高粘度陆基油流模型

D. Mendelsohn, E. Comerma, Matthew Bernardo, Jeremy Fontenault, S. Baboolal
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摘要

高粘度油与其他常规液态烃混合物的性能不同。为了评估潜在的陆基井喷对周围环境的影响,RPS采用了多步骤方法来模拟高粘度原油下坡流动的轨迹和命运。如果泄漏到陆地上,最初温暖的石油会冷却并趋于凝胶,这意味着非牛顿流体。为了预测高粘度原油在下坡、扩散和冷却过程中的行为,RPS开发了一种新的、独特的陆地溢油模型。高粘度原油的行为与火山熔岩流有许多相似之处,特别是当流体冷却时,石油粘度和剪切应力的明显变化。本研究描述了一种“熔岩”流动数值模型,用于模拟高粘度油的响应。粘性流动模型基于Griffiths(2000)的熔岩模型,该模型模拟了Bingham流体沿恒定斜率平面的无约束运动。该模型允许所有物理和化学参数在下坡连续变化。假定横向流动在坡间压力梯度被基底屈服应力平衡时停止,并给出流动中心线上的流动高度(H)作为剪切应力的函数。对于油流运动,下坡压力梯度必须大于油剪应力,因此存在一个基于局部油剪应力和斜率的临界高度,低于此高度将不会有下坡运动。将大气换热方程应用于油表面作为表面边界条件。将该模型应用于高粘原油一维下坡式陆地释放的假设,假定地面坡度沿流道恒定。随着油的下坡,每个单元的温度会在每个时间步被更新,并用于计算新的油性质,如密度、比热、粘度和剪切应力。模型结果提供了下坡水流停止的速率、总距离和时间等信息。
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High Viscosity Land Based Oil Flow Model
Highly viscous oil does not behave the same as other regular liquid hydrocarbon mixtures. To evaluate the effects of a potential land-based blowout on the surrounding environment, RPS implemented a multi-step approach to simulate the trajectory and fate of high viscosity oil downslope flow. If spilled on land, initially warm oil cools and tends to gel, implying a non-Newtonian flow. To predict the behavior of high viscosity oil as it flows downslope, spreads and cools, RPS developed a new unique land-based spill model. The behavior of highly viscous crude oil has many similarities to volcanic lava flows, particularly the stark changes in oil viscosity and shear stress as the fluid cools. This study describes a “lava” flow numerical model developed to simulate the response of high viscosity oils. The viscous flow model is based on the lava model of Griffiths (2000) which simulates the unconfined motion of a Bingham fluid down a plane of constant slope. The model allows all physical and chemical parameters to vary continuously downslope. The lateral flow is assumed to cease when the cross-slope pressure gradient is balanced by the basal-yield stress also giving the height of the flow (H) on the center line of the flow as a function of shear stress. For oil flow motion the downslope pressure gradient must be greater than the oil shear stress and hence there is a critical height, based on the local oil shear stress and slope, below which there will be no downslope motion. An atmospheric heat transfer equation was applied to the oil surface as the surface boundary condition. The model was applied to a hypothetical on land release of highly viscous oil in a one-dimensional, downslope form, where the ground slope was assumed constant along the flow path. As the oil progresses downslope, its temperature was updated each time step in each cell and used to calculate new oil properties for density, specific heat, viscosity, and shear stress. The model results provide information about the rate and total distance travelled and time for the downslope flow to stop.
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