A FIRE-ACE/SHEBA Case Study of Mixed-Phase Arctic Boundary Layer Clouds: Entrainment Rate Limitations on Rapid Primary Ice Nucleation ProcessesSource: Journal of the Atmospheric Sciences:;2011:;Volume( 069 ):;issue: 001::page 365Author:Fridlind, Ann M.
,
van Diedenhoven, Bastiaan
,
Ackerman, Andrew S.
,
Avramov, Alexander
,
Mrowiec, Agnieszka
,
Morrison, Hugh
,
Zuidema, Paquita
,
Shupe, Matthew D.
DOI: 10.1175/JAS-D-11-052.1Publisher: American Meteorological Society
Abstract: bservations of long-lived mixed-phase Arctic boundary layer clouds on 7 May 1998 during the First International Satellite Cloud Climatology Project (ISCCP) Regional Experiment (FIRE)?Arctic Cloud Experiment (ACE)/Surface Heat Budget of the Arctic Ocean (SHEBA) campaign provide a unique opportunity to test understanding of cloud ice formation. Under the microphysically simple conditions observed (apparently negligible ice aggregation, sublimation, and multiplication), the only expected source of new ice crystals is activation of heterogeneous ice nuclei (IN) and the only sink is sedimentation. Large-eddy simulations with size-resolved microphysics are initialized with IN number concentration NIN measured above cloud top, but details of IN activation behavior are unknown. If activated rapidly (in deposition, condensation, or immersion modes), as commonly assumed, IN are depleted from the well-mixed boundary layer within minutes. Quasi-equilibrium ice number concentration Ni is then limited to a small fraction of overlying NIN that is determined by the cloud-top entrainment rate we divided by the number-weighted ice fall speed at the surface ?f. Because wc < 1 cm s?1 and ?f > 10 cm s?1, Ni/NIN ? 1. Such conditions may be common for this cloud type, which has implications for modeling IN diagnostically, interpreting measurements, and quantifying sensitivity to increasing NIN (when we/?f < 1, entrainment rate limitations serve to buffer cloud system response). To reproduce observed ice crystal size distributions and cloud radar reflectivities with rapidly consumed IN in this case, the measured above-cloud NIN must be multiplied by approximately 30. However, results are sensitive to assumed ice crystal properties not constrained by measurements. In addition, simulations do not reproduce the pronounced mesoscale heterogeneity in radar reflectivity that is observed.
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contributor author | Fridlind, Ann M. | |
contributor author | van Diedenhoven, Bastiaan | |
contributor author | Ackerman, Andrew S. | |
contributor author | Avramov, Alexander | |
contributor author | Mrowiec, Agnieszka | |
contributor author | Morrison, Hugh | |
contributor author | Zuidema, Paquita | |
contributor author | Shupe, Matthew D. | |
date accessioned | 2017-06-09T16:55:01Z | |
date available | 2017-06-09T16:55:01Z | |
date copyright | 2012/01/01 | |
date issued | 2011 | |
identifier issn | 0022-4928 | |
identifier other | ams-76453.pdf | |
identifier uri | http://onlinelibrary.yabesh.ir/handle/yetl/4218902 | |
description abstract | bservations of long-lived mixed-phase Arctic boundary layer clouds on 7 May 1998 during the First International Satellite Cloud Climatology Project (ISCCP) Regional Experiment (FIRE)?Arctic Cloud Experiment (ACE)/Surface Heat Budget of the Arctic Ocean (SHEBA) campaign provide a unique opportunity to test understanding of cloud ice formation. Under the microphysically simple conditions observed (apparently negligible ice aggregation, sublimation, and multiplication), the only expected source of new ice crystals is activation of heterogeneous ice nuclei (IN) and the only sink is sedimentation. Large-eddy simulations with size-resolved microphysics are initialized with IN number concentration NIN measured above cloud top, but details of IN activation behavior are unknown. If activated rapidly (in deposition, condensation, or immersion modes), as commonly assumed, IN are depleted from the well-mixed boundary layer within minutes. Quasi-equilibrium ice number concentration Ni is then limited to a small fraction of overlying NIN that is determined by the cloud-top entrainment rate we divided by the number-weighted ice fall speed at the surface ?f. Because wc < 1 cm s?1 and ?f > 10 cm s?1, Ni/NIN ? 1. Such conditions may be common for this cloud type, which has implications for modeling IN diagnostically, interpreting measurements, and quantifying sensitivity to increasing NIN (when we/?f < 1, entrainment rate limitations serve to buffer cloud system response). To reproduce observed ice crystal size distributions and cloud radar reflectivities with rapidly consumed IN in this case, the measured above-cloud NIN must be multiplied by approximately 30. However, results are sensitive to assumed ice crystal properties not constrained by measurements. In addition, simulations do not reproduce the pronounced mesoscale heterogeneity in radar reflectivity that is observed. | |
publisher | American Meteorological Society | |
title | A FIRE-ACE/SHEBA Case Study of Mixed-Phase Arctic Boundary Layer Clouds: Entrainment Rate Limitations on Rapid Primary Ice Nucleation Processes | |
type | Journal Paper | |
journal volume | 69 | |
journal issue | 1 | |
journal title | Journal of the Atmospheric Sciences | |
identifier doi | 10.1175/JAS-D-11-052.1 | |
journal fristpage | 365 | |
journal lastpage | 389 | |
tree | Journal of the Atmospheric Sciences:;2011:;Volume( 069 ):;issue: 001 | |
contenttype | Fulltext |