%超、V:0.010%超、若しくはNb:0.010%超、又はこれらの任意の組み合わせで顕著である。このため、Ti:0.010%以下、V:0.010%以下、かつNb:0.010%以下とする。好ましくは、Ti:0.007%以下、V:0.007%以下、若しくはNb:0.007%以下、又はこれらの任意の組み合わせであり、より好ましくは、Ti:0.004%以下、V:0.004%以下、若しくはNb:0.004%以下、又はこれらの任意の組み合わせである。
第1の試験では、集合組織と磁気特性との関係について調査した。先ず、質量%で、C:0.002%、Si:2.10%、Al:0.0050%、Mn:0.20%、S:0.002%、N:0.002%、P:0.012%、Sn:0.002%、Sb:0.001%、Cr:0.01%、Cu:0.02%、Ni:0.01%、Ti:0.002%、V:0.002%、及びNb:0.003%を含有し、残部がFe及び不純物からなる複数のスラブを作製した。スラブの一部については、熱間圧延により板厚が2.5mmの熱延鋼板とした後、800℃で10時間保持する箱型の焼鈍又は1000℃で30秒保持する連続焼鈍を熱延板焼鈍として施して焼鈍鋼板を得た。次いで、焼鈍鋼板に1回又は中間焼鈍を間に挟む2回の冷間圧延を施して板厚が0.30mmの冷延鋼板を得た。中間焼鈍としては、950℃で10時間保持する箱型の焼鈍、又は900℃以上1100℃以下の温度で30秒保持する連続焼鈍を行った。残りのスラブについては、熱間圧延における粗圧延にて板厚を10mmとした後、表裏面の研削加工によって厚さが3mmの研削板を得た。次いで、研削板を1150℃で30分加熱した後、850℃にて歪速度が35s-1の条件で1パスの仕上圧延を施して、板厚が1.0mmの熱延鋼板を得た。その後、1000℃で30秒保持する熱延板焼鈍を施した後、冷間圧延によって板厚が0.30mmの冷延鋼板を得た。
Bs=2.1561-0.0413×[Si]-0.0198×[Mn]-0.0604×[Al]
B50C/Bs≧0.790 ・・・式7
(B50L-B50C)/Bs≧0.070 ・・・式8
第2の試験では、中間焼鈍の条件と集積度及び磁気特性との関係について調査した。先ず、質量%で、C:0.002%、Si:1.99%、Al:0.0190%、Mn:0.20%、S:0.002%、N:0.002%、及びP:0.012%を含有し、残部がFe及び不純物からなる板厚が2.5mmの複数の熱延鋼板を作製した。次いで、熱延鋼板に800℃の温度で10時間保持する箱型の熱延板焼鈍を施して焼鈍鋼板を得た。焼鈍鋼板の平均結晶粒径は70μmであった。その後、第1の冷間圧延率が60%の第1の冷間圧延を焼鈍鋼板に施すことにより、板厚が1.0mmの中間冷延鋼板を得た。続いて、中間冷延鋼板に下記表2に示す条件で中間焼鈍を施すことにより、中間焼鈍鋼板を得た。表2に示すように、中間焼鈍鋼板の平均結晶粒径は71μm以上355μm以下であった。次いで、中間焼鈍鋼板に第2の冷間圧延を施すことにより、板厚が0.30mmの冷延鋼板を得た。その後、冷延鋼板に1000℃で15秒間保持する仕上焼鈍を施して、電磁鋼板を得た。上記のシュルツ法による測定を行ったところ、下記表2に示すように、集積度ICubeは2.3以上4.1以下であり、集積度IGossは6.5以上24.5以下であった。上記の縦断面組織写真を用いた方法による測定を行ったところ、表2に示すように、平均結晶粒径は70μm以上82μm以下であった。
第3の試験では、成分と集積度及び磁気特性との関係について調査した。先ず、表3に示す成分を含み、更にTi:0.002%、V:0.003%、及びNb:0.002%を含み、残部がFe及び不純物からなる板厚が2.0mmの複数の熱延鋼板を作製した。次いで、熱延板焼鈍として、1000℃で30秒保持する連続焼鈍を施して焼鈍鋼板を得た。焼鈍鋼板の平均結晶粒径は72μm以上85μm以下であった。その後、第1の冷間圧延率が70%の第1の冷間圧延を焼鈍鋼板に施すことにより、板厚が0.6mmの中間冷延鋼板を得た。続いて、中間冷延鋼板に、950℃で100時間保持する箱型の中間焼鈍を施すことにより、中間焼鈍鋼板を得た。中間焼鈍鋼板の平均結晶粒径は280μm以上343μm以下であった。次いで、第2の冷間圧延率が58%の第2の冷間圧延を中間焼鈍鋼板に施すことにより、板厚が0.25mmの冷延鋼板を得た。その後、冷延鋼板に1050℃の温度で30秒間保持する仕上焼鈍を施して、電磁鋼板を得た。上記のシュルツ法による測定を行ったところ、下記表4に示すように、集積度ICubeは1.9以上3.9以下であり、集積度IGossは8.0以上21.3以下であった。上記の縦断面組織写真を用いた方法による測定を行ったところ、表4に示すように、平均結晶粒径は105μm以上123μm以下であった。
