key: cord-0007289-q0cy9dej
authors: Shimazaki, Yasuhiro; Okubo, Masaaki; Yamamoto, Toshiaki
title: Three‐dimensional Numerical Simulation of Gas‐particulate Flow around Breathing Human and Particulate Inhalation
date: 2006-05-05
journal: AIP Conf Proc
DOI: 10.1063/1.2204538
sha: 41166cff16470f45bbcc82eb68aabfdcd503d268
doc_id: 7289
cord_uid: q0cy9dej

It is important to predict the environment around the breathing human because inhalation of virus (avian influenza, SARS) is recently severe worldwide problem, and air pollution caused by diesel emission particle (DEP) and asbestos attract a great deal of attention. In the present study, three‐dimensional numerical simulation was carried out to predict unsteady flows around a breathing human and how suspended particulate matter (SPM, diameter∼1 μm) reaches the human nose in inhalation and exhalation. In the calculation, we find out smaller breathing angle and the closer distance between the human nose and pollutant region are effective in the inhalation of SPM.

In recent years, decline of air quality becomes one of significant problems and people from all over the world are concerned as human safety [1] . There are two main types of air pollutant: particulate pollutant and gas pollutant. Damages by SARS [2] , avian influenza [3] , diesel emission particles [4] , and asbestos [5] are the good examples of particulate pollutant. Many researches have been performed to deal with the increasing problems of such air pollutants [6] , [7] . However, few studies have been performed to address the theme of human with unsteady breathing [8] , [9] . Two-dimensional numerical simulation was carried out, and the time-dependent pollutant concentrations were determined until this point [10] . In this paper, calculating area was advanced to three-dimension, real particle with size and mass. In the simulation, the breathing process alternated between inhalation and exhalation as the unsteady breathing at nose. The governing equations for flow are the mass conservation and the Navier-Stokes equations.

In these equations, ρ is the density and stays constant in the simulations, p is the static pressure, and µ is the viscosity. U r is the velocity of the surrounding air. u, v, w are the velocity of each component. As a turbulence model, standard k-ε model was adopted. It involves solutions of transport equations for turbulent kinetic energy and its rate of dissipation. The model adopted in the simulation is based on Launder and Spalding [11] and is expressed as

The transport equations for k are

And the transport equations for ε are 

The motions of particulates were analyzed by solving the Lagrangian equations for each particle. The equation of particle motion is ( )

where m p is the mass of particle and u r =(u, v, w) is its velocity vector, C D is the drag coefficient, ρ is the density of surrounding air, A p is the projected area of a particle, and g r is the gravity vector, respectively. For a spherical particle, A p =πd 2 /4 where d is the particle diameter. Each of the force considered in the analysis is Stokes drag with Cunningham correction [5] , gravity, Saffman lifting force, pressure gradient force, and Brownian diffusion [12] . The following correlations are used to calculate the drag coefficient, 

For very small particles, when the size of particles is of the same magnitude as distance between gas molecules, slip occurs. Cunningham correction factor to fluid drag on particles should be applied for rarefied fluid-particle flows. Cunningham correction factor is

The Knudsen number, Kn, may be evaluated based on molecular mean free path of the fluid and particle diameter as d Kn

Where λ is the molecular mean free path. The Saffman lifting force arises due to the surface pressure distribution on a particle in the presence of a velocity gradient in the flow field and plays an important role in determining particle deposition patterns in simulations. Generalized Saffman lifting force can be expressed as

. 1 (11) The pressure gradient force on a particle is given by

where p ∇ is the local pressure gradient. The Brownian diffusion experienced by particles results from the impact of carrier fluid molecules on the particles and is significant for sub-micron particles. Brownian diffusion can be evaluated as

where k B is the Boltzmann constant, ∆t is the time step, and R r is a Gaussian random number.

In three-dimensional numerical simulations, general-purpose software, CFD-ACE+2004 (CFD Research Corp.) was used. The grid configuration is shown in FIGURE 2. Linear orthogonal grid is mainly used in the region distant from the human body. Boundary-fitted grid is used near the human body. The maximum cell dimensions ranges from 1.1 mm to 325 mm. The total numbers of cell are 110077. The grids were generated by mesh generator CFD-VisCART (CFD Research Corp.). The finite volume approach is adopted, and then governing equations are numerically solved over each of control volumes. A co-located cell-centered variable arrangement is employed. The checkerboard instability is circumvented by Rhie and Chow [13] . SIMPLEC scheme has been adopted for flow phase analysis, and is an enhancement to the well known SIMPLE algorithm [14] . 

where α is the breathing angle between the vertical lines and breathing velocity vector. Velocity is a time function f (t) and breathing volume is a product of multiplying f (t) by area of nostrils as FIGURE 3.

As a pollutant source, a thousand particles are randomly placed in the box region (0.1 m 0.6 m 1.0 m). The particle region stay away L cm from the human nose, and we describe L as source distance. Particles are set for initial condition as

where u p , v p , w p are particle velocities. Particles are totally absorbed at the nose, on walls, and human surface. Initially, the fluid is considered as stationary fluid.

We first examined the dependence between breathing angles and flow field by a way of comparison of the two dimensional model. Breathing angles were set at 0, 30, 60, and 90 degree. L was 0.1 m at this time. The relationship among breathing angles and time to reach the nose and particle captured efficiency is shown in TABLE 1. The particle captured efficiency tends to become higher and particles tend to reach the human nose faster as the breathing angle becomes smaller. Particles reach the human in 7 s at the earliest, and the particle captured efficiency is 2.9% at the maximum, when breathing angle is 0 degree. No particles are captured with breathing angle of 60 degree or larger. When we look at the flow field, exhalation has an impact on the field as shown in FIGURE 6. (a) (d). In the early period of exhalation, the respiration region is small and the flow is complicated. The respiration area becomes larger and the velocity becomes higher as the time goes on. The downward stream caused by exhalation remains during inhalation, which is to say the downward stream is small in scale, but always stays and particles go down. Note that each breathing cycle seems self-dependence.

We focus on the particulate pollutant in the air and three-dimensional numerical simulation was carried out. The effects of breathing angle and source distance ware clarified around human with unsteady breathing. The main results are summarized as follows:

(1) Exhalation has an impact on the flow field more than inhalation.

(2) The particle captured efficiency tends to become higher and particles tend to reach the human nose faster as source distance becomes near from human body. Particles reach the human nose when source distance is less than 0.2 m. No particles are reached beyond 0.3 m. The maximum 2.6% of particles are captured when the source distance is 0.05 m.

(3) The particle captured efficiency tends to become higher and particles tend to reach the human nose faster as the breathing angle becomes smaller. The human can inhale particles only breathing angle of 30 degree or smaller.

(4) Throughout all simulations, particles are drawn from upper region of the human. When particles are captured, motions of particles away from the human body with right-left unsymmetrical vortexes are observed. Otherwise, particles just move away and no vortexes are induced.

Sources and Measures for Indoor Air Pollution (Shitsunai Kukiosen No Genin To Taisaku), Tokyo: The Nikkan Kogyo Shimbun Ltd

Proceedings of JSAE symposium

Multiphase Flows with Droplets and Particles