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Fighting invisible kicks: Study of Time Dependent Vaporization of Methane Gas Dissolved in Base Oil

机译:战斗隐形踢:研究溶解在基础油中甲烷气体的时间依赖性汽化

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Understanding the interaction between the drilling fluid and the natural gas from a gas kick may be of great importance when predicting how a well control incident evolves during drilling operations. This is especially true for oil based mud, which has the ability to dissolve large quantities of gas under high pressure, thus potentially hide any volumetric impact of a gas kick. When the pressure of the dissolved gas decreases below the bubble pressure, free gas will start to emerge. Dangerous situations can occur if the bubble point pressure is low and located close to the surface. This may result in a rapid volumetric expansion of the free gas, as it emerges from solution, thus little to no time to react and initiate proper well control procedures. Most conventional well control simulators that takes gas solubility into consideration assumes an instantaneous vaporization of gas as the vapour-liquid phase equilibria changes. However, this assumption might not always be realistic. It may take some time before a new equilibrium is reached when the conditions are changed. This will thus affecting the rate of gas liberation from the liquid. To better understand this complex issue, an analytical expression for the transition rate of dissolved gas to free gas in a supersaturated liquid has been derived for low pressure systems. The analytical model is strongly dependent on the solubility coefficient. K_h, and the transition rate factor, γ, and follows an exponential curve. In this expression, K_h is a measure of how much the liquid is supersaturated at any given time and controls how much gas that will be liberated. γ determines how fast the system will reach a new equilibrium, i.e. how fast the gas will be liberated based on the size of the supersaturation. Both K_h and γ are thought to be values given for a specific gas-liquid combination. In order to verify the analytical expression, experimental testing has been conducted. The experiment is carried out by pressurizing a tank partly filled with the base oil Exxsol D60 by feeding it with methane gas. Some of the gas will dissolve into the liquid. The rest will flow to the top as free gas and pressurize the tank. By quickly removing some of the free gas, thus depressurize the tank, the liquid will instantaneously become supersaturated, hence triggering liberation of free gas from the solution until a new equilibrium is established. By measuring the tank pressure throughout the degassing phase, values for K_h and γ can be estimated and compared to the analytical model.
机译:理解钻井液与来自气体踢的天然气之间的相互作用可能是非常重要的,当预测在钻井操作期间的井控制事件如何发展时都具有重要意义。对于油基泥浆尤其如此,能够在高压下溶解大量气体,因此可能隐藏气体踢的任何体积影响。当溶解气体的压力降低低于气泡压力时,将开始出现游离气体。如果气泡点压力低,并且靠近表面,则可能发生危险情况。这可能导致自由气体的快速膨胀,因为它从溶液中出现,因此很少没有时间反应和启动适当的井控制程序。考虑到气体溶解度的大多数传统孔控制模拟器假设气体瞬时蒸发,因为气液相平衡变化。但是,这个假设可能并不总是逼真的。在改变条件时达到新的平衡之前可能需要一段时间。因此,这将影响来自液体的气体释放速率。为了更好地理解这种复杂问题,已经推导出用于低压系统的过饱和液体中溶解气体到空气中的溶解气体过渡率的分析表达。分析模型强烈依赖于溶解度系数。 K_H,以及过渡率因子,γ和遵循指数曲线。在这种表达中,K_H是在任何给定时间在任何时间过度饱和液体的量度,并控制将释放多少气体。 γ确定系统达到新均衡的速度,即基于过饱和度的大小释放天气的速度。 K_H和γ都被认为是特定气液组合给出的值。为了验证分析表达,已经进行了实验测试。通过用甲烷气体进料,通过将部分填充有基础油exxsold60的罐加压来进行实验。一些气体将溶于液体中。其余的将流到顶部作为自由气体并加压罐。通过快速除去一些自由气体,从而减压罐,液体将瞬间变过饱和,因此触发从溶液中释放自由气体直至建立新的均衡。通过在整个脱气阶段测量罐压力,可以估计K_H和γ的值并将其与分析模型进行比较。

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