第4の試験では、熱延板焼鈍、第1の冷間圧延及び第2の冷間圧延の条件と磁気特性との関係について調査した。先ず、質量%で、C:0.002%、Si:2.15%、Al:0.0050%、Mn:0.20%、S:0.003%、N:0.001%、P:0.016%、Sn:0.003%、Sb:0.002%、Cr:0.02%、Cu:0.01%、Ni:0.01%、Ti:0.003%、V:0.001%、及びNb:0.002%を含有し、残部がFe及び不純物からなる板厚が1.6mm以上2.5mm以下の熱延鋼板を作製した。次いで、熱延鋼板に下記表5に示す条件で熱延板焼鈍を施すことにより、焼鈍鋼板を得た。表5に示すように、焼鈍鋼板の平均結晶粒径は24μm以上135μm以下であった。その後、焼鈍鋼板に、第1の冷間圧延率が35%以上75%以下の第1の冷間圧延を施して、板厚が0.5mm以上1.3mm以下の中間冷延鋼板を得た。続いて、中間冷延鋼板に950℃で10時間保持する箱型の中間焼鈍を施して、中間焼鈍鋼板を得た。中間焼鈍鋼板の平均結晶粒径は295μm以上314μm以下であった。次いで、中間焼鈍鋼板に第2の冷間圧延率が30%以上86%以下の第2の冷間圧延を施すことにより、板厚が0.15mm以上0.35mm以下の冷延鋼板を得た。その後、冷延鋼板に800℃以上1120℃で15秒間以上60秒間以下保持する仕上焼鈍を施して、電磁鋼板を得た。上記のシュルツ法による測定を行ったところ、下記表6に示すように、集積度ICubeは1.5以上3.7以下であり、集積度IGossは5.5以上16.4以下であった。上記の縦断面組織写真を用いた方法による測定を行ったところ、表6に示すように、平均結晶粒径は32μm以上192μm以下であった。
第5の試験では、試料No.3、試料No.7、試料No.8の電磁鋼板を鉄心材料として、4極6スロットルの埋込構造永久磁石(interior permanent magnet:IPM)分割鉄心モータを作製し、負荷トルクが1Nm、2Nm、3Nmの下でのトルク定数を測定した。IMP分割鉄心モータにおいては、電磁鋼板のL方向がモータ鉄心のティース部と平行になり、C方向がバックヨーク部と平行になるようにした。トルク定数とは、所定のトルクを、そのトルクを出すために必要な電流値で規格化した値である。言い換えると、トルク定数は電流1A当たりのトルクに相当し、高いほど好ましい。この結果を表7に示す。表7中の下線は、その数値が本発明の範囲から外れていることを示す。
Claims (8)
- [規則91に基づく訂正 22.07.2015]
質量%で、
C :0.010%以下、
Si:1.30%~3.50%、
Al:0.0000%~1.6000%、
Mn:0.01%~3.00%、
S :0.0100%以下、
N :0.010%以下、
P :0.000%~0.150%、
Sn:0.000%~0.150%、
Sb:0.000%~0.150%、
Cr:0.000%~1.000%、
Cu:0.000%~1.000%、
Ni:0.000%~1.000%、
Ti:0.010%以下、
V :0.010%以下、
Nb:0.010%以下、かつ
残部:Fe及び不純物
で表される化学組成を有し、
結晶粒径が20μm~300μmであり、
(001)[100]方位の集積度をICube、(011)[100]方位の集積度をIGossとあらわしたとき、式1、式2及び式3の関係を満たす集合組織を有することを特徴とする電磁鋼板。
IGoss+ICube≧10.5 ・・・式1
IGoss/ICube≧0.50 ・・・式2
ICube≧2.5 ・・・式3 - 前記集合組織は、式4、式5及び式6を満たすことを特徴とする請求項1に記載の電磁鋼板。
IGoss+ICube≧10.7 ・・・式4
IGoss/ICube≧0.52 ・・・式5
ICube≧2.7 ・・・式6 - 飽和磁束密度をBs、5000A/mの磁化力で磁化した際の圧延方向の磁束密度をB50L、5000A/mの磁化力で磁化した際の圧延方向及び板厚方向に直交する方向(板幅方向)の磁束密度をB50Cとあらわしたとき、式7及び式8の関係を満たす磁気特性を有することを特徴とする請求項1又は2に記載の電磁鋼板。
B50C/Bs≧0.790 ・・・式7
(B50L-B50C)/Bs≧0.070 ・・・式8 - 前記磁気特性は、式9の関係を満たす磁気特性を有することを特徴とする請求項3に記載の電磁鋼板。
(B50L-B50C)/Bs≧0.075 ・・・式9 - 前記磁気特性は、式10の関係を満たすことを特徴とする請求項3又は4に記載の電磁鋼板。
B50C/Bs≦0.825 ・・・式10 - 前記化学組成において、
P :0.001%~0.150%、
Sn:0.001%~0.150%、若しくは
Sb:0.001%~0.150%、
又はこれらの任意の組み合わせが満たされることを特徴とする請求項1乃至5のいずれか1項に記載の電磁鋼板。 - 前記化学組成において、
Cr:0.005%~1.000%、
Cu:0.005%~1.000%、
Ni:0.005%~1.000%、
又はこれらの任意の組み合わせが満たされることを特徴とする請求項1乃至6のいずれか1項に記載の電磁鋼板。 - 厚さが0.10mm以上0.50mm以下であることを特徴とする請求項1乃至7のいずれか1項に記載の電磁鋼板。
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---|---|---|---|---|
