[0001] The present invention relates to a process for producing a grain-oriented electrical
steel sheet used as a soft magnetic material for an iron or magnet core of electrical
equipments.
[0002] A grain-oriented electrical steel sheet has a crystal grain orientation referred
to as "Goss-orientation", in which grains are {110}<001>-oriented in terms of the
Miller index, and usually has a Si content of 4.5% or less and a sheet thickness of
from 0.10 to 0.35 mm. The steel sheet should have an excellent magnetic characteristic,
particularly the magnetic flux density and the watt-loss characteristics and, to meet
that requirement, it is important that the crystal grains are highly uniformly aligned
in the Goss-orientation. This extremely high accumulation to the Goss-orientation
is achieved by utilizing a catastrophic grain growth referred to as "secondary recrystallization".
To control the secondary recrystallization, it is indispensable to adjust the primary-recrystallized
structure prior to the secondary recrystallization and also to adjust the fine precipitates
referred to as inhibitors or the elements segregating on the grain boundaries. The
inhibitor suppresses the growth of the primary-recrystallized grains which are out
of the Goss-orientation, and thereby, promotes the preferential growth of grains which
are in the Goss-orientation.
[0003] Typical precipitates are MnS as proposed by M. F. Littman in Japanese Examined Patent
Publication (Kokoku) No. 30-3651 or by J. E. May and D. Turnbull in Trans. Met. Soc.
A.I.M.E. 212, 1958, p769-781, AlN as proposed by Taguchi and Sakakura in Japanese
Examined Patent Publication (Kokoku) No. 40-15644, MnSe as proposed by Imanaka et
al. in Japanese Examined Patent Publication (Kokoku) No. 51-13469, and (Al, Si)N as
proposed by Komatsu et al in Japanese Examined Patent Publication (Kokoku) No. 62-45285.
[0004] The elements segregating on the grain boundaries are Pb, Sb, Nb, Ag, Te, Se, S, etc.,
as reported by Saito et al. in Journal of the Japan Institute of Metals, 27, 1963,
p186-195 but these elements are used as merely an assistive agent for the precipitate
inhibitors in the industries.
[0005] Although the essential conditions under which such precipitates can function as an
inhibitor have not yet been fully clarified, an explanation was proposed by Matsuoka
in Tetsu-to-Hagane (Iron and Steel) 53, 1967, p1007-1023 or by Kuroki et al. in Journal
of the Japan Institute of Metals, 43, 1979, p-175-181 and ibid, 44, 1980, p-419-424,
as summarized below.
(i) Fine precipitates should be present in an amount sufficient to suppress the growth
of the primary-recrystallized grains prior to the secondary recrystallization.
(ii) Precipitates should have a certain size and should not abruptly vary by heat
during annealing for effecting the secondary recrystallization.
[0006] The processes currently used in the manufacture of a grain-oriented electrical steel
sheet are generally classified in the following three types.
[0007] The first type utilizes a two-step cold rolling using MnS disclosed by M. F. Littman
in Japanese Examined Patent Publication (Kokoku) No. 30-3651, the second type utilizes
a large reduction of 80% or more in the final cold rolling step using AlN and MnS
disclosed by Taguchi and Sakakura in Japanese Examined Patent Publication (Kokoku)
No. 40-15644, and the third type utilizes a two-step cold rolling using MnS (or MnSe)
and Sb disclosed by Imanaka et al. in Japanese Examined Patent Publication (Kokoku)
No. 51-13469.
[0008] These processes commonly use a basic technology in which a steel slab is heated at
a high temperature in the hot rolling step so that an in-situ formation of inhibitors
is effected to ensure the necessary precipitate amount and also to refine the precipitates.
[0009] Namely, a steel slab is heated at a high temperature, such as 1260°C or higher in
the first type process, 1350°C or higher in the second type process when the slab
contains 3% Si as disclosed in Japanese Unexamined Patent Publication (Kokai) No.
48-51852 although the temperature varies with the silicon content, or 1230°C or higher
in the third type process as disclosed in Japanese Unexamined Patent Publication (Kokai)
No. 51-20716 including an example in which an extremely high temperature of 1320°C
is adopted to obtain a particularly high flux density. Under such a high temperature
of slab heating, coarse precipitates present in steel matrix are once dissolved in
steel to form a solid solution and then a fine precipitation occurs during hot rolling
and/or the subsequent heat treatment.
