WO2019140819A1 - Method for designing electrode diameter and furnace shell shape of two-phase direct-current (dc) fused magnesia furnace - Google Patents

Method for designing electrode diameter and furnace shell shape of two-phase direct-current (dc) fused magnesia furnace Download PDF

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WO2019140819A1
WO2019140819A1 PCT/CN2018/087696 CN2018087696W WO2019140819A1 WO 2019140819 A1 WO2019140819 A1 WO 2019140819A1 CN 2018087696 W CN2018087696 W CN 2018087696W WO 2019140819 A1 WO2019140819 A1 WO 2019140819A1
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arc
anode
cathode
voltage
molten pool
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PCT/CN2018/087696
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French (fr)
Chinese (zh)
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张颖伟
鹿雪文
刘建昌
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东北大学
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F27FURNACES; KILNS; OVENS; RETORTS
    • F27BFURNACES, KILNS, OVENS, OR RETORTS IN GENERAL; OPEN SINTERING OR LIKE APPARATUS
    • F27B3/00Hearth-type furnaces, e.g. of reverberatory type; Tank furnaces
    • F27B3/08Hearth-type furnaces, e.g. of reverberatory type; Tank furnaces heated electrically, with or without any other source of heat
    • F27B3/085Arc furnaces
    • CCHEMISTRY; METALLURGY
    • C25ELECTROLYTIC OR ELECTROPHORETIC PROCESSES; APPARATUS THEREFOR
    • C25CPROCESSES FOR THE ELECTROLYTIC PRODUCTION, RECOVERY OR REFINING OF METALS; APPARATUS THEREFOR
    • C25C3/00Electrolytic production, recovery or refining of metals by electrolysis of melts
    • C25C3/04Electrolytic production, recovery or refining of metals by electrolysis of melts of magnesium
    • CCHEMISTRY; METALLURGY
    • C25ELECTROLYTIC OR ELECTROPHORETIC PROCESSES; APPARATUS THEREFOR
    • C25CPROCESSES FOR THE ELECTROLYTIC PRODUCTION, RECOVERY OR REFINING OF METALS; APPARATUS THEREFOR
    • C25C7/00Constructional parts, or assemblies thereof, of cells; Servicing or operating of cells
    • CCHEMISTRY; METALLURGY
    • C25ELECTROLYTIC OR ELECTROPHORETIC PROCESSES; APPARATUS THEREFOR
    • C25CPROCESSES FOR THE ELECTROLYTIC PRODUCTION, RECOVERY OR REFINING OF METALS; APPARATUS THEREFOR
    • C25C7/00Constructional parts, or assemblies thereof, of cells; Servicing or operating of cells
    • C25C7/005Constructional parts, or assemblies thereof, of cells; Servicing or operating of cells of cells for the electrolysis of melts
    • CCHEMISTRY; METALLURGY
    • C25ELECTROLYTIC OR ELECTROPHORETIC PROCESSES; APPARATUS THEREFOR
    • C25CPROCESSES FOR THE ELECTROLYTIC PRODUCTION, RECOVERY OR REFINING OF METALS; APPARATUS THEREFOR
    • C25C7/00Constructional parts, or assemblies thereof, of cells; Servicing or operating of cells
    • C25C7/02Electrodes; Connections thereof
    • C25C7/025Electrodes; Connections thereof used in cells for the electrolysis of melts
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F27FURNACES; KILNS; OVENS; RETORTS
    • F27DDETAILS OR ACCESSORIES OF FURNACES, KILNS, OVENS, OR RETORTS, IN SO FAR AS THEY ARE OF KINDS OCCURRING IN MORE THAN ONE KIND OF FURNACE
    • F27D11/00Arrangement of elements for electric heating in or on furnaces
    • F27D11/08Heating by electric discharge, e.g. arc discharge
    • F27D11/10Disposition of electrodes
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02PCLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
    • Y02P10/00Technologies related to metal processing
    • Y02P10/25Process efficiency

Definitions

  • the invention belongs to the technical field of industrial electrolytic molten magnesia extraction magnesia crystal, and particularly relates to a method for designing a pole center distance and a furnace shell shape for a two-phase direct current magnesium melting furnace.
  • the existing three-phase AC fused magnesium furnace in Liaoning Republic generally has a capacity of about 10 tons.
  • the furnace type has a slender cylindrical shape and the transformer capacity is generally above 1000kVA, with an annual output of no more than 2,000 tons.
  • the existing electric furnace transformer needs to work at full power for about 10 hours to complete the heating task.
  • the electric furnace transformer often works in an overload state, and according to statistics, the average overload reaches 1.62 times.
  • Long-term overload operation of the transformer shortens the service life of the transformer and reduces the electrical efficiency of the system.
  • Due to the limitation of the output capacity of the transformer the effective heating space of the arc is small, and it must be matched with an elongated cylindrical furnace body.
  • the maximum heating temperature of the electric arc furnace of this structure is limited, and the purification process of the raw material cannot be sufficiently performed, and the purity and density of the product are low. Due to the long heating time, the carbon pollution caused by the arc is also serious.
  • the existing three-phase AC fused magnesium furnace expands the problem of the AC arc heating technology itself when the capacity is expanded.
  • the main problems are as follows:
  • Three-phase AC fused magnesium furnace is a typical multi-input and multi-output three-phase coupling system with nonlinear, time-varying and distributed parameters. It has the following characteristics: high order, which is described by a simplified mathematical model. At the end of the system, it can reach more than 20 orders; strong nonlinearity, AC arc resistance has strong nonlinearity; disturbance is complex, large-scale disturbance and randomness coexist, and this disturbance exists in the system, non-plus Sexual; strong coupling, the main circuit of the three-phase fused magnesium furnace has strong coupling, so that the change of the arc length of any phase can simultaneously cause the change of the effective value of the three-phase arc AC; the rapidity of the adjustment process, a certain When the phase electrode is short-circuited, the electrode regulator must adjust the electrode to the proper position in time, usually from a few seconds to a few seconds. For such complex systems, conventional control effects are less than ideal and new control strategies must be sought.
  • the present invention provides a use The design method of the center distance and furnace shape of the two-phase direct current magnesium melting furnace.
  • a method for designing a pole center distance and a furnace shell shape for a two-phase direct current magnesium melting furnace comprising:
  • the shape of the furnace shell is determined according to the arc power distribution under the influence of the cathode and the anode and the obtained pole center distance.
  • the specific method for determining the arc power distribution under the influence of the cathode and the anode on the surface of the molten pool includes:
  • the cathode arc length and the anode arc length are obtained according to the voltage across the arc, the cathode cutoff voltage, and the anode cutoff voltage;
  • the method of calculating the cathode cutoff voltage and the anode cutoff voltage is as follows:
  • the cathode cut-off voltage and the anode cut-off voltage were calculated based on the equivalent voltage drop of the electron thermal energy in the cathode region and the equivalent electronic pressure drop of the anode region.
  • the method for solving the arc power is as follows:
  • the arc power P 1 (U d -RI d '-r 3 I d '-U jz1 -U jz2 )I d ' is obtained, and U jz1 is the cathode cutoff voltage U jz2 is the anode cutoff voltage.
  • U d is the rectifier output voltage
  • I d ' is the DC current when the arc power P 1 is maximum when the output voltage of the rectifier is known
  • R is the sum of the resistance of the two electrodes and the short grid resistance
  • r 3 is the bath resistance
  • U jz1 is the cathode cut-off voltage
  • U jz2 is the anode cut-off voltage.
  • l 1 is the length of the cathodic arc
  • l 2 is the length of the anode arc
  • U jz1 is the cathode cutoff voltage
  • U jz2 is the anode cutoff voltage
  • U c is the voltage across the arc
  • b is the arc voltage coefficient.
  • the method for determining the arc power distribution of the surface of the molten pool under the influence of the cathode and the arc power distribution of the surface of the molten pool under the influence of the anode are as follows:
  • the heating heat flow distribution of the arc on the surface of the molten pool is regarded as a normal distribution, and the heating heat flow distribution is expressed as Where q max is the maximum heat flow at the center of the heated spot, r is the distance from any point on the surface of the molten pool to the center of the heated spot, and ⁇ is the coefficient of thermal energy concentration;
  • the straight line of the coordinate line of the center line of the two electrodes is the horizontal axis of the coordinate line
  • the straight line of the center line of the two electrodes is the vertical axis of the coordinate axis
  • the axis of the center of the anode is the positive direction of the horizontal axis
  • the arc power distribution of the surface of the molten pool under the influence of the cathode and the anode is the sum of the arc power distribution of the surface of the molten pool under the influence of the cathode and the arc power distribution of the surface of the molten pool under the influence of the anode.
