期刊文献+

利用D-D中子发生器进行补偿中子孔隙度测井的模拟研究 被引量:7

Monte Carlo Simulation on Compensated Neutron Porosity Logging with D-D Neutron Generator
下载PDF
导出
摘要 利用蒙特卡罗方法模拟研究了D-D脉冲中子源和Am-Be中子源产生的中子与地层的作用过程。得到热中子计数随着源距增加而呈指数下降,源距小于20cm时D-D中子管的热中子相对计数高于Am-Be中子源;源距大于20cm时比Am-Be中子源低。在低孔隙度(小于20%)地层D-D中子管补偿中子孔隙度测井的热中子计数比值略大于Am-Be中子源;高孔隙度(大于20%)地层D-D中子管的热中子计数比值远远大于Am-Be中子源,对地层孔隙度灵敏度增加。与Am-Be中子源相比,D-D中子管补偿中子孔隙度测井的探测深度略为降低,地层孔隙度测量的灵敏度增加,因此利用D-D中子管可以进行补偿中子孔隙度测井。 The process of neutron interaction induced by D-D neutron tube and Am-Be source is simulated using Monte Carlo method. It is concluded that the thermal neutron count descend exponentially as the spacing increases. When the spacing is less than 20 cm, relative count of thermal neutron induced by D-D neutron tube is higher than that by Am-Be neutron source. However, the conclusion is opposite when the spacing is more than 20 cm. In low porosity (less than 20%) formation, the ratio of thermal neutron count in near and far spacing generated by D-D neutron tube is slightly larger than that generated by Am-Be neutron source; but in high porosity (more than 20%) formation, the ratio of thermal neutron count generated by D-D neutron tube is much larger than that generated by AmBe neutron source, so that it increases the sensitivity to formation porosity. Its reflection to porosity is more sensitive if the porosity is higher. In addi- tion, compared with Am-Be neutron source, depth of detection with D-D neutron tube is slightly decreased, and the sensitivity of measurement to the formation porosity increases. Therefore, the compensated neutron porosity logging by using D-D neutron tube is feasible.
作者 张锋 袁超
出处 《测井技术》 CAS CSCD 北大核心 2010年第3期227-232,共6页 Well Logging Technology
基金 国家自然科学基金随钻脉冲中子双孔隙度测井方法基础研究(基金号:40874065)资助
关键词 放射性测井 DD中子管 补偿中子孔隙度测井 探测特性 蒙特卡罗模拟 radioactivity logging, D-D neutron tube, compensated neutron porosity logging, detection characteristics, Monte Carlo simulation
  • 相关文献

参考文献18

  • 1黄隆基.核测井原理[M].东营:中国石油大学出版社,2000.
  • 2姬铜芝,刘杰,申建辉,陈世英,王峰.BZC-IB型补偿中子测井仪及其应用[J].石油仪器,2006,20(6):48-50. 被引量:4
  • 3闫水浪,李养刚,袁昌林,班占全,高士文.高精度遥测补偿中子测井仪[J].石油仪器,2003,17(6):35-36. 被引量:3
  • 4Clark S B,Holenka J.Logging While Drilling:A Three-year Perspective[J].Oilfield Review,1992:30-44.
  • 5Holenka J,Best D,Evans M,et al.Azimuthal Porosity While Drilling[C] // SPWLA 36th Annual Logging Symposium,1995.
  • 6Aitken J D,Adolph R,Evans M,et al.Radiation Sources in Drilling Tools:Comprehensive Risk Analysis in the Design,Development and Operation of LWD Tools[J].SPE73896,2002.
  • 7Weller G,EI-Halawani T,Tribe I,et al.A New Integrated LWD Platform Delivers Implovement Drilling Efficiency,Well Placement,and Formation Evaluation Services[C] //SPE96652,2005.
  • 8Scott Fricke,David P Madio.Thermal Neutron Porosity Using Pulsed-neutlon Measurements[C] //SPWLA 49th Annual Symposium,2008,Paper L.
  • 9Weller G,Griffiths R,Stoller C,et al.A New Integrated LWD Platform Brings Next-generation Formation Evaluation Services[C] //SPWLA 46th Annual Symposium,2005,Paper H.
  • 10Durisi E,Zanini A,Manfredotti C,et al.Design of an EpithermalColumn for BNCT Based on D-D Fusion Neutron Facility[J].Nuclear Instruments and Methods in Physics Research:A,2004,574(1):363-369.

二级参考文献9

  • 1黄隆基.核测井原理[M].东营:石油大学出版社,2001..
  • 2BROWNE E and FIRESTONE R B.Table of Radioactive Isotopes[M].New York:John Wiley & Sons,Inc,1996.
  • 3BRIESMEISTER J F,MCNP T M.A General Monte Carlo N-Particle Transport Code,Version 4C[S].Los Alamos National Laboratory Report LA-13709-M.
  • 4楼顺天, 陈生潭, 雷虎民.MATLAB 5.X 程序设计语言.西安电子科技大学出版社,2001
  • 5蒲卫军.CN241补偿中子测井仪维修手册.西安石油勘探仪器总厂,2002(资料)
  • 6北京七院华力石油设备开发中心.BZC-IB补偿中子测井仪维修手册.1998(资料).
  • 7康华光.电子技术基础简明教程(模拟部分)[M].北京:高等教育出版社,1990.
  • 8陈序三.一种新型储层饱和度测井方法及应用[J].测井技术,2001,25(2):105-109. 被引量:15
  • 9吴文圣.多探测器硼中子伽马测井的可行性[J].测井技术,2003,27(5):369-372. 被引量:6

共引文献22

同被引文献54

引证文献7

二级引证文献22

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部