Journal of Siberian Federal University. Engineering & Technologies, 2018, 11(2), 148-154
yflK 621.745:621.746:621.791
The Heating Process in an Induction Crucible Furnace and the Technology of Chromium Bronze Smelting in Order to Obtain Resistance Welding Electrodes
Sergei L. Busygin, Aleksandr M. Tokmin, Irina S. Dementeva and Vladimir S. Kazakov*
Siberian Federal University 79 Svobodny, Krasnoyarsk, 660041, Russia
Received 21.11.2017, received in revised form 20.12.2017, accepted 14.01.2018
The article describes the process of induction heating and the advantages of an induction furnace. The models of heating of the graphite crucibles and metal at different frequencies are shown. The technology of chromium bronze smelting in order to obtain cast electrodes for resistance welding is introduced in the current paper.
Keywords: induction furnace, modelling, casting, press forming, nanostructured particles, resistance welding, deterioration.
Citation: Busygin S.L., Tokmin A.M., Dementeva I.S., Kazakov V.S. The heating process in an induction crucible furnace and the technology of chromium bronze smelting in order to obtain resistance welding electrodes, J. Sib. Fed. Univ. Eng. technol., 2018, 11(2), 148-154. DOI: 10.17516/1999-494X-0018.
Процессы нагрева в индукционных тигельных печах и технология выплавки хромовой бронзы для получения электродов контактной сварки
С.Л. Бусыгин, А.М. Токмин, И.С. Дементьева, В.С. Казаков
Сибирский федеральный университет Россия, 660041, Красноярск, пр. Свободный, 79
В статье описан индукционный способ нагрева и преимущества использования индукционных печей. Построены модели нагрева графитового тигля и металла при разных частотах. Описана технология выплавки хромовой бронзы и получения литых электродов контактной сварки.
© Siberian Federal University. All rights reserved
Corresponding author E-mail address: [email protected], [email protected]
*
Ключевые слова: индукционная печь, моделирование, литье, штамповка, наноструктурированные частицы, контактная сварка, старение.
Nowadays induction crucible melting process is widely used for melting non-ferrous metals and alloys. This technology makes it possible to produce a kind of metal, which meets the demanding requirements for castings for various purposes. The process of smelting as well as the mixing of the molten metal take place inside the induction furnace, which makes it possible to maintain the temperature of the process within certain limits. Stirring and absence of the temperature differences are, as a rule, the key factors necessary for obtaining a homogeneous copper alloy with precise chemical composition. It can also ensure the repeatability of the results in the subsequent smelting processes.
The induction method of heating is the process of heating an electrically conducting object placed in an alternating magnetic field by electromagnetic induction, through heat generated in the object. The electrical energy of the alternating type transforms into electromagnetic energy, then again into electrical one, which finally converts into thermal energy [1].
An induction crucible furnace has several advantages:
1. High heating rate and, as a result, a short duration of melting.
2. Constancy of the chemical composition and weak segregation.
3. Small combustion loss of alloying elements.
4. The possibility of isolation of the furnace workspace from the external atmosphere during the melting process.
The construction of the induction c rue ible furnace is presented in Fig. 1.
The prog ram ANSYS °1. 0,c fimtcekment ceafys°t(FEA)fool,was used for modelling the process of induction heating0 of a graphite crociblh ond mftai ad diffeecnt frefuencies. This program has been popular with various rpetialitts for )he Last flutfy uoaes. The following tasks can be performed with the help of ANSYS n.O:au)ematic engineermgcakulaticns dCAE, CompoteauAidcd Engmeeain^, linear and nonhnear fimte ekmfii analysis, stationary and non-stationary spatial tasks of the mechanics
Fig. 1. Thecastingunit oftheinductioncruciblefurnace: 1-cylindricalbody; 2-hollow coppertubeinductor; 3 - refractory fcucible; 4- lining; С - rurrent-conlucting andwnter fuppfy piync; p - karliu wuol; 7 - refractory
Fig. 2. Themodel ofinduction heating of £i gr iippliite crucible and metal atafrequencyof2, 5 kHz
of deformaMe solids ond strucfueal mechamcs (includmg nonstationary geometrically and physically nonlinear problems of contaci interantion of structural elements). Other spheres include fluid mechanics, electrodynamics, accusticc and meehames oc coupled i^s^ld^.