  • ⁇ 1 is the heat dissipation efficiency
  • ⁇ 2 is the proportion of heat preservation heat energy
  • q is the product energy consumption of magnesite as raw material
  • is the density of fused magnesia
  • h is the crystal height
  • P 1 is the arc power.
  • the method for determining the shape of the furnace shell includes:
  • the equal power line on the surface of the molten pool is drawn; the shape of the shell is determined according to the equal power line around the surface of the bath.
  • the invention analyzes the operating state and electrical composition of the two-phase direct current fused magnesium furnace, and can effectively calculate the pole center distance and the shape of the furnace shell satisfying the optimal operating state of the two-phase direct current magnesium melting furnace, and can be in the industrial production process. Effectively reduce the loss of materials and electrical energy.
  • 1 is a schematic structural view of a two-phase direct current fused magnesium furnace system according to an embodiment of the present invention; wherein 1-transformer, 2-short mesh, 3-rectifier, 4-electrode, 5-furnace shell, 6-car, 7- Electrode holder, 8-arc, 9-melt pool;
  • Figure 2 shows the static volt-ampere characteristics of a DC arc.
  • the abscissa is the current and the ordinate is the voltage.
  • the current is in the range 0-A
  • the voltage decreases with the increase of the current, which is the falling region.
  • the current is in A ⁇ In the B interval, the voltage does not change with the increase of the current, and is a horizontal region.
  • the current is greater than B, the voltage increases with the increase of the current, and is a rising region;
  • FIG. 3 is a schematic diagram of heat source distribution of arc electric heating on the surface of the molten pool, wherein the abscissa indicates the surface of the molten pool, and the ordinate indicates the electrode;
  • Figure 4 is an equivalent circuit diagram of a two-phase DC fused magnesium furnace, where U d is the DC voltage output from the rectifier, R is the sum of the resistance of the two electrodes and the short grid resistance, U jz1 , U jz2 are the arc cathode and anode cutoff respectively The voltage, r 1 , r 2 are the cathode and anode arc resistance, respectively, and r 3 is the bath resistance;
  • Figure 5 is a graph showing the relationship between arc power and rectifier output current
  • Figure 6 is an approximate view of the surface of the molten pool
  • Figure 7 is a graph showing the arc power distribution on the surface of the molten pool.
  • a method for designing a pole center distance and a furnace shell shape for a two-phase direct current magnesium melting furnace comprising:
  • Step 1 Design a structure of a two-phase direct current molten magnesium furnace system
  • the structure of the two-phase direct current fused magnesium furnace system in the present embodiment is as shown in FIG. 1.
  • the transformer 1, the short net 2, and the rectifier 3 are sequentially connected, the rectifier 3 is connected to the two electrodes 4, and the electrode 4 is sandwiched by the electrode holder 7.
  • the two electrodes 4 are inserted into the molten pool 9 in the furnace shell 5 of the two-phase direct current fused magnesium furnace carried by the carriage 6, and an arc 8 is generated.
  • the control system of the two-phase DC fused magnesium furnace system comprises: a power module, a voltage and current detecting device, a central controller, an amplifying actuator, and a pulse trigger.
  • the power module mainly includes: a transformer 1, a rectifier 3, an isolating switch, and a circuit breaker.
  • Step 2 obtaining an arc power distribution under the influence of the cathode and the anode on the surface of the molten pool;
  • the specific method for determining the arc power distribution under the influence of the cathode and the anode on the surface of the molten pool includes:
  • Step 2.1 calculating a cathode cutoff voltage and an anode cutoff voltage according to an equivalent voltage drop of the electron energy in the cathode region and an equivalent voltage drop of the electron energy in the anode region;
  • the method of calculating the cathode cutoff voltage and the anode cutoff voltage is as follows:
  • Step 2.1.1 Calculate the equivalent voltage drop of the electron energy in the cathode region and the equivalent pressure drop of the electron heat in the anode region according to the temperature at the heating spot of the electrode;
  • the equivalent pressure drop of the electron thermal energy in the cathode region and the calculation formula of the equivalent thermal pressure drop of the electron thermal energy in the anode region are adopted.
  • UT is the equivalent voltage drop
  • k is a constant
  • k 1.38*10 ⁇ -23
  • T is the temperature at the heating spot
  • the temperature of the cathode heating electrode spot is about
  • Step 2.1.2 calculate the cathode cut-off voltage and the anode cut-off voltage according to the equivalent voltage drop of the electron thermal energy in the cathode region and the equivalent electronic pressure drop of the anode region.
  • the current is in the I c >B segment shown in Figure 2, and the voltage corresponding to the point B is called the cut-off voltage.
  • the cathode cut-off voltage U jz1 U 1 - U T1
  • Step 2.2 Find the arc power and the voltage across the arc
  • the method for solving the arc power is as follows:
  • both electrodes are 1 m long and have a diameter
  • the relationship between the arc power and the rectifier output current as shown in FIG. 5 is plotted in the case where the rectifier output voltage U d is different (80 V, 100 V, 120 V, respectively), and the rectifier is known.
  • the output voltage U d 120V
  • the DC current when the arc power P 1 is maximized is obtained. It can be seen from Fig. 5 that the arc power P 1 is the largest when the two-phase DC fused magnesium furnace reaches this current I d ' during constant current operation.
  • U d is the rectifier output voltage
  • I d ' is the DC current when the arc power P 1 is maximum when the output voltage of the rectifier is known
  • R is the sum of the resistance of the two electrodes and the short grid resistance
  • r 3 is the bath resistance
  • U jz1 is the cathode cut-off voltage
  • U jz2 is the anode cut-off voltage.
  • Step 2.3 determining the cathode arc length and the anode arc length according to the voltage across the arc, the cathode cutoff voltage, and the anode cutoff voltage;
  • l 1 is the length of the cathodic arc
  • l 2 is the length of the anode arc
  • U c is the voltage across the arc
  • l 1 20.56 mm
  • l 2 18.83 mm.
  • Step 2.4 Determine the arc power distribution on the surface of the molten pool under the influence of the cathode and the arc power distribution on the surface of the molten pool under the influence of the anode, and then determine the arc power distribution under the influence of the cathode and the anode on the surface of the molten pool.
  • the method for determining the arc power distribution of the surface of the molten pool under the influence of the cathode and the arc power distribution of the surface of the molten pool under the influence of the anode are as follows:
  • the heating heat flow distribution of the arc on the surface of the molten pool is regarded as a normal distribution as shown in FIG. 3, and the heating heat flow distribution is expressed as Where q max is the maximum heat flow at the center of the heated spot, r is the distance from any point on the surface of the molten pool to the center of the heated spot, and ⁇ is the coefficient of thermal energy concentration.
  • the straight line of the coordinate line of the center line of the two electrodes is the horizontal axis of the coordinate line, and the straight line of the center line of the two electrodes is the vertical axis of the coordinate axis, and the axis of the center of the anode is the positive direction of the horizontal axis, according to
  • the distribution of the arc power of a single electrode on the surface of the bath, p(r), represents the arc power distribution p 1 (x, y) of the surface of the bath under the influence of the cathode and the arc power distribution p 2 of the surface of the bath under the influence of the anode (x) , y).
  • Step 3 Determine physical parameters of the two-phase DC fused magnesium furnace system, including:
  • the expression of the surface area of the molten pool is determined: during the operation of the two-phase direct current molten magnesium furnace, the arc power P 1 mainly acts as a molten material, and the resistance of the molten pool is mainly used for heat preservation.
  • the portion of the thermal energy used to melt the material in the arc heat is referred to as the effective arc heat W.
  • the effective arc heat W The portion of the thermal energy used to melt the material in the arc heat.
  • the uppermost layer of the material in contact with the air radiates heat outward, and the heat dissipation efficiency is ⁇ 1 .
  • a small part of the arc heat is also used to heat the molten pool. This part of the heat is called thermal insulation, and its proportion is ⁇ 2 .
  • the surface area of the weld pool is determined by the law of conservation of energy:
  • q 2611 kWh / t
  • 3580 kg / m 3
  • the crystal height h is 0.2 m.
  • the expression of the surface area of the molten pool is determined: in the smelting process, if the pole center distance is too large, the maximum temperature between the two electrodes is low, resulting in an unmelted dead zone in the middle; Small, the maximum temperature between the two electrodes is too high, the temperature gradient is large, and the molten pool area is small. It can be seen that the smelting effect is best when the pole center length is exactly the melting radius of the electrode. At this time, the surface of the molten pool is approximated as shown in Fig. 6, and the expression of the surface area of the molten pool is obtained:
  • the method for determining the shape of the furnace shell includes:

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Abstract

A method for designing an electrode diameter and a furnace shell shape of a two-phase DC fused magnesia furnace, comprising: designing the structure of the two-phase DC fused magnesia furnace system; calculating an arc power distribution on the surface of a fusing pool under joint effects of a cathode and an anode; determining physical parameters of the two-phase DC fused magnesia furnace system, comprising calculating the electrode diameter; and determining the furnace shell shape according to the arc power distribution on the surface of the fusing pool under the joint effects of the cathode and the anode and the calculated electrode diameter. Analyzing the operating state and electrical configuration of the two-phase DC fused magnesia furnace, enables effective calculation of an electrode diameter and a furnace shell shape that satisfy an optimal operating state of the two-phase DC fused magnesia furnace, thereby effectively reducing the consumption of materials and electrical energy in industrial production processes.