[0010] Control of these precipitates, however, is very difficult and various solutions to
this problem have been proposed.
[0011] Japanese Examined Patent Publication (Kokoku) No. 54-14568 proposed that chromium
nitride, titanium nitride, vanadium nitride or the like is added to an annealing separator
to ensure the nitrogen partial pressure in the atmosphere during final annealing in
which the secondary recrystallization is effected and Japanese Examined Patent Publication
(Kokoku) No. 53-50008 proposed that a sulfide such as Fe₂S is added to ensure the
sulfur partial pressure and suppress decomposition of the precipitates so that the
secondary recrystallization is stabilized.
[0012] Nevertheless, these solutions could not enable the production of a product having
an optimum magnetic characteristic.
[0013] This is essential because it is actually impossible in the industrial practice that
precipitates of a fixed size are dispersed in a fixed amount over the length and the
width of a steel sheet coil by the slab heating and that this precipitation condition
is kept unvaried until the secondary recrystallization begins.
[0014] The precipitation occurs under a non-equilibrium condition and is strongly affected
by the prior heat and strain history. In fact, different portions of a steel slab
have different heat and strain histories and a steel slab per se has a nonuniform
crystal structure due to a macro-segregation of component elements over the slab thickness
and to a local dispersion of the α- and the γ-phases.
[0015] Therefore, the process for producing a grain-oriented electrical steel sheet based
on the control of inhibitor is not essentially stable when used in industry.
[0016] The object of the present invention is to provide a process for industrially stably
producing a grain-oriented electrical steel sheet having an excellent magnetic characteristic.
[0017] To achieve the object according to the present invention, there is provided a process
for producing a grain-oriented electrical steel sheet having a high magnetic flux
density, comprising the steps of:
heating a steel slab comprising 1.8 to 4.8 wt% Si, 0.012 to 0.050 wt% acid-soluble
Al, 0.010 wt% or less N, and the balance consisting of Fe and unavoidable impurities
to a temperature for hot rolling;
hot-rolling the heated slab to form a hot-rolled strip;
cold-rolling the hot-rolled strip to a final product sheet thickness under a final
cold rolling reduction of 80% or more by a single step of cold rolling or by two or
more steps of cold rolling with an intermediate annealing step inserted therebetween;
primary-recrystallization-annealing the cold-rolled strip;
final-annealing the primary-recrystallization-annealed strip so that secondary-recrystallized
grains substantially completely grow up in a temperature region of from 1000 to 1100°C
and then purification is effected above 1100°C; and
subjecting the primary-recrystallization-annealed steel strip to a nitriding treatment
before a secondary recrystallization occurs during the final annealing.
[0018] The present invention provides a process for stably producing a steel sheet product
having a high flux density by defining the primary-recrystallized texture and the
secondary recrystallization temperature.
The invention is described in detail in conjunction with the drawings in which
Figure 1 shows the relationship between the magnetic flux density (B₈) and the secondary
recrystallization temperature;
Fig. 2 shows the relationship between the magnetic flux density (B₈) and the nitrogen
content increment achieved by nitriding treatment;
Fig. 3 shows the relationship between the magnetic flux density (B₈) and the nitrogen
partial pressure of atmosphere;
Fig. 4 shows the relationship between the magnetic flux density (B₈) and the final
cold rolling reduction;
Fig. 5 shows the orientation distribution of the secondary-recrystallized grains in
the final product sheets obtained through the final cold rolling reductions of (a)
70%, (b) 80% and (c) 90%;
Fig. 6 shows the pole figures for the primary-recrystallized textures obtained when
the final cold rolling reductions are (a) 70%, (b) 80% and (c) 90%; and
Fig. 7 shows the relationship among the magnetic flux density (B₈), the average diameter
of primary-recrystallized grains, and the secondary recrystallization temperature.
[0019] The present inventors carried out a detailed study on the growth behavior of secondary-recrystallized
grains and found the following novel point.
[0020] When the secondary-recrystallized grains substantially completely grow up in the
temperature region of from 1000 to 1100°C in a material having a primary-recrystallized
texture having a {111}<112> orientation as a main orientation, which is established
under a final cold rolling reduction of 80% or more, grains having the Goss-orientation
can grow preferentially, and under this condition, a mere nitriding treatment is sufficiently
effective to ensure a certain amount of inhibitors for obtaining a good magnetic characteristic.
