US1839802A - Electric induction furnace - Google Patents

Electric induction furnace Download PDF

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Publication number
US1839802A
US1839802A US438967A US43896730A US1839802A US 1839802 A US1839802 A US 1839802A US 438967 A US438967 A US 438967A US 43896730 A US43896730 A US 43896730A US 1839802 A US1839802 A US 1839802A
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Prior art keywords
charge
coil
turns
stirring
induction furnace
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Expired - Lifetime
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US438967A
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Northrup Edwin Fitch
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Ajax Electrothermic Corp
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Ajax Electrothermic Corp
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Priority to US438967A priority Critical patent/US1839802A/en
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    • HELECTRICITY
    • H05ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05BELECTRIC HEATING; ELECTRIC LIGHT SOURCES NOT OTHERWISE PROVIDED FOR; CIRCUIT ARRANGEMENTS FOR ELECTRIC LIGHT SOURCES, IN GENERAL
    • H05B6/00Heating by electric, magnetic or electromagnetic fields
    • H05B6/02Induction heating
    • H05B6/36Coil arrangements
    • H05B6/367Coil arrangements for melting furnaces

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  • My invention relates to methods and apparatus for the control of stirring in a coreless induction furnace.
  • a purpose of my invention is to concentrate the number of ampere turns per unit axial dimension applied to one portion of the charge with respect to that a plied to another portion of the charge, an so regulate the stirringin the charge.
  • a further purpow is to grade the inductor coil of an induction furnace, and to utilize the graded coil to control the stirring of the charge.
  • a furthero purpose is to concentrate the number of inductor coil turns at either or both extremities of the coil and to selectively control the stirring in the charge by the use of an inductor coil so graded as desired.
  • a further purpose is to space from center to center certains turns of a continuous conductor forming an inductor coil relatively closely with respect to the spacing of other turns of the same inductor.
  • a further purpose is to form an inductor coil'of hollow water-cooled tubing, and to flatten the tubing parallelto the coil axis where the turns are to be spaced close together, transversely to the axis where the turns are to be spaced far apart, and to leave the tubing round or partially flattened 'as desired with progressive or abrupt transitions between these two extremes.
  • e point of high concentration is arbitrarily referred to by me as the point toward which the coil is graded.
  • stirring produced is proportional to the square of the number of ampere turns per unit axial dimension in the inductor coil. I have discovered that by concentrating a high number of ampere turns per unit axial dimension at one point alon the inductor coil, and-nsin a lower number 0 ampere turns per unit axi dimension in other parts of the coil, I may produce very fyzlr-l'olrxlounced effects upon the stirring in the ace.
  • Figures 1, 2 and 3 are dia atic sectionsof m ace provided with various to any two of the.
  • Figures 4 and 5 are axial sections showing slightly di ferent forms of my invention suited forwater-cooling.
  • the crucible 20 holds a charge 21 which in the illustrations is assumed to be molten.
  • the inductor coil is graded (i. e., has its turns closer together from the center of one to the center of the next) from the point 22 of low concentration at the bottom of the coil to the oint 23 of high concentration at the top of t e coil.
  • the turns are concentrated at the point 23 at or near the bottom of the coil, while the turns are relatively far apart at the point 22 at or near the top. Intermediate turns are graded from one extremity to the other.
  • the furnace of Figure 2 would then be desirable to heat a charge which should be protected from the atmosphere or in which top stirring would be injurious, as for example a charge containing a high carbon content, where a high carbon content is desired in the final product.
  • the inductor coil is desirably formed of hollow water-cooled tubing, initially round as seen in 30, and fiattened in a direction parallel to the axis as at intermediate turns between 30 and 31 and between 30 and 32 are somewhat less flattened in the respective directions.
  • the ampere turns per unit axial dimension are very low and at 31 very high.
  • the furnaces of Figures 4 and 5 are provided with heat insulation at 33, and are mounted on bases at 34.
  • the furnace of Figure 5 has its inductor coil graded in the opposite direction from that of Figure 4, so that the point of maximum ampere turn concentration will be at the bottom at 31, the point of minimum ampere turn concentration at the top at 32 and the intermediate point 3.0 will lie between.
  • inductor coils may be wound to provide variant numbers of turns per unit axial length at various variously arranged along the coil length, r
  • a source of current and an inductor coil supplied with current from the source, surrounding the charge and having the distance between its turns progressively increasing from a minimum about the bottom of the charge to a maximum about the top of the charge.
  • a source of current and an inductor coil supplied with current from the source, surrounding the charge and having the spacing of its turns progressively decreased from a maximum about the bottom of the charge to a minimum about the top of the charge.