Description

一种用于两相直流电熔镁炉的极心距与炉壳外形设计方法Method for designing pole center distance and furnace shell shape for two-phase direct current magnesium melting furnace 技术领域Technical field
本发明属于工业电解熔融氧化镁提取氧化镁晶体技术领域,具体涉及一种用于两相直流电熔镁炉的极心距与炉壳外形设计方法。The invention belongs to the technical field of industrial electrolytic molten magnesia extraction magnesia crystal, and particularly relates to a method for designing a pole center distance and a furnace shell shape for a two-phase direct current magnesium melting furnace.
技术背景technical background
辽宁省现有的三相交流电熔镁炉容量一般在10吨上下,炉型以细长圆柱形为主变压器容量一般在1000kVA上下,年产不超过2000吨。按熔坨质量占总料的40%计算,现有的电炉变压器需要全功率工作10小时左右才能完成加热任务。电炉变压器常常工作在过载状态,据统计平均过载到达1.62倍。变压器长期超载运行,缩短了变压器的使用寿命,降低了系统的电效率。而受到变压器输出容量的限制,电弧的有效加热空间小,必须配合以细长圆柱形炉体。这种结构的电弧炉的最高加热温度有限,造成原料的纯化过程无法充分进行,产品的纯度和密度低。由于加热时间长,电弧造成的碳污染也较为严重。The existing three-phase AC fused magnesium furnace in Liaoning Province generally has a capacity of about 10 tons. The furnace type has a slender cylindrical shape and the transformer capacity is generally above 1000kVA, with an annual output of no more than 2,000 tons. According to the melting mass accounting for 40% of the total material, the existing electric furnace transformer needs to work at full power for about 10 hours to complete the heating task. The electric furnace transformer often works in an overload state, and according to statistics, the average overload reaches 1.62 times. Long-term overload operation of the transformer shortens the service life of the transformer and reduces the electrical efficiency of the system. Due to the limitation of the output capacity of the transformer, the effective heating space of the arc is small, and it must be matched with an elongated cylindrical furnace body. The maximum heating temperature of the electric arc furnace of this structure is limited, and the purification process of the raw material cannot be sufficiently performed, and the purity and density of the product are low. Due to the long heating time, the carbon pollution caused by the arc is also serious.
现已认识到,为系统配备高容量的电炉变压器是提高产量和质量的前提。提高熔炼系统的单位功率能够显著缩短熔炼时间,大幅度提高生产率。另外,提高功率密度还可以提高电弧的熔炼温度和能量效率。It has been recognized that the provision of high capacity electric furnace transformers for systems is a prerequisite for increased throughput and quality. Increasing the unit power of the smelting system can significantly shorten the smelting time and greatly increase productivity. In addition, increasing the power density can also increase the melting temperature and energy efficiency of the arc.
现有的三相交流电熔镁炉在容量扩大时会使交流电弧加热技术本身的问题扩大化,主要问题如下:The existing three-phase AC fused magnesium furnace expands the problem of the AC arc heating technology itself when the capacity is expanded. The main problems are as follows:
(1)交流电弧每秒过零点100次到120次,在零点附近电弧熄灭,然后在下半周重新点弧,因而交流电弧的稳定性差。(1) The alternating current arc crosses zero to 100 times per second, the arc is extinguished near the zero point, and then the arc is re-arced in the second half, so the stability of the alternating current arc is poor.
(2)交流系统功率因数低,无功功率频繁波动,引起电网电压闪变,需要配备昂贵的动态补偿装置。(2) The AC system has low power factor and frequent fluctuations in reactive power, causing the grid voltage to flicker and requires expensive dynamic compensation devices.
(3)三相电弧的弧长和功率的变化在时间上不一致,三相负载不对称,三项电弧功率不均衡,同时产生了炉壁热点。(3) The arc length and power variation of the three-phase arc are inconsistent in time, the three-phase load is asymmetrical, the three arc powers are unbalanced, and the furnace wall hot spot is generated.
(4)三相交流电熔镁炉是一种典型的非线性、时变和分布参数的多输入多输出的三相耦合系统,它具有以下特点:阶数高,即使用比较简化的数学模型描述,系统结束也可以达到二十多阶;强非线性,交流电弧电阻具有很强的非线性;扰动复杂,大范围的扰动及随机性并存,并且这种扰动是存在于系统内部的,是 非加和性的;强耦合性,三相电熔镁炉主电路具有很强的耦合性,使得任意相弧长的变化可以同时引起三相电弧交流有效值的变化;调节过程的快速性,某一相电极短路时,电极调节器必须及时将电极调至合适的位置,这一过程通常为零点几秒至几秒。对这样复杂的系统,常规的控制效果不太理想,必须寻找新的控制策略。(4) Three-phase AC fused magnesium furnace is a typical multi-input and multi-output three-phase coupling system with nonlinear, time-varying and distributed parameters. It has the following characteristics: high order, which is described by a simplified mathematical model. At the end of the system, it can reach more than 20 orders; strong nonlinearity, AC arc resistance has strong nonlinearity; disturbance is complex, large-scale disturbance and randomness coexist, and this disturbance exists in the system, non-plus Sexual; strong coupling, the main circuit of the three-phase fused magnesium furnace has strong coupling, so that the change of the arc length of any phase can simultaneously cause the change of the effective value of the three-phase arc AC; the rapidity of the adjustment process, a certain When the phase electrode is short-circuited, the electrode regulator must adjust the electrode to the proper position in time, usually from a few seconds to a few seconds. For such complex systems, conventional control effects are less than ideal and new control strategies must be sought.
发明内容Summary of the invention
针对到传统三相交流电熔镁炉的诸多缺点,以及现有的两相直流电熔镁炉由于极心距与炉型设计不合理,导致的电能与物料的浪费问题,本发明提供了一种用于两相直流电熔镁炉的极心距与炉壳外形设计方法。In view of the many shortcomings of the traditional three-phase alternating current fused magnesium furnace, and the existing two-phase direct current fused magnesium furnace, the problem of waste of electric energy and materials due to the unreasonable design of the center distance and the furnace type, the present invention provides a use The design method of the center distance and furnace shape of the two-phase direct current magnesium melting furnace.
本发明技术方案如下:The technical scheme of the present invention is as follows:
一种用于两相直流电熔镁炉的极心距与炉壳外形设计方法,包括:A method for designing a pole center distance and a furnace shell shape for a two-phase direct current magnesium melting furnace, comprising:
设计两相直流电熔镁炉系统的结构;Designing the structure of a two-phase direct current fused magnesium furnace system;
求得熔池表面在阴极与阳极共同影响下的电弧功率分布;Obtaining an arc power distribution under the influence of the cathode and the anode on the surface of the molten pool;
确定两相直流电熔镁炉系统的物理参数,包括:Determine the physical parameters of the two-phase DC fused magnesium furnace system, including:
求极心距;Find the center of the heart;
根据熔池表面在阴极与阳极共同影响下的电弧功率分布以及求得的极心距确定炉壳外形。The shape of the furnace shell is determined according to the arc power distribution under the influence of the cathode and the anode and the obtained pole center distance.
所述求得熔池表面在阴极与阳极共同影响下的电弧功率分布的具体方法包括:The specific method for determining the arc power distribution under the influence of the cathode and the anode on the surface of the molten pool includes:
根据阴极区电子热能的等值压降和阳极区的电子热能等值压降,计算阴极截止电压和阳极截止电压;Calculating the cathode cutoff voltage and the anode cutoff voltage according to the equivalent voltage drop of the electron energy in the cathode region and the equivalent electronic pressure drop of the anode region;
求电弧功率及电弧两端电压;Find the arc power and the voltage across the arc;
根据电弧两端电压、阴极截止电压、阳极截止电压,求出阴极电弧长度和阳极电弧长度;The cathode arc length and the anode arc length are obtained according to the voltage across the arc, the cathode cutoff voltage, and the anode cutoff voltage;
确定阴极影响下熔池表面的电弧功率分布以及阳极影响下熔池表面的电弧功率分布,进而求出熔池表面在阴极与阳极共同影响下的电弧功率分布。Determine the arc power distribution on the surface of the molten pool under the influence of the cathode and the arc power distribution on the surface of the molten pool under the influence of the anode, and then determine the arc power distribution under the influence of the cathode and the anode on the surface of the molten pool.