[0021] This finding was obtained through the following experiment.
[0022] A steel slab comprising 3.3 wt% Si, 0.027 wt% acid-soluble Al, 0.007 wt% N, 0.054
wt% C, 0.13 wt% Mn, 0.007 wt% S, and the balance consisting of Fe and unavoidable
impurities was hot-rolled to form a 2.3 mm thick hot-rolled strip, which was then
annealed at 1100°C for 2 min and cold-rolled at a reduction of 88% to a final product
thickness of 0.2 mm. The cold-rolled strip was subjected to a primary recrystallization
annealing, during which a decarburization treatment was also effected, followed by
a nitriding treatment in an ammonia atmosphere to increase the nitrogen content of
the steel strip by 0.005% or 0.018%. MgO was applied on the samples from the steel
strip, which samples were then heated to 900°C at a heating rate of 30°C/hr in an
atmosphere of 10% N₂ plus 90% H₂ and rapidly heated to temperatures of from 950 to
1200°C and held there for 20 hours to effect an annealing so that secondary-recrystallized
grains fully grew up. During this sequence, some samples were taken out of the heating
furnace when they were heated to 900°C and an observation showed that the primary-recrystallized
structure remained unchanged.
[0023] Figure 1 shows the relationship between the magnetic flux density (B₈ value) and
the secondary recrystallization temperature for the thus obtained sample products.
[0024] From Fig. 1, it is evident that a high flux density of 1.90 Tesla or higher is obtained
for the secondary recrystallization temperatures of from 1000 to 1100°C and that samples
of higher nitriding amount (or nitrogen content increase) exhibit a higher flux density.
[0025] Based on these results, the following experiment was carried out for studying the
nitriding amount and the secondary recrystallization temperature.
[0026] Other samples from the above-mentioned primary-recrystallized strip were subjected
to a nitriding treatment to cause various amounts of the nitrogen content to increase,
followed by an application of MgO. The MgO-applied samples were final-annealed in
an atmosphere of 10% N₂ plus 90% H₂ through the following heat cycle (A) or (B):
(A) Heating to 1050°C at a heating rate of 25°C/hour, holding there for 20 hours,
and heating to 1200°C at a heating rate of 25°C/hour.
(B) Heating to 1200°C at a heating rate of 25°C/hour.
[0027] Thereafter, the atmosphere was changed to a 100% H₂ atmosphere and the samples were
held in this condition for 20 hours to effect a purification annealing. Figure 2 shows
the flux density (B₈ value) for the thus obtained sample products.
[0028] From Fig. 2, it is evident that a product having a higher flux density is obtained
through the heat cycle (A), in which the secondary recrystallization temperature is
optimized, than through the conventional heat cycle (B). It should be noted as a more
important fact that, although a high flux density exceeding 1.90 Tesla can be obtained
only for a narrow range between 0.005% and 0.040% of the nitrogen content increase
in the conventional heat cycle (B), the high flux density can be obtained for a wider
range of 0.005% or higher of the nitrogen content increase in the heat cycle (A),
in which the secondary recrystallization temperature is controlled according to the
present invention.
[0029] This is due to the fact that, in the conventional process, the secondary-recrystallized
grains grow at lower temperatures when the nitriding amount is low and, when the nitriding
amount is high, the secondary-recrystallized grains grow at higher temperatures outside
the optimum temperature region where the grains having the Goss-orientation grow preferentially.
[0030] A study showed that nitriding suppresses the reduction rate of the inhibitor amount.
An experiment was then carried out for the nitrogen partial pressure in the temperature
range of from 1000 to 1100°C as a main parameter to affect a denitriding rate.
[0031] Figure 3 shows the relationship between the flux density (B₈) of the product sheets
and the partial nitrogen pressure of the atmosphere when the secondary-recrystallized
grains grow at 1050°C in a material preliminarily subjected to a nitriding treatment
to increase the nitrogen content by 0.018%.
[0032] From Fig. 3, it is evident that a product sheet having a high flux density of 1.90
Tesla or higher is obtained for a partial nitrogen pressure of 10% or higher and,
in particular, a flux density higher than 1.95 Tesla is obtained when the partial
nitrogen pressure is 75% or higher.
