Loading…

Flow and Mixing Behavior in a New Bottom Blown Copper Smelting Furnace

A mathematical model was developed to describe gas-liquid flow and mixing behavior in a new bottom blown oxygen copper smelting furnace, and the model validation was carried out through a water model experiment. The effects of different nozzle locations, nozzle numbers, and gas flow rates on the gas...

Full description

Saved in:
Bibliographic Details
Published in:International journal of molecular sciences 2019-11, Vol.20 (22), p.5757
Main Authors: Shao, Pin, Jiang, Lepeng
Format: Article
Language:English
Subjects:
Citations: Items that this one cites
Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by cdi_FETCH-LOGICAL-c478t-da50d46a18b52189deef203796548cd64dd5d08ffda73b561946c6340f833f1b3
cites cdi_FETCH-LOGICAL-c478t-da50d46a18b52189deef203796548cd64dd5d08ffda73b561946c6340f833f1b3
container_end_page
container_issue 22
container_start_page 5757
container_title International journal of molecular sciences
container_volume 20
creator Shao, Pin
Jiang, Lepeng
description A mathematical model was developed to describe gas-liquid flow and mixing behavior in a new bottom blown oxygen copper smelting furnace, and the model validation was carried out through a water model experiment. The effects of different nozzle locations, nozzle numbers, and gas flow rates on the gas-liquid flow, gas total volume, and mixing efficiency were investigated. The results show that the gas-liquid two-phase flow and mixing time predicted by the present model agree well with the experimental data. When the nozzles are located near the center of the bath bottom, the gas total volume is larger, but the mixing efficiency is very low. With the increase of nozzle arrangement angle, the mixing time decreased. However, the excessive angle arrangement of nozzles exceeding 21° was found to be detrimental to the bubble residence time and mixing efficiency. With the increase in nozzle numbers from nine to 13, the gas total volume in the furnace increases, and the mixing efficiency does not change greatly. When the number of nozzles is further increased to 18, the mixing efficiency begins to decrease significantly. As the gas flow rate increases from 4.7 m /h to 14.1 m /h, the gas total volume in the furnace increases, and the mixing time is rapidly reduced from 314.5 s to 251.5 s. When the gas flow rate exceeds 18.8 m /h, the gas total volume and mixing efficiency change little.
doi_str_mv 10.3390/ijms20225757
format article
fullrecord <record><control><sourceid>proquest_doaj_</sourceid><recordid>TN_cdi_doaj_primary_oai_doaj_org_article_e500137da74e4848a2bf3d5846399e39</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><doaj_id>oai_doaj_org_article_e500137da74e4848a2bf3d5846399e39</doaj_id><sourcerecordid>2333601517</sourcerecordid><originalsourceid>FETCH-LOGICAL-c478t-da50d46a18b52189deef203796548cd64dd5d08ffda73b561946c6340f833f1b3</originalsourceid><addsrcrecordid>eNpdkU1vEzEURS1ERT9gxxpZYsOiaW0_22NvkEhEoFILC2BtecZvUkcz42BPWvj3TEipUlbPej468vUl5DVnFwCWXcZ1XwQTQlWqekZOuBRixpiunh-cj8lpKWvGBAhlX5Bj4JWUTMoTslx26Z76IdCb-CsOKzrHW38XU6ZxoJ5-wXs6T-OYejqfwIEu0maDmX7rsRt3-HKbB9_gS3LU-q7gq4d5Rn4sP35ffJ5df_10tfhwPWtkZcZZ8IoFqT03tRLc2IDYCgaV1UqaJmgZggrMtG3wFdRKcyt1o0Gy1gC0vIYzcrX3huTXbpNj7_Nvl3x0fxcpr5zPY2w6dKgY41BNJonSSONF3UJQRmqwFsFOrvd712Zb9xgaHMbsuyfSpzdDvHWrdOe0MUZZOQnePQhy-rnFMro-lga7zg-YtsUJ4FrCFE9N6Nv_0HXa_Vy3owA044pXE3W-p5qcSsnYPj6GM7cr2x2WPeFvDgM8wv_ahT_w5qMi</addsrcrecordid><sourcetype>Open Website</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2333601517</pqid></control><display><type>article</type><title>Flow and Mixing Behavior in a New Bottom Blown Copper Smelting Furnace</title><source>Publicly Available Content Database (Proquest) (PQ_SDU_P3)</source><source>PubMed Central Free</source><creator>Shao, Pin ; Jiang, Lepeng</creator><creatorcontrib>Shao, Pin ; Jiang, Lepeng</creatorcontrib><description>A mathematical model was developed to describe gas-liquid flow and mixing behavior in a new bottom blown oxygen copper smelting furnace, and the model validation was carried out through a water model experiment. The effects of different nozzle locations, nozzle numbers, and gas flow rates on the gas-liquid flow, gas total volume, and mixing