所述计算阴极截止电压和阳极截止电压的方法如下:The method of calculating the cathode cutoff voltage and the anode cutoff voltage is as follows:
根据电极的加热斑点处温度计算阴极区电子热能的等值压降和阳极区的电子热能等值压降;Calculating the equivalent voltage drop of the electron energy in the cathode region and the equivalent pressure drop of the electron energy in the anode region according to the temperature at the heating spot of the electrode;
根据阴极区电子热能的等值压降和阳极区的电子热能等值压降,计算阴极截止电压和阳极截止电压。The cathode cut-off voltage and the anode cut-off voltage were calculated based on the equivalent voltage drop of the electron thermal energy in the cathode region and the equivalent electronic pressure drop of the anode region.
所述电弧功率的求解方法如下:The method for solving the arc power is as follows:
根据电极尺寸及电阻率计算两根电极的电阻,同时测量短网电阻,计算出两根电极的电阻与短网电阻之和R;Calculate the resistance of the two electrodes according to the electrode size and resistivity, and measure the resistance of the short grid, and calculate the sum R of the resistance of the two electrodes and the short grid resistance;
根据熔池大小和熔池电阻率估算熔池电阻r 3Estimate the weld pool resistance r 3 according to the size of the weld pool and the resistivity of the weld pool;
在已知整流器输出电压U d时求得使电弧功率P 1最大时的直流电流I d′; Calculating a DC current I d ' when the arc power P 1 is maximum when the rectifier output voltage U d is known;
求得电弧功率P 1=(U d-RI d′-r 3I d′-U jz1-U jz2)I d′,U jz1为阴极截止电压U jz2为阳极截止电压。 The arc power P 1 =(U d -RI d '-r 3 I d '-U jz1 -U jz2 )I d ' is obtained, and U jz1 is the cathode cutoff voltage U jz2 is the anode cutoff voltage.
所述电弧两端电压采用如下公式求解:The voltage across the arc is solved by the following formula:
U c=0.5×(U d-RI d′-r 3I d′-U jx1-U jz2) U c =0.5×(U d -RI d '-r 3 I d '-U jx1 -U jz2 )
其中,U d为整流器输出电压,I d′为已知整流器输出电压时使电弧功率P 1最大时的直流电流,R为两根电极的电阻与短网电阻之和,r 3为熔池电阻,U jz1为阴极截止电压,U jz2为阳极截止电压。 Where U d is the rectifier output voltage, I d ' is the DC current when the arc power P 1 is maximum when the output voltage of the rectifier is known, R is the sum of the resistance of the two electrodes and the short grid resistance, and r 3 is the bath resistance , U jz1 is the cathode cut-off voltage, and U jz2 is the anode cut-off voltage.
所述阴极电弧长度和阳极电弧长度的计算公式分别如下:The calculation formulas of the cathode arc length and the anode arc length are as follows:
Figure PCTCN2018087696-appb-000001
Figure PCTCN2018087696-appb-000001
Figure PCTCN2018087696-appb-000002
Figure PCTCN2018087696-appb-000002
其中,l 1为阴极电弧长度,l 2为阳极电弧长度,U jz1为阴极截止电压,U jz2为阳极截止电压,U c为电弧两端电压,b为弧压系数。 Wherein l 1 is the length of the cathodic arc, l 2 is the length of the anode arc, U jz1 is the cathode cutoff voltage, U jz2 is the anode cutoff voltage, U c is the voltage across the arc, and b is the arc voltage coefficient.
所述确定阴极影响下熔池表面的电弧功率分布以及阳极影响下熔池表面的电弧功率分布的方法如下:The method for determining the arc power distribution of the surface of the molten pool under the influence of the cathode and the arc power distribution of the surface of the molten pool under the influence of the anode are as follows:
将电弧在熔池表面的加热热流分布视为正态分布,则加热热流分布表示为
Figure PCTCN2018087696-appb-000003
其中,q max为加热斑点中心的最大热流,r为熔池表面任意一点到加热斑点中心的距离,α为热能集中系数;
The heating heat flow distribution of the arc on the surface of the molten pool is regarded as a normal distribution, and the heating heat flow distribution is expressed as
Figure PCTCN2018087696-appb-000003
Where q max is the maximum heat flow at the center of the heated spot, r is the distance from any point on the surface of the molten pool to the center of the heated spot, and α is the coefficient of thermal energy concentration;
求加热斑点中心的最大热流
Figure PCTCN2018087696-appb-000004
其中Q为实际单极电弧功率在熔池表面的分布,由加热热流分布公式
Figure PCTCN2018087696-appb-000005
在加热斑点面积上进行积分得到,P 1为电弧功率;热能集中系数
Figure PCTCN2018087696-appb-000006
D为电极直径,l为电弧长度,指代阴极电弧长度或阳极电弧长度;
Find the maximum heat flow at the center of the heated spot
Figure PCTCN2018087696-appb-000004
Where Q is the distribution of the actual unipolar arc power on the surface of the molten pool, and the heating heat flow distribution formula
Figure PCTCN2018087696-appb-000005
Integrate on the heated spot area, P 1 is the arc power; thermal energy concentration factor
Figure PCTCN2018087696-appb-000006
D is the diameter of the electrode, l is the length of the arc, and refers to the length of the cathodic arc or the length of the anode arc;
求单电极的电弧功率在熔池表面的分布;Find the distribution of the arc power of the single electrode on the surface of the molten pool;
以两个电极的中心连接线所在直线为坐标轴的横轴,以两个电极的中心连接线的中垂线所在直线为坐标轴的纵轴,以阳极中心所在轴为横轴正方向,根据单电极的电弧功率在熔池表面的分布,表示出阴极影响下熔池表面的电弧功率分布以及阳极影响下熔池表面的电弧功率分布。The straight line of the coordinate line of the center line of the two electrodes is the horizontal axis of the coordinate line, and the straight line of the center line of the two electrodes is the vertical axis of the coordinate axis, and the axis of the center of the anode is the positive direction of the horizontal axis, according to The distribution of the arc power of the single electrode on the surface of the molten pool indicates the arc power distribution of the surface of the molten pool under the influence of the cathode and the arc power distribution of the surface of the molten pool under the influence of the anode.
所述熔池表面在阴极与阳极共同影响下的电弧功率分布为阴极影响下熔池表面的电弧功率分布与阳极影响下熔池表面的电弧功率分布之和。The arc power distribution of the surface of the molten pool under the influence of the cathode and the anode is the sum of the arc power distribution of the surface of the molten pool under the influence of the cathode and the arc power distribution of the surface of the molten pool under the influence of the anode.
所述极心距的计算公式如下:The formula for calculating the pole center distance is as follows:
Figure PCTCN2018087696-appb-000007
Figure PCTCN2018087696-appb-000007
其中,η 1为散热效率,η 2为保温热能所占比例,q为菱镁矿作原料时的产品单位能耗,ρ为电熔镁砂的密度,h为结晶高度,P 1为电弧功率。 Where η 1 is the heat dissipation efficiency, η 2 is the proportion of heat preservation heat energy, q is the product energy consumption of magnesite as raw material, ρ is the density of fused magnesia, h is the crystal height, and P 1 is the arc power. .
所述炉壳外形的确定方法包括:The method for determining the shape of the furnace shell includes:
根据熔池表面在阴极与阳极共同影响下的电弧功率分布以及求得的极心距,画出熔池表面的等功率线;根据熔池表面外围的等功率线,确定炉壳外形。According to the arc power distribution under the influence of the cathode and the anode and the obtained pole center distance, the equal power line on the surface of the molten pool is drawn; the shape of the shell is determined according to the equal power line around the surface of the bath.
有益效果:Beneficial effects:
本发明通过对两相直流电熔镁炉的运行状态与电气构成进行分析,能够有效地计算出满足两相直流电熔镁炉最佳运行状态的极心距与炉壳外形,能够在工业生产过程中有效地减小物料与电能的损耗。The invention analyzes the operating state and electrical composition of the two-phase direct current fused magnesium furnace, and can effectively calculate the pole center distance and the shape of the furnace shell satisfying the optimal operating state of the two-phase direct current magnesium melting furnace, and can be in the industrial production process. Effectively reduce the loss of materials and electrical energy.
