非金属夹杂物在单股钢筋束中的碰撞-凝聚、传输和清除行为模型研究

Qinghua Xie, Peiyuan Ni, Ying Li
{"title":"非金属夹杂物在单股钢筋束中的碰撞-凝聚、传输和清除行为模型研究","authors":"Qinghua Xie, Peiyuan Ni, Ying Li","doi":"10.1007/s11663-024-03142-x","DOIUrl":null,"url":null,"abstract":"<p>A computational fluid dynamics-population balance model-boundary transfer model (CFD-PBM-BTM) coupled model was developed to predict the dynamic change behaviors of inclusions in molten steel. Brownian collision, turbulent collision, and Stokes collision were used to describe the collision–coalescence of inclusions in molten steel. Moreover, three boundary transfer models, namely ideal removal model, Stokes removal model, and Fan-Ahmadi removal model, were adopted to calculate the removal rate of inclusions at the steel/slag interface. The results show that inclusion size and number density distribution predicted by the developed model, with the Flint-Howarth coalescence probability sub-model, Fan-Ahmadi removal sub-model, were in good agreement with the industrial measurements. The deviation of model predictions with 21 inclusion size groups was only around 9 pct from industrial measurements. Turbulent collision was found to significantly affect the collision–coalescence rate of small size inclusions. For inclusions larger than around 10 <i>μ</i>m, Stokes collision becomes critical and the Stokes collision rate can reach 1×10<sup>-13</sup> m<sup>3</sup>/s for the collision between 24.3 and 42.5 <i>μ</i>m inclusions. In addition, the inclusion removal ratio in the pouring region was about 50 pct of that in the casting region. This is due to the impinging steel flow effect on inclusion moving. As inclusion diameter increased from 1.1 to 42.2 <i>μ</i>m, the removal rate increased from 1.4×10<sup>-4</sup> to 7.7×10<sup>−4</sup> m/s. Furthermore, the inclusion removal rate increased with an increased steel/slag interface roughness. Specifically, the total removal ratio of 1.1, 10.6, 24.3, and 42.2 <i>μ</i>m inclusions was 0.1, 3, 14, and 42 pct for the roughness value of 0 mm, respectively. The ratio increased to 7, 10, 21, and 50 pct, respectively, when the roughness value was 1 mm.</p><h3 data-test=\"abstract-sub-heading\">Graphical Abstract</h3>\n","PeriodicalId":18613,"journal":{"name":"Metallurgical and Materials Transactions B","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2024-06-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A Model Study on Collision–Coalescence, Transport, and Removal Behavior of Non-metallic Inclusions in a Single-Strand Tundish\",\"authors\":\"Qinghua Xie, Peiyuan Ni, Ying Li\",\"doi\":\"10.1007/s11663-024-03142-x\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>A computational fluid dynamics-population balance model-boundary transfer model (CFD-PBM-BTM) coupled model was developed to predict the dynamic change behaviors of inclusions in molten steel. Brownian collision, turbulent collision, and Stokes collision were used to describe the collision–coalescence of inclusions in molten steel. Moreover, three boundary transfer models, namely ideal removal model, Stokes removal model, and Fan-Ahmadi removal model, were adopted to calculate the removal rate of inclusions at the steel/slag interface. The results show that inclusion size and number density distribution predicted by the developed model, with the Flint-Howarth coalescence probability sub-model, Fan-Ahmadi removal sub-model, were in good agreement with the industrial measurements. The deviation of model predictions with 21 inclusion size groups was only around 9 pct from industrial measurements. Turbulent collision was found to significantly affect the collision–coalescence rate of small size inclusions. For inclusions larger than around 10 <i>μ</i>m, Stokes collision becomes critical and the Stokes collision rate can reach 1×10<sup>-13</sup> m<sup>3</sup>/s for the collision between 24.3 and 42.5 <i>μ</i>m inclusions. In addition, the inclusion removal ratio in the pouring region was about 50 pct of that in the casting region. This is due to the impinging steel flow effect on inclusion moving. As inclusion diameter increased from 1.1 to 42.2 <i>μ</i>m, the removal rate increased from 1.4×10<sup>-4</sup> to 7.7×10<sup>−4</sup> m/s. Furthermore, the inclusion removal rate increased with an increased steel/slag interface roughness. Specifically, the total removal ratio of 1.1, 10.6, 24.3, and 42.2 <i>μ</i>m inclusions was 0.1, 3, 14, and 42 pct for the roughness value of 0 mm, respectively. The ratio increased to 7, 10, 21, and 50 pct, respectively, when the roughness value was 1 mm.</p><h3 data-test=\\\"abstract-sub-heading\\\">Graphical Abstract</h3>\\n\",\"PeriodicalId\":18613,\"journal\":{\"name\":\"Metallurgical and Materials Transactions B\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-06-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Metallurgical and Materials Transactions B\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1007/s11663-024-03142-x\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Metallurgical and Materials Transactions B","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1007/s11663-024-03142-x","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