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  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • General Induction Heating (AREA)

Description

Jan. 5, 1932. E. F. NORTHRUP ELECTRIC INDUCTION FURNACE Filed llaich 2a, 1930 2 Sheets-Sheet 'llllII/IIIIll/I/ fllllllllllllllll .IIIIIIIIIIIIII Jan. 5, 1932. E. F. NORTHRUP ELECTRIC INDUCTION FURNACE Filed March 26, 1930 2 Sheets-Sheet 2 Patented Jan. 5, 1 932 UNITED STATES PATENT OFFICE xnwm rrrcn 1103mm, or rnmcn'rou, NEW mam, assreuon 'ro aux mmcrno- THER'MIO CORPORATION, 01? JERSEY AJAX PARK, NEW JERSEY, A CORPORATION 01 m ELEUI'BIC INDUCTION FURNACE 'Applicatlon filed Iarah 28, 1980'. Serial Io. 438,887.
My invention relates to methods and apparatus for the control of stirring in a coreless induction furnace.
A purpose of my invention is to concentrate the number of ampere turns per unit axial dimension applied to one portion of the charge with respect to that a plied to another portion of the charge, an so regulate the stirringin the charge. Y
A further purpow is to grade the inductor coil of an induction furnace, and to utilize the graded coil to control the stirring of the charge.
A furthero purpose is to concentrate the number of inductor coil turns at either or both extremities of the coil and to selectively control the stirring in the charge by the use of an inductor coil so graded as desired.
A further purpose is to space from center to center certains turns of a continuous conductor forming an inductor coil relatively closely with respect to the spacing of other turns of the same inductor.
. A further purpose is to form an inductor coil'of hollow water-cooled tubing, and to flatten the tubing parallelto the coil axis where the turns are to be spaced close together, transversely to the axis where the turns are to be spaced far apart, and to leave the tubing round or partially flattened 'as desired with progressive or abrupt transitions between these two extremes. Further purposes will appear in the specification and in the claims.
. I intend the present application to include number of turns per unit of axial dimension is increased at one point along the II with respect to that at another point. e point of high concentration is arbitrarily referred to by me as the point toward which the coil is graded.
typesofin uctorcoil.
Ordinarily in inductor coils according to my invention the number of turns, r unit axial dimension between any two ar itrarily chosen points will progressively change from that in the neighborhood of one point to that in the neighborhod of the other pint.
It has previously been proposed to control the stirring in a coreless induction furnace by physically elevating or lowering the inductor coil. This I consider undesirable at times because of the mechanism r uired. It has further been suggested that t e inductor coil be provided with taps, and the power current be connected selectivel taps at a chosen heig t on the furnace .in
order to regulate the stirring. This structure is limited in utility because the idle portions of the inductor coil will be heated by the flux from the live portions of the coil, thus wasting energy and cooling capacity. Further more, tapping the coil is expensive and sometimes not otherwise wholly satisfactory.
Stirring in the coreless induction furnace is due to the combined action upon the charge .of motor effect of the inducing current upon the charge carrying the induced current and pinch effect of the secondary currentfilaments upon each other. In both cases, the
stirring produced is proportional to the square of the number of ampere turns per unit axial dimension in the inductor coil. I have discovered that by concentrating a high number of ampere turns per unit axial dimension at one point alon the inductor coil, and-nsin a lower number 0 ampere turns per unit axi dimension in other parts of the coil, I may produce very fyzlr-l'olrxlounced effects upon the stirring in the ace.
Stated in another'way, I find that chan in theefiective center of gravity of the mductor coil with r to the center of gravity of the charge tend to afiect the stirring in the charge in a very pronounced manner.
For the of clear illustration of my invention I have chosen toshow a few forms only in the drawings. 7
Figures 1, 2 and 3 are dia atic sectionsof m ace provided with various to any two of the.
Figures 4 and 5 are axial sections showing slightly di ferent forms of my invention suited forwater-cooling.
Like numerals refer to like parts throughout.
Referring to Figures 1 to 3, the same furnace and circuit connections appear throughout. I show an inductor coil 15 supplied with current from a conventional source 16 through lines 17 and 18. The power factor may be very desirably corrected, as for example by the condenser shown at 19.
The crucible 20 holds a charge 21 which in the illustrations is assumed to be molten.
In Figure 1 the inductor coil is graded (i. e., has its turns closer together from the center of one to the center of the next) from the point 22 of low concentration at the bottom of the coil to the oint 23 of high concentration at the top of t e coil.
The spacing of the turns intermediate between these points of low and hi h concentra tions varies progressively from t emaximum spacing in my most desirable form.
While progressive grading is desirable, it is not necessary, and advantage might be obtained from my invention by passing abruptly from a point of low turn concentration to a point of high concentration, or by changing the intermediate spacing according to any desired law, arithmetical or geometrical.
Since in Figure 1 the number of ampere turns per unit axial dimension is high at the top and low at the bottom of the inductor coil, the point of maximum flux density in the charge will be relatively high with respect to the osition which it would assume in an .ungra ed coil of the same size and character. As a result, the stirring in the furnace will be vigorous, and considerable arching of the top of the charge 'will be apparent, as shown from' the elevation of the meniscus 24.
