referring now to the figures of the drawing in detail and first , particularly , to fig1 thereof , there is shown an electromagnetic stirring system which includes an in - mold stirrer 4 and one or two line / final electromagnetic stirrers 6 , 7 that are located downstream of the in - mold stirrer 4 . the in - mold electromagnetic stirrer 4 integrated into a mold 3 or could locate outside mold , and the mold 3 receives through a submerged nozzle 1 or by free jet , liquid steel 2 into the mold copper crystallizer 3 . the in - mold electromagnetic stirrer 4 could be any kind , could be formed of one or , as best shown in fig2 a and 2b , of two — one upper and one lower four - pole or six - pole waterproof magnetic cores 4 a such as inductors 4 a . one or both upper and lower inductors 4 a of the in - mold stirrer 4 are connected to a frequency inverter which is shown in fig3 . each pole of the magnetic cores 4 a is surrounded by one coil 5 , formed of a waterproof and flexible winding . the upper and lower magnetic cores 4 a surround a baffle 9 that is disposed around the copper crystallizer or mold 3 . the connection of the coils 5 could be like in classical rotational stirrer or could provides the electrical joining of the coils 5 of the upper magnetic core 4 a with the coils 5 of the lower magnetic core 4 a with a space shift of 90 °. therefore , the same current that flows in the upper coil no . 1 , flows in the lower coil no . 2 or no . 4 , that is the upper coil no . 1 is shifted relative to the lower coils no . 2 or no . 4 by 90 °. the above defined electric connection of the windings of the upper and lower magnetic core of the in - mold electromagnetic stirrer 4 in accordance with the invention are determined from the standpoint of the appearance of an axial component of the electromagnetic force that can generate pressure waves , spreading outside the stirrer 4 into a liquid part of the billet 2 . according to the in - mold electromagnetic stirring method of the invention , an alternating multi - frequency three - phase or two - phase current to be applied to a set of coils to the asynchronous rotation stirrer is in the frequency range of 1 . 0 - 20 . 0 hz and a ratio of current amplitudes ( i low / i high ) is in range 0 . 2 - 5 . 0 , for all kinds and sizes of billet or bloom during casting . the three - phase or two - phase currents of different frequency components have a different phase sequence . it suppresses the rotating velocity of the melt on the meniscus and suppresses the vertical downward velocity components at the meniscus for preventing the entrapment of nonmetallic inclusions . the above - defined frequencies of current - components for feeding to the in - mold electromagnetic stirrer in accordance with invention are determined from the standpoint of : b ) suppression of vertical components of the molten steel velocity at the meniscus for preventing the entrapment of nonmetallic inclusions ; c ) generation of short - wave vibration of meniscus edges for increasing mold powder access into gaps between the ingot and mold walls ; and d ) generation of joule heating sources on the meniscus edges especially for lowering the point of initial solidification and preventing a touching of the steel with a solid slag ring formed above the meniscus during casting ; e ) generation of pulse magnetic pressure with frequency equals to intrinsic frequency of acoustic waves spreading in the liquid portion of continuously castled ingot . all of the above - mentioned points lead to better surface quality and internal quality of the ingot . upon the passing of the alternating multi - frequency current of the above - defined ranges through the exciting coils 5 of the in - mold electromagnetic stirrer 4 shown in fig1 and 2 , the multi - frequency magnetic field , which is induced by the exciting coils , penetrates through the crystallizer or mold 3 into the ingot with different intensities : the low frequency magnetic flux ( 3 . 0 - 6 . 5 hz ,) penetrates more intensive , and the high frequency magnetic flux component ( 13 - 20 hz ) undergo a magnetic resistance of the copper mold 3 , and try to avoid the mold above the meniscus and is best shown in fig4 . therefore , the magnetic flux of the high frequency component concentrates at the meniscus edges , penetrates downward into the ingot through the meniscus and creates a reverse braking electromagnetic forces or torque , which is shown in fig5 a , due to the current of the high frequency component having a reverse phases sequence comparatively with the currents of the low frequency component . at the same time , the interaction of the high frequency induced current components that concentrate on the meniscus edges , with the low frequency magnetic field component , which exists here , creates the electromagnetic force that leads to vibration of the meniscus edges and increases the molten mold powder inflow into the gap between the mold and the ingot walls especially on the billet corners ( if the billet is rectangular ). the increased mold powder flow into the gap between the billet and the mold wall , which increases the heat resistance in the slag layer between the mold and the ingot — on the one hand , and a concentration of electromagnetic power on the meniscus edges and generate here the joule heating — on the other hand — leads to partial melting of shell edges and a lowering of the point of initial solidification of the ingot . during the submerged casting , the edge of the initial solidification moves down a distance h mm , which is shown in fig6 and 7 and does not touch the slag rim and therefore oscillation marks decrease or disappear . the intensity of low frequency magnetic field ( 3 . 