1. Lecture Objectives -Finish with age of air modeling -Introduce particle dynamics modeling -Analyze some examples related to natural ventilation

2. Air-change efficiency (  v ) Depends only on airflow pattern in a room We need to calculate age of air (  ) Average time of exchange What is the age of air at the exhaust? Type of flow – Perfect mixing – Piston (unidirectional) flow – Flow with stagnation and short-circuiting flow

3. Contaminant removal effectiveness (  ) Depends on: -position of a contaminant source -Airflow in the room Questions 1) Is the concentration of pollutant in the room with stratified flow larger or smaller that the concentration with perfect mixing? 2) How to find the concentration at exhaust of the room?

4. Differences and similarities of E v and  Depending on the source position: - similar or - completely different air quality  v = 0.41  = 0.19  = 2.20

5. Particulate matters (PM) Properties – Size, density, liquid, solid, combination, … Sources – Airborne, infiltration, resuspension, ventilation,… Sinks -Deposition, filtration, ventilation (dilution),… Distribution - Uniform and nonuniform Human exposure

6. ASHRAE Transaction 2004 Properties

7. Particle size distribution ASHRAE Transaction 2004 Ventilation system affect the PM concentration in indoor environment !

8. Human exposure ASHRAE Transaction 2004

9. Two basic approaches for modeling of particle dynamics Lagrangian Model – particle tracking – For each particle ma=  F Eulerian Model – Multiphase flow (fluid and particles) – Set of two systems of equations

10. Lagrangian Model particle tracking A trajectory of the particle in the vicinity of the spherical collector is governed by the Newton’s equation m∙a=  F (  V volume ) particle ∙dv x /dt=  F x (  V volume ) particle ∙dv y /dt=  F y (  V volume ) particle ∙dv z /dt=  F z System of equation for each particle Solution is velocity and direction of each particle Forces that affect the particle

11. Lagrangian Model particle tracking Basic equations - momentum equation based on Newton's second law - d p is the particle's diameter, -  p is the particle density, - u p and u are the particle and fluid instantaneous velocities in the i direction, - F e represents the external forces (for example gravity force). This equation is solved at each time step for every particle. The particle position x i of each particle are obtained using the following equation: Drag force due to the friction between particle and air For finite time step

12. Algorithm for CFD and particle tracking Airflow (u,v,w) Steady state airflow Unsteady state airflow Particle distribution for time step  Particle distribution for time step  +  Particle distribution for time step  +2  Steady state Injection of particles ….. Airflow (u,v,w) for time step  Particle distribution for time step  Particle distribution for time step  +  Injection of particles ….. Airflow (u,v,w) for time step  +  Case 1 when airflow is not affected by particle flow Case 2 particle dynamics affects the airflow One way coupling Two way coupling

14. Natural Ventilation: Science Park, Gelsenkirchen, Germany

15. Natural Ventilation and CFD simulation Wind driven outdoor flow Buoyancy driven indoor flow Solution approach – Model boundary condition in-between outdoor and indoor domain – Couple CFD with 1) energy simulation program (buoyancy driven flow) 2) multi-zone modeling program (inter-zonal flow)

16. External flow Wind profile

17. Buoyancy driven indoor flow Important parameters Geometry Heat sources – Intensity (defined temperature or heat flux) – Distribution – Change (for unsteady-state problem) Openings Defined – Pressure – Velocity

18. Natural Ventilation: Stack-driven flow in an atrium

19. Natural Ventilation: Wind scoop

20. Natural Ventilation: Solar-assisted ventilation

21. Window Design

22. Natural Ventilation: