Background of the invention
[0001] This invention relates to a method for operating a top-and-bottom blown converter,
and a top-blowing lance used in the practice of a method for operating a top-and-bottom
blowing converter.
[0002] As is well known in the art, conventional top-blown converters which are also referred
to as LD converters often experience operating troubles due to the phenomenon that
molten metal is ejected out of the converter, which is generally called slopping and
attributable to excessive oxidation of molten metal by the top blowing oxygen gas.
To eliminate such a problem, top-and-bottom blown converters were recently developed
by taking advantage of the oxygen bottom blown converter and have been commercially
used in iron works. The top-and-bottom blown converters are generally constructed
by modifying existing top-blown converters. More specifically, referring to Fig. 10,
the top-blown converter is modified by providing a plurality of bottom blowing tuyeres
2 extending through a converter bottom 1 which is removably secured to a converter
housing 7. A top-blowing lance 3 is vertically inserted through a top opening of the
converter. With this arrangement, jets 4 of oxygen gas are blown through the top-blowing
lance 3 onto the surface of a molten metal bath 6 while an agitating gas 5 such as
oxygen gas or argon gas is blown into the molten metal bath 6 through the tuyeres
2. This type of top-and-bottom blown converter is free of slopping since the molten
metal is vigorously agitated by the bottom blowing gas to prevent the molten metal
from being excessively oxidized with the top-blowing gas. Since top-and-bottom blown
converters constructed by modifying LD converters, however, has a housing of a specific
profile designed forthe LD converter operation requiring top blowing only, the bottom
blowing gas causes the molten metal to wave or vibrate and eventually, the converter
housing to severely vibrate, resulting in a variety of troublesome problems.
[0003] The problems involved in the conventional top-and-bottom blown converters will be
described in more detail. Since the molten metal and hence, the converter housing
vibrates to a less extent in usual top-blown converter operation than in the oxygen
bottom-blown converter operation, a supportforthe housing of the top-blown converter
is generally of a less strength as compared with that for the oxygen bottom-blown
converter. On the other hand, the molten metal bath is vibrated to a large extent
with the bottom blowing gas in the top-and-bottom blown converter. If a top-and-bottom
blown converter is a modification of a top-blown converter having the housing support
of a relatively low strength, the vibration of molten metal is transmitted to the
converter housing so that the converter housing is severely vibrated. This vibration
leads to several drawbacks that the housing support is susceptible to fatigue failure
and the operation of the converter becomes unstable and in some cases, the vibration
is detrimental to keep the operators safe.
[0004] In order to minimize the above-mentioned vibration caused by the blowing of bottom-blowing
gas, it is believed effective to locate bottom-blowing tuyeres remote from the center
of the converter bottom and spaced apart from each other. Such a top- and bottom-blown
converter was proposed in the WO-A1-82/01012 (EP-Al-60305). In this converter the
top-blowing multi-nozzle lance is arranged such with respect to the bubbling tuyeres
located at the bottom of the converter, that hot spots are created between the bubbling
regions of the respective tuyeres. However, in a top-and-bottom blown converter which
is constructed by modifying a top-blown converter, it is difficult to distribute the
bottom-blowing tuyeres in a spaced-apart relationship because of the housing profile
and other factors. It is known that the life of tuyeres is considerably shortened
if the tuyeres are washed with molten metal, that is, alternately exposed to air and
molten metal during charging and tapping of molten metal. The oxygen bottom-blown
converter has a housing profile approximating a spherical shape, that is, a housing
profile having a reduced ratio H/D of a housing height H to the maximum D of a housing
inner diameter, such that the bulge of a converter barrel serves as a reservoir for
molten metal when the converter housing is tilted for charging or tapping of molten
metal. Then the bottom blowing tuyeres are prevented from being washed upon charging
or tapping even when they are spaced apart from each other and from the axis of the
converter. However, a top-and-bottom blown converter which is constructed by modifying
a conventional top-blown converter maintains the housing profile as it is in the top-blown
converter, that is, a vertically elongated profile approximating a rotary oval body
having a less bulged barrel and an increased height-to-diameter ratio H/D. It should
thus be precluded to tilt the modified converter over a too large angle for charging
or tapping of molten metal. Since the lower portion of the converter barrel and the
peripheral portion of the converter bottom constitute a metal reservoir upon loading
and tapping of molten metal, the bottom blowing tuyeres should be collectively arranged
on or in proximity of a line passing the axis of the converter and parallel to the
trunnion axis to prevent the bottom-blowing tuyeres from being washed with the molten
metal upon charging or tapping thereof. The location of bottom blowing tuyeres is
limited in the top-and-bottom blown converter which is constructed by modifying a
top-blown converter, it is very difficult in practice to reduce the vibration of a
molten metal bath by arranging the bottom-blowing tuyeres in a spaced-apart relationship.