Twi types (rf frfs^iser^cki were chossn for the analyais of the eonnection beinien the current frequencymfluence anptha heating proc;i^^t. Ai iir:^^, c mosle l cf mduction heeting of ei graphs arucible and melad at a aelalipaly ir^ev frequencn ef^^ta kHzwas made tFig. e). iat ehircase, tltcit^^e^tr^g of the metal is iniensive, becapte ehe megnatic fleca; lq laaga aod tte affect of the
induced cgarents is lnsigntfiaant, wliic;h agrees well with the visual ofaervetion of ihe melting process. The disieibution of the flux and the inductive cuntints density ceci be considered uniform thaoughout the entire cross section of the crucible at this moment. The current density is proportional to the frequency, and tha enirgy transferred to the cnicible is proportional to the sguare of the freque ncy.
The nexi model was mtde at si frequency oi 44 kHa. which ir wadelp used Os)ii tndoction heating. It is known [2] tnat as the frequency ef fhe eurre ne ihC5nasec,CУe cnetgyifHicators of heat increase as well, whereas the skin depth decreases.
At such a frequency, an intense heating of the graphite crucible occurs (Fig. 3). As the frequency increases, the electric field intensity in the crucible increases as well. However, this change is no longer directly proportional to the increase in frequency, since the magnetic field penetration through the crucible is weakened by demagnetization. As a result, when the frequency is increased, the energy transferred to the crucible increases proportionally to the square root of the frequency rather than to the square of the frequency [3]. Frequency modulation of the current was used in order to increase the mixing intensity at this frequency and ensure an even distribution of chromium particles over the volume of the melt.
It must be noted that the graphite crucible resistance increases at a frequency of 44 kHz. In this case, the process of its destruction is slower, because the amplitude of melt oscillation at the boundary with the crucible is much smaller than at a lower frequency of 2,5 kHz.
These models of induction heating of a graphite crucible at different frequencies show that when the frequency of the current increases, the heating of the crucible becomes more intense.
The technology of melting
The copper melt was obtained from the waste copper scrap of the A 1/1 type (GOST 1639-93). The mass of the metal loaded into the induction crucible furnace was 1 kilo. Melting was conducted under the 25-30 mm thick layer of charcoal, at a frequency of 44±4 kHz. The copper melt was deoxidized with phosphorus, which was added as an alloy MF 9 (GOST 4515-93) in the amount of 0,7% [4]. An alloying element in the form of a tablet (Fig. 4), consisting of 83% of PMS-1 copper powder (GOST 4960-75) and 17% of nanostructured chromium particles X99 (GOST 5905-79), was then added [5].
The mixing of the liquid metal took place under the influence of an alternating magnetic field with a frequency modulation of the current. It allowed to obtain an alloy with homogeneous chemical composition.
The technology of obtaining the resistance welding electrodes
The molten metal was poured into the matrix (Fig. 5). Then the alloy was cooled down to the temperature of 850-900 °C and the press forming of the cooling channel was performed with the help of a punch (Fig. 6). After that, the bottom of the matrix was opened and the electrode was pushed down into the cooling chamber located in the base of the press for quenching in running water [6, 7]. The obtained sample of the electrode is presented in Fig. 7.
NODAL SOLUTION
.363E-07 .002201 .004413 .006622 .008829
.001104 -003311 .005518 .007726 .009933
electromag
Fig. 3. Themodelofinduction heating; of a graphite crucible and metal at afrequencyoe44kHz
Fig. 4. An olloying elemetrt in t°re fotm of otoblet
Fig. 5.Pouringthe metalintothematrix
Fig. 6. Punchingofthecoolingchannel
Fig. 7. The obtamedsampie ofthe electrode
The electrode deterioration was carried out in a muffle furnace SNOL-1.62.5.1/11-IZ at the temperature of 450 °C for 4 hours to achieve the highest level of physical and mechanical properties
(strength and electrical conductivity) [8].