0 - 6 . 5 hz ,) and the main electromagnetic average torque remain on the exciting level and the stirring intensity does not change because the braking torque is applied to a comparatively small volume of the cast steel . according to the electromagnetic method of stirring in the final solidification zone , the alternating three - phase or two - phase current is to be applied to a set of three coils , shown best in fig8 . a first coil , consists of one or two sections an inductor 15 are supported on the one or two of four rods of a rectangular magnetic core 13 , which surrounds the continuously castled billet 2 , and two second coil magnets 14 , having a saddle - shape form , are disposed between the magnetic core 13 and the billet 2 . the first coil of inductor 15 generates a magnetic flux , which is confined inside the magnetic core 13 , the second two coils 14 ( magnets ) responsible for pushing out a part of the above - mentioned magnetic flux from magnetic core and imposition it into billet . when all the coils are connected to the system of three - phase or two - phase voltage , the magnetic flux , which is pushing out of magnetic core , is revolving — similar to a non - salient - pole asynchronous motor . the first coil 15 ( inductor ), generating the magnetic flux , surrounding the ingot , induces in the billet a longitudinal current that never can be equal to zero in the geometrical and metallurgical center of the ingot . according to the electromagnetic stirring method of the invention two stirrers are installed along the same cast strand , induce the currents in the cast billet that join together into a common loop that includes the billet and elements of the casting arc . the common current exists between the stirrers and it reaches 10 - 20 ka . elements of the longitudinal current flowing through the billet cross section in the liquid portion and in the solid portion interact and as a result of this interaction , strong cross electromagnetic forces appear in both portions of the billet — in the solid portion and in the liquid portion . the cross electromagnetic forces in the liquid portion leads to a flow of the liquid steel or mushy zone . as a result , there is a movement of the molten steel in the ingot and an intensity in the stirring forces . so , as result of induced current existence in the liquid portion of billet , the stirring of the molten steel in the ingot exists even between final stirrers independent from the distance between the stirrers . in contrast to the conventional asynchronous stirrers , by this phenomenon , the molten steel in the center portion of the molten pool is stirred sufficiently enough to cause a uniform temperature distribution along all the ingot where the stirring effect is present . thanks to force convection at the interface the increasing of heat transfer and diffusion on the solidification front the non - uniform growth of columnar dendrites is suppressed everywhere , where the induced current exists , and the conditions for segregation development disappear , so that a white band in such a distinctive form as would result from conventional stirring does not occur either . referring again to fig1 , there is schematically shown the electromagnetic stirring system , which is employed in the method of the invention for use in continuous casting processes of molten medium and high carbon steels . the system of electromagnetic stirring is formed of multiple adjacent stirring elements , namely : the mold single or dual asynchronous stirrer 4 , and a two - section stirrer 6 , 7 having an intermediate ( line ) 6 and a final section 7 . the distance between the intermediate 6 and final sections 7 of the two - section stirrer can be as long as the casting ark allows . referring to fig2 a and 2b , there is schematically shown that the mold stirrer creates the rotational magnetic flux with four or six electromagnetic coils 5 located on a common magnetic core 4 a and , referring to fig3 , fed by three - phase or two phase currents from the frequency inverter or from another power supply that generates the multiphase poly - harmonic currents with controlled phase sequences , amplitudes and harmonic structure . a low frequency current component has a direct phases sequence , frequency of f 1 = 3 . 0 - 6 . 5 hz , and an amplitude 100 %, being dependent on the castled ingot sizes and casting speed . a high frequency ( 13 - 20 hz ) component has the reverse phases sequence , and a current amplitude equal to 20 - 500 %. all above mentioned polyharmonic currents periodically changes with frequency equals to 0 . 5 of intrinsic frequency of castled mold ( about 1 hz for billet 7 × 7 inch of cross section ) increases the amplitudes k times , 0 . 2 & lt ; k & lt ; 1 . 