[0005] A primary object of the present invention is to minimize vibration of a molten metal
bath in a top-and-bottom blown converter to thereby diminish vibration of a converter
housing.
[0006] Taking into account the advantage of the top-and-bottom blown converter that the
location of hot spots created by oxygen gas from a top-blowing lance need not be limited
to the proximity of the axis of the converter because agitation of a molten metal
bath is improved over the top-blown converter, and more specifically, the molten metal
is agitated with the bottom-blowing gas to such a full extent that the top-blowing
oxygen gas need not assist in agitating the molten metal, we determined the relationship
of the location of hot spots to the vibration of molten metal by changing the top-blowing
lance to vary the location of hot spots associated therewith. Finding that the magnitude
of vibration of molten metal is closely related to the relative location of the hot
spots and the bottom-blowing gas bubbling region, and more specifically, the vibration
of molten metal can be minimized by designing the top-blowing multi-nozzle lance such
that a hot spot created by a jet of oxygen gas from each of the nozzles of the lance
is located outside the bottom-blowing gas bubbling region, we have achieved the present
invention.
[0007] In conventional top-blown converters, it is a common practice to blow oxygen gas
onto the surface of molten metal through a top-blowing lance thereabove for the purpose
of effecting desiliconization, decarbonization and dephosphorization. The top-blowing
lance usually has a plurality of, for example, three orfour nozzles. A typical top-blowing
lance is shown in Fig. 1 as having four nozzles 8 whose axis is at a small angle of
about 8°-10° with respect to the axis of the lance 3. The angle of the nozzle axis
with respect to the lance axis is referred to as nozzle inclination angle, hereinafter.
A nozzle inclination angle on the order of 8°-10° is generally used in a multi-nozzle
lance for conventional top-blown converters for the following reason. To increase
of the efficiency of decarbonization, it is required that the nozzle inclination angle
be reduced to concentrate the associated oxygen jets within a relatively narrow region
on the molten metal surface to allow the oxygen jets to impinge against the molten
metal without dispersing their kinetic energy to reduce the kinetic energy per unit
area. The concentrated energy causes the molten metal to be vigorously agitated. On
the other hand, to promote slagging and dephosphorization, the nozzle inclination
angle is desirably increased to cause part of the oxygen to be absorbed in a slag
layer on the molten metal surface over a relatively large area. As a compromise between
these contradictory requirements, the nozzle inclination angle is determined as described
above. Furthermore, in conventional top-blown converters, the top-blowing lance is
aligned with the axis of the converter for the purpose of rendering the molten metal
reaction uniform and because of its location relative to the converter opening. The
high temperature zones which are created on the molten metal surface by oxygen gas
jets injected thereon through the top-blowing lance, that is, the so-called hot spots
are located with a relatively narrow region which is confined around the axis of the
converter on the basis of the nozzle inclination angle.
[0008] Nevertheless, the top-and-bottom blown converters constructed by modifying top-blown
converters actually use the same lance as used in the top-blown converters although
metallurgical effect, particularly, molten metal agitating effect is apparently different
therebetween. As a result, the hot spots created by the top blowing gas from the lance
are generally located within a relatively narrow region extending about the axis of
the converter as in the case of the top-blown converters. On the other hand, the bottom-blowing
tuyeres in the modified type of top-and-bottom blown converter must be collectively
arranged on or in proximity of a line passing the converter axis and parallel to the
trunnion axis for the reason of tuyere life as described earlier. Consequently, the
hot spots P created by the top-blowing gas from the lance 3 are located within a bubbling
region of the molten metal surface which rising bubbles of the bottom-blowing gas
from the tuyeres 2 reach (bottom-blowing gas bubbling region) or the hot spots P largely
overlap the bottom-blowing gas bubbling region as seen from Fig. 10. When a conventional
top-blowing lance was used in the top-and-bottom blown converter, it was difficult
to locate the hot spots created by the gas from the top-blowing lance outside the
bottom-blowing gas bubbling region.
