Charge balance for the mesosphere with meteoric dust particles

被引:11
作者
Asmus, H. [1 ]
Robertson, S. [2 ]
Dickson, S. [2 ]
Friedrich, M. [3 ]
Megner, L. [4 ]
机构
[1] Univ Rostock, Leibniz Inst Atmospher Phys, D-18225 Kuhlungsborn, Germany
[2] Univ Colorado, Dept Phys, Boulder, CO 80309 USA
[3] Graz Univ Technol, A-8010 Graz, Austria
[4] Stockholm Univ, Dept Meteorol, S-10691 Stockholm, Sweden
基金
奥地利科学基金会; 美国国家航空航天局;
关键词
ATOMIC OXYGEN CONCENTRATION; POLAR SUMMER MESOSPHERE; D-REGION; AEROSOL-PARTICLES; ELECTRON-DENSITY; ION CHEMISTRY; ICE PARTICLES; ROCKET-BORNE; SMOKE; MODEL;
D O I
10.1016/j.jastp.2014.07.010
中图分类号
P3 [地球物理学]; P59 [地球化学];
学科分类号
0708 ; 070902 ;
摘要
An aerosol particle charging model initially developed for noctilucent cloud ice particles has been extended in several steps in order to better explain the data for charged meteoric smoke particles (MSPs) obtained by the nighttime and daytime CHAMPS rockets launched from Andoya, Norway, in October 2011. Addition of photodetachment to the model shows that this process reduces the number density of positively charged MSPs as well as the number density of negatively charged MSPs as a consequence of the photodetached electrons neutralizing the positively charged MSPs. In addition, the model shows that the ionization rate can be deduced from the electron number density and the electron-ion recombination rate only at the highest altitudes (those with ionization rates above 20 cm(-3) s(-1)) as a consequence of recombination on the MSPs being dominant at lower altitudes. The differences between the daytime and the nighttime rocket data suggest a photodetachment rate between 0.1 and 0.01 s(-1). A further extension of the model to include the formation of negative ions and their destruction helps explain the ledge seen in the number density of the lightest negatively charged particles. The MSP number densities that are the inputs to the charging model are taken from the CARMA/CHEM2D model. The CHAMPS data are more consistent with number densities generated with an assumed input flux from ablation of 4 t d(-1) than with 44 t d(-1) assumed previously. (C) 2015 Elsevier Ltd. All rights reserved.
引用
收藏
页码:137 / 149
页数:13
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