Zierenberg Jennifer R, Halpern David, Filoche Marcel, Sapoval Bernard, Grotberg James B
Department of Biomedical Engineering, University of Michigan, Ann Arbor, MI 48109, USA.
Math Med Biol. 2013 Jun;30(2):131-56. doi: 10.1093/imammb/dqs002. Epub 2012 Feb 29.
Particle transport and deposition associated with flow over a wedge is investigated as a model for particle transport and flow at the carina of an airway bifurcation during inspiration. Using matched asymptotics, a uniformly valid solution is obtained to represent the high Reynolds number flow over a wedge that considers the viscous boundary layer near the wedge and the outer inviscid region and is then used to solve the particle transport equations. Sometimes particle impaction on the wedge is prevented due to the boundary layer. We call this boundary layer shielding (BLS). This effect can be broken down into different types: rejection, trapping and deflection that are described by what happens to the particle's initial negative velocity normal to the wall either changing sign, reaching zero, or remaining negative in the boundary layer region. The deposition efficiency depends on the critical Stokes number but exhibits a weak dependence on Reynolds number. Deposition efficiency for S(c) in the range 0 < S(c) < 0.4 yields the following relationship De ≈ (1.867S(c)¹·⁷⁸-0.016) sin(βπ/2) at large Reynolds numbers, where βπ is the wedge angle. For a specific deposition efficiency, S(c) decreases as βπ increases. The distribution of impacted particles was also computed and revealed that particles primarily impact within one airway diameter of the carina, consistent with computational fluid dynamics approaches. This work provides a new insight that the BLS inherent to the wedge component of the structure is the dominant reason for the particle distribution. This finding is important in linking aerosol deposition to the location of airway disease as well as target sites for therapeutic deposition.
研究了与楔形体上的流动相关的颗粒输运和沉积,以此作为吸气过程中气道分叉处隆突处颗粒输运和流动的模型。利用匹配渐近法,得到了一个一致有效的解,以表示楔形体上的高雷诺数流动,该解考虑了楔形体附近的粘性边界层和外部无粘区域,然后用于求解颗粒输运方程。有时,由于边界层的存在,颗粒不会撞击到楔形体上。我们将此称为边界层屏蔽(BLS)。这种效应可细分为不同类型:排斥、捕获和偏转,它们由颗粒初始垂直于壁面的负速度在边界层区域是改变符号、达到零还是保持为负来描述。沉积效率取决于临界斯托克斯数,但对雷诺数的依赖性较弱。在大雷诺数下,0 < S(c) < 0.4范围内的S(c)的沉积效率给出以下关系De ≈ (1.867S(c)¹·⁷⁸ - 0.016) sin(βπ/2),其中βπ是楔角。对于特定的沉积效率,S(c)随着βπ的增加而减小。还计算了撞击颗粒的分布,结果表明颗粒主要在隆突的一个气道直径范围内撞击,这与计算流体动力学方法一致。这项工作提供了一个新的见解,即结构楔形体部分固有的BLS是颗粒分布的主要原因。这一发现对于将气溶胶沉积与气道疾病的位置以及治疗性沉积的目标部位联系起来很重要。