efficiency were investigated. The results show that the gas-liquid two-phase flow and mixing time predicted by the present model agree well with the experimental data. When the nozzles are located near the center of the bath bottom, the gas total volume is larger, but the mixing efficiency is very low. With the increase of nozzle arrangement angle, the mixing time decreased. However, the excessive angle arrangement of nozzles exceeding 21° was found to be detrimental to the bubble residence time and mixing efficiency. With the increase in nozzle numbers from nine to 13, the gas total volume in the furnace increases, and the mixing efficiency does not change greatly. When the number of nozzles is further increased to 18, the mixing efficiency begins to decrease significantly. As the gas flow rate increases from 4.7 m /h to 14.1 m /h, the gas total volume in the furnace increases, and the mixing time is rapidly reduced from 314.5 s to 251.5 s. When the gas flow rate exceeds 18.8 m /h, the gas total volume and mixing efficiency change little.</description><identifier>ISSN: 1422-0067</identifier><identifier>ISSN: 1661-6596</identifier><identifier>EISSN: 1422-0067</identifier><identifier>DOI: 10.3390/ijms20225757</identifier><identifier>PMID: 31744044</identifier><language>eng</language><publisher>Switzerland: MDPI AG</publisher><subject>bottom blown ; Copper ; Copper - chemistry ; copper smelting ; Efficiency ; Flow velocity ; Fluid dynamics ; Gas flow ; gas-liquid flow ; Gases - chemistry ; Liquid flow ; Metallurgy ; mixing behavior ; modeling ; Models, Theoretical ; Monitoring ; Nozzles ; Oxygen - chemistry ; Smelting ; Smelting furnaces ; Two phase flow ; Water - chemistry</subject><ispartof>International journal of molecular sciences, 2019-11, Vol.20 (22), p.5757</ispartof><rights>2019. This work is licensed under http://creativecommons.org/licenses/by/3.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><rights>2019 by the authors. 2019</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c478t-da50d46a18b52189deef203796548cd64dd5d08ffda73b561946c6340f833f1b3</citedby><cites>FETCH-LOGICAL-c478t-da50d46a18b52189deef203796548cd64dd5d08ffda73b561946c6340f833f1b3</cites><orcidid>0000-0001-6017-1168</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.proquest.com/docview/2333601517/fulltextPDF?pq-origsite=primo$$EPDF$$P50$$Gproquest$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://www.proquest.com/docview/2333601517?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>230,314,727,780,784,885,25753,27924,27925,37012,37013,44590,53791,53793,75126</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/31744044$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Shao, Pin</creatorcontrib><creatorcontrib>Jiang, Lepeng</creatorcontrib><title>Flow and Mixing Behavior in a New Bottom Blown Copper Smelting Furnace</title><title>International journal of molecular sciences</title><addtitle>Int J Mol Sci</addtitle><description>A mathematical model was developed to describe gas-liquid flow and mixing behavior in a new bottom blown oxygen copper smelting furnace, and the model validation was carried out through a water model experiment. The effects of different nozzle locations, nozzle numbers, and gas flow rates on the gas-liquid flow, gas total volume, and mixing efficiency were investigated. The results show that the gas-liquid two-phase flow and mixing time predicted by the present model agree well with the experimental data. When the nozzles are located near the center of the bath bottom, the gas total volume is larger, but the mixing efficiency is very low. With the increase of nozzle arrangement angle, the mixing time decreased. However, the excessive angle arrangement of nozzles exceeding 21° was found to be detrimental to the bubble residence time and mixing efficiency. With the increase in nozzle numbers from nine to 13, the gas total volume in the furnace increases, and the mixing efficiency does not change greatly. When the number of nozzles is further increased to 18, the mixing efficiency begins to decrease significantly. As the gas flow rate increases from 4.7 m /h to 14.1 m /h, the gas total volume in the furnace increases, and the mixing time is rapidly reduced from 314.5 s to 251.5 s. When the gas flow rate exceeds 18.8 m /h, the gas total volume and mixing efficiency change little.