Article(id=1314917563621015883, tenantId=1146029695717560320, journalId=1234093305789726721, issueId=1314917454552327005, articleNumber=null, orderNo=null, doi=null, pmid=null, cstr=null, oa=null, hot=null, price=null, onlineType=0, articleFormat=0, articleType=null, articleTypeStr=null, receivedDate=1731340800000, receivedDateStr=2024-11-12, revisedDate=null, revisedDateStr=null, acceptedDate=null, acceptedDateStr=null, onlineDate=1791430377154, onlineDateStr=2026-10-08, pubDate=1752940800000, pubDateStr=2025-07-20, doiRegisterDate=null, doiRegisterDateStr=null, onlineIssueDate=1791430377154, onlineIssueDateStr=2026-10-08, onlineJustAcceptDate=null, onlineJustAcceptDateStr=null, onlineFirstDate=null, onlineFirstDateStr=null, sourceXml=null, magXml=null, createTime=1791430377154, creator=13701087609, updateTime=1791430377154, updator=13701087609, issue=Issue{id=1314917454552327005, tenantId=1146029695717560320, journalId=1234093305789726721, year='2025', volume='45', issue='7', pageStart='3553', pageEnd='4144', issueExtLink='null', onlineDate='null', pubDate='1752940800000', pubDateStr='2025-07-20', beforeIssueId=null, nextIssueId=null, price=null, status=1, issueComplete=1, articleOrder=1, issueType=-1, specialIssue=null, createTime=1791430351150, creator='13701087609', updateTime=1791431931754, updator='13701087609', preIssue=null, nextIssue=null, articleTotal=null, ext={EN=IssueExt(id=1314924084186669335, tenantId=1146029695717560320, journalId=1234093305789726721, issueId=1314917454552327005, language=EN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=), CN=IssueExt(id=1314924084186669336, tenantId=1146029695717560320, journalId=1234093305789726721, issueId=1314917454552327005, language=CN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=)}, issueFiles=null, downloadFileDto=null}, startPage=3944, endPage=3953, ext={EN=ArticleExt(id=1314917563834925388, articleId=1314917563621015883, tenantId=1146029695717560320, journalId=1234093305789726721, language=EN, title=A comparative investigation of the monitoring effects of DNAPL infiltration and remediation processes based on ERT and image method, columnId=1234106388083954308, journalTitle=China Environmental Science, columnName=Environmental Ecology, runingTitle=null, highlight=null, articleAbstract=
Based on the indoor two-dimensional sandbox DNAPL remediation experiment, the changes of DNAPL were monitored by the imaging method and the resistivity imaging method to evaluate the effectiveness and feasibility of the resistivity imaging method for monitoring. The results showed that: In the DNAPL infiltration experiment, both the resistivity imaging method and the imaging method could reflect that the DNAPL infiltration was mainly vertical and was mainly affected by gravity. Through the spatial moment analysis of the saturations obtained by the two methods, it was found that the trends of the horizontal centroids of the two methods were quite different, while the trends of the changes in the vertical centroid positions were basically the same. In the DNAPL remediation experiment, with the injection of the SDS solution, the relative resistivity value at the center of the DNAPL pollutant decreased from 25 Ω·m to - 10 Ω·m, and the saturation decreased from 0.42 to 0.15. When the correlation analysis was carried out at specific positions in the sandbox, the correlations between resistivity and saturation were 0.72, 0.84, and 0.92 respectively, and the correlation coefficients were all greater than 0.6, indicating that the two monitoring methods had consistency in interpreting the remediation process. By comparing the monitoring effects of the two methods on the DNAPL infiltration and remediation processes, it was found that during the infiltration process, the imaging method had a better monitoring effect. The imaging method could provide high - precision infiltration images and had a meticulous ability to capture the dynamic changes of DNAPL. During the remediation process, the resistivity imaging method had a better effect. The resistivity imaging could penetrate the medium to monitor the diffusion of the surfactant in different layers and spaces and obtain the macroscopic distribution trend.
, authors=Heng LIU, Han-le LIU
*, Wen-han CAO, authorsList=Heng LIU, Han-le LIU, Wen-han CAO, authorCompany=null, correspAuthors=Han-le LIU, authorNote=null, correspAuthorsNote=null, copyrightStatement=null, copyrightOwner=null, extLink=null, articleAbsUrl=null, sourceXml=null, magXml=null, pdfUrl=null, pdf=null, pdfFileSize=null, pdfExtLink=null, richHtmlUrl=null, mobilePdfUrl=null, reviewReport=null, pdfFirstPage=null, abstractGraph=null, abstractGraphContent=null, abstractVideo=null, citation=null, cebUrl=null, magXmlContent=null, mapNumber=null, fund=null), CN=ArticleExt(id=1314917564224995661, articleId=1314917563621015883, tenantId=1146029695717560320, journalId=1234093305789726721, language=CN, title=基于ERT与图像法的DNAPL入渗和修复过程监测, columnId=1234106388268503686, journalTitle=中国环境科学, columnName=环境生态, runingTitle=null, highlight=null, articleAbstract=
以室内二维砂箱DNAPL修复实验为基础,通过图像法和电阻率成像法对DNAPL的变化进行监测,评估电阻率成像法监测的有效性和可行性.结果表明:在DNAPL入渗实验中,电阻率成像法和图像法均能反应出DNAPL入渗以垂向入渗为主,主要受重力影响.对两种方法所获得的饱和度进行空间矩分析,发现两种方法的水平质心趋势差距较大,垂向质心位置变化趋势基本一致.在DNAPL的修复实验中,随着SDS溶液的注入,DNAPL污染物中心的相对电阻率值从25 Ω·m降至-10 Ω·m,饱和度从0.42降至0.15.选取砂箱特定位置进行相关性分析,电阻率与饱和度的相关性分别为0.72、0.84和0.92,相关性系数均大于0.6,说明两种监测手段对修复过程的解释具有一致性.通过2种方法对DNAPL入渗和修复过程的监测效果比较,在入渗过程中,图像法的监测效果更好,图像法可以提供高精度的入渗图像,特别是对DNAPL的动态变化有着细致的捕捉能力;在修复过程中,电阻率成像法的效果更好,电阻率成像法可以电阻率成像能够穿透介质,实现对表面活性剂在不同层位和空间中的扩散情况监测,获取宏观分布趋势.
, authors=刘恒, 刘汉乐
*, 曹文翰, authorsList=刘恒, 刘汉乐, 曹文翰, authorCompany=null, correspAuthors=刘汉乐, authorNote=
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刘恒(1999-),男,吉林四平人,桂林理工大学硕士研究生,主要研究方向为地下水DNAPL污染物监测.3112600195@qq.com.
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刘恒(1999-),男,吉林四平人,桂林理工大学硕士研究生,主要研究方向为地下水DNAPL污染物监测.3112600195@qq.com.
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