' With a condition of high stirring of this type, very thorough mixing will take place in the top of the charge, and this portion of the charge will be readily exposed to the action of the atmosphere or to slagging reactions, depending upon contact of the slag with the charge. Thus, for example, carbon could be very advantageously burned off dur ing stirring of this sort.
As seen in Figure 2, the turns are concentrated at the point 23 at or near the bottom of the coil, while the turns are relatively far apart at the point 22 at or near the top. Intermediate turns are graded from one extremity to the other.-
In Figure 2 the effect of the coil will be to lower the point of maximum flux density in the charge with respect to such a point in the same character of coil ungraded. This will operate to reduce the stirring at the top .of I
the furnace, as seen by the shape of the meniscus 25. The furnace of Figure 2 would then be desirable to heat a charge which should be protected from the atmosphere or in which top stirring would be injurious, as for example a charge containing a high carbon content, where a high carbon content is desired in the final product.
In Figure 3 the coil is graded in both directions from an intermediate point 26 of low concentration to extremities 27 and 28 of high concentration. In this form there will be two points of high flux density, one relatively high and one relatively low in the charge. The effect upon the charge is to produce a condition intermediate between those seen in Figures 1 and 2, as shown by the shape of the meniscus 29. Moderate stirring will take place throughout the charge.
In Figures 4 and 5 the faces of the inductor coil turns are at all places relatively close together, but the turns are of variant widths, so that at points where high concentration of ampere turns is desired the turns will be wound very closely together, and where a low concentration iswished for it may also be obtained.
In Figures 4 and 5 the inductor coil is desirably formed of hollow water-cooled tubing, initially round as seen in 30, and fiattened in a direction parallel to the axis as at intermediate turns between 30 and 31 and between 30 and 32 are somewhat less flattened in the respective directions. Thus at 32 the ampere turns per unit axial dimension are very low and at 31 very high.
In general the stirring in Figure 4 Wlll be vigorous as in Figure 1, as shown by the meniscus 24'.
The furnaces of Figures 4 and 5 are provided with heat insulation at 33, and are mounted on bases at 34.
The furnace of Figure 5 has its inductor coil graded in the opposite direction from that of Figure 4, so that the point of maximum ampere turn concentration will be at the bottom at 31, the point of minimum ampere turn concentration at the top at 32 and the intermediate point 3.0 will lie between.
Thus the point of maximum flux densitv at the axis will be relatively low in the coil and there will be little stirring according to the principles explained in connection with Figure 2. The meniscus 25' will be relatively fiat.
It will be obvious that I may grade my inductor coil from the middle toward both extremities as shown in Figure 3, but nevertheless use hollow tubing as shown in Figures 4 and 5. According to the principles discussed this would produce a stirring efl'ect intermed into between those of Figure 4 and Figure 5. This is shown in my copendin'g applications.
Doubtless the ingenuity of the designer willsua'gest many other ways in which inductor coils may be wound to provide variant numbers of turns per unit axial length at various variously arranged along the coil length, r
without using the forms shown by me in my drawings.
I believe that the use of variant ampere turn concentrations along different points of 19 the same inductor coil which is carrying the same current throughout is broadly new, and I desire to be protected in the use of any structure embodying the same to control the stirring in the charge.
Having thus described my invention, what I claim as new and desire to secure by Letters Patent is:
1. The method of increasing the normal stirring in an electric induction furnace,
20 which consists in'passing an electric current close together at one end of the coil as compared with the spacing of the turns at the about the charge and increasing the number of ampere turns per unit axial dimension progressively from one end of the section stirred to the other.
'2. The method of increasing the normal stirring in an electric induction furnace, which consists in passing an electric current about the charge and progressivelyincreasing the number of ampere turns per unit axial dimension about the charge from a minimum about the bottom of the charge to a maximum about the top of the charge.
3. The method of decreasing the normal stirring in an electric induction furnace, which consists in passing an electric current about the charge and progressively decreasing the number of ampere turns per unit axial dimension about the charge from a maximum about the bottom of the charge to a minimum about the top of the charge.
4. In an electric induction furnace, a source of current, an inductor coil supplied with current from the source, surrounding the charge and having its turns relatively other end of the coil.
5. In an electric induction furnace, a source of current, and an inductor coil supplied with current from the source, surrounding the charge and having the distance between its turns progressively increasing from a minimum about the bottom of the charge to a maximum about the top of the charge.
6. In an electric. induction furnace, a source of current, and an inductor coil supplied with current from the source, surrounding the charge and having the spacing of its turns progressively decreased from a maximum about the bottom of the charge to a minimum about the top of the charge.
7. In an electric induction furnace, at source of current, and an inductor coil supplied with current from the source, surrounding the charge and consisting of hollow water cooled tubing edgewo'und about a portion of the charge at one end of the coil and progressively wound and fiat wound toward and at the other end of the coil.
EDWIN FITCH NORTHRUP.
US438967A 1930-03-26 1930-03-26 Electric induction furnace Expired - Lifetime US1839802A (en)

