Field of the Invention:
[0001] The present invention relates to a method of manufacturing a grain-oriented electrical
steel strip adapted to be used as an iron core in a power supply transformer and a
large size rotary machine. In more detail, the present invention relates to a method
of manufacturing a grain-oriented electrical steel strip having an extremely high
magnetic flux density by controlling the average value of grain sizes and the deviation
of primary recrystallization grain to desired values in a grain-oriented electrical
steel strip manufacturing process.
Background of the Invention:
[0002] A grain-oriented electrical steel strip is used as an iron core in a power supply
transformer or a large size rotary machine, and is required to have excellent magnetic
properties such as excitation property, a core loss property and the like. The magnetic
property is generally exhibited by a magnetic flux density (B₈ value) at a magnetic
field intensity of 800 A/m. Meanwhile, the core loss property is exhibited in general
by a power loss W
17/50 (W/kg) per Kg of an iron core which is magnetized up to 1.7 tesla at a frequency
of 50 Hz. The magnetic flux density of the grain-oriented electrical steel strip is
a very important property, that is, the higher the magnetic flux density the more
satisfactory the core loss property becomes (the core loss value is decreased).
[0003] On the contrary, a grain-oriented electrical steel strip having a high magnetic flux
density has in general a large grain size of secondary recrystallization grain so
that the core loss thereof would be possibly unsatisfactory. The core loss value of
such a grain-oriented electrical steel strip can be decreased remarkable by a magnetic
domain control technology disclosed in, for example, U.S. Patent No. 4,770,720.
[0004] A grain-oriented electrical steel strip has a magnetic easy axis of <001> orientation
in its rolling direction, and also has a {110} plane on its rolled surface.
[0005] The aggregation to {110}<001> orientation in electrical steel strip is achieved by
utilizing a catastrophic phenomenon of grain growth called secondary recrystallization.
The control of secondary recrystallization essentially requires the control of a primary
recrystallization texture and structure prior to the secondary recrystallization thereof
and the control of an inhibitor, i.e. a fine precipitate, or an element of the intergranular
segregation type. The inhibitor inhibits the growth of any grains other than those
having a {110}<001> orientation in the primary recrystallization texture and enables
the selective growth of the grains having a {110}<001> orientation.
[0006] The following are the three typical processes which are known for the industrial
manufacture of grain-oriented electrical steel strips or sheets:
(1) The process as disclosed by M.F. Littmann in U.S. Patent No. 2,599,340 (Japanese
Patent Publication No. 3651/1955) which employs two steps of cold rolling utilizing
MnS as the inhibitor;
(2) The process as disclosed by Taguchi and Sakakura in U.S. Patent No. 3,287,183
(Japanese Patent Publication No. 15644/1965) which adopts a reduction rate exceeding
80% in final cold rolling utilizing an inhibitor comprising A1N and MnS; and
(3) The process as disclosed by Imanaka et al. in U.S. Patent No. 3,932,234 (Japanese
Patent Publication No. 13469/1976) which employs two steps of cold rolling utilizing
an inhibitor comprising MnS (or MnSe) and Sb.
[0007] These processes have made it possible to produce on a commercial basis grain-oriented
electrical steel strips having so high a degree of the aggregation to {110}<001> orientation
that the strips have a magnetic flux density (B₈ value) of about 1.92 tesla.
[0008] In a process of manufacturing a grain-oriented electrical steel strip, various factors
during the steps thereof affect upon the magnetic properties of products, and the
conditions to the manufacture are seriously controlled during operation. Even with
a such a seriously controlled manufacturing process, there are sometimes produced
products having an inferior secondary recrystallization and bad magnetic properties
about which the particular reason can't be found. In such a case, if occurrence of
products having an inferior secondary recrystallization and bad magnetic properties
can be known beforehand at upstream steps, a composition system and manufacturing
conditions would be adjusted to make the secondary recrystallization satisfactory
so as to produce a product in excellent in secondary recrystallization and in magnetic
properties.