[0009] It is, therefore, another object of the present invention to provide a top-blowing
lance which is adapted for use in the top-and-bottom blown converter steel making
process and allows the associated hot spots to be located outside the bottom-blowing
gas bubbling region.
Summary of the invention
[0010] The present invention is concerned in a top-and-bottom blown converter comprising
tuyeres arranged at the bottom for blowing a gas into a molten metal bath in the converter
and a multi-nozzle lance inserted through a top opening of the converter for blowing
jets of oxygen gas onto the bath surface. According to a first aspect of the present
invention, there is provided a method for operating the top-and-bottom blown converter
wherein the top-blowing oxygen gas is blown such that the center of a hot spot created
by the oxygen gas jet from each of the nozzles of the lance is positioned outside
a bubbling region of the molten metal surface which rising bubbles of the bottom-blowing
gas reach, thereby minimizing vibration of the molten metal bath. Preferably, in an
orthogonal coordinate system assumed on a stationary (imaginary) molten metal surface
as having an origin on the vertical axis of the converter and an x axis parallel to
the axis of trunnions supporting the converter, the coordinates (x, y) of the centers
of at least four of the hot spots created on the molten metal surface by the oxygen
gas jets from the nozzles of the top-blowing multi-nozzle lance fall within the range
defined by the inequalities:

wherein
a is a diameter of the bubbling region in a direction parallel to the trunnion axis,
b is a diameter of the bubbling region in a direction perpendicular to the trunnion
axis, and
c is a radius of a concave defined by the hot spot.
[0011] According to a second aspect of the present invention, there is provided a top-blowing
lance for use in the operation of a top-and-bottom blown converter comprising a plurality
of nozzles at the tip thereof. The nozzles are oriented such that the axis of each
of the nozzles is at an angle between 20° and 30° with respect to the axis of the
lance.
Brief description of the drawings
[0012] The above and other objects, features and advantages of the present invention will
be more fully understood from the following description in conjunction with the accompanying
drawings, in which;
Fig. 1 is a schematic axial cross section of a top-blowing multi-nozzle lance;
Fig. 2 is a schematic plan view of the bottom of a top-and-bottom blown converter
showing the arrangement of tuyeres;
Fig. 3 is a schematic partial illustration of the converter which is being operated
by the method of the present invention;
Fig. 4 is a coordinate diagram showing the centers of hot spots relative to the bottom
blowing gas bubbling region in a model experiment using water;
Fig. 5 illustrates the inclination angle of a nozzle of the top-blowing lance;
Fig. 6 is a coordinate diagram showing the centers of hot spots relative to the bottom-blowing
gas bubbling region in an experiment using an actual converter;
Fig. 7 is a graph showing the relationship of the nozzle inclination angle <p to the
acceleration of converter housing vibration;
Fig. 8 is a schematic view showing the location of hot spots created in an example
where the nozzle inclination angle is set to 28°;
Fig. 9 is a schematic view showing the location of hot spots created in a comparative
example where the nozzle inclination angle is set to 9.1°; and
Fig. 10 is a schematic cross section of a top-and-bottom blown converter which is-constructed
by modifying a conventional top-blown converter.
Detailed description of the invention
[0013] As shown in Fig. 2, it is a common practice in a top-and-bottom blown converter 7
to arrange a plurality of tuyeres 2 at the bottom 1 in one or two rows on or in proximity
of a line passing the axis of the converter and parallel to the axis 9 of trunnions
supporting the converter for pivotal motion. In this case, the molten metal bath waves
or vibrates mainly in a direction perpendicular to the tuyere aligning line as if
water moved alternately in opposite directions in a U-shaped tube. A rotational vibration
about the converter axis takes place additionally. We have found that such vibration
of the molten metal bath is attributable to a change with time of passage of bubbles
resulting from gas jets injected from the bottom blowing tuyeres, and that once the
molten metal bath has waved or vibrated, the direction of the bottom-blowing gas jets
is also declined toward the vibrating direction to increasingly enhance the vibration.
