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A study of 732.0 nm dayglow emission at the equator under varying atomic oxygen density conditions for equinox and solstice cases

机译:在春分和冬至情况下,在不同原子氧密度条件下,赤道732.0 nm日光发射的研究

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AbstractA comprehensive model is developed to compute the volume emission rate of O+(2P) 732.0 nm dayglow emission. The modeled volume emission rates are compared with the measurements as provided by Atmosphere Explorer C satellite and Dynamics Explorer 2 spacecraft. It is found that the model explains quite well the measured emission profiles. The present model is used to study the effect of atomic oxygen abundance on the volume emission rate of 732.0 nm dayglow emission at the equator for equinox and solstice. To study the effect of atomic oxygen abundance on 732.0 nm dayglow emission, the atomic oxygen number densities obtained from the NRLMSISE-00 model are increased (or decreased) in an increment (or decrement) of 20% and are incorporated into the model to compute volume emission rate profiles. The present study shows that the peak emission rate (PER) varies linearly below the reference level of atomic oxygen number density and does not vary linearly above the reference level of atomic oxygen number density. The atomic oxygen number density at reference level corresponds to that value which is obtained from the NRLMSISE-00 model. It is found that the altitude of peak emission rate moves upward as the F10.7 solar index increases. On average the upward movement of altitude of PER is about 9 km for both the equinox and solstice cases. The upward movement of the altitude of peak emission rate is due to the enhancement in atomic oxygen number density with increase in F10.7 solar index.
机译:摘要建立了一个综合模型来计算O + ( 2 P)732.0 nm日光发射的体积发射率。将建模的体积发射率与Atmosphere Explorer C卫星和Dynamics Explorer 2航天器提供的测量值进行比较。发现该模型很好地解释了测得的排放曲线。本模型用于研究春分和至日赤道原子氧丰度对732.0 nm日光发射体体积发射率的影响。为了研究原子氧丰度对732.0 nm日光发射的影响,从NRLMSISE-00模型获得的原子氧原子数密度以20%的增量(或减量)增加(或减少),并纳入模型中进行计算体积排放率曲线。本研究表明,峰值发射率(PER)在原子氧数密度的参考水平以下线性变化,在原子氧数密度的参考水平以上线性变化。参考水平的原子氧数密度对应于从NRLMSISE-00模型获得的那个值。研究发现,随着F 10.7 太阳指数的升高,峰值发射率的高度向上移动。对于春分和冬至,平均来说,PER的上升高度约为9 km。峰值发射率高度的上升是由于原子氧数密度随着F 10.7 太阳指数的增加而增加。

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