摘要

为预测钢水中夹杂物的动态变化行为,建立了计算流体动力学-种群平衡模型-边界传递模型(CFD-PBM-BTM)耦合模型。布朗碰撞、湍流碰撞和斯托克斯碰撞被用来描述钢水中夹杂物的碰撞-凝聚。此外,还采用了三种边界转移模型,即理想去除模型、斯托克斯去除模型和 Fan-Ahmadi 去除模型,来计算钢/渣界面夹杂物的去除率。结果表明,采用 Flint-Howarth 凝聚概率子模型和 Fan-Ahmadi 清除子模型所建立的模型预测的夹杂物粒度和数量密度分布与工业测量结果非常吻合。模型预测的 21 个夹杂物尺寸组与工业测量值的偏差仅为 9%左右。研究发现,湍流碰撞对小尺寸夹杂物的碰撞凝聚率有显著影响。对于大于 10 μm 左右的夹杂物,斯托克斯碰撞变得至关重要,在 24.3 μm 至 42.5 μm 之间的夹杂物碰撞时,斯托克斯碰撞率可达 1×10-13 m3/s。此外,浇注区的夹杂物去除率约为铸造区的 50%。这是由于冲击钢流对夹杂物移动的影响。当夹杂物直径从 1.1 μm 增加到 42.2 μm 时,去除率从 1.4×10-4 m/s 增加到 7.7×10-4 m/s。此外,夹杂物去除率随着钢/渣界面粗糙度的增加而增加。具体来说,粗糙度值为 0 mm 时,1.1、10.6、24.3 和 42.2 μm 夹杂的总去除率分别为 0.1、3、14 和 42 pct。当粗糙度值为 1 毫米时,该比率分别增至 7、10、21 和 50%。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

A Model Study on Collision–Coalescence, Transport, and Removal Behavior of Non-metallic Inclusions in a Single-Strand Tundish

A Model Study on Collision–Coalescence, Transport, and Removal Behavior of Non-metallic Inclusions in a Single-Strand Tundish

A computational fluid dynamics-population balance model-boundary transfer model (CFD-PBM-BTM) coupled model was developed to predict the dynamic change behaviors of inclusions in molten steel. Brownian collision, turbulent collision, and Stokes collision were used to describe the collision–coalescence of inclusions in molten steel. Moreover, three boundary transfer models, namely ideal removal model, Stokes removal model, and Fan-Ahmadi removal model, were adopted to calculate the removal rate of inclusions at the steel/slag interface. The results show that inclusion size and number density distribution predicted by the developed model, with the Flint-Howarth coalescence probability sub-model, Fan-Ahmadi removal sub-model, were in good agreement with the industrial measurements. The deviation of model predictions with 21 inclusion size groups was only around 9 pct from industrial measurements. Turbulent collision was found to significantly affect the collision–coalescence rate of small size inclusions. For inclusions larger than around 10 μm, Stokes collision becomes critical and the Stokes collision rate can reach 1×10-13 m3/s for the collision between 24.3 and 42.5 μm inclusions. In addition, the inclusion removal ratio in the pouring region was about 50 pct of that in the casting region. This is due to the impinging steel flow effect on inclusion moving. As inclusion diameter increased from 1.1 to 42.2 μm, the removal rate increased from 1.4×10-4 to 7.7×10−4 m/s. Furthermore, the inclusion removal rate increased with an increased steel/slag interface roughness. Specifically, the total removal ratio of 1.1, 10.6, 24.3, and 42.2 μm inclusions was 0.1, 3, 14, and 42 pct for the roughness value of 0 mm, respectively. The ratio increased to 7, 10, 21, and 50 pct, respectively, when the roughness value was 1 mm.

Graphical Abstract

求助全文
通过发布文献求助,成功后即可免费获取论文全文。 去求助
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信