Since it is unnecessary in the top-and-bottom blown converter for the impact energy
imparted to the molten metal surface by-the oxygen gas jets from the top-blowing lance
to assist in agitating the molten metal, the hot spots created on the molten metal
surface by the oxygen gas jets from the lance nozzles need not be concentrated at
or in proximity of the axis of the converter. Based on the speculation that the impact
energy of the top-blowing oxygen gas jets might be used as an energy for overcoming
the vibration of the molten metal bath, that is, a vibration damping or absorbing
energy by changing the location of hot spots from the conventional arrangement, we
made a model experiment using water under similar conditions as might occur in an
actual top-and-bottom blown converter. We found that vibration of molten metal bath
due to the bottom-blowing gas is enhanced when the centers of the hot spots created
on the molten metal surface by oxygen gas jets injected from the nozzles of a top-blowing
multi-nozzle lance were positioned within the bottom-blowing gas bubbling region,
as experienced in the prior art, whereas vibration of the bath was diminished when
the centers P
o of the hot spots P were positioned outside the bottom-blowing gas bubbling region
Q as shown in Fig. 3, and a remarkable vibration attenuation effect was obtained particularly
when the centers of the hot spots were outside, but adjacent the corners of the bubbling
region. This novel finding was proved to be correct in actual converter operations.
[0014] The above-mentioned water model experiment will be described in detail. The bubbling
region which rising bubbles of the bottom-blowing gas reach may be defined as follows.
Provided that H is a depth of the molten metal bath 6 and 8 is an angle of dispersion
of an oxygen jet from each tuyere 2 as shown in Fig. 3, a bubbling zone of the molten
metal surface that bubbles of the oxygen gas from each tuyere reach is horizontally
and radially spread from the center vertically aligned with the tuyere over a radius
d:

Then, the gas bubbling region covering all the tuyeres may be given by horizontally
expanding an envelope encircling the tuyeres outward over the distance d. For example,
an overall bottom-blowing gas bubbling region Q is shown in Fig. 2 as being defined
by horizontally expanding an envelope encircling the vertical projections on a stationary
molten metal surface of the tuyeres 2 over the distance d. It has also been empirically
determined that the angle 8 of dispersion of the bottom-blowing gas jet is approximately
20°
~ under normal conditions.
[0015] In a 1/10 scale water model, that is, a converter model made to a scale of 1/10 of
an actual top-and-bottom blown converter and using water instead of molten iron, magnitude
of vibration (or acceleration) of the model housing was measured while the location
of hot spots created by oxygen gas jets from the nozzles of a top-blowing four-nozzle
lance was changed in relation to the above-defined bottom-blowing gas bubbling region.
In this water model experiment, the depth of the bath was 170 mm, and the distance
from the stationary bath surface to the opening end of the nozzles of the four-nozzle
lance, that is, the nozzle height was 250 mm. A number of four-nozzle lances having
different nozzle inclination angles were prepared and the lance was exchanged one
by one to change the location of hot spots. Among a number of hot spots with which
the magnitude of vibration was determined in this water model experiment, the centers
of representative hot spots are plotted at cross (x) signs (Nos. 1-10) in the diagram
of Fig. 4. The vibration attenuation factor and the nozzle inclination angles a and
for each location are shown in Table 1. In Fig. 4, origin 0 coincides with the axis
of the converter, axis x is a line passing the converter axis 0 and parallel to the
trunnion axis, axis y is a line passing the converter axis 0 and perpendicular to
the trunnion axis, a represents a longer diameter of the bottom-blowing gas bubbling
region in a direction parallel to the trunnion axis, and b represents a shorter diameter
of the bubbling region in a direction perpendicular to the trunnion axis. A region
defined by two sets of broken lines (corresponding to

in Fig. 4 substantially corresponds to the bottom-blowing gas bubbling region Q. In
addition, c represents a radius of a concave created by a jet from each lance nozzle,
that is, a hot spot. Although the centers of the hot spots are depicted by cross signs
only in the first quadrant for the sake of illustration, of course, similar hot spots
appear in the second, third and fourth quadrants symmetrically with respect to x and
y axes. In Table 1, a repressnts an angle obtained by projecting on plane x-z the
angle between the axis of each nozzle and the axis of the four nozzle lance, wherein
z represents a vertical axis extending from the origin 0 above the plane of the sheet
of Fig. 4, and β represents an angle obtained by projecting the same nozzle angle
on plane x-y. These angles are clearly shown in Fig. 5. Provided that the distance
from the stationary bath surface to the opening end of the lance nozzle, that is,
the lance height is represented by h, as readily understood from Fig. 5, position
P
o (x, y) representative of the center of a hot spot created by a gas jet from' a nozzle
having projected inclination angles a and β may be given by the equations:


It is to be noted that in Table 1, the vibration attenuation factor (%) is obtained
by measuring the acceleration in a direction parallel to the trunnion axis at a trunnion
support stand and comparing the measured value with the standard value which is measured
when the vibration of a molten metal bath is solely caused by the bottom-blowing gas
without blowing any gas onto the bath surface through the top-blowing lance.

[0016] As apparent from the data of Table 1, vibration is undesirably enhanced in experiment
No. 10 where the center of a hot spot is positioned within the bottom-blowing gas
bubbling region Q, and vibration is more or less attenuated in experiment Nos. 1-9
where the hot spot center is positioned outside the bubbling region Q. It is also
evident that vibration attenuation is remarkable in experiment Nos. 1, 3, 5 and 7-9
where the hot spot center is within a hatched area shown in Fig. 4, for example, defined
by ineaualities:

for the first quadrant. This may be extrapolated for all the quadrants, which indicates
that the optimum vibration attenuation is achieved when the centers of hot spots are
positioned in the areas defined by

[0017] From equations (1) and (2), a and (3 may be given by the following equations:


Accordingly, the optimum vibration attenuation is achieved by setting the projected
inclination angles a and (3 of the lance nozzle to meet equations (5) and (6) in accordance
with the lance height h as long as (x, y) satisfies equation (4).
[0018] On the basis of the data obtained in the water model experiment, another experiment
was made in an actual converter. A top-and-bottom blown converter used was a modification
of a 250-ton LD converter. Five four-nozzle lances having different nozzle inclination
angles were prepared. A blowing experiment was done for each lance under the conditions
that the lance height h was 2500 mm, the flow rate of bottom-blowing gas was 300 Nm
3/min., the flow rate of oxygen through the top-blowing lance was 450 Nm
3/min., and the average depth of a molten iron bath was 1700 mm. The magnitude of vibration
or acceleration at a trunnion support stand was measured in a direction parallel to
the trunnion axis. The positions of the centers of hot spots created by an oxygen
gas jet from a nozzle of various lances are depicted at cross (x) signs referred to
Nos. 11-15 in Fig. 6. The angle of inclination of a lance nozzle in a direction of
x axis. The projected inclination angles a and β of a lance nozzle in directions of
x and y axes and the vibration attenuation factor (%) corresponding to each of the
hot spots are shown in Table 2. The meanings of x and y axes, a, b, c and Q in Fig.
6 are as defined in Fig. 4, and the vibration attenuation factor in Table 2 is as
defined in Table 1.

[0019] As seen from Fig. 6 and Table 2, it was demonstrated in the actual converter than
vibration of a molten iron bath is enhanced when the center of a hot spot is within
the bottom-blowing gas bubbling region Q (experiment No. 15), vibration is attenuated
when the hot spot center is outside the bubbling region Q (experiment Nos. 11-14),
and the vibration attenuation effect is remarkable when the hot spot center is within
a hatched zone in Fig. 6, that is, the hot spot center has a coordinate (x, y) satisfying
the above-mentioned inequalities (4) (experiment Nos. 12-14).
[0020] As readily understood from equations (1) and (2), the hot spot center represented
by a coordinate (x, y) may vary with the lance height h. This means that when a lance
having nozzles with a given inclination angle is set at different lance heights, the
hot spot centers also appear at different positions. In an actual operation, the lance
height h is previously set to a certain value, and the inclination angle of the lance
nozzle is then determined in relation to the preset lance height such that the resultant
hot spot centers may be outside the bottom-blowing gas bubbling region, and more preferably,
the resultant hot spot centers may have a coordinate (x, y) satisfying the above-mentioned
inequalities (4). A lance having nozzles with such a predetermined inclination angle
must be used. However, even when the operation has started with the lance height h
of a preset value, the lance height h is often changed in response to varying conditions
in the progress of an actual converter operation. If the lance height h is lowered
during the operation, for example, the hot spot centers are inwardly moved to within
a bottom-blowing gas bubbling region to undesirably enhance vibration. Furthermore,
it is cumbersome in the actual operation to exchange the lance in accordance with
the lance height h and the dimensions of the bottom-blowing gas bubbling region before
the operation of a new batch is started. For these reasons, the preferred top-blowing
multi-nozzle lances for use in the practice of the method of the present invention
are those lances having oriented nozzles in which the angle included between the axes
of each nozzle and lance, that is, the nozzle inclination . angle (angle <p as depicted
in Fig. 1) is from 20° to 30°, which value is remarkably larger than the previously
used nozzle inclination angle of 8°-1 0°. With a nozzle inclination angle of at least
20°, the resultant hot spot centers will possibly appear outside the bottom-blowing
gas bubbling region under normal operating conditions in a commonly used top-and-bottom
blown converter having a capacity of about 80 tons or more. In the case of the top-and-bottom
blown converter, the top-blowing oxygen gas jet is not expected to effect substantial
decarbonization unlike the top-blown. converter, and the lance height is often set
at a higher value than in the top-blown converter, thereby providing a soft blow.
Generally, the lance height is about 1500 mm or more. With the lance height of about
1500 mm, if the nozzle inclination angle (p is at least 20°, the resultant hot spot
centers will appear outside the bottom-blowing gas bubbling region to suppress vibration
of a molten metal bath. In this manner, the bath vibration will be effectively suppressed
even when the lance height h and other conditions are altered during the actual operation.
On the other hand, if the nozzle inclination angle (p exceeds 30°, there is the likelihood
that oxygen gas be directly blown onto a refractory brick on the converter barrel
during vertical movement of the top-blowing lance, causing wear or failure of the
refractory brick. For the above reasons, a multi-nozzle lance having a nozzle inclination
angle between 20° and 30° is preferably used in the actual operation of a top-and-bottom
blown converter.
[0021] A further experiment was made to determine the relationship of the nozzle inclination
angle (p to the vibration of a converter housing when the lance height was set to
1500-1800 mm. The results are shown in Fig. 7. In a top-and-bottom blown converter
constructed by modifying a 250-ton top-blown converter, a number of blowing operations
were carried out using a corresponding number of top-blowing lances having different
nozzle inclination angles. The acceleration was measured at a trunnion support stand
in a direction parallel to the trunnion axis. The oxygen flow rate through the top-blowing
lance was 400―600 Nm
3/min., the oxygen flow rate through the bottom-blowing tuyeres was 350-250 Nm
3/min., and the top-blowing lance used was a four-nozzle lance having a throat diameter
of 38-40 mm. As seen from Fig. 6, when the lance height is 1500-1800 mm, the vibration
of the converter housing is reduced to a substantially negligible level by setting
the nozzle inclination angle ϕ to 20° or more.
[0022] Figs. 8 and 9 show the confines on the molten metal surface at which oxygen gas jets
from the nozzles of the top-blowing lance impinge to create hot spots, in an example
wherein the nozzle inclination angle is in the range between 20° and 30° and a comparative
example wherein the nozzle inclination angle is less than 20°, respectively. In the
case of Fig. 8, blowing operation was carried out in a top-and-bottom blown converter
equipped with bottom-blowing tuyeres arranged on a line parallel to the trunnion axis
and a four-nozzle lance having a throat diameter of 42 mm and a nozzle inclination
angle of 28°. The top-blowing oxygen gas flow rate was 560 Nm
3/min. and the bottom-blowing gas flow rate was 370 Nm
3/min. In this case, hot spots Pa-Pd were definitely outside the bottom-blowing gas
bubbling region Q encircled by a broken line in Fig. 8. The acceleration measured
at a trunnion support stand in a direction parallel to the trunnion axis was as small
as 0.02 G (wherein G is the acceleration of gravity). In the case of Fig. 9, a blowing
operation was carried out in the same manner as described for the example of Fig.
8 except that the nozzle inclination angle was 9.1°. In this comparative example,
hot spots Pa'-Pd' largely overlap the bottom-blowing gas bubbling region- Q. The acceleration
measured as above was 0.08 G.
[0023] As seen from the foregoing, the method of the present invention for operating a top-and-bottom
blown converter by blowing the top-blowing oxygen gas such that the center of a hot
spot created by an oxygen gas jet from each of the nozzles of a top-blowing multi-nozzle
lance is positioned outside a bubbling region of the molten metal surface which rising
bubbles of the bottom-blowing gas reach, has many advantages that vibration of a molten
metal bath is significantly reduced as compared with the prior art, to thereby minimize
vibration of the converter housing, and consequently, even a top-and-bottom blown
converter of the type which is constructed by modifying an existing top-blown converter
is unlikely to undergo fatigue failure at its housing support, blowing operation can
be carried out in a stable manner, and the possible danger to the operators is minimized.
Furthermore, by using a top-blowing lance having nozzles with an inclination angle
between 20° and 30° in the operation of a top-and-bottom blown converter, the centers
of hot spots created therewith can be positioned outside the bottom-blowing gas bubbling
region, thereby ensuring the stable and effective operation of the converter.
[0024] It should be understood that the application of the present invention is not limited
to the above-described type of top-and-bottom blown converter which is constructed
by modifying a top-blown converter, and the present invention is also applicable to
those converters constructed by adding a top-blowing lance to a bottom-blown converter.
1. Verfahren zum Betreiben eines Auf- und Durchblasekonverters mit einer Vielzahl
von Einblasöffnungen, die am Boden zum Einblasen eines Gases in ein im Konverter befindliches
Metallschmelzenbad angeordnet sind, und mit einer mehrere Düsen aufweisenden Aufblas-Lanze,
die durch eine obere Öffnung des Konverters zum Einblasen von Sauerstoffgasstrahlen
auf die Oberfläche der Metallschmelze eingeführt wird, dadurch gekennzeichnet, daß
das Sauerstoffgas so eingeblasen wird, daß der Mittelpunkt einer von dem Sauerstoffgasstrahl
jeder Düse der Lanze erzeugten Aufblasestelle außerhalb eines Gesamtblasenbereiches
der Metallschmelzenoberfläche, den die aufsteigenden Blasen des Durchblase-Gases überdecken,
angeordnet ist, wobei der Gesamtblasenbereich dadurch definiert ist, daß ein die vertikalen
Projektionen der Einblasöffnungen auf eine feststehende Metallschmelzenoberfläche
umgebender Bereich auf einen Abstand d=Hxtan (6/2) aufgeweitet ist, wobei θ der Verteilungswinkel
des durch die Einblasöffnungen dem Metallschmelzenbad zugeführten Durchblase-Gases
und H die Tiefe des Metallschmelzenbades zwischen seiner Oberfläche und dem Konverterboden
ist.
2. Verfahren nach Anspruch 1, dadurch gekennzeichnet, daß eine Vielzahl von Einblasöffnungen
verwendet werden, die in einer oder zwei Reihen angeordnet sind, die parallel zu den
Enden der den Konverter tragenden Drehzapfen verlaufen.
3. Verfahren nach Anspruch 1 oder 2, dadurch gekennzeichnet, daß in einem orthogonalen
Koordinatensystem, das auf die feststehende Metallschmelzenoberfläche aufgebracht
ist, seinen Ursprung in der Vertikalachse des Konverters besitzt und dessen x-Achse
parallel zu der Achse der den Konverter tragenden Drehzapfen verläuft, wobei die Koordinaten
(x, y) der Mittelpunkte von mindestens 4 von den Sauerstoffgasstrahlen der Düsen der
Lanze an der Metallschmelzenoberfläche erzeugten Aufblasestellen in einen Bereich
fallen, der durch folgende Ungleichungen definiert ist:

wobei a der Durchmesser des Blasenbereichs in Richtung parallel zu der Drehzapfenachse,
b der Durchmesser des Blasenbereichs in Richtung senkrecht zu der Drehzapfenachse
und c der Radius einer von der Aufblasestelle definierten Aushöhlung ist.
4. Verfahren nach einem der vorhergehenden Ansprüche, dadurch gekennzeichnet, daß
eine mehrere Düsen aufweisende Aufblas-Lanze verwendet wird, die Düsen aufweist, deren
Achse einen Winkel von 20° bis 30° bezüglich der Achse der Lanze aufweist.
5. Aufblas-Lanze zur Durchführung des Verfahrens nach einem der vorhergehenden Ansprüche,
an deren Spitze sich eine Vielzahl von Düsen befindet, dadurch gekennzeichnet, daß
die Düsen (8) so ausgerichtet sind, daß die Achse jeder Düse einen Winkel von 20°
bis 30° bezüglich der Achse der Lanze (3) aufweist.