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Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2442776A (en) * 1944-11-08 1948-06-08 Thomas A Newkirk Radio-frequency choke coil
US2457179A (en) * 1945-09-18 1948-12-28 Ronay Bela Coreless induction heater and method of making same
US2515211A (en) * 1947-01-24 1950-07-18 Armstrong Cork Co Method and apparatus for dielectric heating
US2793242A (en) * 1955-09-12 1957-05-21 Asea Ab Electric furnace for the production of silicon and other materials having similar conditions of reaction
US2946834A (en) * 1955-11-25 1960-07-26 Junker Otto Method and apparatus for electric induction furnace melting
US3314670A (en) * 1963-11-15 1967-04-18 Inductotherm Corp Molten metal stirring apparatus
US3890562A (en) * 1972-11-13 1975-06-17 Gen Electric Regulated power supply utilizing a halfwave switch
EP0391067A2 (en) * 1989-04-04 1990-10-10 Leybold Aktiengesellschaft Device with a metallic crucible
US5446269A (en) * 1993-05-27 1995-08-29 Inductotherm Corp. Tubing shape, particularly for fabricating an induction coil

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2442776A (en) * 1944-11-08 1948-06-08 Thomas A Newkirk Radio-frequency choke coil
US2457179A (en) * 1945-09-18 1948-12-28 Ronay Bela Coreless induction heater and method of making same
US2515211A (en) * 1947-01-24 1950-07-18 Armstrong Cork Co Method and apparatus for dielectric heating
US2793242A (en) * 1955-09-12 1957-05-21 Asea Ab Electric furnace for the production of silicon and other materials having similar conditions of reaction
US2946834A (en) * 1955-11-25 1960-07-26 Junker Otto Method and apparatus for electric induction furnace melting
US3314670A (en) * 1963-11-15 1967-04-18 Inductotherm Corp Molten metal stirring apparatus
US3890562A (en) * 1972-11-13 1975-06-17 Gen Electric Regulated power supply utilizing a halfwave switch
EP0391067A2 (en) * 1989-04-04 1990-10-10 Leybold Aktiengesellschaft Device with a metallic crucible
US5109389A (en) * 1989-04-04 1992-04-28 Otto Stenzel Apparatus for generating an inductive heating field which interacts with metallic stock in a crucible
EP0391067B1 (en) * 1989-04-04 1996-09-11 Leybold Aktiengesellschaft Device with a metallic crucible
US5446269A (en) * 1993-05-27 1995-08-29 Inductotherm Corp. Tubing shape, particularly for fabricating an induction coil

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