</description><subject>bottom blown</subject><subject>Copper</subject><subject>Copper - chemistry</subject><subject>copper smelting</subject><subject>Efficiency</subject><subject>Flow velocity</subject><subject>Fluid dynamics</subject><subject>Gas flow</subject><subject>gas-liquid flow</subject><subject>Gases - chemistry</subject><subject>Liquid flow</subject><subject>Metallurgy</subject><subject>mixing behavior</subject><subject>modeling</subject><subject>Models, Theoretical</subject><subject>Monitoring</subject><subject>Nozzles</subject><subject>Oxygen - chemistry</subject><subject>Smelting</subject><subject>Smelting furnaces</subject><subject>Two phase flow</subject><subject>Water - chemistry</subject><issn>1422-0067</issn><issn>1661-6596</issn><issn>1422-0067</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><sourceid>DOA</sourceid><recordid>eNpdkU1vEzEURS1ERT9gxxpZYsOiaW0_22NvkEhEoFILC2BtecZvUkcz42BPWvj3TEipUlbPej468vUl5DVnFwCWXcZ1XwQTQlWqekZOuBRixpiunh-cj8lpKWvGBAhlX5Bj4JWUTMoTslx26Z76IdCb-CsOKzrHW38XU6ZxoJ5-wXs6T-OYejqfwIEu0maDmX7rsRt3-HKbB9_gS3LU-q7gq4d5Rn4sP35ffJ5df_10tfhwPWtkZcZZ8IoFqT03tRLc2IDYCgaV1UqaJmgZggrMtG3wFdRKcyt1o0Gy1gC0vIYzcrX3huTXbpNj7_Nvl3x0fxcpr5zPY2w6dKgY41BNJonSSONF3UJQRmqwFsFOrvd712Zb9xgaHMbsuyfSpzdDvHWrdOe0MUZZOQnePQhy-rnFMro-lga7zg-YtsUJ4FrCFE9N6Nv_0HXa_Vy3owA044pXE3W-p5qcSsnYPj6GM7cr2x2WPeFvDgM8wv_ahT_w5qMi</recordid><startdate>20191116</startdate><enddate>20191116</enddate><creator>Shao, Pin</creator><creator>Jiang, Lepeng</creator><general>MDPI AG</general><general>MDPI</general><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>3V.</scope><scope>7X7</scope><scope>7XB</scope><scope>88E</scope><scope>8FI</scope><scope>8FJ</scope><scope>8FK</scope><scope>8G5</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>FYUFA</scope><scope>GHDGH</scope><scope>GNUQQ</scope><scope>GUQSH</scope><scope>K9.</scope><scope>M0S</scope><scope>M1P</scope><scope>M2O</scope><scope>MBDVC</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>Q9U</scope><scope>7X8</scope><scope>5PM</scope><scope>DOA</scope><orcidid>https://orcid.org/0000-0001-6017-1168</orcidid></search><sort><creationdate>20191116</creationdate><title>Flow and Mixing Behavior in a New Bottom Blown Copper Smelting Furnace</title><author>Shao, Pin ; Jiang, Lepeng</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c478t-da50d46a18b52189deef203796548cd64dd5d08ffda73b561946c6340f833f1b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>bottom blown</topic><topic>Copper</topic><topic>Copper - chemistry</topic><topic>copper smelting</topic><topic>Efficiency</topic><topic>Flow velocity</topic><topic>Fluid dynamics</topic><topic>Gas flow</topic><topic>gas-liquid flow</topic><topic>Gases - chemistry</topic><topic>Liquid flow</topic><topic>Metallurgy</topic><topic>mixing behavior</topic><topic>modeling</topic><topic>Models, Theoretical</topic><topic>Monitoring</topic><topic>Nozzles</topic><topic>Oxygen - chemistry</topic><topic>Smelting</topic><topic>Smelting furnaces</topic><topic>Two phase flow</topic><topic>Water - chemistry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Shao, Pin</creatorcontrib><creatorcontrib>Jiang, Lepeng</creatorcontrib><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>ProQuest Central (Corporate)</collection><collection>ProQuest Health &amp; Medical Collection</collection><collection>ProQuest Central (purchase pre-March 2016)</collection><collection>Medical Database (Alumni Edition)</collection><collection>Hospital Premium Collection</collection><collection>Hospital Premium Collection (Alumni Edition)</collection><collection>ProQuest Central (Alumni) (purchase pre-March 2016)</collection><collection>Research Library (Alumni Edition)</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central</collection><collection>ProQuest Central Essentials</collection><collection>AUTh Library subscriptions: ProQuest Central</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central</collection><collection>Health Research Premium Collection</collection><collection>Health Research Premium Collection (Alumni)</collection><collection>ProQuest Central Student</collection><collection>Research Library