The Relationship Between the Shape of a Disced Core and Three-Dimensional in-Situ Stresses Estimated by a Tensile Principal Stress Analysis.

K. Matsuki, K. Hongo, K. Sakaguchi
{"title":"The Relationship Between the Shape of a Disced Core and Three-Dimensional in-Situ Stresses Estimated by a Tensile Principal Stress Analysis.","authors":"K. Matsuki, K. Hongo, K. Sakaguchi","doi":"10.2473/SHIGENTOSOZAI.113.317","DOIUrl":null,"url":null,"abstract":"Based upon the assumption that core discing results from tensile stresses within and below a core during boring, the direction of the principal tensile stress was analyzed in detail for the stress conditions where core discing is likely to occur to investigate the relationship between the shape of a disced core and in-situ stresses for the case of a long disced core. Main results obtained in this study are summarized as follows: 1) In the central parts of the end surfaces, a relatively flat plane is formed. The azimuth of the normal direction of the plane coincides with that of the minimum principal stress, ƒÐ3. The inclination, Om of the normal direction from the core axis is approximately one thirds of that,.753 of ƒÐ3. By using the two equations, (1) and (3), a method for estimating more accurate ƒÓ3 (•}23%) was proposed. 2) By combining the additional equation, (1) on the magnitudes of ƒÐ3, the mean stress, um and the stress in the direction of the core axis, aZ with the previously proposed equation, (2), which is the condition of core discing, two of the above stresses can be determined if Om is measured and if one of them is determined independently. For the vertical borehole, by assuming uz to be an overburden pressure, um and u3 can be determined from the two equations. 3) When the difference between the maximum principal stress, ƒÐ1 and the intermediate principal stress, σ2 is large enough, a saddle shaped disc is formed and the shape becomes more distinct with the difference.For","PeriodicalId":22754,"journal":{"name":"The Mining and Materials Processing Institute of Japan","volume":"11 1","pages":"317-324"},"PeriodicalIF":0.0000,"publicationDate":"1997-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"The Mining and Materials Processing Institute of Japan","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.2473/SHIGENTOSOZAI.113.317","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 3

Abstract

Based upon the assumption that core discing results from tensile stresses within and below a core during boring, the direction of the principal tensile stress was analyzed in detail for the stress conditions where core discing is likely to occur to investigate the relationship between the shape of a disced core and in-situ stresses for the case of a long disced core. Main results obtained in this study are summarized as follows: 1) In the central parts of the end surfaces, a relatively flat plane is formed. The azimuth of the normal direction of the plane coincides with that of the minimum principal stress, ƒÐ3. The inclination, Om of the normal direction from the core axis is approximately one thirds of that,.753 of ƒÐ3. By using the two equations, (1) and (3), a method for estimating more accurate ƒÓ3 (•}23%) was proposed. 2) By combining the additional equation, (1) on the magnitudes of ƒÐ3, the mean stress, um and the stress in the direction of the core axis, aZ with the previously proposed equation, (2), which is the condition of core discing, two of the above stresses can be determined if Om is measured and if one of them is determined independently. For the vertical borehole, by assuming uz to be an overburden pressure, um and u3 can be determined from the two equations. 3) When the difference between the maximum principal stress, ƒÐ1 and the intermediate principal stress, σ2 is large enough, a saddle shaped disc is formed and the shape becomes more distinct with the difference.For
查看原文
分享 分享
微信好友 朋友圈 QQ好友 复制链接
本刊更多论文
用张主应力分析估算岩心切面形状与三维地应力的关系。
基于钻孔过程中岩心内部和下方的拉应力导致岩心剥离的假设,详细分析了可能发生岩心剥离的应力条件下的主拉应力方向,以研究长岩心剥离的岩心形状与地应力之间的关系。本研究的主要结果总结如下:1)在端面的中心部分形成了一个相对平坦的平面。平面法向的方位角与最小主应力的方位角重合,ƒÐ3。法线方向从核心轴的倾斜度,大约是它的三分之一。753的ƒÐ3。利用(1)和(3)两个方程,提出了一种更准确的ƒÓ3(•}23%)估计方法。2)将附加式(1)ƒÐ3的大小、平均应力um和岩心轴向应力aZ与先前提出的公式(2)相结合,即岩心盘化的条件,即测量Om和单独确定其中一个时,可以确定上述两个应力。对于垂直井眼,假设uz为上覆岩层压力,可由这两个方程确定um和u3。(3)当最大主应力ƒÐ1与中间主应力σ2的差值足够大时,形成鞍状盘,且形状随着差值的增大而更加明显。为
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 去求助
来源期刊
自引率
0.00%
发文量
0
期刊最新文献
Hydrometallurgical Recovery of Tin from Harris Dross Recent Development of EAF Dust Treating at Shisaka Smelting Co., Ltd. Tin Treatment in Kosaka Lead Smelting Growth of Nodules in Copper Electrorefining: Numerical Simulation of Natural Convection Start-up and Improvements of the New Electrolysis Plant at Annaka Refinery
×
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
现在去查看 取消
×
提示
确定
0
微信
客服QQ
Book学术公众号 扫码关注我们
反馈
×
意见反馈
请填写您的意见或建议
请填写您的手机或邮箱
已复制链接
已复制链接
快去分享给好友吧!
我知道了
×
扫码分享
扫码分享
Book学术官方微信
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术
文献互助 智能选刊 最新文献 互助须知 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 Book学术 All rights reserved.
ghs 京公网安备 11010802042870号 京ICP备2023020795号-1