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Experimental Determination of Optimized Production Rate and Its Upscaling Analysis in Strong Water Drive Gas Reservoirs

机译:强水驱储气储层优化生产率及其升高分析的实验测定

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Gas reservoirs were founded as clean and valuable energy sources. Gas recovery from strong water drive gas reservoirs (WDGR) may decrease because water influx may trap gas. The gas is trapped as an immobile phase. WDGR performance is complicated and depends on many parameters and uncertainty associated with reservoirs. In WDGR, accelerating production rate can let more gases scape but question is accelerating with what flow rate. We investigated the optimum accelerating production rate on WDGR recovery in laboratory scale systems. The experimental flow rates were designed over reasonable range by considering critical rate and Darcy flow condition in first step. By determining optimum flow rate from experiments, the upscaling processes were implemented with a defined theoretical “Sarab” Dimensionless Time Number (TDS) and it was verified by comparing with others porous media length (from 40cm length to 8 cm and 1 meter) .The experimental models were contained distinct gas and water zone (aquifer portion) with thickness proportion of one to two. Gas zone was exposed in initial water saturation in all of experiments. These permeable media were systematically characterized in three lengths. Dimensionless numbers were applied to adequately design the experiments. The pressure operational condition was 3160 psia. We found that optimum flow rate for a WDGR can be obtained in laboratory scale and then can be applied into larger models as well as reservoir sizes with corresponding scale factor of TDS. Connecting of this laboratory flow rate into field application with TDS can be a new revelation into gas recovery and development management of WDGR.
机译:气体储层成立为清洁和有价值的能源。来自强水驱动气体储层(WDGR)的气体回收可能降低,因为水流入可以捕获气体。气体被捕获为固定相。 WDGR性能复杂且取决于许多与储层相关的参数和不确定性。在WDGR中,加速生产率可以让更多的气体景观,但问题正在加速流速。我们调查了在实验室规模系统中对WDGR回收的最佳加速生产率。通过考虑第一步中的临界速率和达西流动条件,在合理范围内设计了实验流速。通过从实验中确定最佳流速,用规定的理论“Sarab”无量纲时间数(TDS)实现了上升过程,并且通过与其他多孔介质长度(从40cm长到8cm和1米)进行验证。实验模型含有不同的气体和水区(含水层部分),厚度比例为一到两个。在所有实验中,气体区暴露在初始水饱和度中。这些可渗透的介质以三个长度系统地表征。应用无量纲数量以充分设计实验。压力运行条件为3160psia。我们发现,可以在实验室规模中获得WDGR的最佳流速,然后可以应用于较大的模型以及具有相应TDS的比例因子的储层大小。将该实验室流量的连接与TDS的现场应用可能是对WDGR气体回收和发展管理的新启示。

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