感应加热时铁磁电荷的磁化

G. Levshin
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引用次数: 1

摘要

本文对两种类型的感应炉坩埚中铁磁电荷的磁化和加热进行了分析。在电感炉中,电荷被垂直的电磁流磁化,而在具有弯曲U型、C型或o型磁路(MPr)的电磁炉中,电荷被水平流磁化。对这些普遍的磁化过程的认识是不够的。电荷材料中的双磁感应是相当重要的。该参数在单电荷磁化过程中以及与之相关的其他磁量(Bm感应强度、Nm退磁强度、N退磁系数、M磁化强度、μi物质和μt体的磁导率、km磁化率等)的确定存在困难。如果坩埚体积为~V ~ t的多孔体,且该体积的铁磁片填充系数Kv≤0.5,则磁化难度增大。它还可以产生具有Bmt感应和Hmt强度的退磁场。除此之外,毛孔还有一个额外的消磁作用。因此,多孔体中的感应强度Вiт小于固体体中的感应强度Вi。为了比较50 Hz频率水平流和垂直流对铁磁荷磁化强度的影响,采用Kv≈0.53的高碳钢(GOST 11964 - 83) DSL08松散试样进行了模拟实验。样品被放置在电感器和u型芯片的两极之间。用直径为1-15毫米的圆柱形和扁平探针单元在空气和样品中测量感应。电磁炉比电感炉的优点是炉料中铋感应分布更均匀,比炉内工作腔中Be感应多出1.7倍,表明该炉在加热过程中更有效地利用了电磁能。作者提出用电阻丝制成的测量线圈,用安培计-伏特计法控制加热电荷时的Вi感应。
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Magnetization of ferromagnetic charge at induction heating
The article presents analysis of magnetization and heating of ferromagnetic charge in crucibles of induction furnaces of two types. In inductor furnaces, the charge is magnetized by a vertical electromagnetic flow, and in electromagnetic furnaces with a curved U-, C-, or O-shaped magnetic circuit (MPr) – by a horizontal flow. Knowledge of these largely general magnetization processes is insufficient. Bi magnetic induction in charge material is rather important. There are difficulties in determining this parameter during magnetization of a single piece of charge and other magnetic quantities associated with it: Bm induction and Nm  strength of the demagnetizing field, N demagnetization coefficient, M magnetization, magnetic permeabilities of μi substance and μt body, km susceptibility, etc. Difficulties increase at magnetization, if it is a porous body with crucible volume of ~V t and a factor of filling with ferromagnetic pieces of this volume of Kv ≤ 0.5. It also creates a demagnetizing field with Bmt induction and Hmt strength. Beyond that, pores have an additional demagnetizing effect. Therefore, the induction Вiт in a porous body is less than the induction Вi in a solid one. To compare magnetization of ferromagnetic charge with horizontal and vertical flows with frequency of 50 Hz, modeling experiments were carried out with the samples of DSL08 unconsolidated shot from high-carbon steel (GOST 11964 – 83) with Kv ≈ 0.53. The samples were placed in the inductor and between the poles of a U-shaped core piece. Induction was measured by a cylindrical and flat probe unit of Sh1-15 militeslameter in air and in the sample. An advantage of electromagnetic furnace over an inductor one is more uniform distribution of Bi induction in charge and its significant excess (1.7 times) over the Be induction in a furnace working cavity, which indicates more efficient use of electromagnetic energy in this furnace during heating. The author proposed to control Вi induction when heating the charge by the ammeter-voltmeter method using measuring coil made of heat-resistant wire.
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