Energy transport in the thermosphere during the solar storms of April 2002

被引:114
作者
Mlynczak, MG
Martin-Torres, FJ
Crowley, G
Kratz, DP
Funke, B
Lu, G
Lopez-Puertas, M
Russell, JM
Kozyra, J
Mertens, C
Sharma, R
Gordley, L
Picard, R
Winick, J
Paxton, L
机构
[1] NASA, Langley Res Ctr, Sci Directorate, Hampton, VA 23681 USA
[2] AS & M Inc, Hampton, VA 23681 USA
[3] SW Res Inst, San Antonio, TX 78228 USA
[4] Inst Astrofis Andalucia, E-18080 Granada, Spain
[5] Natl Ctr Atmospher Res, Boulder, CO 80307 USA
[6] Hampton Univ, Ctr Atmospher Sci, Hampton, VA 23668 USA
[7] Univ Michigan, Ann Arbor, MI 48109 USA
[8] USAF, Res Lab, Hanscom AFB, MA 01731 USA
[9] G & A Tech Software, Newport News, VA 23606 USA
[10] Johns Hopkins Univ, Appl Phys Lab, Laurel, MD USA
基金
美国国家航空航天局;
关键词
D O I
10.1029/2005JA011141
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
[1] The dramatic solar storm events of April 2002 deposited a large amount of energy into the Earth's upper atmosphere, substantially altering the thermal structure, the chemical composition, the dynamics, and the radiative environment. We examine the flow of energy within the thermosphere during this storm period from the perspective of infrared radiation transport and heat conduction. Observations from the SABER instrument on the TIMED satellite are coupled with computations based on the ASPEN thermospheric general circulation model to assess the energy flow. The dominant radiative response is associated with dramatically enhanced infrared emission from nitric oxide at 5.3 mu m from which a total of similar to 7.7 x 10(23) ergs of energy are radiated during the storm. Energy loss rates due to NO emission exceed 2200 Kelvin per day. In contrast, energy loss from carbon dioxide emission at 15 mm is only similar to 2.3% that of nitric oxide. Atomic oxygen emission at 63 mu m is essentially constant during the storm. Energy loss from molecular heat conduction may be as large as 3.8% of the NO emission. These results confirm the "natural thermostat'' effect of nitric oxide emission as the primary mechanism by which storm energy is lost from the thermosphere below 210 km.
引用
收藏
页码:1 / 19
页数:19
相关论文
共 32 条
[1]   THE TEMPERATURE OF THE UPPER ATMOSPHERE [J].
BATES, DR .
PROCEEDINGS OF THE PHYSICAL SOCIETY OF LONDON SECTION B, 1951, 64 (381) :805-821
[2]  
CROWLEY G, 1999, ION EFF S OFF NAV RE
[3]   A model of odd nitrogen in the aurorally dosed nighttime terrestrial thermosphere [J].
Dothe, H ;
Duff, JW ;
Sharma, RD ;
Wheeler, NB .
JOURNAL OF GEOPHYSICAL RESEARCH-SPACE PHYSICS, 2002, 107 (A6)
[4]   AN ELECTRIC QUADRUPOLE TRANSITION - THE B1-SIGMA-G+-A1-DELTA-G EMISSION SYSTEM OF OXYGEN [J].
FINK, EH ;
KRUSE, H ;
RAMSAY, DA ;
VERVLOET, M .
CANADIAN JOURNAL OF PHYSICS, 1986, 64 (03) :242-245
[5]   Nonlocal thermodynamic equilibrium vibrational, rotational, and spin state distribution of NO(ν=0,1,2) under quiescent atmospheric conditions [J].
Funke, B ;
López-Puertas, M .
JOURNAL OF GEOPHYSICAL RESEARCH-ATMOSPHERES, 2000, 105 (D4) :4409-4426
[6]   A NEW NUMERICAL-MODEL OF THE MIDDLE ATMOSPHERE .2. OZONE AND RELATED SPECIES [J].
GARCIA, RR ;
SOLOMON, S .
JOURNAL OF GEOPHYSICAL RESEARCH-ATMOSPHERES, 1994, 99 (D6) :12937-12951
[7]   A NEW NUMERICAL-MODEL OF THE MIDDLE ATMOSPHERE .1. DYNAMICS AND TRANSPORT OF TROPOSPHERIC SOURCE GASES [J].
GARCIA, RR ;
STORDAL, F ;
SOLOMON, S ;
KIEHL, JT .
JOURNAL OF GEOPHYSICAL RESEARCH-ATMOSPHERES, 1992, 97 (D12) :12967-12991
[8]  
GILLE JC, 1971, J ATMOS SCI, V28, P1427, DOI 10.1175/1520-0469(1971)028<1427:OTIOLR>2.0.CO
[9]  
2
[10]   Thermal infrared measurements in the middle and upper atmosphere [J].
Grossmann, KU ;
Vollmann, K .
MIDDLE AND UPPER ATMOSPHERES: SMALL SCALE STRUCTURES AND REMOTE SENSING, 1997, 19 (04) :631-638