断裂静止期有无输导油气能力的判别方法

通过断裂内部结构及输导通道特征研究,得到断裂静止期输导油气通道主要是碎裂岩的连通孔隙,其是否具有输导油气能力主要取决于碎裂岩颗粒粒度、泥质含量和断裂倾角大小。在此基础上,利用物理模拟实验模拟了油气在浮力作用下沿断裂碎裂岩运移速度与碎裂岩颗粒粒度、泥质含量和断裂倾角之间的关系。利用此关系建立了一套断裂静止期有无输导油气能力的判别方法,即运移速度大于零,断裂具输导油气能力,反之则无。并将其应用于海拉尔盆地苏仁诺尔断裂静止期在各组地层中有无输导油气能力的判别中,其结果与地下油气分布情况相符,表明该方法定量判别断裂静止期有无输导油气能力是可行的。     

油气沿不同时期断裂穿过泥岩盖层渗滤散失的地质条件及其识别方法

为了研究含油气盆地断裂发育区油气分布规律,在确定油气沿活动期和静止期断裂穿过泥岩盖层发生渗滤散失机理的基础上,针对油气沿活动期和静止期断裂穿过泥岩盖层渗滤散失的地质条件及识别方法进行了研究。研究结果表明：油气沿活动期断裂穿过泥岩盖层渗滤散失所需的地质条件是活动期断裂在盖层内上下连接分布,作为油气穿过泥岩盖层的输导通道;油气沿静止期断裂穿过泥岩盖层渗滤散失所需的地质条件是下伏储层油气剩余压力大于断层岩排替压力。通过比较泥岩盖层断接厚度与油气沿活动期断裂穿过泥岩盖层渗滤散失所需最小断接厚度的相对大小和下伏储层剩余压力与断层岩排替压力的相对大小,分别建立了油气是否沿活动期断裂和静止期断裂穿过泥岩盖层渗滤散失的识别方法,并将其应用于渤海湾盆地南堡凹陷南堡5号构造天然气能否通过活动期和静止期NP5 2断裂穿过东二段泥岩盖层渗滤散失的识别。结果表明：在断裂活动期,仅在L2和L8测线处天然气可以沿着NP5 2断裂穿过东二段泥岩盖层渗滤散失,其余测线处(L1、L3、L4、L5、L6、L7、L9)则不能;但是在断裂静止期,天然气不能沿NP5 2断裂穿过东二段泥岩盖层渗滤散失,与目前南堡5号构造东二段泥岩盖层之下已发现的天然气分布相吻合,表明这2种方法分别用于识别油气是否通过静止期断裂和活动期断裂穿过泥岩盖层渗滤散失是可行的。     

逆断层中天然气运移特征的物理模拟

逆断层在活动期时易形成断层空腔,该空腔为天然气的穿层运移提供了畅通的通道,天然气在其中运移具涌流特征。如果断层空腔连通地表,天然气则大部分沿其逸出地表,仅有少量的天然气能注入断层两侧的相邻储层中。进入储层的天然气具有明显的选择性,气体首先向物性好、倾角陡和埋藏浅的储层中注入。如果没有其它动力,仅靠天然气自身浮力作用,断层下盘储层不能或很少能有天然气的注入。当断层处于静止期时,断层空腔消亡,天然气穿塑性层段的运移通道是破碎带中的岩石孔隙,天然气在其中的运移遵循达西渗流规律。天然气在断层带中的运移速度随断层充填物颗粒粒度的增加而呈指数关系增大,随断层倾角的增大呈指数关系增大,随断层充填物中泥质含量的增加呈幂函数关系减小。     

Characterization of Stratospheric Aerosol Distributions during the Volcanically Quiescent Period of 1998–2004

The Stratospheric Aerosol and Gas Experiment （SAGE） II aerosol extinction profiles at 1020 nm were used to study the distribution characteristics of stratospheric aerosols during the volcanically quiescent period of 1998-2004. The stratospheric aerosol distributions exhibited hemispheric asymmetry between the Northern Hemisphere （NH） and the Southern Hemisphere （SH）. In the lower stratosphere below 20 km, the zonal averaged aerosol optical depths in the NH were higher than those of the corresponding SH; whereas at higher altitudes above 20 km, the optical depths in the SH-- except the equatorial region--were higher than those of the NH. At 0-10°N and 10-20°N, the stratospheric aerosol optical depth （SAOD） exhibited larger values in boreal winter and lower values in the spring and summer; at 0-10°S and 10-20°S, the SAOD presented small seasonal variations. At 30-40°N, the SAOD presented larger values in the boreal fall and winter and lower values in the spring and summer; while at 30-40°S, the SAOD exhibited larger values in the austral winter and early spring and lower values in the summer and fall. These characteristics can mainly be attributed to the seasonal cycle of the dynamic transport, and the effects of the buildup and breakdown of the polar vortex. At 50-60°S, the SAOD exhibited extremely high values during austral winter associated with the Antarctic polar vortex boundary; at 50-60°N, the SAOD also exhibited larger values during the boreal winter, but it was much less obvious than that of its southern counterpart.