附图说明DRAWINGS
图1为本发明具体实施方式中的两相直流电熔镁炉系统的结构示意图;其中1-变压器、2-短网、3-整流器、4-电极、5-炉壳、6-小车、7-电极夹、8-电弧、9-熔池;1 is a schematic structural view of a two-phase direct current fused magnesium furnace system according to an embodiment of the present invention; wherein 1-transformer, 2-short mesh, 3-rectifier, 4-electrode, 5-furnace shell, 6-car, 7- Electrode holder, 8-arc, 9-melt pool;
图2为直流电弧的静态伏安特性,其中横坐标为电流,纵坐标为电压,当电流在0~A区间时,电压随电流的增大而减小,为下降区,当电流在A~B区间时,电压基本不随电流的增大而变化,为水平区,当电流大于B时,电压随电流的增大而增大,为上升区;Figure 2 shows the static volt-ampere characteristics of a DC arc. The abscissa is the current and the ordinate is the voltage. When the current is in the range 0-A, the voltage decreases with the increase of the current, which is the falling region. When the current is in A~ In the B interval, the voltage does not change with the increase of the current, and is a horizontal region. When the current is greater than B, the voltage increases with the increase of the current, and is a rising region;
图3为电弧电热在熔池表面的热源分布示意图,其中横坐标表示熔池表面,纵坐标表示电极;3 is a schematic diagram of heat source distribution of arc electric heating on the surface of the molten pool, wherein the abscissa indicates the surface of the molten pool, and the ordinate indicates the electrode;
图4为两相直流电熔镁炉的等效电路图,其中U d为整流器输出的直流电压,R为两根电极的电阻与短网电阻之和,U jz1、U jz2分别为电弧阴极与阳极截止电压,r 1、r 2分别为阴极与阳极电弧电阻,r 3为熔池电阻; Figure 4 is an equivalent circuit diagram of a two-phase DC fused magnesium furnace, where U d is the DC voltage output from the rectifier, R is the sum of the resistance of the two electrodes and the short grid resistance, U jz1 , U jz2 are the arc cathode and anode cutoff respectively The voltage, r 1 , r 2 are the cathode and anode arc resistance, respectively, and r 3 is the bath resistance;
图5为电弧功率与整流器输出电流的关系图;Figure 5 is a graph showing the relationship between arc power and rectifier output current;
图6为熔池表面近似图;Figure 6 is an approximate view of the surface of the molten pool;
图7为熔池表面电弧功率分布图。Figure 7 is a graph showing the arc power distribution on the surface of the molten pool.
具体实施方式Detailed ways
下面结合附图对本发明具体实施方式加以详细的说明。The specific embodiments of the present invention are described in detail below with reference to the accompanying drawings.
一种用于两相直流电熔镁炉的极心距与炉壳外形设计方法,包括:A method for designing a pole center distance and a furnace shell shape for a two-phase direct current magnesium melting furnace, comprising:
步骤1、设计两相直流电熔镁炉系统的结构; Step 1. Design a structure of a two-phase direct current molten magnesium furnace system;
本实施方式中的两相直流电熔镁炉系统的结构如图1所示,变压器1、短网2、整流器3依次连接,整流器3分别连接两根电极4,电极4由电极夹7夹持,两根电极4插入由小车6承载的两相直流电熔镁炉的炉壳5内熔池9中,产生电弧8。该两相直流电熔镁炉系统的控制系统,包括:电源模块、电压电流检测装置、中央控制器、放大执行机构、脉冲触发器。其中电源模块主要包括:变压器1、整流器3、隔离开关、断路器。The structure of the two-phase direct current fused magnesium furnace system in the present embodiment is as shown in FIG. 1. The transformer 1, the short net 2, and the rectifier 3 are sequentially connected, the rectifier 3 is connected to the two electrodes 4, and the electrode 4 is sandwiched by the electrode holder 7. The two electrodes 4 are inserted into the molten pool 9 in the furnace shell 5 of the two-phase direct current fused magnesium furnace carried by the carriage 6, and an arc 8 is generated. The control system of the two-phase DC fused magnesium furnace system comprises: a power module, a voltage and current detecting device, a central controller, an amplifying actuator, and a pulse trigger. The power module mainly includes: a transformer 1, a rectifier 3, an isolating switch, and a circuit breaker.
步骤2、求得熔池表面在阴极与阳极共同影响下的电弧功率分布;Step 2: obtaining an arc power distribution under the influence of the cathode and the anode on the surface of the molten pool;
所述求得熔池表面在阴极与阳极共同影响下的电弧功率分布的具体方法包括:The specific method for determining the arc power distribution under the influence of the cathode and the anode on the surface of the molten pool includes:
步骤2.1、根据阴极区电子热能的等值压降和阳极区的电子热能等值压降,计算阴极截止电压和阳极截止电压;Step 2.1: calculating a cathode cutoff voltage and an anode cutoff voltage according to an equivalent voltage drop of the electron energy in the cathode region and an equivalent voltage drop of the electron energy in the anode region;
所述计算阴极截止电压和阳极截止电压的方法如下:The method of calculating the cathode cutoff voltage and the anode cutoff voltage is as follows:
步骤2.1.1、根据电极的加热斑点处温度计算阴极区电子热能的等值压降和阳极区的电子热能等值压降;Step 2.1.1. Calculate the equivalent voltage drop of the electron energy in the cathode region and the equivalent pressure drop of the electron heat in the anode region according to the temperature at the heating spot of the electrode;
本实施方式中,阴极区电子热能的等值压降和阳极区的电子热能等值压降的计算公式均采用
Figure PCTCN2018087696-appb-000008
其中UT为等值压降,e为电子电量e=1.602*10^-19库仑;k为常数,k=1.38*10^-23,T为加热斑点处温度,阴极的加热电极斑点处温度约为4000K,阳极的电极加热斑点处温度约为6000K。因此,可求得阴极区电子热能的等值压降U T1=0.52V,阳极区的电子热能等值压降U T2=0.78V。
In this embodiment, the equivalent pressure drop of the electron thermal energy in the cathode region and the calculation formula of the equivalent thermal pressure drop of the electron thermal energy in the anode region are adopted.
Figure PCTCN2018087696-appb-000008
Where UT is the equivalent voltage drop, e is the electron charge e=1.602*10^-19 coulomb; k is a constant, k=1.38*10^-23, T is the temperature at the heating spot, and the temperature of the cathode heating electrode spot is about At 4000K, the anode electrode heats the spot at a temperature of about 6000K. Therefore, the equivalent voltage drop U T1 =0.52V of the electron thermal energy in the cathode region can be obtained, and the electron thermal equivalent voltage drop U T2 of the anode region is 0.98V.
步骤2.1.2、根据阴极区电子热能的等值压降和阳极区的电子热能等值压降,计算阴极截止电压和阳极截止电压。Step 2.1.2, calculate the cathode cut-off voltage and the anode cut-off voltage according to the equivalent voltage drop of the electron thermal energy in the cathode region and the equivalent electronic pressure drop of the anode region.
两相直流电熔镁炉系统工作过程中,电流处于图2所示I c>B段,点B处所对应的电压称为截止电压。阴极截止电压U jz1=U 1-U T1,阳极截止电压U jz2=U 2+U T2;其中,U 1、U 2分别为阴极区压降和阳极区压降,均10V。因此,求得U jz1=9.48V,U jz2=10.78V。 During the operation of the two-phase DC fused magnesium furnace system, the current is in the I c >B segment shown in Figure 2, and the voltage corresponding to the point B is called the cut-off voltage. The cathode cut-off voltage U jz1 = U 1 - U T1 , the anode cutoff voltage U jz2 = U 2 + U T2 ; wherein U 1 and U 2 are the cathode region voltage drop and the anode region voltage drop, respectively, both being 10V. Therefore, U jz1 = 9.48V and U jz2 = 10.78V are obtained.
步骤2.2、求电弧功率及电弧两端电压;Step 2.2: Find the arc power and the voltage across the arc;
所述电弧功率的求解方法如下:The method for solving the arc power is as follows:
(a)根据电极尺寸及电阻率计算两根电极的电阻,同时测量短网电阻,计算出两根电极的电阻与短网电阻之和R;本实施方式中两根电极均为长1m、直径100mm的圆柱体石墨电极,由于石墨电阻率为1×10 -5Ω·m,因此求得单根电极的电阻为1.27mΩ,测量得到的短网电阻约为0.55mΩ,因此,两根电极的电阻与短网电阻之和R=3.09mΩ。 (a) Calculate the resistance of the two electrodes according to the electrode size and the resistivity, and measure the resistance of the short grid, and calculate the sum R of the resistance of the two electrodes and the resistance of the short grid; in the present embodiment, both electrodes are 1 m long and have a diameter The 100mm cylindrical graphite electrode has a graphite resistivity of 1×10 -5 Ω·m, so the resistance of the single electrode is 1.27mΩ, and the measured short-net resistance is about 0.55mΩ. Therefore, the two electrodes are The sum of the resistance and the short-wire resistance is R=3.09mΩ.
