“…distance to the surface (wall) y + dimensionless distance to the surface (wall) y + = yu * / z 0 surface roughness parameter , u d pollutant dry deposition velocity air molecular path air dynamic viscosity air kinematic (molecular) viscosity = / t air turbulent viscosity air density p particle density p characteristic time of particle relaxation (deceleration) p = u s /g L Lagrangian timescale of turbulence + dimensionless relaxation time + = p u * 2 / Numerous papers (Davies, 1966;Fan & Ahmadi, 1993;Johansen, 1991;Kharchenko, 1997;Liu & Agarwal, 1974;Nho-Kim, Michou, and Peuch, 2004;Sehmel, 1973Sehmel, , 1980Sehmel & Hodgson, 1978;Sippola & Nazaroff, 2002;Slinn, 1978Slinn, , 1982Valentine and Smith, 2005;Wood, 1981aWood, , 1981bZaichik and Alipchenkov, 2007) describe semiempirical relations for the velocities of deposition onto vertical and horizontal walls. These were determined mainly from experimental data on turbulent deposition in ducts and channels.…”