Measurement of Propane and Butane Diffusion into Heavy Oil using Microfluidics - Is Small Better?

Hongying Zhao, S. Pierobon, Adam Pettigrew, Jacques Doan-Prevost, O. Garnier, T. Haas
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引用次数: 2

Abstract

The high energy intensity of steam-based heavy oil extraction processes is leading the industry to investigate solvent-aided processes for heavy oil/bitumen recovery. The diffusion coefficient of solvent in heavy oil is a key parameter to determine how effective these processes are. Measuring the diffusion coefficient is challenging, especially at in-situ conditions, i.e., at elevated temperature and pressure. This paper presents a microfluidics-based method for measuring the diffusion coefficient of propane and butane, the most commonly used light hydrocarbons in solvent process, into heavy oil at high temperature and pressure conditions. A silicon-glass microfluidic chip was designed and fabricated using the Deep Reactive Ion Etching (DRIE) and anodic bonding. The diffusion tests were performed at temperatures ranging from 20°C to 120°C and pressures up to 100 bar. Upon blue light excitation, heavy oil naturally fluoresces at visible wavelengths, and the intensity varies with solvent concentration. Based on this mechanism, the light intensity change of the heavy oil in a 100-micron channel was recorded with a camera connected to the microscope during the diffusion process. An image processing method was developed accordingly to create a map of fluorescence light intensity versus diffusion time and distance, which was further processed numerically to calculate the diffusion coefficient with measured correlations between light intensity and solvent concentration. At all testing conditions both solvents were liquid which inevitably would cause asphaltene precipitation at oil-solvent interface as demonstrated by the observations during the diffusion tests. It was also found that the asphaltene precipitation phenomena were more pronounced with butane than propane. To measure the diffusion coefficient, a method using solvent diluted oil was developed to avoid the asphaltene precipitation issue. The measured diffusion coefficient of propane was around 0.6 × 10-10 m2/s using pure solvent method, and that of butane was in the range of 1—9 × 10-9 m2/s, at their corresponding testing conditions. For both solvents the diffusion coefficients increased with temperature while no satisfactory trend was observed with pressure within 100 bar.
用微流体测量丙烷和丁烷在重油中的扩散——小的更好吗?
蒸汽基稠油提取工艺的高能量强度促使业界研究溶剂辅助稠油/沥青回收工艺。溶剂在重油中的扩散系数是决定这些工艺效果的关键参数。测量扩散系数具有挑战性,特别是在原位条件下,即在高温高压下。本文提出了一种基于微流体的方法,用于测量溶剂法中最常用的轻烃丙烷和丁烷在高温高压条件下向重油中的扩散系数。采用深度反应离子刻蚀(Deep Reactive Ion Etching, DRIE)和阳极键合技术,设计并制备了硅玻璃微流控芯片。扩散试验的温度范围为20°C至120°C,压力可达100 bar。在蓝光激发下,重油自然发出可见波长的荧光,其强度随溶剂浓度而变化。基于这一机理,用连接在显微镜上的摄像机记录了重油在100微米通道内扩散过程中的光强变化。据此,开发了一种图像处理方法,创建荧光光强度与扩散时间和距离的关系图,并对其进行进一步的数值处理,以测量光强度与溶剂浓度之间的相关性来计算扩散系数。在所有的测试条件下,两种溶剂都是液态的,这不可避免地会导致沥青质在油-溶剂界面上的沉淀,正如扩散试验中观察到的那样。丁烷比丙烷的沥青质沉淀现象更为明显。为了解决沥青质析出的问题,提出了用溶剂稀释油测量扩散系数的方法。在相应的测试条件下,用纯溶剂法测得丙烷的扩散系数约为0.6 × 10-10 m2/s,丁烷的扩散系数为1-9 × 10-9 m2/s。两种溶剂的扩散系数均随温度的升高而增大,但在100 bar以内的压力下,扩散系数没有令人满意的变化趋势。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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