(b)根据熔池大小和熔池电阻率估算熔池电阻r 3(b) Estimating the weld pool resistance r 3 according to the size of the molten pool and the resistivity of the molten pool;
设熔池大小为长宽高均为200mm的立方体,熔池电阻率约为1.2×10 -3Ω·m,则熔池电阻r 3=6mΩ。 Set the size of the weld pool to a cube with a length, width and height of 200 mm. The weld pool resistivity is about 1.2 × 10 -3 Ω·m, and the weld pool resistance is r 3 = 6 mΩ.
(c)在已知整流器输出电压U d时求得使电弧功率P 1最大时的直流电流I d′; (c) determining a direct current I d ' when the arc power P 1 is maximized when the rectifier output voltage U d is known;
根据图4所示的两相直流电熔镁炉的等效电路,得出电弧功率P 1的表达式: P 1=(U d-RI d-r 3I d-U jz1-U jz2)I d,其中,U d为整流器输出电压,I d为电路电流。 According to the equivalent circuit of the two-phase DC fused magnesium furnace shown in Fig. 4, the expression of the arc power P 1 is obtained: P 1 =(U d -RI d -r 3 I d -U jz1 -U jz2 )I d Where U d is the rectifier output voltage and I d is the circuit current.
根据电弧功率P 1的表达式,在整流器输出电压U d不同(分别为80V、100V、120V)的情况下画出如图5所示的电弧功率与整流器输出电流的关系图,在已知整流器输出电压U d=120V时求得使电弧功率P 1最大时的直流电流
Figure PCTCN2018087696-appb-000009
由图5可以看出,两相直流电熔镁炉恒流运行时达到此电流I d′时,电弧功率P 1最大。
According to the expression of the arc power P 1 , the relationship between the arc power and the rectifier output current as shown in FIG. 5 is plotted in the case where the rectifier output voltage U d is different (80 V, 100 V, 120 V, respectively), and the rectifier is known. When the output voltage U d =120V, the DC current when the arc power P 1 is maximized is obtained.
Figure PCTCN2018087696-appb-000009
It can be seen from Fig. 5 that the arc power P 1 is the largest when the two-phase DC fused magnesium furnace reaches this current I d ' during constant current operation.
(d)根据电弧功率P 1的表达式,以及使电弧功率P 1最大时的直流电流I d′,求得电弧功率P 1=(U d-RI d′-r 3I d′-U jz1-U jz2)I d′=355288W。 (d) to the arc power P 1 expression, and direct current arc when the maximum power P 1 I d ', determined arc power P 1 = (U d -RI d ' -r 3 I d '-U jz1 -U jz2 )I d '=355288W.
所述电弧两端电压采用如下公式求解:The voltage across the arc is solved by the following formula:
U c=0.5×(U d-RI d′-r 3I d′-U jx1-U jz2)≈24.9V U c =0.5×(U d -RI d '-r 3 I d '-U jx1 -U jz2 )≈24.9V
其中,U d为整流器输出电压,I d′为已知整流器输出电压时使电弧功率P 1最大时的直流电流,R为两根电极的电阻与短网电阻之和,r 3为熔池电阻,U jz1为阴极截止电压,U jz2为阳极截止电压。 Where U d is the rectifier output voltage, I d ' is the DC current when the arc power P 1 is maximum when the output voltage of the rectifier is known, R is the sum of the resistance of the two electrodes and the short grid resistance, and r 3 is the bath resistance , U jz1 is the cathode cut-off voltage, and U jz2 is the anode cut-off voltage.
步骤2.3、根据电弧两端电压、阴极截止电压、阳极截止电压,求出阴极电弧长度和阳极电弧长度;Step 2.3, determining the cathode arc length and the anode arc length according to the voltage across the arc, the cathode cutoff voltage, and the anode cutoff voltage;
电弧长度计算公式为:
Figure PCTCN2018087696-appb-000010
其中b为弧压系数,弧压系数由实验确定,由文献查得b=0.75V/mm,其中的U jz为u jz1或U jz2,因此所述阴极电弧长度和阳极电弧长度的计算公式分别如下:
The arc length calculation formula is:
Figure PCTCN2018087696-appb-000010
Where b is the arc pressure coefficient, the arc pressure coefficient is determined experimentally, and b=0.75V/mm is found in the literature, where U jz is u jz1 or U jz2 , so the calculation formulas of the cathodic arc length and the anode arc length are respectively as follows:
Figure PCTCN2018087696-appb-000011
Figure PCTCN2018087696-appb-000011
Figure PCTCN2018087696-appb-000012
Figure PCTCN2018087696-appb-000012
其中,l 1为阴极电弧长度,l 2为阳极电弧长度,U c为电弧两端电压, l 1=20.56mm,l 2=18.83mm。 Wherein l 1 is the length of the cathodic arc, l 2 is the length of the anode arc, U c is the voltage across the arc, l 1 = 20.56 mm, l 2 = 18.83 mm.
步骤2.4、确定阴极影响下熔池表面的电弧功率分布以及阳极影响下熔池表面的电弧功率分布,进而求出熔池表面在阴极与阳极共同影响下的电弧功率分布。Step 2.4: Determine the arc power distribution on the surface of the molten pool under the influence of the cathode and the arc power distribution on the surface of the molten pool under the influence of the anode, and then determine the arc power distribution under the influence of the cathode and the anode on the surface of the molten pool.
所述确定阴极影响下熔池表面的电弧功率分布以及阳极影响下熔池表面的电弧功率分布的方法如下:The method for determining the arc power distribution of the surface of the molten pool under the influence of the cathode and the arc power distribution of the surface of the molten pool under the influence of the anode are as follows:
将电弧在熔池表面的加热热流分布视为如图3所示的正态分布,则加热热流分布表示为
Figure PCTCN2018087696-appb-000013
其中,q max为加热斑点中心的最大热流,r为熔池表面任意一点到加热斑点中心的距离,α为热能集中系数。
The heating heat flow distribution of the arc on the surface of the molten pool is regarded as a normal distribution as shown in FIG. 3, and the heating heat flow distribution is expressed as
Figure PCTCN2018087696-appb-000013
Where q max is the maximum heat flow at the center of the heated spot, r is the distance from any point on the surface of the molten pool to the center of the heated spot, and α is the coefficient of thermal energy concentration.
对加热热流分布公式
Figure PCTCN2018087696-appb-000014
在加热斑点面积上进行积分,求得实际单极电弧功率在熔池表面的分布
Figure PCTCN2018087696-appb-000015
由于功率损耗,经验上Q=(0.65~0.7)P 1′,本实施方式取0.68,P 1′为单电极的电弧功率,即P 1′=0.5P 1,求得加热斑点中心的最大热流
Figure PCTCN2018087696-appb-000016
其中Q为实际单极电弧功率在熔池表面的分布,由加热热流分布公式
Figure PCTCN2018087696-appb-000017
在加热斑点面积上进行积分得到,P 1为电弧功率;根据加热斑点边界半径r m=0.5D+2l、边界热流q(r m)=0.05q max,以及加热热流分布表达式q(r),求得热能集中系数
Figure PCTCN2018087696-appb-000018
D为电极直径,l为电弧长度,指代阴极电弧长度或阳极电弧长度。
Formula for heating heat flow distribution
Figure PCTCN2018087696-appb-000014
Integrate on the heated spot area to find the distribution of the actual unipolar arc power on the surface of the molten pool
Figure PCTCN2018087696-appb-000015
Due to power loss, empirically Q = (0.65 ~ 0.7) P 1 ', this embodiment takes 0.68, P 1 ' is the arc power of a single electrode, that is, P 1 ' = 0.5P 1 , and the maximum heat flow at the center of the heated spot is obtained.
Figure PCTCN2018087696-appb-000016
Where Q is the distribution of the actual unipolar arc power on the surface of the molten pool, and the heating heat flow distribution formula
Figure PCTCN2018087696-appb-000017
Integral on the heated spot area, P 1 is the arc power; according to the heating spot boundary radius r m =0.5D+2l, the boundary heat flow q(r m )=0.05q max , and the heating heat flow distribution expression q(r) Find the thermal energy concentration factor
Figure PCTCN2018087696-appb-000018
D is the electrode diameter, l is the arc length, and refers to the cathodic arc length or the anode arc length.
求单电极的电弧功率在熔池表面的分布:根据已求得的加热斑点中心的最大热流q max、热能集中系数α和加热热流分布表达式q(r),求出单电极的电弧功率在熔池表面的分布表达式:
Figure PCTCN2018087696-appb-000019
其中r为熔池表面某点到加热斑点中心的距离。
Find the distribution of the arc power of the single electrode on the surface of the molten pool: according to the obtained maximum heat flow q max of the heating spot center, the thermal energy concentration coefficient α and the heating heat flow distribution expression q(r), the arc power of the single electrode is obtained. The distribution expression of the surface of the molten pool:
Figure PCTCN2018087696-appb-000019
Where r is the distance from a point on the surface of the bath to the center of the heated spot.