Prep (ProQuest)</collection><collection>ProQuest Health &amp; Medical Complete (Alumni)</collection><collection>Health &amp; Medical Collection (Alumni Edition)</collection><collection>Medical Database</collection><collection>ProQuest research library</collection><collection>Research Library (Corporate)</collection><collection>Publicly Available Content Database (Proquest) (PQ_SDU_P3)</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>ProQuest Central Basic</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><collection>DOAJ Directory of Open Access Journals</collection><jtitle>International journal of molecular sciences</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Shao, Pin</au><au>Jiang, Lepeng</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Flow and Mixing Behavior in a New Bottom Blown Copper Smelting Furnace</atitle><jtitle>International journal of molecular sciences</jtitle><addtitle>Int J Mol Sci</addtitle><date>2019-11-16</date><risdate>2019</risdate><volume>20</volume><issue>22</issue><spage>5757</spage><pages>5757-</pages><issn>1422-0067</issn><issn>1661-6596</issn><eissn>1422-0067</eissn><abstract>A mathematical model was developed to describe gas-liquid flow and mixing behavior in a new bottom blown oxygen copper smelting furnace, and the model validation was carried out through a water model experiment. The effects of different nozzle locations, nozzle numbers, and gas flow rates on the gas-liquid flow, gas total volume, and mixing efficiency were investigated. The results show that the gas-liquid two-phase flow and mixing time predicted by the present model agree well with the experimental data. When the nozzles are located near the center of the bath bottom, the gas total volume is larger, but the mixing efficiency is very low. With the increase of nozzle arrangement angle, the mixing time decreased. However, the excessive angle arrangement of nozzles exceeding 21° was found to be detrimental to the bubble residence time and mixing efficiency. With the increase in nozzle numbers from nine to 13, the gas total volume in the furnace increases, and the mixing efficiency does not change greatly. When the number of nozzles is further increased to 18, the mixing efficiency begins to decrease significantly. As the gas flow rate increases from 4.7 m /h to 14.1 m /h, the gas total volume in the furnace increases, and the mixing time is rapidly reduced from 314.5 s to 251.5 s. When the gas flow rate exceeds 18.8 m /h, the gas total volume and mixing efficiency change little.</abstract><cop>Switzerland</cop><pub>MDPI AG</pub><pmid>31744044</pmid><doi>10.3390/ijms20225757</doi><orcidid>https://orcid.org/0000-0001-6017-1168</orcidid><oa>free_for_read</oa></addata></record>
fulltext fulltext
identifier ISSN: 1422-0067
ispartof International journal of molecular sciences, 2019-11, Vol.20 (22), p.5757
issn 1422-0067
1661-6596
1422-0067
language eng
recordid cdi_doaj_primary_oai_doaj_org_article_e500137da74e4848a2bf3d5846399e39
source Publicly Available Content Database (Proquest) (PQ_SDU_P3); PubMed Central Free
subjects bottom blown
Copper
Copper - chemistry
copper smelting
Efficiency
Flow velocity
Fluid dynamics
Gas flow
gas-liquid flow
Gases - chemistry
Liquid flow
Metallurgy
mixing behavior
modeling
Models, Theoretical
Monitoring
Nozzles
Oxygen - chemistry
Smelting
Smelting furnaces
Two phase flow
Water - chemistry
title Flow and Mixing Behavior in a New Bottom Blown Copper Smelting Furnace
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-02T17%3A59%3A45IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_doaj_&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Flow%20and%20Mixing%20Behavior%20in%20a%20New%20Bottom%20Blown%20Copper%20Smelting%20Furnace&rft.jtitle=International%20journal%20of%20molecular%20sciences&rft.au=Shao,%20Pin&rft.date=2019-11-16&rft.volume=20&rft.issue=22&rft.spage=5757&rft.pages=5757-&rft.issn=1422-0067&rft.eissn=1422-0067&rft_id=info:doi/10.3390/ijms20225757&rft_dat=%3Cproquest_doaj_%3E2333601517%3C/proquest_doaj_%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c478t-da50d46a18b52189deef203796548cd64dd5d08ffda73b561946c6340f833f1b3%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=2333601517&rft_id=info:pmid/31744044&rfr_iscdi=true