[0033] The optimum temperature range of from 1000 to 1100°C is considered to enable the
preferential growth of grains having a sharp Goss-orientation when the primary-recrystallized
texture has as a main orientation a {111}<112>-orientation established through a cold
rolling reduction of 80% or higher. To study the influence of the final cold rolling
reduction, an experiment was carried out, in which sheet samples cold-rolled at various
final reductions of from 50 to 90% were final-annealed at 1050°C during which the
secondary-recrystallized grains grew. The result showed that a sharp Goss-orientation
was established for the final cold rolling reduction (R) of 80% or higher as shown
in Figs. 4 and 5 and a product sheet having a high flux density was obtained. A study
showed that, for the product sheets for a final reduction (R) of 80% or higher and
exhibiting a high flux density, the corresponding primary-recrystallized materials
had a texture having a main orientation of {111}<112>-orientation as shown in Fig.
6.
[0034] It is a novel finding which has never been known that grains having the Goss-orientation
grow preferentially in a certain temperature range in response to the primary-recrystallized
texture.
[0035] The essential principle on which the present invention is based is summarized as
follows.
[0036] The basic fact is that grains having the Goss-orientation grow preferentially in
the specified temperature range of from 1000 to 1100°C in response to the primary-recrystallized
texture established through the final cold rolling reduction of 80% or higher. Under
the provision that the secondary-recrystallized grains are allowed to grow in the
specified temperature range, merely nitriding or increasing the partial nitrogen pressure
of the atmosphere is sufficient to ensure a certain amount of inhibitors and to suppress
the reduction rate of the inhibitor amount during the secondary recrystallization,
so that the conventional problems due to nonuniform distribution of inhibitors is
solved to enable the stable production of a grain-oriented electrical steel sheet
having a high flux density.
[0037] This principle of the present invention is quite different from that of the conventional
process.
[0038] Although Japanese Unexamined Patent Publication (Kokai) No. 48-72025 disclosed a
process in which the secondary recrystallization temperature is limited in the range
of from 1000 to 1100°C, the primary-recrystallized texture was not taken into consideration,
and moreover, MnS used as an inhibitor is unstable in that temperature range as shown
by W. M. Swift in Metallurgical Transaction, 4, 1973, p153-157 with the result that
a low flux density of merely 1.8 Tesla was obtained.
[0039] The specified limitations of the present invention will be described below.
[0040] A steel slab used in the present invention contains 1.8 to 4.8 wt% Si, 0.012 to 0.050
wt% acid-soluble Al, 0.010 wt% or less N, and the balance consisting of Fe and unavoidable
impurities, but may contain elements other than those specified above.
[0041] A material containing Si in an amount more than 4.8 wt% cannot be cold-rolled because
cracking easily occurs during cold rolling. On the other hand, when the Si content
is reduced, an α-to-γ transformation occurs during final annealing and the orientation
of crystal grains is broken. The Si content of 1.8 wt% or more does not substantially
affect the crystal orientation due to the α-to-γ transformation. The acid-soluble
Al is bonded with N to form AlN or (Al, Si) N, which functions as an inhibitor. When
Al is utilized for this purpose by a later nitriding treatment, it is particularly
effective that Al is present as a free Al. The acid-soluble Al content is limited
in the range of from 0.012 to 0.050 wt%, in which a high flux density is obtained.
[0042] The N content must not exceed 0.010 wt% because a void referred to as a "blister"
is formed in a steel sheet for a higher amount of N.
[0043] Additive elements such as Mn, S, Se, B, Bi, Nb, Cr, Sn, and Ti may be used as inhibitor
forming elements.
[0044] The slab heating temperature is not necessarily limited and need not be as high as
that used in the conventional process because inhibitors can be formed in-situ in
a later step of nitriding treatment. The slab heating temperature should not preferably
exceed 1300°C from the viewpoint of production cost.
[0045] In a preferred embodiment of the present invention, the slab heating temperature
is more specifically controlled in accordance with the Al and the N contents not to
exceed a temperature above which AlN is completely dissolved in steel. Generally,
the slab heating temperature is not preferably lower than 1000°C because the deformation
resistance of the slab increases with lowering of the heating temperature and the
steel sheet shape becomes difficult to ensure. On the other hand, when a slab is heated
to a temperature higher than 1270°C, oxidation of the slab surface excessively occurs
to form a melt referred to as "scum". The slab heating temperature is preferably in
the range of from 1000 to 1270°C.
[0046] In relation to the above point of view, the present inventors carried out a more
detailed study on inhibitors.
