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IN SITU EVALUATION OF VAPOR PROPERTIES USING CONDENSED VAPOR GAMMA

机译:利用冷凝蒸气伽玛原位评估蒸气特性

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Gamma ray (GR) logs from infill wells in heavy oil development projects frequently exceed 1000 GAPI, but only through the hot vapor cloud that develops as injected steam displaces heavy oil. GR values in the same sands that are liquid-filled, and immediately below the vapor-filled rock, are typically less than 100 GAPI. Previous work (O’Sullivan, 2008) shows that high GR values are caused by drilling-related cooling of vapor-filled rock. GR is thought to increase when water- and hydrocarbon-molecules, with solubilized radon atoms attached, are concentrated by 100 times or more as they approach the dew point and condense around a chilled well. After the chilled well begins to re-heat and equilibrate with the hot reservoir (36 hours or less) GR returns to normal levels. An experiment demonstrated that the cycle of GR increase and decrease can be repeated indefinitely, simply by chilling the well and then allowing it to warm back.Samples of the condensed vapor have not been acquired, nor has condensed vapor gamma (“CVG”) been generated in a lab under controlled conditions, so much remains to be learned about the nature of CVG, and how it can be used to understand reservoir processes.To put the condensed vapor gamma (CVG) effect into context, logs from thousands of heavy oil development wells from two large oil fields of the San Joaquin Valley, California were systematically reviewed. GR logs through vapor-filled rock for reservoirs in Midway-Sunset Field show that CVG amplitude is higher (≈ 2000 GAPI) in poorly-sorted rocks than in well-sorted clean sands (≈ 200 GAPI). The difference is driven by higher residual oil saturation in poorly-sorted rocks. Higher radon solubility and vapor pressure for oil, compared to water, lead to higher CVG values.GR logs through well-sorted sands in Belridge Field, were anticipated to be low, and similar to those for well-sorted sands in Midway-Sunset Field. Instead, the CVG amplitude is unexpectedly high, exceeding 10,000 GAPI. A cross section of seven closely-spaced wells, drilled within an eight-year time span, shows that these very high GR values strongly correlate within a 60-foot interval. For the entire field, maps that track the year-by-year onset of high GR show interesting, but unexplained patterns that are restricted to limited areas and time intervals.The difference between the CVG responses in the two fields may be explained by the observation that, for Belridge Field, the very high GR values occurred years after the steam flood on this reservoir peaked, during the time when development of a deeper reservoir containing light hydrocarbons was accelerating. CVG amplitude may have increased when the heavy oil vapor cloud was overprinted with light hydrocarbon from the deeper reservoir. With the light hydrocarbon, vapor pressure increases and improves the efficiency of radon absorption.The observations suggest that, under certain conditions, it is possible to develop a method for in situ evaluation of vapor properties. Although the condensation-induced gamma signal has only been documented to occur in wells drilled in heavy oil steam floods, the effect could occur in any reservoir containing condensable vapor, provided that the vapor can be cooled to the dew point. Applications include evaluation of vapor composition, identification of barriers, and time-lapse monitoring of changes in vapor properties as an indicator of enhanced recovery process efficiency.Controlled generation of CVG in the laboratory is a logical next step toward improved understanding of this phenomena. Continuous in situ observation and monitoring of CVG is also recommended, in order to explore the linkage between CVG and development activities.
机译:重油开发项目中的填充井中的伽马射线(GR)测井经常超过1000 GAPI,但仅通过注入蒸汽驱替重油时产生的热蒸气云形成。在充满液体的同一砂岩中,紧接在充满蒸气的岩石下面的GR值通常小于100 GAPI。先前的工作(O’Sullivan,2008年)表明,高GR值是由与钻进有关的蒸气填充岩石的冷却引起的。人们认为,当附着了ra原子的水和碳氢化合物分子接近露点并在冷却的井中冷凝时,其浓缩程度将达到100倍或更多,从而GR会增加。冷却后的井开始重新加热并与热储层平衡(36小时或更短)后,GR恢复到正常水平。实验表明,只需将井冷却然后使其回温即可无限期重复GR增大和减小的循环。 尚未获得冷凝蒸汽的样本,也没有在受控条件下在实验室中产生冷凝蒸汽伽玛(“ CVG”),因此,关于CVG的性质以及如何使用它来了解储层还有很多知识要学习。流程。 为了将凝结的凝析气伽玛(CVG)效应作为背景,对来自加利福尼亚州圣华金河谷两个大型油田的数千个重油开发井的测井资料进行了系统地审查。通过中途日落油田储集层的蒸气充填岩石的GR测井表明,分类不好的岩石的CVG振幅(≈2000 GAPI)要比分类良好的干净沙子(≈200 GAPI)要高。差异是由分类不良的岩石中较高的残余油饱和度驱动的。与水相比,油的ra溶解度和蒸气压更高,导致CVG值更高。 预计在Belridge田地中经过良好分类的沙子的原木原木很低,与中途日落田地中经过良好分类的沙子的原木相似。取而代之的是,CVG振幅出乎意料的高,超过了10,000 GAPI。在八年的时间跨度内钻出的七个紧密间隔的井的横截面表明,这些非常高的GR值在60英尺的间隔内具有很强的相关性。对于整个领域,跟踪逐年出现高GR的地图显示出有趣的但无法解释的模式,这些模式仅限于有限的区域和时间间隔。 可以通过以下观察解释这两个油田之间的CVG响应之间的差异:对于Belridge油田,该油藏的蒸汽驱达到峰值后数年,即在开发一个较深的含轻烃的油藏期间,发生了非常高的GR值。在加速。当重油蒸气云被深层储层中的轻烃覆盖时,CVG振幅可能会增加。使用轻质烃,蒸气压增加并提高了absorption的吸收效率。 观察结果表明,在某些条件下,有可能开发一种就地评估蒸气性质的方法。尽管冷凝水诱发的伽马信号仅被记录在重油蒸汽驱钻井中,但只要能将其冷却至露点,任何含有可冷凝蒸气的油藏都可能发生这种影响。其应用包括评估蒸气成分,确定障碍物以及对蒸气性质变化进行时延监视,以作为提高回收工艺效率的指标。 在实验室中控制CVG的产生是朝着对这种现象的更好理解的逻辑下一步。还建议对CVG进行连续的原位观察和监测,以探索CVG与发展活动之间的联系。

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