0 and save this value during 1 / f 1 . the above - mentioned current structure is determined from a standpoint of using an edge effect for : a ) applying a reverse electromagnetic torque to the meniscus and to suppress a vortex at the meniscus ; b ) reducing the vertical components of the steel velocity for preventing the entrapment of inclusions in the ingot ; c ) saving the stirring intensity inside the mold and nevertheless , an opposite torque is applied to the meniscus of the molten steel ; d ) oscillating with an amplitude of 2 mm the meniscus edges for increasing the flow of molten mold powder into the gap between the mold and the ingot walls ; e ) providing joule heating of solidified shell edges with the molten steel for lowering the point of initial solidification by 2 mm for preventing a touching and bending of shell edges during mold oscillates ; and f ) generation of pulse magnetic pressure , spreading in the liquid portion along of billet as acoustic waves and extending the zone experiencing of the force convection below the mold to a final point of solidification for increasing the stirring effect . the magnetic system of the dual or single mold stirrer does not differ from regular asynchronous stirrers that provide the rotational motion of the molten steel inside the mold , and , at the same time the reverse electromagnetic torque , as shown in fig5 , and the joule heating and increased oscillation of the meniscus edges , fig7 . the magnetic flux of the lowest frequency component easily penetrates into the mold and the ingot . referring to fig3 , there is the principal electric schematic layout of the polyharmonic current source for the mold stirrer . the logical programmable electronic block , which contains the frequency inverter , forms the control signals for power components that transform the direct current from the rectifier into alternating two - or three - harmonic two - phase or three - phase currents , having the above mentioned or any harmonic consistency , amplitudes and phase sequence . the poly - harmonic currents passing in the coils of the inductor create the magnetic field of the same frequency content . referring to fig4 and 6 , an explanation of the edge effect of an asynchronous stirrer is now explained . the magnetic flux , generated in the coils 5 ( stator ), flows through the copper mold 3 and the steel ingot 2 . the magnetic flux meets the electromagnetic resistance in the highly conductive mold 3 and the ingot and as a result induces eddy currents . the eddy currents create their own magnetic flux that prevents the penetration of the primary flux into the mold and the ingot . this results in that the primary magnetic flux tries to avoid the copper mold 3 from above and below . at the mold top , above the meniscus , the magnetic flux meets comparatively low screening and tries to penetrate into the conductive steel ingot 2 through the meniscus . the higher the frequency of the magnetic field component the more the magnetic flux tries to avoid the copper mold 3 and the ingot 2 and thus a greater portion of the magnetic flux penetrates through the meniscus and concentrates on the meniscus edges . the reverse braking torque is formed because the current of the high frequency component has adjusted with the reverse phases sequence comparatively with the currents of the low frequency component . referring to fig5 a , there is schematically shown a distribution of electromagnetic forces at the meniscus by the different frequencies of the magnetic flux generated by the coils of the stirrer stator including the distribution of electromagnetic forces at the meniscus when the feed current has two frequency components : 3 . 0 hz and 17 hz . at the same time the main stirring effect — revolving electromagnetic forces on the middle of stator of in - mold stirrer are shown in fig5 b . nevertheless , the high component of the magnetic flux creates the reversing torque at the meniscus , the main revolving force in the center section of the in - mold stirrer remains high , so the efficiency of stirring and the possibility of superheating decreasing remains strong too . at the same time the next low frequency current component f 3 = 0 . 5 f intr ( about 1 hz ) and amplitude 1 . 5 - 2 . 0 times higher then for current of second frequency component f 2 = 3 / 0 - 6 . 5 hz — creates the pressure pulsation with frequency equal to intrinsic frequency of melt oscillation in the liquid portion of ingot . this oscillating pressure spreads along billet and generates the pulse flow at the solidification front . referring to fig7 there is schematically shown the formation of meniscus edge vibrations when strong high frequency currents concentrate at the meniscus edges ( because of the strong edge effect ) and interact with a strong , low frequency magnetic flux . the resulting intensity of the mold powder inflow into the gap between the mold and the ingot increases 15 - 30 % and a heat resistance of the slag scum increases also directly at the point of beginning of solidification . the concentration of electromagnetic power on the meniscus edges and the simultaneous generation here of the joule heating together with the increase of heat resistance in slag layer between the mold and the ingot leads to a partial melting of shell edges and a lowering of the point of initial solidification . referring to fig6 and 7 , there is schematically shown the lowering of the initial solidification at the ingot shell and the prevention of touching of the solidifying ingot with the slag rim above the meniscus , when the mold oscillates . referring to table 1 , there is shown the comparison of cinematic characteristics of two asynchronous stirrers with different kinds of feed currents . the electromagnetic mold unit , which is employed in the method of the invention for use in continuous casting of steel billet and bloom , and which is adapted so that the poly - harmonic currents fed to the stirrer magnetic system , leads to the meniscus becoming quiet , and the melt velocity components — azimuth and vertical are suppressed . the resulting suppression of the velocities at the meniscus leads to a decrease of mold powder droplets and particles being entrapped . the intensity of melt stirring decreases on average by 10 % when