[0009] However, although there have been made many trials to the forecast of occurrence
of products having an inferior secondary recrystallization and bad magnetic properties
up to now, no success have yet been achieved.
Summary of the Invention:
[0010] The present invention is devised in view of such a new finding by the inventors that
the micro structure of a material after the step of annealing for decarburization
but before the step of final annealing greatly affects upon the quality of secondary
recrystallization and the magnetic properties of a product, and accordingly one object
of the present invention is to provide a grain-oriented electrical steel strip having
an extremely high magnetic flux density by controlling the primary recrystallization
structure to a desired one.
[0011] According to the present invention, a cold-rolled electrical steel strip is controlled
so as to change the temperature and the time during the annealing step for decarburization
so as to have a micro structure having an average grain size d of greater than 15
µm, and a coefficient σ* of deviation in grain size of less than 0.6 (standard deviation
of a distribution normalized by the average grain size d) between the annealing step
for decarburization and the final annealing. Prior to the annealing step for decarburization,
the material might be subjected to a final high-reduction cold-rolling step for applying
a reduction ratio of greater than 80%, thereby it is possible to obtain a grain-oriented
electrical steel strip more excellent in the magnetic properties.
[0012] A grain-oriented electrical steel strip according to the present invention is obtained
by a manufacturing process comprising the steps of: casting molten metal obtained
by a conventionally used steel manufacturing process, into an ingot with the use of
a continuously casting process or an ingot making process and then forming a slab,
as necessary, through a blooming process; hot-rolling said ingot or slab so as to
obtain a hot-rolled steel strip; annealing said hot-rolled steel strip as necessary;
cold-rolling said hot-rolled steel strip by one time or by more than two times between
which an intermediate annealing step is included, so as to form a cold-rolled steel
strip having a final thickness; and annealing said cold-rolled steel strip for decarburization
and then final annealing.
[0013] The present inventors paid attention to the micro structure of a material after the
above-mentioned annealing step for decarburization so as to study the relationship
between the recrystallization structure of a strip after the annealing step for decarburization
(which strip will be hereinafter denoted as "decarburization-annealed strip") and
the magnetic properties (magnetic flux density) over a wide range with various kinds
of view points, and found that the relationship therebetween is very close. The result
of carried-out experiments from which the above-mentioned finding was obtained will
be explained in detail hereinbelow:
[0014] Figs. 1 and 2 show affection upon the magnetic flux density (B₈ value) of a product
by an average diameter (d) of a primary recrystallization grain (d is the diameter
of the circle with the same area as the grain has.) and a coefficient σ* of deviation
in the diameter of the recrystallization grain which were obtained by image-analyzing
the micro structure of a decarburization-annealed strip that was observed by an optical
microscope (over entire area in the strip-thicknesswise direction).
[0015] Further, Fig. 3 shows micro structures (strip-thicknesswise direction) of decarburization-annealed
strips having average diameter (d) of recrystallization grains and coefficients σ*
of deviation in the diameter of the recrystallization grains, which are different
variously.
[0016] In the above-mentioned experiment, a slab consisting of 0.020 to 0.090 % (by weight)
of C, 3.2 to 3.3 % of Si, 0.010 to 0.045 % of acid-soluble Al, 0.0030 to 0.0100 %
of N, 0.0030 to 0.0300 % of S, 0.070 to 0.500 % of Mn and the balance of Fe and impurities,
was heated up to 1,150 to 1,400°C, and then was hot-rolled into a hot-rolled strip
(hot strip) having a thickness of 2.3 mm. The hot-rolled strip was further subjected
to a final high reduction cold-rolling step for applying a reduction ratio of about
88 % thereto after annealing the hot-rolled strip at a temperature in a temperature
range of 900 to 1,200°C so as to obtain a cold-rolled strip having a final thickness
of 0.285 mm, and the thus obtained cold-rolled strip was annealed for decarburization
at a temperature of a temperature range of 830 to 1,000°C, and then was annealed after
an annealing separation agent containing MgO as a main component being coated thereon.