Based on the results of the research, the following conclusions can be drawn.
1) The models of induction heating of a graphite crucible at different frequencies show that when the current frequency increases, the heating of the crucible becomes more intense.
2) The use of copper tablets, which contain nanostructured particles of chromium, makes it possible to obtain an alloy with precise chemical composition, eliminating expensive and complicated operations of preparation of the Cu-Cr alloy.
3) The proposed melting technology ensures a uniform distribution of chromium in the alloy due to the use of frequency modulation of the current. It has a positive effect on the strength and electrical conductivity properties of the electrodes.
4) This technology enables to produce resistance welding electrodes from secondary raw materials, which reduces the final cost of the product.
Reference
[1] Фарбман С.А., Колобнев И.Ф. Индукционные печи для плавки металлов и сплавов. М.: Металлургия, 1968. 496 с. [Farbman S.A., Kolobnev I.F. Induction furnaces for melting metals and alloys. Moscow, Metallurgiia, 1968, 496 p. (in Russian)]
[2] Слухоцкий А.Е., Рыскин С.Е. Индукторы для индукционного нагрева. Л.: Энергия, 1974, 264 с. [Slukhotskii A.E., Ryskin S.E. Inductors for induction heating. Leningrad, Energiia, 1974, 264 p. (in Russian)]
[3] Шамов А.Н., Бодажков В.А. Проектирование и эксплуатация высокочастотных установок. Л.: Машиностроение, 1974. 280 с. [Shamov A.N., Bodazhkov V.A. Design and operation of high-frequency installations. Leningrad, Mashinostroenie, 1974, 280 p. (in Russian)]
[4] Ватрушин Л.С., Осинцев В.Г., Козырев А.С. Бескислородная медь. М.: Металлургия, 1982. 192 с. [Vatrushin L.S., Osintsev V.G., Kozyrev A.S. Oxygen-free copper. Moscow, Metallurgiia, 1982, 192 p. (in Russian)]
[5] Бусыгин С.Л., Синичкин А.М., Токмин А.М. Получение электродов контактной сварки совмещенным способом литья и штамповки. Металлургия машиностроения, 2013, 2, 39-43. [Busygin S.L., Sinichkin A.M., Tokmin A.M. Obtainment of resistance welding electrodes by a combined method of casting and stamping. Metallurgiia mashinostroeniia, 2013, 2, 39-43 (in Russian)]
[6] Бусыгин С.Л., Рукосуев А.П., Крушатина С.К., Демченко А.И., Рафальский А.С. Применение ресурсосберегающей технологии металлургической переработки меди и медных сплавов для получения электродов контактной сварки. Вестник СибГАУ, 2010, 6, 119-121. [Busygin S.L., Rukosuev A.P., Krushatina S.K., Demchenko A.I., Rafalskii A.S. The use of resource-saving technology of metallurgical processing of copper and copper alloys for obtaining resistance welding electrodes. VestnikSibGAU, 2010, 6, 119-121 (in Russian)]
[7] Бусыгин С.Л., Демченко А.И., Рафальский А.С. Способ изготовления электродов для контактной сварки. Патент РФ №2412035. Бюллетень №5, 2011 [Busygin S.L., Demchenko A.I.,
Rafalskii A.S. A method of manufacturing electrodes for resistance welding. Patent of the Russian Federation №2412035. Bulletin 5, 2011 (in Russian)]
[8] Николаев А.К., Новиков А.И., Розенберг В.М.Хромовые бронзы. М.: Металлургия, 1983. 176 с. [Nikolaev A.K., Novikov A.I., Rozenberg V.M. Chromium bronze. Moscow, Metallurgiia, 1983, 176 p. (in Russian)]