JP2018148119A (ja) * | 2017-03-08 | 2018-09-20 | 株式会社神戸製鋼所 | イグニッションコイル用鉄心及びイグニッションコイル用鉄心の製造方法 |
JP2018529021A (ja) * | 2015-07-29 | 2018-10-04 | アペラム | FeCo合金、FeSi合金またはFeシートもしくはストリップおよびその製造方法、前記シートまたはストリップから製造された磁気変圧器コア、ならびにそれを備える変圧器 |
KR20190034585A (ko) * | 2016-07-29 | 2019-04-02 | 잘쯔기터 플래시슈탈 게엠베하 | 무방향성 전기 강을 제조하기 위한 강 스트립 및 이러한 강 스트립을 제조하기 위한 방법 |
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KR20240011574A (ko) | 2022-07-19 | 2024-01-26 | 김학규 | 하우스의 수로관 연결시스템 |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH11236618A (ja) * | 1998-02-24 | 1999-08-31 | Kawasaki Steel Corp | 低鉄損無方向性電磁鋼板の製造方法 |
JP2000104144A (ja) * | 1998-07-29 | 2000-04-11 | Kawasaki Steel Corp | L方向及びc方向の磁気特性に優れた電磁鋼板及びその製造方法 |
JP2012036457A (ja) * | 2010-08-09 | 2012-02-23 | Sumitomo Metal Ind Ltd | 無方向性電磁鋼板およびその製造方法 |
JP2012036454A (ja) * | 2010-08-09 | 2012-02-23 | Sumitomo Metal Ind Ltd | 無方向性電磁鋼板およびその製造方法 |
Family Cites Families (16)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2639226B2 (ja) * | 1991-03-15 | 1997-08-06 | 住友金属工業株式会社 | 方向性電磁鋼板およびその製造方法 |
JPH05186828A (ja) * | 1992-01-10 | 1993-07-27 | Sumitomo Metal Ind Ltd | 低鉄損方向性電磁鋼板の製造方法 |
JP2000160250A (ja) | 1998-11-26 | 2000-06-13 | Kawasaki Steel Corp | L方向及びc方向の磁気特性に優れた電磁鋼板の製造方法 |
JP2000160256A (ja) | 1998-11-26 | 2000-06-13 | Kawasaki Steel Corp | L方向及びc方向の磁気特性に優れた電磁鋼板の製造方法 |
TW476790B (en) | 1998-05-18 | 2002-02-21 | Kawasaki Steel Co | Electrical sheet of excellent magnetic characteristics and its manufacturing method |
CN1102670C (zh) * | 1999-06-16 | 2003-03-05 | 住友金属工业株式会社 | 无方向性电磁钢片及其制造方法 |
WO2007007423A1 (ja) * | 2005-07-07 | 2007-01-18 | Sumitomo Metal Industries, Ltd. | 無方向性電磁鋼板およびその製造方法 |
JP4855220B2 (ja) * | 2006-11-17 | 2012-01-18 | 新日本製鐵株式会社 | 分割コア用無方向性電磁鋼板 |
JP2008189976A (ja) | 2007-02-02 | 2008-08-21 | Nippon Steel Corp | 圧縮応力による鉄損劣化の小さい無方向性電磁鋼板およびその製造方法 |
EP2602335B1 (en) | 2010-08-04 | 2020-03-18 | Nippon Steel Corporation | Manufacturing method of non-oriented electrical steel sheet |
JP5668460B2 (ja) * | 2010-12-22 | 2015-02-12 | Jfeスチール株式会社 | 無方向性電磁鋼板の製造方法 |
PL2703514T3 (pl) * | 2011-04-27 | 2017-09-29 | Nippon Steel & Sumitomo Metal Corporation | Oparta na Fe blacha metalowa i sposób jej wytwarzania |
