Diffusion Model for a Convective Layer. Part II: Plume Released from a Continuous Point SourceSource: Journal of Climate and Applied Meteorology:;1986:;Volume( 025 ):;Issue: 010::page 1454DOI: 10.1175/1520-0450(1986)025<1454:DMFACL>2.0.CO;2Publisher: American Meteorological Society
Abstract: A two-dimensional diffusion model for a convective planetary boundary layer is presented. Three prognostic equations are employed for the concentration, the concentration flux, and the covariance of temperature and concentration. The environmental background, which includes the mean wind, the mean virtual potential temperature, the turbulent kinetic energy and other second moments, is generated from Part I of this study. For an elevated point source, the plume concentration centerline descends until it intercepts the ground, then it rebounds and returns to the mixed layer, while the material released from a surface point source gradually ascends into the mixed layer, carried aloft by the updrafts of the convective motion. Compared to the laboratory and field experiments, this model simulates well the diffusion of passive pollutants released from a continuous point source into the convective layer.
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| contributor author | Sun, Wen-Yih | |
| contributor author | Chang, Chiao-zen | |
| date accessioned | 2017-06-09T14:01:24Z | |
| date available | 2017-06-09T14:01:24Z | |
| date copyright | 1986/10/01 | |
| date issued | 1986 | |
| identifier issn | 0733-3021 | |
| identifier other | ams-11066.pdf | |
| identifier uri | http://onlinelibrary.yabesh.ir/handle/yetl/4146253 | |
| description abstract | A two-dimensional diffusion model for a convective planetary boundary layer is presented. Three prognostic equations are employed for the concentration, the concentration flux, and the covariance of temperature and concentration. The environmental background, which includes the mean wind, the mean virtual potential temperature, the turbulent kinetic energy and other second moments, is generated from Part I of this study. For an elevated point source, the plume concentration centerline descends until it intercepts the ground, then it rebounds and returns to the mixed layer, while the material released from a surface point source gradually ascends into the mixed layer, carried aloft by the updrafts of the convective motion. Compared to the laboratory and field experiments, this model simulates well the diffusion of passive pollutants released from a continuous point source into the convective layer. | |
| publisher | American Meteorological Society | |
| title | Diffusion Model for a Convective Layer. Part II: Plume Released from a Continuous Point Source | |
| type | Journal Paper | |
| journal volume | 25 | |
| journal issue | 10 | |
| journal title | Journal of Climate and Applied Meteorology | |
| identifier doi | 10.1175/1520-0450(1986)025<1454:DMFACL>2.0.CO;2 | |
| journal fristpage | 1454 | |
| journal lastpage | 1463 | |
| tree | Journal of Climate and Applied Meteorology:;1986:;Volume( 025 ):;Issue: 010 | |
| contenttype | Fulltext |