[0017] As clearly understood from Figs. 1 and 2, it is possible to obtain a product having
an extremely high magnetic flux density B₈ equal to or greater than 1.88 tesla with
an average diameter d of primary recrystallization grain (decarburization-annealed
strip) which is equal to or greater than 15 µm and with a coefficient σ* of deviation
in the grain diameter which is equal to or less than 0.6. Further, Figs. 1 and 2 show
such a fact that a satisfactory recrystallization and a product having satisfactory
magnetic properties can be obtained by setting the average diameter d of grain in
a decarburization-annealed strip and the coefficient σ* of deviation in the diameter
in suitable ranges.
[0018] The inventors have considered that causes affecting upon the relationship between
the average diameter d of grain as well as the coefficient σ* of deviation in the
diameter of grain and occurrence of inferior secondary recrystallization or the magnetic
flux density B₈ of a product are as follows although these are not always sure:
[0019] There are considered the micro structure (average diameter of grain, and distribution
of grain diameters) of primary recrystallization, the texture, the inhibitor strength
and the like as factors affecting upon the secondary recrystallization, including
the orientation of secondary recrystallization.
[0020] Since variations in the texture and the distribution of diameters of grain occur
along with the growth of grain after completion of primary recrystallization, the
average diameter of the primary recrystallization grain indirectly exhibits the texture
and the distribution of diameters of grain. The average diameter of grain in the decarburization-annealed
strip itself is a value reversely proportional to the sum total of grain boundary
areas (per unit area), and the intergranular energy give a drive force to the growth
of grain in secondary recrystallization. Accordingly, the average diameter of grain
in decarburization-annealed strip is considered as a parameter which is simultaneously
descriptive of the texture, the distribution of grain diameters and the sum total
of grain boundary areas which affect upon the secondary recrystallization.
[0021] The texture exhibits qualitative rates of crystal orientation ({110}<001> oriented
grain or the like), oriented grain facilitating the grain growth of secondary recrystallization
grain ({111}<112> oriented grain or the like) and other orientated grains, and further,
the distribution of grain diameters affects upon the nucleation of secondary recrystallization
grain, the ease of the grain growth and the nonuniformity of the grain growth. Accordingly,
it can be considered that the average diameter d of grain in the decarburization-annealed
strip which is a parameter simultaneously descriptive of the texture, the distribution
of grain diameters and the sum total of grain boundary areas, has a strong correlation
to the orientation of secondary recrystallization grain.
[0022] Meanwhile, the coefficient σ* of deviation in the diameter of grain in the decarburization-annealed
strip exhibits the nonuniformity of grain diameter, that is, the larger the coefficient
σ* of deviation in the diameter of grain, the harder the nucleation of secondary recrystallization
grain and the growth of the grain become, and inferior secondary recrystallization
seems to occur. Thus, the coefficient σ* of deviation in the diameter of grain has
a close relationship with occurrence of inferior secondary recrystallization, the
average diameter d of grain in the decarburization-annealed strip has a close relationship
with magnetic flux density of a product in the case of satisfactory secondary recrystallization.
Accordingly, products having a high magnetic flux density (B₈) at a high yield rate
can be manufactured by controlling the above-mentioned parameters in predetermined
ranges:
Brief Description of the Drawings:
[0023]
Fig. 1 is a graph indicating affection upon the magnetic flux density (B₈) of a product
by an average diameter d of grain in a decarburization-annealed strip;
Fig. 2 is a graph indicating affection upon the magnetic flux density (B₈) of the
product by the coefficient σ* of deviation in the diameter of grain which is normalized
by the average diameter d of grain in the decarburization-annealed strip;
Fig. 3 is a microscopic photograph view illustrating the micro structures of decarburization-annealed
strips having variously different average diameters d of grain and coefficients σ*
of deviation in the diameter of grain;
Fig. 4 is a graph showing the relationship between the core loss value and the diameter
of primary recrystallization grain in decarburization-annealed strip; and
Fig. 5 is a graph showing the relationship between the core loss value and the temperature
of annealing for decarburization.
Best Preferred Embodiment Carrying out the Invention:
[0024] Explanation will be made hereinbelow of requisites of the present invention.
[0025] The components of a slab used in the present invention, although they should not
be limited specifically, are very important in order to stabilize the magnetic properties
of a product, and include preferably 0.025 to 0.100 % by weight of C and 2.5 to 4.5
% of Si. Further, Al, N, Mn, S, Se, Sb, B, Cu, Si, Nb, Cr, Sn, Ti and the like can
be added as elements for forming an inhibitor.
[0026] The heated temperature of the slab is preferably less than 1,300°C in view of the
energy cost although it should not be limited specifically to this temperature. The
heated slab is then hot-rolled into a hot-rolled strip. The hot-rolled strip after
being annealed as necessary is then cold-rolled by one time or by more than two times
between which an intermediate annealing is carried out, into a cold-rolled strip having
a final thickness. The reduction ratio in the final cold-rolling step is preferably
greater than 80 %, although it should not be limited specifically to this value, in
order to increase the magnetic flux density (B₈) of the product. By setting the reduction
ratio in the final cold-rolling step to greater than 80 %, it is possible to obtain,
suitable amounts of {110}<001> orientated grain which is sharp and coincidence orientation
grain ({111}<112> orientated grain or the like) which is likely eroded by the aforementioned
orientated grain.
[0027] After the final cold-rolling step, the cold-rolled strip is annealed for decarburization,
and is coated with an annealing separation agent containing MgO as a main component
before it is formed into a strip coil which is then annealed.
[0028] According to the present invention, it is important to set the average diameter d
of grain in the material before final annealing (primary recrystallization grain)
to greater than 15 µm, and the coefficient σ* of deviation in the diameter of grain
is set to less than 0.6.
[0029] In order to obtain a decarburization-annealed strip having such a micro structure,
it is possible to employ, for example, a process of adjusting the number of primary
recrystallization nucleuses by a reduction ratio in cold-rolling, grain diameters
in a material to be cold-rolled and the like, a process of controlling the grain growth
during annealing for decarburization in which the strength of the inhibitor during
annealing for decarburization is adjusted by manipulating the content amounts of elements
forming the inhibitor, the heating temperature of the slab, the coiling temperature
of the strip after hot-rolling, the temperature of annealing of the hot-rolled strip
or the like, a process of controlling the grain growth by adjusting the temperature
and time of the annealing for decarburization, and the like.
[0030] Further, it is possible to set the average diameter d of material grain before final
annealing (primary recrystallization grain) to greater than 15 µm, and the coefficient
σ* of deviation in the diameter of grain to less than 0.6 by additionally annealing
the material between the steps of annealing for decarburization and final annealing.
[0031] In order to on-line measure the diameter of primary recrystallization grain in the
material (strip) during or after annealing for decarburization, a core loss value
is measured by passing the strip between primary and secondary core loss measuring
coils, and then the diameter of primary recrystallization grain in the material is
detected with the use of the relationship shown in Fig. 4. With the use of such a
grain diameter measuring means, the diameter of primary recrystallization grain is
on-line measured, and then feed-back or feed-forward control for changing the temperature
and time of annealing for decarburization are carried out so as to set the diameter
of primary recrystallization grain to greater than 15 µm. Fig. 5 shows the relationship
between the temperature obtained during annealing for decarburization and the diameter
of primary recrystallization grain. Although the diameter of primary recrystallization
grain is indicated with the use of a core loss value of a decarburization-annealed
strip, the diameter of primary recrystallization grain can be known from Fig. 5 with
the use of the relationship between the core loss value and the diameter of primary
recrystallization grain in the decarburization-annealed strip, shown in Fig. 4.
[0032] The result shown in Fig. 5 gives the diameters of primary recrystallization grain
(Fig. 5 shows corresponding core loss values) which are obtained by variously changing
the temperature of annealing while the time of annealing is fixed to 150 sec. For
example, the diameter of primary recrystallization grain can be also controlled by
changing the duration of annealing (strip feeding ratio) while fixing the annealing
temperature to, for example, 850°C.
[0033] As to the composition and coating amount of the annealing separation agent, the final
annealing and the like, there are applied no specific conditions in particular. However,
in order to prevent a suitable micro structure of the decarburization-annealed strip
from being turned into an unsuitable micro structure with grain growth during an increase
in temperature of final annealing, the material after primary recrystallization is
preferably to nitrided in the atmosphere in which NH₃ having a concentration of higher
than 1,000 ppm is mixed in mixture gas containing hydrogen gas and nitrogen gas while
oxidation potential P
H20/P
H2 being set to be equal to or less than 0.04 under a temperature range from 500 to
900°C and under, for example, such a condition that the strip is made to run, thereby
to heighten the strength of the inhibitor during increase in temperature of final
annealing, in view of stable manufacture of electrical steel strips. Sulphurizing
treatment can be also used for increasing the strength of the inhibitor. Further,
although the strength of the inhibitor should be lowered during annealing for decarburization
in order to obtain a desired primary recrystallization structure by annealing for
decarburization in a relative low temperature range (less than 800°C), if the strength
of the inhibitor is insufficient to stably carry out secondary recrystallization,
it is required during final annealing to heighten the above-mentioned inhibitor strength.
As to an example of inhibitor strengthening processes, there has been known a process
of setting the partial pressure of nitrogen in atmospheric gas for final annealing
to a comparatively high value with steel containing Al.
[0034] The reason why the average diameter d ≧ 15 µm and the coefficient σ* ≦ 0.6 of deviation
in the diameter of grain are provided, is such that a product having a satisfactory
magnetic flux density B₈ of greater than 1.88 tesla can be obtained when the average
diameter d and the coefficient σ* of deviation in the diameter of grain fall in the
above-mentioned ranges, as is clear from Figs. 1 and 2. It is noted that although
the upper limit of the average diameter d is not defined in particular, the upper
limit of the average diameter d is 50 µm in view of the condition of usual components
and the conditions of steps. More than 50 µm of average diameter d is unpreferable
since a cost-up is caused due to higher purities of the components, a rise in annealing
temperature and the like. On the other hand, the coefficient σ* of deviation in the
diameter of grain is allowed to have a value down to zero.
[0035] As mentioned above, the reason why the condition of primary recrystallization grain
before final annealing is provided, is such that satisfactory magnetic properties
can be obtained by additional heat-treatment after annealing for decarburization
and before final annealing so as to adjust the average diameter d of primary recrystallization
grain to a value equal to or greater than 15 µm and the coefficient σ* of deviation
in the diameter of grain to a value equal to or less than 0.6.
--Reference Example 1--
[0036] A slab containing 0.054 wt.% of C, 3.25 wt.% of Si, 0.15 wt.% of Mn, 0.005 wt.% of
S, 0.027 wt.% of acid-soluble Al and 0.0078 wt.% of N was heated up to 1,150°C, and
was then hot-rolled into a hot-rolled strip having a thickness of 2.3 mm. This hot-rolled
strip was annealed at a temperature of 1,150°C and 900°C, and thereafter was cold-rolled
at a cold-rolling reduction of about 88 % into a cold-rolled strip having a final
thickness of 0.285 mm. The cold-rolled strip was held at a temperature of 810°C for
150 sec. and was then annealed for decarburization at a temperature of 830°C, 890°C
and 950°C for 20 sec., respectively. The thus obtained decarburization-annealed strip
was coated thereover with annealing separation agent having MgO as a main component,
and was heated up to 1,200°C at a rate of 10°C/hour in the atmospheric gas containing
25 % of N₂ and 75 % of H₂, and was then held at a temperature of 1,200°C for 20 hours
in the atmospheric gas containing 100 % of H₂ in order to carry out final annealing.