JP6043808B2 (ja) | 2011-12-28 | 2016-12-14 | ポスコPosco | 無方向性電磁鋼板およびその製造方法 |
US8840734B2 (en) * | 2012-02-14 | 2014-09-23 | Nippon Steel & Sumitomo Metal Corporation | Non-oriented electrical steel sheet |
JP5716811B2 (ja) | 2013-11-07 | 2015-05-13 | 新日鐵住金株式会社 | 無方向性電磁鋼板の製造方法 |
US10604818B2 (en) * | 2014-09-01 | 2020-03-31 | Nippon Steel Corporation | Grain-oriented electrical steel sheet |
-
2015
- 2015-06-26 TW TW104120927A patent/TWI557241B/zh active
- 2015-06-26 WO PCT/JP2015/068497 patent/WO2015199211A1/ja active Application Filing
- 2015-06-26 US US15/311,609 patent/US10541071B2/en active Active
- 2015-06-26 EP EP15812138.4A patent/EP3162907B1/en active Active
- 2015-06-26 BR BR112016029465-3A patent/BR112016029465B1/pt active IP Right Grant
- 2015-06-26 JP JP2016529674A patent/JP6226072B2/ja active Active
- 2015-06-26 KR KR1020167033727A patent/KR101897886B1/ko active IP Right Grant
- 2015-06-26 PL PL15812138T patent/PL3162907T3/pl unknown
- 2015-06-26 CN CN201580031816.3A patent/CN106460122B/zh active Active
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH11236618A (ja) * | 1998-02-24 | 1999-08-31 | Kawasaki Steel Corp | 低鉄損無方向性電磁鋼板の製造方法 |
JP2000104144A (ja) * | 1998-07-29 | 2000-04-11 | Kawasaki Steel Corp | L方向及びc方向の磁気特性に優れた電磁鋼板及びその製造方法 |
JP2012036457A (ja) * | 2010-08-09 | 2012-02-23 | Sumitomo Metal Ind Ltd | 無方向性電磁鋼板およびその製造方法 |
JP2012036454A (ja) * | 2010-08-09 | 2012-02-23 | Sumitomo Metal Ind Ltd | 無方向性電磁鋼板およびその製造方法 |
Non-Patent Citations (2)
Title |
---|
HIROTOSHI TADA ET AL.: "A Hysteresis Loss Modeling of Grain Oriented Electrical Steel Sheet", JOURNAL OF THE IRON & STEEL INSTITUTE OF JAPAN, vol. 99, no. 3, 1 March 2013 (2013-03-01), pages 254 - 259, XP055375805 * |
HIROTOSHI TADA ET AL.: "Influence of magnetostriction on hysteresis loss of electrical steel sheet", JOURNAL OF MAGNETISM AND MAGNETIC MATERIALS, vol. 326, 16 September 2012 (2012-09-16), pages 217 - 219, XP055248772, ISSN: 0304-8853 * |
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KR102364477B1 (ko) * | 2016-07-29 | 2022-02-16 | 잘쯔기터 플래시슈탈 게엠베하 | 무방향성 전기 강을 제조하기 위한 강 스트립 및 이러한 강 스트립을 제조하기 위한 방법 |
KR20190034585A (ko) * | 2016-07-29 | 2019-04-02 | 잘쯔기터 플래시슈탈 게엠베하 | 무방향성 전기 강을 제조하기 위한 강 스트립 및 이러한 강 스트립을 제조하기 위한 방법 |
JP2018148119A (ja) * | 2017-03-08 | 2018-09-20 | 株式会社神戸製鋼所 | イグニッションコイル用鉄心及びイグニッションコイル用鉄心の製造方法 |
JP2022003868A (ja) * | 2018-05-18 | 2022-01-11 | ダイキン工業株式会社 | 冷凍サイクル装置 |
WO2019221178A1 (ja) * | 2018-05-18 | 2019-11-21 | ダイキン工業株式会社 | 冷凍サイクル装置 |
JPWO2019221178A1 (ja) * | 2018-05-18 | 2021-07-08 | ダイキン工業株式会社 | 冷凍サイクル装置 |
WO2022196807A1 (ja) | 2021-03-19 | 2022-09-22 | 日本製鉄株式会社 | 無方向性電磁鋼板およびその製造方法 |
WO2022196800A1 (ja) | 2021-03-19 | 2022-09-22 | 日本製鉄株式会社 | 無方向性電磁鋼板およびその製造方法 |
KR20230145142A (ko) | 2021-03-19 | 2023-10-17 | 닛폰세이테츠 가부시키가이샤 | 무방향성 전자 강판 및 그 제조 방법 |
WO2022196805A1 (ja) | 2021-03-19 | 2022-09-22 | 日本製鉄株式会社 | 無方向性電磁鋼板およびその製造方法 |
KR20230144606A (ko) | 2021-03-19 | 2023-10-16 | 닛폰세이테츠 가부시키가이샤 | 무방향성 전자 강판 및 그 제조 방법 |
KR20230142784A (ko) | 2021-03-19 | 2023-10-11 | 닛폰세이테츠 가부시키가이샤 | 무방향성 전자 강판 및 그 제조 방법 |
US12009709B2 (en) | 2021-03-31 | 2024-06-11 | Nippon Steel Corporation | Rotating electrical machine, stator core and rotor core set, method for manufacturing rotating electrical machine, method for manufacturing non-oriented electrical steel sheet, method for manufacturing rotor and stator of rotating electrical machine, and non-oriented electrical steel sheet set |
JP7184226B1 (ja) * | 2021-03-31 | 2022-12-06 | 日本製鉄株式会社 | 回転電機、ステータの鉄心およびロータの鉄心のセット、回転電機の製造方法、無方向性電磁鋼板の製造方法、回転電機のロータおよびステータの製造方法並びに無方向性電磁鋼板のセット |
WO2022250157A1 (ja) * | 2021-05-28 | 2022-12-01 | Jfeスチール株式会社 | 方向性電磁鋼板の製造方法 |
JP7287584B2 (ja) | 2021-05-28 | 2023-06-06 | Jfeスチール株式会社 | 方向性電磁鋼板の製造方法 |
JP7255761B1 (ja) * | 2021-05-28 | 2023-04-11 | Jfeスチール株式会社 | 方向性電磁鋼板の製造方法 |
WO2022250159A1 (ja) * | 2021-05-28 | 2022-12-01 | Jfeスチール株式会社 | 方向性電磁鋼板の製造方法 |
JPWO2022250157A1 (ja) * | 2021-05-28 | 2022-12-01 |
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BR112016029465B1 (pt) | 2021-03-23 |
BR112016029465A2 (pt) | 2017-08-22 |
JP6226072B2 (ja) | 2017-11-08 |
KR101897886B1 (ko) | 2018-09-12 |
EP3162907B1 (en) | 2021-05-26 |
US20170098498A1 (en) | 2017-04-06 |
CN106460122B (zh) | 2018-06-05 |
EP3162907A4 (en) | 2017-11-29 |
CN106460122A (zh) | 2017-02-22 |
TW201606097A (zh) | 2016-02-16 |
EP3162907A1 (en) | 2017-05-03 |
KR20170002536A (ko) | 2017-01-06 |
US10541071B2 (en) | 2020-01-21 |
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