[0047] The primary-recrystallized grain size is determined by the condition of primary recrystallization
annealing including the annealing temperature and duration time and is affected more
essentially by the inhibitors which are present before the primary recrystallization
annealing.
[0048] If an inhibitor necessary for the secondary recrystallization is formed in-situ prior
to the primary recrystallization annealing by a high temperature heating of the slab
as in the conventional process, the primary recrystallization annealing must be carried
out at a higher temperature and/or for a longer time duration to undesirably raise
the production cost, in order to obtain a grain size comparable with that obtained
by the present invention, for example, the average grain diameter (D) of about 15
µm or greater. Moreover, a higher temperature and/or a longer time may cause an abnormal
grain growth during the primary recrystallization temperature, with the result that
the secondary recrystallization becomes unstable.
[0049] Therefore, with regard to inhibitors, it is more reasonable that, contrary to the
conventional process, a steel slab is heated to a relatively lower temperature at
which AlN is not completely dissolved to form a weak inhibitor to be present prior
to the primary recrystallization annealing and, after adjusting the primary-recrystallized
structure, the inhibitor necessary for the secondary recrystallization is formed in-situ
by a nitriding treatment.
[0050] The dissolving temperature of AlN is determined by the product of the Al and the
N contents of a steel slab and is typically expressed by the following equation by
Iwayama et al. in Journal of Magnetism and Magnetic Materials, 19, 1980, p15-17:
log[Al%][N%] = -10062/T + 2.72.
[0051] The slab heating temperature can be determined from the Al and the N contents by
using the above equation.
[0052] The above-described idea that inhibitors are separately utilized in the stages before
and after the primary recrystallization annealing is quite novel and has never been
present in the conventional process. The present inventors developed this idea through
finding the important effect of the primary-recrystallized grain structure.
[0053] The heated steel slab is subsequently hot-rolled to form a hot-rolled strip.
[0054] The hot-rolled strip is annealed, if necessary, at a temperature of from 750 to 1200°C
for 30 sec to 30 min.
[0055] The hot-rolled strip is cold-rolled to a final product sheet thickness under a final
cold rolling reduction of 80% or more by a single step of cold rolling or by two or
more steps of cold rolling with an intermediate annealing therebetween. The reduction
of 80% or more is essential for obtaining a desired primary-recrystallized texture.
[0056] A cold-rolled strip is subjected to a primary-recrystallization annealing, in which
a decarburization is effected to remove carbon usually contained in steel. The annealing
condition including temperature and duration time should be determined so that the
primary-recrystallized grains have an average grain diameter of about 15 µm or greater.
[0057] The strip thus obtained is coated with an annealing separator and is then subjected
to a final annealing for effecting a secondary recrystallization and a purification.
[0058] It is essential in the present invention that the strip which has been primary-recrystallization-annealed
is subjected to a nitriding treatment before the secondary recrystallization in the
final annealing step occurs and that the secondary-recrystallized grains are allowed
to substantially completely grow in the temperature region of from 1000 to 1100°C.
The nitriding treatment may be carried out in any conventional way for nitriding,
for example, nitriding using a gas atmosphere having a nitriding ability such as ammonia
gas, nitriding during the final annealing by using an annealing separator containing
a metal nitride additive having a nitriding ability such as manganese nitride, chromium
nitride, or the like.
[0059] As previously described, the nitriding carried out after the primary recrystallization
annealing and before the beginning of the secondary recrystallization, strengthens
the previously formed weak inhibitor to stabilize the secondary recrystallization.
[0060] In a preferred embodiment of the present invention, the final annealing of the primary-recrystallization-annealed
strip is carried out so that secondary-recrystallized grains substantially grow in
a temperature region T defined in the following expressions (1) and (2), as specified
in claim 2:
T ≦ 20D + 700 (1)
1000 ≦ T ≦ 1100 (2)
where "D" denotes the average grain diameter of primary-recrystallized grains, in
µm.
[0061] This is based on the novel finding that grains having the Goss-orientation can grow
preferentially by defining the texture and the grain structure of primary-recrystallized
grains and the secondary recrystallization temperature and controlling the thermal
growth behavior of crystal grains.
[0062] This finding was obtained through the following experiment.
