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數(shù)值模擬電極縮孔對(duì)IN718合金電渣重熔過(guò)程的影響
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1.寶鋼股份研究院;2.東北大學(xué)

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國(guó)家自然科學(xué)基金項(xiàng)目(U1708253)


Numerical simulation of the influence of electrode shrinkage cavity on the ESR process of IN718 alloy
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Affiliation:

1.Research Institue, Baoshan Iron & Steel Co., Ltd;2.Key Lab for Anisotropy and Texture of Materials (Ministry of Education), Northeastern University, Shenyang

Fund Project:

National Natural Science Foundation of China (U1708253)

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    摘要:

    利用自主開(kāi)發(fā)的ESR過(guò)程仿真軟件,針對(duì)直徑430 mm的IN718合金鑄錠,通過(guò)設(shè)計(jì)不同形狀尺寸的電極縮孔,進(jìn)行電渣重熔過(guò)程的數(shù)值模擬計(jì)算和分析。結(jié)果表明,基于電磁場(chǎng)、流場(chǎng)和溫度場(chǎng)等多物理場(chǎng)耦合計(jì)算自主開(kāi)發(fā)的ESR數(shù)學(xué)模型及仿真軟件,可以用于ESR冶煉全過(guò)程數(shù)值模擬,模型計(jì)算的熔池形狀和深度、二次枝晶臂間距分布規(guī)律與實(shí)際剖錠分析結(jié)果接近。電極中存在縮孔改變了電極與渣池的接觸面積,從而顯著影響渣池的焦耳熱和電磁力分布,而縮孔沿電極軸向尺寸的變化對(duì)二者分布的影響則很少。在恒熔速條件下,當(dāng)縮孔半徑小于0.025 m時(shí),縮孔對(duì)熔煉過(guò)程幾乎沒(méi)有影響;當(dāng)縮孔尺寸繼續(xù)增大時(shí),渣池溫度場(chǎng)和流場(chǎng)發(fā)生明顯改變,渣池溫度逐步升高,中心向下流速相對(duì)減弱;電極縮孔尺寸變化對(duì)熔池溫度場(chǎng)及兩相區(qū)尺寸影響不明顯??s孔半徑尺寸對(duì)電流和功率等熔煉參數(shù)的影響呈非線性關(guān)系,臨界變化值約為0.05 m,當(dāng)縮孔半徑低于臨界值時(shí),對(duì)電流和功率等影響較小;高于臨界值時(shí),隨著縮孔半徑增加,電流和功率顯著增加,并且增速不斷加快。從工藝過(guò)程控制穩(wěn)定性角度而言,該尺寸電極縮孔半徑應(yīng)控制在0.05 m以下。

    Abstract:

    Abstract: Numerical simulation and analysis of the influence of electrode shrinkage cavity on electroslag remelting (ESR) process of a 430mm diameter ingot of IN718 alloy were carried out using the self-developed ESR process model. Electromagnetic fields of ESR system were simulated with specially designed various shape and size of cavity in the electrode. The results show that the changed contacting area between the electrode and the slag, owing to the cavity, plays the predominant role on the distributions of the Joule heat and electromagnetic force in the slag, while the effect of axial dimension change of the shrinkage cavity is negligible. Constant melt rate ESR processes were simulated for the different radius cavity situations. It is shown that, at a constant melt rate, no effect of shrinkage cavity on the ESR process can be seen as its radius is less than 0.025 m, and only minute influence on the slag flow when the radius reaches 0.05 m. As the radius increases over 0.05 m, increasingly evident influence on the slag zone appears with the center downward flow weakened and temperature risen. Nevertheless, there is no obvious influence of the cavity on the ingot including the melt pool and mush zone. There are nonlinear relations between the shrinkage cavity radius and the ESR melting parameters including current and power, with a critical value about 0.05 m for the radius. Below the critical value, faint or even no change of the parameters appears, while, above the value, the parameters of power and current soon turn into high speed increase, approximately in a linear manner. From the standpoint of process control stability, the shrinkage cavity radius should be controlled less than 0.05 m.

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王資興,李青,王磊.數(shù)值模擬電極縮孔對(duì)IN718合金電渣重熔過(guò)程的影響[J].稀有金屬材料與工程,2018,47(12):3579~3589.[wangzixing, liqing, wanglei. Numerical simulation of the influence of electrode shrinkage cavity on the ESR process of IN718 alloy[J]. Rare Metal Materials and Engineering,2018,47(12):3579~3589.]
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  • 收稿日期:2018-04-06
  • 最后修改日期:2018-06-10
  • 錄用日期:2018-06-29
  • 在線發(fā)布日期: 2019-01-04
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