FIELD OF INVENTION
[0001] The present invention relates to the continuous casting of metals and alloys, for
example, steel.
BACKGROUND OF INVENTION
[0002] In continuous steel casting by pouring liquid metal into an open-end mold, stability
of the free surface of the metal in the mold, often called the meniscus, plays a significant
role in both process control and the quality of as-cast product.
[0003] Electromagnetic stirring of liquid steel within the mold, commonly known as M-EMS
or simply EMS, is broadly employed in continuous casting mainly to improve quality
of the strand surface/sub-surface and solidification structure (i.e., structure refinement,
soundness and chemical homogeneity).
[0004] The two most common practices of continuous steel casting impose entirely opposite
requirements to the stirring conditions within the region of molten metal near its
free surface at the mold top, i.e. the meniscus region.
[0005] Accordingly, casting mainly Al-killed steel grades via a submerged entry nozzle under
mold powder requires meniscus stability in order to prevent disruption of mold lubrication
and powder entrapment into the cast body. A rotary stirring motion at the meniscus
causes meniscus depression in the centre, waves, and excessive erosion of the casting
nozzle when stirring intensity exceeds a certain level. On the other hand, casting
of Si-Mn deoxidized steel with an open stream is often accompanied by the defects
of cast product surface. Pinholes, blowholes, surface slag entrapment and subsurface
inclusions are examples of those surface defects. In order to minimize or eliminate
the surface defects, an intensive stirring motion of the molten metal is required
in the meniscus region. The same requirement applies for casting low deoxidized, or
so-called rimming substitute steel. However, overly intensive stirring motion of the
meniscus may cause undesirable deterioration of the surface by producing deep oscillation
marks and lappings.
[0006] Maximizing stirring intensity within the portion of metal confined by the mold is
beneficial for obtaining improvements of the internal quality of cast material. Improvements
in the solidification structure refinement and soundness, especially in high-carbon
and certain alloy steels, strongly respond to the intensity of stirring. Having a
rather limited operating space determined by the mold length, it is difficult to satisfy,
with a single system, varying stirring requirements without significantly compromising
some of them. For example, the limitation imposed by an acceptable level of meniscus
disturbances with casting under mold powder restricts maximizing stirring intensity
induced by EMS within the bulk of liquid pool.
[0007] Attainment of different stirring conditions in the mold is difficult, if possible
at all, when more than one of the casting techniques mentioned above are being practised
at the same casting facility.
[0008] There are some known methods in prior art with the objective to change or control
the stirring motion in the meniscus area. Japanese Patent Publication No. 58-23554
describes a method of decreasing the intensity of stirring in the meniscus region
by means of an induction coil arranged on the mold adjacent to that region and providing
rotating stirring motion opposite to that induced by the main EMS coil arranged below.
[0009] The main drawback of this method is that the induction coil adjacent to the meniscus
region provides only a deceleration of the stirring velocity produced by EMS. In the
case when an intensive stirring action within the meniscus region is required, this
method would need to relinquish its decelerating action by de-energizing the coil.
The coil is not intended to enhance stirring action if the need of such enhancement
arises, for the reasons discussed above.
[0010] In addition, the range and criterion of stirring deceleration are not disclosed in
the publication. For example, a complete or near to it deceleration of stirring velocity
can be related to meniscus flatness. The meniscus depression caused by rotational
motion is proportional to angular stirring velocity, as seen from the expression:

where,
h is the depth of meniscus depression
W is the angular stirring velocity
R is the radius of the stirred pool
g is the acceleration due to gravity
[0011] The depth of meniscus depression h approaches zero when the angular stirring velocity
at the meniscus caused by EMS is equalized by counter-stirring angular velocity produced
by a braking induction coil.
[0012] Without such equalizing, the merits of that method for application to the casting
under the mold powder will be limited.
[0013] Another possible way of alleviating the problem of meniscus instability and decreasing
stirring motion at the surface in on application of a strong horizontal D.C. magnetic
field to the meniscus region. Such a field produces an electromagnetic (Lorentz) force
directed opposite to the liquid metal motion and thereby reduces that motion velocity,
providing a quiescent surface. An application of this concept is described in the
U.S. Patent No. 4,933,005 of June 12, 1990, assigned to the assignee hereof.
[0014] AT-PS 189751 discloses electromagnetic stirring in an open stream process using two
electromagnetic coil arrangements are above the other operated in unison.