the poly - harmonic current uses the same current amplitude that is used in regular mono - harmonic current . referring to fig8 , there is schematically shown a line / final electromagnetic stirrer 6 , 7 of fig1 in accordance with the invention . according to the electromagnetic method of stirring within a mold or in the final solidification zone , the alternating single - phase , two - or three phase current of mono - harmonic industrial frequency is to be applied to a set of two coils . the first coil 15 is located on the one of four rods of the rectangular magnetic core 13 that surrounds the continuously castled ingot 2 , and the second coil 14 having a saddle - shape form and located between the magnetic core 13 and the ingot 2 . both coils 14 can be manufactured as a double coil especially for adjusting the necessary voltage . the first coil 15 generates the magnetic flux that is confined in the magnetic core 13 , the saddle shaped coils 14 are provided for pushing out part of the above - mentioned magnetic flux from the magnetic core 13 and imposition of it into the ingot . the magnetic core 13 is formed of two parts : a first part 12 has a u - shape , the second part 16 is straight . between the core parts 12 and 16 is an adjustable air gap 18 , filled with a dielectric , provided for controlling a ratio between the magnetic flux inside and outside of the magnetic core . when all the coils of the system are connected to a two - or three - phase voltage , the magnetic flux that is pushing out of the magnetic core 12 , 16 is jumping similar to a regular asynchronous stirrer . the first coil 15 , generating the magnetic flux surrounding the ingot 2 , generates here the longitudinal and jumping or revolving current that never can be equal to zero ( irms ≠ 0 ) at the geometrical center of ingot , if the ingot has a galvanic contact with elements of the casting arc or is grounded . referring to fig9 a , there is shown the superposition of magnetic fluxes generated by the coils 14 and 15 when the ingot does not have perfect contact with elements of the casting arc or is not grounded . this results in that induced currents in the cast ingot remain in the ingot , do not pass out of the ingot , and have different directions relative to an ingot axis , so that a current in the ingot center equals to zero . fig9 a shows the case of an asynchronous stirrer , having a zero value for the induced current ( irms = 0 ) and electromagnetic force in the ingot center . referring to fig9 b , there is shown the superposition of magnetic fluxes , generated by the coils 14 and 15 when the ingot has perfect contact with the elements of the casting arc or grounded via connectors 17 , see fig8 and 11 . this results in that an induced current in the cast ingot 2 creates a path that goes out of the ingot and through the casting arc embrace of the stirrer inductor and has one direction relative to the ingot axis , and never can equal zero in the ingot center . this case represents the case of a regular transformer , where the ingot plays the role of the single - turn secondary winding and the secondary current of the single direction flows a cross section of the ingot . referring to fig1 a , 10 b , there is shown the distribution of induced currents and electromagnetic forces inside the liquid portion of the ingot ( a diameter of the liquid portion being 50 mm and an ingot cross section being 178 × 178 mm ). referring to fig1 a , there is shown the distribution of the induced current in the ingot cross section , when the cast ingot has a perfect galvanic contact with elements of the casting arc and does not have a good galvanic contact with elements of the casting arc within the stirrer referring to fig1 b , there is shown the distribution of the lorenz forces in the ingot cross section , when the cast ingot has a perfect galvanic contact with elements of the casting arc within the stirrer and does not have a good galvanic contact with elements of the casting arc within the stirrer . the case of absence of galvanic contact with elements of the casting arc is similar to an open secondary circuit of transformer ( no current in the secondary winding ) or regular regime of asynchronous motor with a massive rotor — the electromagnetic force equals to zero in the ingot center . the case when ingot has a good galvanic contact with elements of the casting arc before and after the stirrer is similar to a shorted secondary circuit of a transformer — the induced current flows in the same direction though the ingot cross section , including the center of ingot . in this case the electromagnetic force in the billet center does not equal zero , and the level of electromagnetic forces is sufficiently higher than in the case of an “ open circuit ”. this results in a the motion of molten steel in the ingot center , because of the radial component of the electromagnetic force . referring to fig1 , there is shown how the stirring occurs between the line - line or line - final stirrers . if two similar line stirrers 6 , or two line stirrers 6 and one final stirrer 7 are installed on the strand in any combination , and the ingot has a perfect galvanic contact with the casting arc before and after the stirrer groups , induced currents from each of the stirrers join together and obtain a revolving component relative to the ingot axis because of the current induced from the revolving magnetic flux . interaction of current elements of the above - mentioned revolving loop that flows in the solid ( periphery ) and liquid ( central ) portion of the billet leads to the