[0063] Steel slabs comprising 3.2 to 3.3 wt% Si, 0.010 to 0.045 wt% acid-soluble Al, 0.0030
to 0.0090 wt% N, 0.020 to 0.090 wt% C, 0.070 to 0.500 wt% Mn, 0.0030 to 0.0300 wt%
S, and the balance Fe and unavoidable impurities were heated to different temperatures
of from 1150 to 1400°C and hot-rolled to form 2.3 mm thick hot-rolled strips, which
were then annealed at different temperatures of from 900 to 1200°C and cold-rolled
at a reduction of 88% to a final thickness of 0.285 mm. The cold-rolled strips were
primary-recrystallization-annealed at temperatures of from 830 to 1000°C, during
which a decarburization was also effected. An annealing separator containing MgO as
a main component was then applied on the strips.
[0064] Samples from the strips were heated to 900°C at a heating rate of 20°C/hour in an
atmosphere of 10% N₂ plus 90% H₂ and then rapidly heated to predetermined different
temperatures of from 950 to 1200°C and held there for 20 hours so that the secondary-recrystallized
grains were allowed to fully grow. During this sequence, some samples were taken out
of the heating furnace when they were heated to 900°C and an observation showed that
the primary-recrystallized grain sizes remained unchanged.
[0065] Fig. 7 shows the relationship among the magnetic flux density (B₈), the average grain
diameter of primary-recrystallized grains, and the secondary recrystallization temperature
for the above-obtained sample products.
[0066] It is seen from Fig. 7 that the product sheets have a high flux density exceeding
1.92 T when the average grain diameter D (µm) of primary-recrystallized grains and
the secondary recrystallization temperature T (°C) satisfy the following relationship:
T ≦ 20D + 700 (1)
1000 ≦ T ≦ 1100 (2)
[0067] The present inventors consider that the reason for this result is as follows.
[0068] The secondary recrystallization is a phenomenon in which the thermal change of primary-recrystallized
structure and the thermal change of inhibitor are competing. Namely, as the inhibitor
becomes weak during final annealing, the grains having orientations close to the Goss-orientation,
which are present in a scattered condition, form a nucleus and begin to grow. The
growth rate V (cm/sec) of secondary-recrystallized grains is generally expressed by
the following equation:
V ∝ exp(-Q/RT)·

where Q is the activation energy for the grain growth and R is a gas constant.
[0069] Therefore, when the primary-recrystallized grain diameter (D) is large and the secondary
recrystallization temperature (T) is low, the growth rate of secondary-recrystallized
grains is generally slow and grains having a sharp Goss-orientation can grow relatively
faster overcoming the suppression by inhibitors, whereas, when the primary-recrystallized
grain diameter (D) is small and the secondary recrystallization temperature (T) is
high, grains having orientations near the Goss-orientation also can grow to degrade
the accumulation degree of grain orientation. Accordingly, in a preferred embodiment
of the present invention, as specified in claim 2, the secondary recrystallization
temperature is defined in accordance with the primary-recrystallized grain diameter
(D). In this preferred embodiment in which the secondary recrystallization temperature
(T) is further limited by the primary-recrystallized grain size (D), a sharp Goss-orientation
as shown in Figs. 3 and 4 can be more easily ensured than in the case in which the
temperature is only limited to the range between 1000 and 1100°C.
[0070] The method of controlling the secondary recrystallization temperature, i.e., the
temperature at which the secondary-recrystallized grains are allowed to grow is not
limited and may carried out by holding or slow heating in the corresponding temperature
region.
EXAMPLES
Example 1
[0071] A steel slab consisting of 3.3 wt% Si, 0.030 wt% acid-soluble Al, 0.008 wt% N, 0.05
wt% C, 0.14 wt% Mn, 0.007 wt% S and the balance Fe and unavoidable impurities was
hot-rolled to form a 1.8 mm thick hot-rolled strip. The hot-rolled strip was annealed
at 1100°C for 2 min and then cold-rolled at a reduction of 88% to a final product
thickness of 0.20 mm. The cold-rolled strip was subjected to a primary recrystallization
annealing at 830°C, during which a decarburization was also effected. Thereafter,
MgO mixed with 0, 3, 5, and 15% of ferro-manganese nitride was applied on the strip
for the following nitriding treatment. The strip was final annealed by heating to
1070°C in an atmosphere of 25% N₂ plus 75% H₂ and held at the temperature for 20 hours
in a changed atmosphere of 75% N₂ plus 25% H₂ , so that the secondary-recrystallized
grains were allowed to almost completely grow. The strip was then subjected to a purification
treatment by annealing at 1200°C for 20 hours in an atmosphere of 100% H₂. The magnetic
characteristic of the thus obtained product sheets is shown in Table 1.