[0015] EP-A-0 096 077 discloses a plurality of electromagnetic agitations arranged in a
horizontal direction along a wall of a mold to accelerate or decelerate the circulatory
flow along the flow direction but does not provide a second magnetic field at a location
upstream of the stirring by a first rotating magnetic field. DE-A-3 819 492 discloses
two stirrers, one upon the other, and discloses operating one or both of the stirrers
in a casting method. EP-A-0 080326 discloses one rotational field only together with
an axial field. JP-A-59 89649 discloses a submerged nozzle process in which an upper
coil produces a field rotating in the opposite direction to that produced by a lower
coil to provide a braking effect at the surface of the molder metal.
[0016] An electromagnetic volume force will be produced in either of two situations, firstly,
when an A.C. rotating magnetic field interacts with liquid metal which is in the state
of complete rest, the metal will be set into a motion with a velocity lower than that
of the A.C. field; and, secondly, when a stationary, i.e. D.C. magnetic field, interacts
with liquid metal already in motion. The volumetric magnetic force is proportional
to velocity slip, i.e., the difference between the velocities of magnetic field and
liquid metal, in accordance with the relationship:

[0017] In this expression describing a tangential component of the electromagnetic force
produced by a two-pole induction stirrer, the parameters are:
σ is the electrical conductivity of liquid metal
B is the magnetic flux density
Wf is the angular velocity of magnetic field
Wm is the angular velocity of liquid metal
R is the radius of liquid metal pool
[0018] In the case of electromagnetic stirring with an A.C. magnetic field, W
f >> W
m, while W
f = 0 for a D.C. magnetic field and W
m is comparatively low in both cases. Thus, the velocity slip between an A.C. magnetic
field and moving liquid metal is much greater than that between the moving metal and
a stationary field. Therefore, in order to attain magnetic force of the same value,
a much greater value of magnetic flux density B is employed for a D.C. magnetic field
than would be required for an A.C. magnetic field. This demand for magnetic flux increases
with the requirement to reduce metal velocity to a lower level.
[0019] Laboratory experiments have shown that a magnetic flux density of the order of 300
mT was required to reduce a stirring velocity in a pool of mercury by 70 to 90 percent.
Considering a scaling-up effect of industrial application, it is difficult to attain
both the level of magnetic field intensity and the degree of stirring velocity reduction.
SUMMARY OF INVENTION
[0020] The process according to the invention is defined in claim 1.
[0021] The present invention thus provides an improved method of controlling electromagnetic
stirring intensity within a continuous casting mold. This method provides both the
flexibility of adaptation of stirring conditions to the casting processes and the
accuracy of stirring control which were lacking by prior art.
[0022] The present invention may be performed using an apparatus which includes an electromagnetic
A.C. coil similar to but smaller than that of a main electromagnetic stirrer installed
downstream and arranged around the mold in the meniscus area. This device is in essence
another induction stirrer, similar to the main stirrer which is arranged axially symmetrical
around the mold and farther down from the meniscus. However, the coil in the upper
part of the mold is suitable for counterbalancing and equalizing, or enhancing, depending
on specific objectives, the stirring motion in the adjacent volume of liquid metal,
whose motion is originated by the main stirrer. Therefore, the working function of
this stirrer is to modify the pattern and/or intensity of the stirring induced by
the main stirrer and henceforth the device performing that function will be called
A.C. magnetic stirring modifier or A.C. MSM. The action of the A.C. MSM is typically
contained within the upper portion of molten metal pool, comprising approximately
10 to 15 percent of its volume confined by the mold.
[0023] The stirring motion within that portion of the metal pool is caused and maintained
by the inertia forces, i.e. velocity drag, which transmit the momentum from the part
of the pool where the motion has been commenced by M-EMS. Therefore, the stirring
velocity at the meniscus area is less than that in the area of maximum value of M-EMS
magnetic flux density, i.e. the area corresponding to the middle of EMS coil. Consequently
less magnetic energy is required to counterbalance the kinetic energy of molten metal
motion in the meniscus area than is provided by the M-EMS coil. Being a part of a
single magnetohydrodynamic system, both the A.C. MSM and M-EMS operate at a common
frequency determined by the parameters of the mold. The current supplied to both sets
of the coils can be of the same variable value or it can be controlled separately.
These operating features conveniently allow for a single power source for both sets
of coils.
[0024] The invention is broadly applicable to all electroconductive materials, i.e. metals
and alloys, which can be electromagnetically stirred and where control of stirring
intensity is required within some region or regions without interference with stirring
within other regions of the liquid pool. The invention is applicable to a wide variety
of spacial orientation of a vessel containing the molten method. For example, a casting
mold may be arranged vertically, inclined or horizontally.
BRIEF DESCRIPTION OF DRAWINGS
[0025]
Figure 1 is a schematic of an arrangement of an A.C. magnetic stirring modifier and
an electromagnetic stirrer (EMS), with respect to a casting mold ;
Figure 2 is a schematic representation of the magnetic flux density axial profiles
for the A.C. magnetic stirring modifier and the EMS of Figure 1 and the axial profile
of rotational stirring velocity produced thereby;
Figure 3 is a graphical representation of the relationship of meniscus depression
without and with an A.C. magnetic stirring modifier at varying current of an EMS;
Figure 4 is a single-line diagram of possible electrical connections for the induction
coils of the A.C. magnetic stirrer modifier and the EMS of Figure 1; and
Figure 5 is an elevational sectional view of the mechanical arrangement of the A.C.
MSM and the EMS within the mold housing and corresponding to the schematic arrangement
of Figure 1.
[0026] Referring to the drawings, Figure 1 is a schematic depiction of an arrangement of
an A.C. MSM and an EMS within a mold housing assembly of a continuous casting machine
10 . Figure 5 is a more detailed depiction of the mechanical elements of the mold
assembly.
[0027] A series of induction coils 12, is arranged equally spaced around the periphery of
a vertical casting mold 14, at its lower portion to comprise an A.C. electromagnetic
stirrer (EMS). The EMS coils 12, when energized, induce rotary motion of a strand
of molten metal 16 within the mold 14 about its longitudinal axis.
[0028] A casting ceramic tube 18 is axially located with respect to the strand of molten
metal 16, if the apparatus is to be used for casting with a submerged entrance nozzle
instead of the open pouring method. A.C. MSM induction coils 20, are equally spaced
around the vertical mold 14, adjacent to a free upper surface or meniscus 22 of the
strand of molten metal 16. The EMS coils 12 are designed to induce a strong rotational
flow of molten metal in the strand of molten metal 16 within the mold 14. The intensity
of this rotational flow is characterized by its rotational velocity U
R which, in turn, depends on the parameters comprising the expression:

wherein,
K is a proportionality coefficient
T is the magnetic torque applied to the molten metal
L is a characteristic length of stirrer
[0029] The magnetic torque T is defined by other parameters of the electromagnetic system:

where,
f is the current frequency
σ is the liquid metal electrical conductivity
B is the magnetic flux density
R is the stirred pool radius
[0030] A maximum value of rotational velocity is attained within and about the region of
molten metal defined by a characteristic length of stirrer L which corresponds to
a magnetic flux density B distribution along stirring axis. A typical magnetic flux
density distribution for the two sets of induction coils 12 and 20 are shown in Figure
2.
[0031] The axial distribution of rotational stirring velocity, U
R, also is presented in Figure 2. As seen from this schematic, the rotational velocity
U
R extends well beyond the active stirring zone L of the EMS coils 12 within the molten
metal pool 16. This effect is due to the fact that angular momentum originated by
the stirring coils 12 is transported by secondary poloidal flow within the metal strand
16. The secondary flow is originated at the stirring symmetry area, i.e., the stirrer
neutral horizontal axis, and is directed from the active stirring zone L along the
solidification front, making a return loop towards the stirrer at the stirred pool
centre.
[0032] The value of the maximum stirring velocity within and about the active stirring zone
L and the rate of its axial attenuation within the metal 16 determine the stirring
velocity at the meniscus area 22 in the absence of other effects.
[0033] Along with the value of magnetic flux density and the frequency, the stirring velocity
value and its lengthwise axial range depend on the stirrer length L, the radius of
the stirred pool R, and the roughness of the solidification interface with liquid
metal. Accordingly, it is difficult to quantitatively and accurately predict the stirring
velocity at the meniscus, based upon the design and operating parameters of the EMS
coils 12 and the distance from EMS neutral axis to the meniscus.
[0034] For a typical EMS arrangement within a steel billet/bloom continuous caster mold
housing, the stirring velocity at the meniscus generally is about 0.5 to 0.7 (about
50 to 70 percent) of maximum stirring velocity value while the EMS coils 12 are located
at a lowest position with respect to the meniscus. Therefore, a substantial stirring
action can be expected at the meniscus area produced by the EMS coils even if the
latter is located at the farthest possible distance from the meniscus. Meniscus depression
and, more generally, turbulence at this location manifest themselves as a result of
this stirring action.
[0035] The meniscus depression depth, as was shown earlier in the expression (1), is strongly
correlated to the angular stirring velocity at the meniscus. At given EMS design parameters,
for example, active stirring length, power input, frequency and distance from the
meniscus, the meniscus stirring velocity and depression are proportional to the current
supplied to the EMS coils 12, as shown schematically in Figure 3.
[0036] Depending on the factors mentioned above, the meniscus depression for industrial
systems can range from approximately 6 to 27 mm, for example.
[0037] In order to counterbalance the stirring velocity at the meniscus area produced by
the EMS coils 12, the induction coils 20 of A.C. MSM are energized, to induce a stirring
action within the liquid metal at the meniscus opposite to that caused by the EMS
coils 12. All the previous considerations with respect to a rotary movement of liquid
metal are applicable to the stirring produced by the A.C. MSM coils 20.
[0038] The A.C. MSM coils 20 are substantially smaller and require less power for their
operation than the EMS coils 12 due to a much less stirring velocity expected for
them to produce to counteract the rotational motion at the meniscus induced by the
EMS coils 12.
[0039] The A.C. MSM coils 20 are energized from a power supply common with the EMS coils
12, as shown by single line diagrams in Figure 4. Schemes I and II appearing in Figure
4 show the A.C. MSM and EMS coils 20 and 12 respectively connected in series and,
therefore, operating at the time same current and frequency supplied from a common
power source. The coil connections presented in Scheme I provide for unidirectional
rotating magnetic fields produced by both the EMS and A.C. MSM coils. This mode of
operation is employed for enhancing the stirring motion at the meniscus area by the
A.C. MSM coils 20 when performing the process of the present invention with the illustrated
apparatus. The coil connections presented in Scheme II provide for counter-rotating
magnetic fields and cause counter-rotating liquid metal motions in the areas corresponding
to the EMS and A.C. MSM coils. In order to provide fine control over stirring action
at the meniscus which is determined by the variables of EMS (for example, B-flux),
the current level supplied to the A.C. MSM coils 20 may have an independent control
from that of the EMS coils 12, as shown by Scheme III in Figure 4. This arrangement
allows for independent control of stirring actions of either of the EMS or the A.C.
MSM coils regardless of the directional pattem of stirring, namely unirotational or
counter-rotational.
[0040] The independent control of stirring motion at the meniscus provided by the use of
the A.C. MSM coils 20 enables a greater flexibility of the stirring process control
with a possibility of achieving equalization of the opposite stirring motions at the
meniscus, and minimization of its depression, as illustrated in Figure 3.
[0041] As seen therein, the line OA corresponds to the meniscus depression caused by the
stirring induced by EMS coils 12 without being opposed or added by A.C. MSM stirring.
Similarly, the line OD represents meniscus depression associated with isolated stirring
action induced by the A.C. MSM coils 20. In order to equalize the stirring velocities
caused by the EMS and A.C. MSM coils, the meniscus depression must be of the same
value in either of the situations. For example, if the meniscus depression caused
by EMS stirring corresponds to the level A, then counter-rotational stirring provided
by A.C. MSM stirring should have corresponding meniscus depression, i.e. level D.
[0042] The line OC is the resultant of two opposite stirring actions produced respectively
by the EMS and AC MSM coils and equalized at the meniscus.
[0043] The line AB represents the resultant of two unidirectional stirring actions. In this
case, the range of stirring enhancement expressed through the meniscus depression
can be adjusted in accordance with the casting practice requirements, so that the
stirring intensity of EMS is fully utilized.
SUMMARY OF DISCLOSURE
[0044] In summery of this disclosure, there is provided an improved method of controlling
disturbance of the free surface of molten steel or other metal or alloy being cast
through a mold and caused by electromagnetic stirring applied to the liquid metal,
to minimize such disturbance or achieve an enhanced, within a single casting unit
stirring motion at the meniscus, by employing an induction modifier in the form of
an electromagnetic stirrer adjacent to the location of the meniscus.
1. Verfahren zum kontinuierlichen Gießen von Knüppeln und Vorblöcken aus Metallschmelze
mittels einer Vorrichtung, die eine Gießform aufweist, in die Metallschmelze durch
einen Vorgang des offenen Gießens der Metallschmelze eingeführt wird, und Durchführung
eines Induktionsrührens in der Metallschmelze in der Form, wobei das Induktionsrührverfahren
umfasst:
elektromagnetisches Induzieren des Rührens von geschmolzenem Metall mit einer Intensität,
die normalerweise zu einer Turbulenz in dem geschmolzenen Metall einschließlich seiner
freien Oberfläche führt, durch Anlegen eines ersten rotierenden Magnetfeldes an das
geschmolzene Metall, und
Anlegen eines zweiten rotierenden Magnetfeldes, das von einer von der das erste Magnetfeld
liefernden Quelle getrennten Quelle und an einer Stelle stromaufwärts des Rührens
erzeugt wird, wobei das zweite rotierende Magnetfeld in derselben Richtung rotiert
wie die Rotationsrichtung des ersten Feldes, um die Rührbewegung im Bereich der freien
Oberfläche zu verstärken, aber ein Drehmoment auf das geschmolzene Metall ausübt,
welches niedriger ist als das von dem ersten Feld ausgeübte Drehmoment.