以两个电极的中心连接线所在直线为坐标轴的横轴,以两个电极的中心连接线的中垂线所在直线为坐标轴的纵轴,以阳极中心所在轴为横轴正方向,根据单 电极的电弧功率在熔池表面的分布p(r),表示出阴极影响下熔池表面的电弧功率分布p 1(x,y)以及阳极影响下熔池表面的电弧功率分布p 2(x,y)。 The straight line of the coordinate line of the center line of the two electrodes is the horizontal axis of the coordinate line, and the straight line of the center line of the two electrodes is the vertical axis of the coordinate axis, and the axis of the center of the anode is the positive direction of the horizontal axis, according to The distribution of the arc power of a single electrode on the surface of the bath, p(r), represents the arc power distribution p 1 (x, y) of the surface of the bath under the influence of the cathode and the arc power distribution p 2 of the surface of the bath under the influence of the anode (x) , y).
对于两相直流电熔镁炉,由于两方向相反的电弧间存在互斥的电磁力,导致两电弧分别向远离对方的方向上偏离,则斑点中心向电极外侧移动约20~30mm,此处取中间值25mm。因此:For a two-phase direct current fused magnesium furnace, due to the mutual exclusion of the electromagnetic force between the two opposite arcs, the two arcs are respectively shifted away from each other, and the center of the spot moves to the outside of the electrode by about 20 to 30 mm. The value is 25mm. therefore:
Figure PCTCN2018087696-appb-000020
Figure PCTCN2018087696-appb-000020
Figure PCTCN2018087696-appb-000021
Figure PCTCN2018087696-appb-000021
其中,(x,y)为熔池表面某点的坐标,d为极心距。Where (x, y) is the coordinate of a point on the surface of the molten pool, and d is the center distance.
所述熔池表面在阴极与阳极共同影响下的电弧功率分布为阴极影响下熔池表面的电弧功率分布与阳极影响下熔池表面的电弧功率分布之和,即p(x,y)=p 1(x,y)+p 2(x,y)。 The arc power distribution under the influence of the cathode and the anode on the surface of the molten pool is the sum of the arc power distribution on the surface of the molten pool under the influence of the cathode and the arc power distribution on the surface of the molten pool under the influence of the anode, that is, p(x, y)=p 1 (x, y) + p 2 (x, y).
步骤3、确定两相直流电熔镁炉系统的物理参数,包括:Step 3: Determine physical parameters of the two-phase DC fused magnesium furnace system, including:
(1)求极心距;(1) Find the center distance;
根据能量守恒定律,确定熔池表面积的表达式:在两相直流电熔镁炉的工作过程中,电弧功率P 1主要起熔化物料的作用,而熔池电阻功率主要起保温作用。电弧热中用于熔化物料的那部分热能称为有效电弧热W。熔炼过程中,物料最上层与空气接触的部分会向外散热,散热效率为η 1。少部分电弧热也会用于对熔池的保温,这部分热能称为保温热能,其所占比例为η 2。由能量守恒定律得熔池表面积为: According to the law of conservation of energy, the expression of the surface area of the molten pool is determined: during the operation of the two-phase direct current molten magnesium furnace, the arc power P 1 mainly acts as a molten material, and the resistance of the molten pool is mainly used for heat preservation. The portion of the thermal energy used to melt the material in the arc heat is referred to as the effective arc heat W. During the smelting process, the uppermost layer of the material in contact with the air radiates heat outward, and the heat dissipation efficiency is η 1 . A small part of the arc heat is also used to heat the molten pool. This part of the heat is called thermal insulation, and its proportion is η 2 . The surface area of the weld pool is determined by the law of conservation of energy:
Figure PCTCN2018087696-appb-000022
Figure PCTCN2018087696-appb-000022
其中,q为菱镁矿作原料时的产品单位能耗,ρ为电熔镁砂的密度,h为结晶高度。由文献可查得q=2611kWh/t,ρ=3580kg/m 3,η 1=0.03,η 2=0.16,结晶高度h为0.2m。 Where q is the unit energy consumption of the magnesite as a raw material, ρ is the density of the fused magnesia, and h is the crystallization height. From the literature, it can be found that q = 2611 kWh / t, ρ = 3580 kg / m 3 , η 1 = 0.03, η 2 = 0.16, and the crystal height h is 0.2 m.
根据熔池表面的形状,确定熔池表面积的表达式:在熔炼过程中,若极心距过大,使两电极间的最高温度较低,导致中间存在未熔死区;若极心距过小,则会使两电极间的最高温度过高,温度梯度大,熔池面积小。由此可知,当极心距长度恰好为电极的熔化半径时,熔炼效果最好。此时,熔池表面的近似图6所示,至此得到熔池表面积表达式:According to the shape of the surface of the molten pool, the expression of the surface area of the molten pool is determined: in the smelting process, if the pole center distance is too large, the maximum temperature between the two electrodes is low, resulting in an unmelted dead zone in the middle; Small, the maximum temperature between the two electrodes is too high, the temperature gradient is large, and the molten pool area is small. It can be seen that the smelting effect is best when the pole center length is exactly the melting radius of the electrode. At this time, the surface of the molten pool is approximated as shown in Fig. 6, and the expression of the surface area of the molten pool is obtained:
Figure PCTCN2018087696-appb-000023
Figure PCTCN2018087696-appb-000023
联立两个熔池表面积表达式,得到所述极心距的计算公式如下:The two molten pool surface area expressions are combined to obtain the formula for calculating the pole center distance as follows:
Figure PCTCN2018087696-appb-000024
Figure PCTCN2018087696-appb-000024
代入数值得d≈0.175m。Substituting the value is d≈0.175m.
(2)根据熔池表面在阴极与阳极共同影响下的电弧功率分布以及求得的极心距确定炉壳外形。(2) Determine the shape of the furnace shell according to the arc power distribution under the influence of the cathode and the anode and the obtained pole center distance.
所述炉壳外形的确定方法包括:The method for determining the shape of the furnace shell includes:
根据熔池表面在阴极与阳极共同影响下的电弧功率分布p(x,y)以及求得的极心距d,画出熔池表面的等功率线,如图7所示;根据熔池表面外围的等功率线,确定炉壳外形为“花生”型。According to the arc power distribution p(x, y) and the obtained pole center distance d under the influence of the cathode and the anode on the surface of the molten pool, draw the equal power line on the surface of the molten pool, as shown in Fig. 7; according to the surface of the molten pool The outer power line determines the shape of the furnace shell as "peanut" type.

Claims (10)

  1. 一种用于两相直流电熔镁炉的极心距与炉壳外形设计方法,其特征在于,包括:A method for designing a pole center distance and a furnace shell shape for a two-phase direct current magnesium melting furnace, characterized in that it comprises:
    设计两相直流电熔镁炉系统的结构;Designing the structure of a two-phase direct current fused magnesium furnace system;
    求得熔池表面在阴极与阳极共同影响下的电弧功率分布;Obtaining an arc power distribution under the influence of the cathode and the anode on the surface of the molten pool;
    确定两相直流电熔镁炉系统的物理参数,包括:Determine the physical parameters of the two-phase DC fused magnesium furnace system, including:
    求极心距;Find the center of the heart;
    根据熔池表面在阴极与阳极共同影响下的电弧功率分布以及求得的极心距确定炉壳外形。The shape of the furnace shell is determined according to the arc power distribution under the influence of the cathode and the anode and the obtained pole center distance.
  2. 根据权利要求1所述的方法,其特征在于,所述求得熔池表面在阴极与阳极共同影响下的电弧功率分布的具体方法包括:The method according to claim 1, wherein the specific method for determining the arc power distribution under the influence of the cathode and the anode on the surface of the molten pool comprises:
    根据阴极区电子热能的等值压降和阳极区的电子热能等值压降,计算阴极截止电压和阳极截止电压;Calculating the cathode cutoff voltage and the anode cutoff voltage according to the equivalent voltage drop of the electron energy in the cathode region and the equivalent electronic pressure drop of the anode region;
    求电弧功率及电弧两端电压;Find the arc power and the voltage across the arc;
    根据电弧两端电压、阴极截止电压、阳极截止电压,求出阴极电弧长度和阳极电弧长度;The cathode arc length and the anode arc length are obtained according to the voltage across the arc, the cathode cutoff voltage, and the anode cutoff voltage;
    确定阴极影响下熔池表面的电弧功率分布以及阳极影响下熔池表面的电弧功率分布,进而求出熔池表面在阴极与阳极共同影响下的电弧功率分布。Determine the arc power distribution on the surface of the molten pool under the influence of the cathode and the arc power distribution on the surface of the molten pool under the influence of the anode, and then determine the arc power distribution under the influence of the cathode and the anode on the surface of the molten pool.