Table 1
| Ferro-manganese nitride percentage |
Flux density (B₈) |
Note |
| 0 |
1.88 T |
Comparative sample |
| 3 |
1.94 T |
Present invention |
| 5 |
1.96 T |
" |
| 15 |
1.97 T |
" |
Example 2
[0072] Steel slabs comprising 3.28 wt% Si, 0.027 wt% acid-soluble Al, 0.0060 wt% N, 0.14
wt% Mn, 0.007 wt% S and the balance Fe and unavoidable impurities were heated to different
temperatures of 1150 and 1300°C and hot-rolled to form 1.8 mm thick hot-rolled strips.
The strips were annealed by heating at 1150°C for 30 sec and subsequently holding
at 900°C for 30 sec. The strips were then cold-rolled at a reduction of 89% to a final
sheet thickness of 0.20 mm. The cold-rolled strips were primary-recrystallization-annealed
at 850°C for 90 sec, during which a decarburization was also effected. An annealing
separator containing MgO as a main component and mixed with ferro-manganese nitride
was applied on the annealed strips, which were then final-annealed in an atmosphere
of 25% N₂ plus 75% H₂ through the following heat cycles (A) and (B):
(A) Heating to 1200°C at a heating rate of 30°C/hr.
(B) Heating to 1070°C at a heating rate of 30°C/hr, holding there 10 hours and then
heating to 1200°C at a heating rate of 30°C/hr.
[0073] Thereafter, the strips were heated at 1200°C for 20 hours in an atmosphere of 100%
H₂ to effect a purification. The characteristics of the thus obtained product sheet
are shown in Table 2.
Table 2
| Slab heating temperature |
Primary-recrystallized grain diameter |
Heat cycle of final annealing |
Flux density (B₈) |
| 1150°C |
22 µm |
A |
1.88 T |
| B |
1.95 T |
| 1300°C |
13 µm |
A |
1.78 T |
| B |
1.84 T |
Example 3
[0074] Samples from the primary-recrystallization-annealed strip obtained when the steel
slab was heated at 1300°C were additionally heat-treated at 950°C. A primary-recrystallized
grain has a grain diameter of 20 µm. A final annealing was carried out under the same
condition as that in Example 2. The characteristics of the thus obtained products
are shown in Table 3.
Table 3
| Heat cycle of final annealing |
Flux density (B₈) |
| A |
1.87 T |
| B |
1.92 T |
Example 4
[0075] A steel slab comprising 3.3 wt% Si, 0.030 wt% acid-soluble Al, 0.003 wt% N, 0.048
wt% C, 0.13 wt% Mn, 0.010 wt% S, and the balance Fe and unavoidable impurities was
heated to 1100°C and hot-rolled to a 2.0 mm thick hot-rolled strip. The strip was
annealed at 1000°C and cold-rolled at a reduction of 89% to a final thickness of 0.23
mm. Samples from the cold-rolled strip were primary-recrystallization-annealed at
different temperatures of 800, 850, and 900°C for 120 sec, during which a decarburization
was also effected. The samples were then subjected to a nitriding treatment in an
atmosphere of ammonia gas so that the nitrogen content was increased by 0.02 to 0.03
wt%. An annealing separator was applied on the nitrided samples, which were then final-annealed
by heating to 1000°C at a heating rate of 25°C/hr in an atmosphere of 10% N₂ plus
90% H₂ , then heating to 1100°C at a heating rate of 5°C/hr, subsequently heating
to 1200°C at a heating rate of 25°C/hr and holding there in a changed atmosphere of
100% H₂ to effect purification. During this sequence, some samples were taken out
of the heating furnace when heated to temperatures of 1000 and 1100°C and an observation
showed that the secondary recrystallization was substantially performed between these
temperatures. The thus obtained products had the characteristics as shown in Table
4.
Table 4
| Primary recrystallization temperature |
Primary-recrystallized grain diameter |
Flux density (B₈) |
| 800°C |
14 µm |
1.89 T |
| 850°C |
24 µm |
1.94 T |
| 900°C |
27 µm |
1.95 T |