2. Verfahren nach Anspruch 1, bei dem das zweite rotierende Magnetfeld durch einen Satz
von Induktionsspulen geliefert wird, die nahe der freien Oberfläche der Metallschmelze
angeordnet sind.
3. Verfahren nach Anspruch 1 oder 2, bei dem das zweite rotierende Magnetfeld von einem
Satz von Induktionsspulen erzeugt wird, die von einem Wechselstrom beaufschlagt sind,
der von einer Stromquelle geliefert wird, die unabhängig ist von einer Stromquelle
für einen das erste rotierende Magnetfeld erzeugenden Satz von Induktionsspulen.
4. Verfahren nach Anspruch 3, bei dem die Sätze von Induktionsspulen Spulen mit Multiphasen-
und Multipol-Anordnung sind, die in Umfangsrichtung beabstandet um die Form herum
angeordnet sind, um die jeweiligen rotierenden Magnetfelder zu erzeugen.
5. Verfahren nach einem der Ansprüche 1 bis 4, bei dem das zweite rotierende Magnetfeld
dazu dient, eine Rührbewegung in dem Meniskusbereich zu bewirken, die ausreicht, um
die von dem ersten rotierenden Magnetfeld in dem Meniskusbereich bewirkte Rührbewegung
auf ein Niveau anzuheben, das bei oder nahe dem Niveau der Rührbewegung liegt, die
von dem ersten rotierenden Magnetfeld an seiner stromabwärts liegenden Aufbringungsstelle
erzeugt wird.
6. Verfahren nach einem der Ansprüche 1 bis 5, bei dem die Metallschmelze Stahl ist.
1. Un procédé pour mouler en continu des billettes et des lingots épais (blooms) à partir
de métaux fondus faisant emploi d'un moule de coulée dans lequel le métal fondu est
introduit par un procédé d'alimentation ouverte du métal fondu avec mise en oeuvre
d'un procédé d'agitation en continu du métal fondu dans le moule, le procédé d'agitation
par induction comprenant:
- le brassage par induction électromagnétique du métal fondu avec une intensité telle
qu'on obtient normalement une turbulence du métal fondu y compris de sa surface libre
par application audit métal fondu d'un premier champ magnétique tournant, et
- l'application d'un second champ magnétique tournant, obtenu par une source distincte
de celle qui produit ledit premier champ magnétique et à un endroit en amont de ladite
agitation,
dans lequel le second champ magnétique tournant tourne selon la même direction que
la direction de rotation du premier champ magnétique tournant, pour augmenter le mouvement
d'agitation dans la zone de ladite surface libre mais exerce une action de couple
sur le métal fondu qui est inférieure à celle exercée par le premier champ.
2. Le procédé selon la revendication 1, dans lequel ledit second champ magnétique tournant
est appliqué au moyen d'un jeu de bobines d'induction en un endroit adjacent à la
zone de la surface libre dudit métal fondu.
3. Le procédé selon la revendication 1 ou 2, dans lequel le second champ magnétique tournant
est produit par un jeu de bobines d'induction contrôlées par un courant alternatif,
alimentées par une source de puissance indépendante par rapport à la source de puissance
pour le jeu de bobines d'induction produisant ledit premier champ magnétique tournant.
4. Le procédé selon la revendication 3, dans lequel les jeux de bobines d'induction sont
des bobines à disposition multiphase et multipôle écartées périphériquement autour
de la zone du métal fondu afin de produire les champs magnétiques tournants respectifs.
5. Le procédé selon l'une quelconque des revendications 1 à 4, dans lequel le second
champ magnétique tournant est utilisé pour obtenir un mouvement d'agitation dans la
zone du ménisque suffisant pour augmenter, dans ladite zone du ménisque, le mouvement
d'agitation produit par le premier champ magnétique tournant à un niveau, ou au voisinage
dudit niveau, du mouvement d'agitation produit par le premier champ magnétique tournant
en un emplacement adjacent à sa position d'application en aval.
6. Le procédé selon l'une quelconque des revendications 1 à 5, dans lequel le métal liquide
est l'acier.