  3. 根据权利要求2所述的方法,其特征在于,所述计算阴极截止电压和阳极截止电压的方法如下:The method according to claim 2, wherein said method of calculating a cathode cutoff voltage and an anode cutoff voltage is as follows:
    根据电极的加热斑点处温度计算阴极区电子热能的等值压降和阳极区的电子热能等值压降;Calculating the equivalent voltage drop of the electron energy in the cathode region and the equivalent pressure drop of the electron energy in the anode region according to the temperature at the heating spot of the electrode;
    根据阴极区电子热能的等值压降和阳极区的电子热能等值压降,计算阴极截止电压和阳极截止电压。The cathode cut-off voltage and the anode cut-off voltage were calculated based on the equivalent voltage drop of the electron thermal energy in the cathode region and the equivalent electronic pressure drop of the anode region.
  4. 根据权利要求2所述的方法,其特征在于,所述电弧功率的求解方法如下:The method of claim 2 wherein the method of solving the arc power is as follows:
    根据电极尺寸及电阻率计算两根电极的电阻,同时测量短网电阻,计算出两根电极的电阻与短网电阻之和R;Calculate the resistance of the two electrodes according to the electrode size and resistivity, and measure the resistance of the short grid, and calculate the sum R of the resistance of the two electrodes and the short grid resistance;
    根据熔池大小和熔池电阻率估算熔池电阻r 3Estimate the weld pool resistance r 3 according to the size of the weld pool and the resistivity of the weld pool;
    在已知整流器输出电压U d时求得使电弧功率P 1最大时的直流电流I d′; Calculating a DC current I d ' when the arc power P 1 is maximum when the rectifier output voltage U d is known;
    求得电弧功率P 1=(U d-RI d′-r 3I d′-U jz1-U jz2)I d′,U jz1为阴极截止电压U jz2为阳极截止电压。 The arc power P 1 =(U d -RI d '-r 3 I d '-U jz1 -U jz2 )I d ' is obtained, and U jz1 is the cathode cutoff voltage U jz2 is the anode cutoff voltage.
  5. 根据权利要求2所述的方法,其特征在于,所述电弧两端电压采用如下公式求解:The method according to claim 2, wherein the voltage across the arc is solved by the following formula:
    U c=0.5×(U d-RI d′-r 3I d′-U jx1-U jz2) U c =0.5×(U d -RI d '-r 3 I d '-U jx1 -U jz2 )
    其中,U d为整流器输出电压,I d′为已知整流器输出电压时使电弧功率P 1最大时的直流电流,R为两根电极的电阻与短网电阻之和,r 3为熔池电阻,U jz1为阴极截止电压,U jz2为阳极截止电压。 Where U d is the rectifier output voltage, I d ' is the DC current when the arc power P 1 is maximum when the output voltage of the rectifier is known, R is the sum of the resistance of the two electrodes and the short grid resistance, and r 3 is the bath resistance , U jz1 is the cathode cut-off voltage, and U jz2 is the anode cut-off voltage.
  6. 根据权利要求2所述的方法,其特征在于,所述阴极电弧长度和阳极电弧长度的计算公式分别如下:The method of claim 2 wherein said cathode arc length and anode arc length are calculated as follows:
    Figure PCTCN2018087696-appb-100001
    Figure PCTCN2018087696-appb-100001
    Figure PCTCN2018087696-appb-100002
    Figure PCTCN2018087696-appb-100002
    其中,l 1为阴极电弧长度,l 2为阳极电弧长度,U jz1为阴极截止电压,U jz2为阳极截止电压,U c为电弧两端电压,b为弧压系数。 Wherein l 1 is the length of the cathodic arc, l 2 is the length of the anode arc, U jz1 is the cathode cutoff voltage, U jz2 is the anode cutoff voltage, U c is the voltage across the arc, and b is the arc voltage coefficient.
  7. 根据权利要求2所述的方法,其特征在于,所述确定阴极影响下熔池表面的电弧功率分布以及阳极影响下熔池表面的电弧功率分布的方法如下:The method according to claim 2, wherein the method for determining the arc power distribution of the surface of the molten pool under the influence of the cathode and the arc power distribution of the surface of the molten pool under the influence of the anode are as follows:
    将电弧在熔池表面的加热热流分布视为正态分布,则加热热流分布表示为
    Figure PCTCN2018087696-appb-100003
    其中,q max为加热斑点中心的最大热流,r为熔池表面任意一点到加热斑点中心的距离,α为热能集中系数;
    The heating heat flow distribution of the arc on the surface of the molten pool is regarded as a normal distribution, and the heating heat flow distribution is expressed as
    Figure PCTCN2018087696-appb-100003
    Where q max is the maximum heat flow at the center of the heated spot, r is the distance from any point on the surface of the molten pool to the center of the heated spot, and α is the coefficient of thermal energy concentration;
    求加热斑点中心的最大热流
    Figure PCTCN2018087696-appb-100004
    其中Q为实际单极电弧功率在熔池表面的分布,由加热热流分布公式
    Figure PCTCN2018087696-appb-100005
    在加热斑点面积上进行积分得到,P 1为电弧功率;热能集中系数
    Figure PCTCN2018087696-appb-100006
    D为电极直径,l为电弧长度,指代阴极电弧长度或阳极电弧长度;
    Find the maximum heat flow at the center of the heated spot
    Figure PCTCN2018087696-appb-100004
    Where Q is the distribution of the actual unipolar arc power on the surface of the molten pool, and the heating heat flow distribution formula
    Figure PCTCN2018087696-appb-100005
    Integrate on the heated spot area, P 1 is the arc power; thermal energy concentration factor
    Figure PCTCN2018087696-appb-100006
    D is the diameter of the electrode, l is the length of the arc, and refers to the length of the cathodic arc or the length of the anode arc;
    求单电极的电弧功率在熔池表面的分布;Find the distribution of the arc power of the single electrode on the surface of the molten pool;
    以两个电极的中心连接线所在直线为坐标轴的横轴,以两个电极的中心连接线的中垂线所在直线为坐标轴的纵轴,以阳极中心所在轴为横轴正方向,根据单电极的电弧功率在熔池表面的分布,表示出阴极影响下熔池表面的电弧功率分布以及阳极影响下熔池表面的电弧功率分布。The straight line of the coordinate line of the center line of the two electrodes is the horizontal axis of the coordinate line, and the straight line of the center line of the two electrodes is the vertical axis of the coordinate axis, and the axis of the center of the anode is the positive direction of the horizontal axis, according to The distribution of the arc power of the single electrode on the surface of the molten pool indicates the arc power distribution of the surface of the molten pool under the influence of the cathode and the arc power distribution of the surface of the molten pool under the influence of the anode.
  8. 根据权利要求2所述的方法,其特征在于,所述熔池表面在阴极与阳极共同影响下的电弧功率分布为阴极影响下熔池表面的电弧功率分布与阳极影响下熔池表面的电弧功率分布之和。The method according to claim 2, wherein the arc power distribution of the surface of the molten pool under the influence of the cathode and the anode is an arc power distribution of the surface of the molten pool under the influence of the cathode and an arc power of the surface of the molten pool under the influence of the anode The sum of the distribution.
  9. 根据权利要求1所述的方法,其特征在于,所述极心距的计算公式如下:The method of claim 1 wherein said polar distance is calculated as follows:
    Figure PCTCN2018087696-appb-100007
    Figure PCTCN2018087696-appb-100007
    其中,η 1为散热效率,η 2为保温热能所占比例,q为菱镁矿作原料时的产品单位能耗,ρ为电熔镁砂的密度,h为结晶高度,P 1为电弧功率。 Where η 1 is the heat dissipation efficiency, η 2 is the proportion of heat preservation heat energy, q is the product energy consumption of magnesite as raw material, ρ is the density of fused magnesia, h is the crystal height, and P 1 is the arc power. .
  10. 根据权利要求1所述的方法,其特征在于,所述炉壳外形的确定方法包括:The method of claim 1 wherein the method of determining the shape of the furnace shell comprises:
    根据熔池表面在阴极与阳极共同影响下的电弧功率分布以及求得的极心距,画出熔池表面的等功率线;根据熔池表面外围的等功率线,确定炉壳外形。According to the arc power distribution under the influence of the cathode and the anode and the obtained pole center distance, the equal power line on the surface of the molten pool is drawn; the shape of the shell is determined according to the equal power line around the surface of the bath.
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