[0037] After annealing for decarburization, the average diameter d and the coefficient σ*
of deviation in the diameter of grain of the decarburization-annealed strip were measured
with the use of an image analyzer. Table 1 shows the results of the image analysis
and the magnetic properties of products.
TABLE 1
Anneal Temp. of Hot-Rolled Strip (°C) |
Anneal Temp. for Decarbu. (°C) |
Average Dia. d (µm) |
Deviat. Coeffi. in Dia. σ* |
Magnetic Flux Density B₈ (T) |
Second. Recryst. Rate (%) |
Remark |
1,150 |
830 |
13 |
0.45 |
1.85 |
100 |
C.E. |
1,150 |
890 |
19 |
0.48 |
1.92 |
100 |
P.I. |
1,150 |
950 |
23 |
0.53 |
1.92 |
100 |
P.I. |
900 |
830 |
18 |
0.47 |
1.92 |
100 |
P.I. |
900 |
890 |
23 |
0.52 |
1.93 |
100 |
P.I. |
900 |
950 |
30 |
0.62 |
1.68 |
30 |
C.E. |
Note: C.E. = Comparison Example, |
P.I. = Present Invention |
--Reference Example 2--
[0038] A slab containing 0.058 wt.% of C, 3.28 wt.% of Si, 0.14 wt.% of Mn, 0.007 wt.% of
S, 0.025 wt.% of acid-soluble Al and 0.0075 wt.% of N was heated up to a temperature
of 1,150°C or 1,250°C, and then was hot-rolled into a hot-rolled strip having a thickness
of 2.3 mm. This hot-rolled strip was held at a temperature of 1,150°C for 30 sec.,
and was then held at a temperature of 900°C for 30 sec. in order to be annealed. Then,
the hot-rolled strip was cold-rolled at a reduction ratio of about 88% into a cold-rolled
strip having a final thickness of 0.285 mm, which was then annealed for decarburization
by being held at a temperature of 850°C for 150 sec.
[0039] The thus obtained decarburization-annealed strip is coated thereover with annealing
separation agent containing MgO as a main component, heated up to 1,200°C at a rate
of 10°C/hour in the atmospheric gas containing 25 % of N₂ and 75 % of H₂, and was
then held at a temperature of 1,200°C for 20 hours in the atmospheric gas containing
100 % of H₂ for final annealing.
[0040] After annealing for decarburization, the average diameter d and the coefficient σ*
of deviation in the diameter of grain of the decarburization-annealed strip were measured
with the use of an image analyzer. Table 2 shows the results of the image analysis
and the magnetic properties of products.
TABLE 2
Slab Heating Temp. (°C) |
Average Dia. d (µm) |
Deviat. Coeffi. in Dia. σ* |
Magnetic Flux Density B₈ (T) |
Secondary Recryst. Rate (%) |
Remarks |
1,150 |
21 |
0.49 |
1.93 |
100 |
P.I. |
1,250 |
14 |
0.44 |
1.87 |
100 |
C.E. |
--Reference Example 3--
[0041] The decarburization-annealed strip obtained at a slab heating temperature of 1,250°C
in the conditions mentioned in the reference example 2, was heat-treated at a temperature
of 950°C for 30 sec., coated with annealing separation agent containing MgO as a main
component, and then was annealed under the conditions mentioned in the reference example
2.
[0042] Table 3 shows the average diameter d and diameter deviation coefficient σ* of the
steel strip (entire thickness in cross-section) together with the magnetic flux density
B₈ of the product.
TABLE 3
Presence of Additional Heat-Treat. |
Average Dia. d (µm) |
Deviat. Coeffi. in Dia. σ* |
Magnetic Flux Density B₈ (T) |
Secondary Recryst. Rate (%) |
Remarks |
No |
14 |
0.45 |
1.87 |
100 |
C.E. |
Yes |
18 |
0.49 |
1.92 |
100 |
P.I. |
--Reference Example 4--
[0043] A slab containing 0.056 wt.% of C, 3.27 wt.% of Si, 0.14 wt.% of Mn, 0.006 wt.% of
S, 0.027 wt.% of acid-soluble Al and 0.0078 wt.% of N was heated up to a temperature
of 1,150°C and then was hot-rolled into a hot-rolled strip having a thickness of 2.0
mm. The hot-rolled strip was held at 1,120°C for 30 sec., then held at 900°C for
30 sec., for annealing, and was then cold-rolled at a reduction ratio of about 89
% into a cold-rolled strip having a final thickness of 0.220 mm, which was held at
830°C for 90 sec. and was then annealed for decarburization at a temperature of 890°C
and 920°C for 20 sec., respectively. The thus obtained decarburization-annealed strip
was coated thereover with annealing separation agent containing MgO as a main component,
heated up to 880°C in the atmospheric gas containing 25 % of N₂ and 75 % of H₂, and
then heated up to 1,200°C from 880°C in the atmospheric gas containing 75 % of N₂
and 25 % of H₂, and was then held at 1,200°C for 20 hours in the atmospheric gas containing
100 % of H₂ for final annealing. At this time, the rate of temperature rise up to
1,200°C was set to 10°C/hour and 25°C/hour.
[0044] After annealing for decarburization, the average diameter d and diameter deviation
coefficient σ* of the decarburization-annealed strip (entire thickness in cross-section)
were measured with the use of an image analyzer. Table 4 shows the conditions of heat-treatment,
the results of the image analysis and the magnetic properties.
TABLE 4
Anneal Temp. for Decarbu. (°C) |
Temp. Rise. Rate (°C/hr) |
Average Dia. d (µm) |
Deviat. Coeffi. in Dia. σ* |
Magnetic Flux Density B₈ (T) |
Second. Recryst. Rate (%) |
Remark |
890 |
10 |
22 |
0.55 |
1.94 |
100 |
P.I. |
890 |
25 |
22 |
0.55 |
1.93 |
100 |
P.I. |
920 |
10 |
25 |
0.61 |
1.73 |
52 |
C.E. |
920 |
25 |
25 |
0.61 |
1.70 |
40 |
C.E. |
--Reference Example 5--
[0045] The decarburization-annealed strip obtained under the conditions mentioned in the
reference example 4, was coated thereover with annealing separation agent containing
MgO as a main component, heated up to 1,200°C at a heating rate of 15°C/hour in the
atmospheric gas of containing 25 % of N₂ and 75 % of H₂ and in the atmospheric gas
containing 50 % of N₂ and 50 % of H₂, and was then held at 1,200°C for 20 hours in
the atmospheric gas containing 100 % of H₂ for final annealing.
[0046] After annealing for decarburization, the average diameter d and the diameter deviation
coefficient σ* of the decarburization-annealed strip were measured with the use of
an image analyzer. Table 5 shows the conditions of treatment, the results of the image
analysis and the magnetic properties of products.
