首页> 外文期刊>Journal of Geophysical Research. Biogeosciences >Tidal influence on the oxygen and hydroxyl nightglows: Wind Imaging Interferometer observations and thermosphere/ionosphere/mesosphere electrodynamics general circulation model
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Tidal influence on the oxygen and hydroxyl nightglows: Wind Imaging Interferometer observations and thermosphere/ionosphere/mesosphere electrodynamics general circulation model

机译:潮汐对氧气和羟基夜光的影响:风成象干涉仪观测和热层/电离层/中层电动力学一般循环模型

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Longitudinal zonally averaged Wind Imaging Interferometer (WINDII) (on UARS) nighttime oxygen (O(S-1)) and hydroxyl (P(3) line in the OH(8,3) Meinel band) volume emission rates exhibit dramatic spatial and temporal variations. The recently improved thermosphere/ionosphere/mesosphere electrodynamics general circulation model (TIME-GCM) produces simulations for the two airglows through the input of (1,1) upward propagating diurnal tides. The model simulations show excellent agreement with WINDII observations in both the local time domain and the latitudinal domain between 40 degreesS and 40 degreesN. The influence of diurnal tides on the two airglows in strongest in the tropical region. In the local solar time domain the emission rate and peak altitude at the equator show large tidal perturbations, but they are fairly stable at midlatitude. In the latitudinal domain there is an equatorial trough in the oxygen emission rate which exists regardless of local time and season. The hydroxyl emission rate is more dependent on local time and season. At equinox it has a prominent equatorial maximum which disappears at dawn, whereas at solstice it has a very weak equatorial maximum at dusk, changing soon after midnight to an equatorial minimum. These features of emission rates are also compared to TIME-GCM simulations for meridional wind, temperature, and atomic oxygen density, [O], with and without upward propagating diurnal tides. The results are as follows: (1) The large oscillations of the two nightglows as well the atomic oxygen density in the tropical region are driven by the diurnal propagating tides. In altitude the mesosphere and lower thermosphere is divided into two type of cells, one with meridional winds converging at the equator, higher temperature, and enhanced [O] and airglow emission rates, and the other with meridional winds diverging from the equator, lower temperature, and depleted [O] and airglow emission rates; all these are essentially related to the wavelength and phase of the diurnal tides. (2) The relatively stable airglow emission rates at around 20 degrees are related to the minimum fluctuation of temperature and stable meridional wind directions in spite of the maximized wind speed in this region. (3) The year-around equatorial depletion in the oxygen airglow and the double-peaked profile in the hydroxyl airglow are most likely produced by the diurnal tides. Further investigation is needed particularly for the absolute value of the oxygen emission rate, the interhemispheric comparison of the oxygen emission rate, why WINDII observes maximum summer emissions whereas the TIME-GCM gives maximum winter emission, and the effects of waves in addition to the diurnal tides. [References: 36]
机译:纵向纬向平均风成像干涉仪(WINDII)(在UARS上)夜间氧气(O(S-1))和羟基(OH(8,3)Meinel谱带中的P(3)线)体积发射率显示出戏剧性的空间和时间分布变化。最近改进的热层/电离层/中层电动力学一般循环模型(TIME-GCM)通过输入(1,1)向上传播的昼夜潮汐产生了两个气辉的模拟。模型仿真表明,在本地时域和纬度范围在40°S和40°N之间的WINDII观测值都具有极好的一致性。昼夜潮对热带地区最强烈的两个气辉的影响。在当地太阳时域中,赤道的辐射速率和峰值高度显示出较大的潮汐扰动,但在中纬度时相当稳定。在纬度范围内,氧气释放速率存在一个赤道低谷,与当地时间和季节无关。羟基释放速率更多地取决于当地时间和季节。在春分点,它的赤道最大值明显,在黎明时消失,而在冬至时,它的黄昏赤道最大值非常弱,在午夜之后很快变为赤道最小值。在有或没有向上传播的日潮的情况下,还将排放速率的这些特征与TIME-GCM模拟的子午风,温度和原子氧密度[O]进行了比较。结果如下:(1)两个夜光的大振荡以及热带地区的原子氧密度是由昼夜传播的潮汐驱动的。在海拔高度,中层和下层热层分为两种类型的单元,一种是子午风在赤道处会聚,温度较高,[O]和气辉发射率提高,另一种是子午风从赤道发散,温度较低。 ,并耗尽[O]和气辉排放率;所有这些基本上都与昼夜潮的波长和相位有关。 (2)尽管该区域的风速最大,但相对稳定的20%左右的气辉发射率与温度的最小波动和稳定的子午风向有关。 (3)氧气气辉的全年赤道损耗和羟基气辉的双峰轮廓很可能是由日潮产生的。特别是需要进一步研究氧气排放速率的绝对值,半球氧气排放速率的比较,为什么WINDII观测到夏季最大排放量,而TIME-GCM观测到最大冬季排放量,以及昼夜波的影响潮汐。 [参考:36]

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