creation of electromagnetic torque inside the liquid ( central ) portion of the ingot . so the induced currents revolve with the same frequency as the magnetic flux in the inductors of each stirrer and puts the liquid portion of the ingot in rotation . the resulting electromagnetic torque and rotational motion of the molten steel occur in the central portion of ingot between the stirrers independent of a distance between them . another case of motion of molten steel on the solidification front is the existence here of induced current that concentrates on the apexes of dendrites having higher electric conductivity then liquid steel . here at the dendrites apexes thanks to interaction of mentioned induced currents with own magnetic field the local electro - vortex flows appear . referring to fig1 a , 12 b and 12 c , there is shown how a cross ( relatively ingot axis ) motion of molten steel occurs in the liquid portion of the ingot between the line - line or line - final stirrers . if the inductor 15 and saddle coil 14 of a first neighbor stirrer , installed on the strand , connected to a two - phase voltage system , for example to phases a and b or to three phase voltage system a , b , and c , and the inductor 15 and saddle coil 14 of a second neighbor stirrer , installed on the strand , connected to next two b , a voltage phases if two phase voltage system , and to next b , c , and a if the three phase voltage system . resulting , the loop of induced currents in the ingot is twisting , see fig1 a , obtaining a helical component . the twisting current , flowing inside the solid portion of the ingot along its axis , creates a magnetic flux , shown in fig1 b , that induces the current inside the liquid portion of the ingot . as a result of the helical current component and the radial component of the magnetic induction , the axial component of the electromagnetic force and the longitudinal motion of the molten steel occur simultaneously with a revolving motion , see fig1 c . referring to fig1 a and 14b , there is shown the stirring velocities in the liquid portion of the steel ingot in different cross sections of the ingot in the middle of line / final stirrer ( fig1 a ) and between neighbor line stirrers ( fig1 b ). the stirring effect between stirrers remains strong and the maximum velocity decreases only 28 % comparatively with the stirrer center . the direction of longitudinal flow of the molten metal depends from sequence of phases of the connection to electric network . referring to fig1 a - 13c , there is shown the electric schemes coils connections to the single or three phase voltage system of network frequency , when the line or final electromagnetic unit is employed in the present invention . by this phenomenon , the molten steel in the center portion of the molten pool is stirred sufficiently enough to cause a uniform temperature distribution in the interdendritic space which produces a broad equiaxed crystal zone , and , in contrast to the conventional stirring , the conditions of segregation are absent , so a white band in such a distinctive form as would result from conventional stirring does not appear . the electromagnetic stirring method of the invention was analyzed in comparison with a conventional method in a continuous casting process of 0 . 58 % c steel of a composition containing 1 . 58 % si , 0 . 8 % mn , 0 . 025 % p , 0 . 02 % s , and 0 . 032 % al . the steel continuously cast by a bloom caster , has an ingot size of 300 × 400 mm in section , with a casting speed of 1 . 25 m / min and superheated to 50 ° c . for the molten steel in the tundish . the mold electromagnetic stirrer is affected at the poly - harmonic current having a low frequency component f = 3 hz and current amplitude 275 a , and high frequency components of 13 hz , current amplitude 200 a , reverse phase sequence . for comparison , the same in - mold electromagnetic stirrer is affected at the mono - harmonic current , having frequency 5 hz and the same current amplitude 275 a . the range of flux density of the magnetic field in the molten steel remains very similar but the distribution of it is significantly different , resulting in the rotational velocity of the molten steel ( responses for intensity of inclusions entrapping ) decreases from 0 . 52 m / sec to 0 . 35 m / sec . thanks to the vibration of the meniscus edges the mold powder supply into the gap between the ingot and the mold increases on average 15 % and the thickness of slag layer increases 15 %. thanks to the increase in the thickness of the slag layer and the thermal resistance of it , the point of initial solidification lowers on average about 3 - 4 mm and an apex of a solid shell does touch the slag ring located on the internal mold wall above the meniscus . this results in that the shell edges do not bend and oscillation marks at the lateral surface of ingot are greatly reduced . thanks to the high frequency component of the magnetic flux and the resultant edge effect at the outlet of the mold , the rotation of molten steel remains and is intensive downstream of the mold to a distance of 1 meter instead of a distance of 0 . 4 meter when the coils of stirrer energize with a monoharmonic current of frequency 5 hz . thanks to the pulse magnetic pressure in the mold the melt motion appears downstream of the mold , the temperature difference between the solid and liquid phases of the ingot decreases and this prevents columnar crystals from growing and further prevents segregation . therefore , the white bands do not develop because the columnar crystals did not grow .