TABLE 5
Anneal Temp. for Decarbu. (°C) |
Atmospheric Gas N₂/H₂ |
Average Dia. d (µm) |
Deviat. Coeffi. in Dia. σ* |
Magnetic Flux Density B₈ (T) |
Second Recryst. Rate (%) |
Remark |
890 |
25/75 |
22 |
0.55 |
1.93 |
100 |
P.I. |
890 |
50/50 |
22 |
0.55 |
1.92 |
100 |
P.I. |
920 |
25/75 |
25 |
0.61 |
1.71 |
43 |
C.E. |
920 |
50/50 |
25 |
0.61 |
1.79 |
58 |
C.E. |
--Reference Example 6--
[0047] A slab containing 0.045 wt.% of C, 3.20 wt.% of Si, 0.065 wt.% of Mn, 0.023 wt.%
of S, 0.08 wt.% of Cu and 0.018 wt.% of Sb was heated up to 1,300°C, and was thereafter
hot-rolled into a hot-rolled strip having a thickness of 2.6 mm. This hot-rolled strip
was held at 900°C for three minutes for annealing, and was then cold-rolled at a reduction
ratio of about 63 % into a cold-rolled strip having a thickness of 0.95 mm, and was
held at 950°C for three minutes for intermediate annealing. Then the cold-rolled strip
was cold-rolled at a reduction ratio of 70 % so as to have a final thickness of 0.285
mm, and was held 810°C, 850°C and 890°C for 200 sec., respectively, in order to be
annealed for decarburization. The thus obtained decarburization-annealed strip was
coated thereover with annealing separation agent containing MgO as a main component,
was heated up to 1,200°C at a rate of 5°C/hour in the atmospheric gas containing 25
% of N₂ and 75 % of H₂, and then was held at 1,200°C for 20 hours in the atmospheric
gas containing 100 % of H₂ for final annealing.
[0048] After annealing for decarburization, the average diameter d and diameter deviation
coefficient σ* of the decarburization-annealed strip (entire thickness in cross-section)
were measured with the use of an image analyzer. Table 6 shows the conditions of treatment,
the results of the image analysis and the magnetic properties of products.
TABLE 6
Anneal Temp. for Decarbu. (°C) |
Average Dia. d (µm) |
Deviat. Coeffi. in Dia. σ* |
Magnetic Flux Density B₈ (T) |
Secondary Recryst. Rate (%) |
Remarks |
810 |
14 |
0.55 |
1.84 |
100 |
C.E. |
850 |
16 |
0.57 |
1.88 |
100 |
P.I. |
890 |
18 |
0.63 |
1.75 |
71 |
C.E. |
--Reference Example 7--
[0049] A slab containing 0.05 % by weight of C, 3.25 % of Si, 0.028 % of acid-soluble Al,
0.0075 % of N, 0.007 % of S and 0.014 % of Mn was heated up to 1,150°C, and was hot-rolled
in a conventional manner so as to obtain a hot-rolled strip having a thickness of
1.8 mm.
[0050] Then the hot-rolled strip was annealed at 1,150°C, and was cold-rolled into a cold-rolled
strip having a thickness of 0.19 mm after pickling, which was then slitted into test
pieces having a width of 60 mm, and core loss thereof were on-line measured in an
experimental continuous annealing furnace. The annealing was carried out by changing
the annealing temperature in a range from 810 to 870°C and the annealing duration
in a range from 90 to 150 sec. in the atmosphere of 75 % of H₂ and 25 % of N₂ having
a dew point of 55°C.
[0051] Fig. 4 shows the relationship between the core loss value W
14/50 of the steel strip and the average grain diameter of a test pieces taken out from
a part of the core loss measuring section. That is, it can be understood that the
average diameter d (µm) can be obtained from the core loss value W (W/kg) with the
use of the following formula (1) within a degree of accuracy of +/- 1 µm:
d = -11.17 W + 52.33 (µm) (1)
[0052] Further, it can be understood in comparison with Fig. 1 that the above-mentioned
degree of accuracy is sufficient to ensure a high magnetic flux density while preventing
inferior secondary recrystallization.
Advantages of the Invention:
[0053] As mentioned above, according to the present invention, the average grain diameter
d and diameter deviation coefficient σ* of primary recrystallization grain before
final annealing are controlled so as to stably manufacture a grain-oriented electrical
steel strip having excellent magnetic properties. Further, the average diameter d
and the diameter deviation coefficient σ* can be used as parameters for forecasting
the magnetic flux density of the product, and therefore, the magnetic flux density
of the product can be set to a desired value by adjusting, for example, the conditions
of final annealing.