1. What is the significance of HO2 catalytic cycles in the lower stratosphere?
Catalytic cycles involving HO2 are crucial in the lower stratosphere (10-30 km) due to their role in ozone destruction. The fastest of these cycles, shown in Reactions R14, R15, and R16, involve the reaction of OH with O3 to produce HO2, O2, and O. This process contributes to the net loss of ozone (O3 + O + O2). Another important HOx catalytic destruction cycle occurs in the middle and upper mesosphere (above 60 km), as demonstrated by Reactions R17 and R18. In these reactions, one molecule of O3, O(3P), or O(1D) is lost while reforming H and OH, resulting in the production of a net ozone loss (Reaction R19). Overall, these catalytic cycles play a significant role in the depletion of ozone in different atmospheric layers.
read more
2. How are ionisation rates obtained for Halloween SPE?
Ionisation rates for Halloween SPE are obtained from the Atmospheric Ionization during Substorm (AISstorm) model, an enhanced version of the Atmospheric Ionization Module Osnabruck (AIMOS) model. The AIMOS model computes ionization rates by precipitating electrons, protons, and alpha particles for the whole atmosphere based on particle flux measurements from Polar Operational Environmental Satellites (POES), the Meteorological Operational satellites (Metop), and the Geostationary Operational Environmental Satellites (GOES). The treatment of electron fluxes is in the energy range of 0.154-300 keV, while protons have an energy range of 0.154 eV to 500 MeV. The AIMOS v2.0-AISstorm model has improved time resolution (0.5 hr) and spatial resolution compared to AIMOS. Integrated ionization rates for the extreme event were taken from an extreme SPE of 23 February 1956 (SPE 56) and scaled by a factor of 70 to represent a one in a 1000 year event. The profiles for the Halloween SPE show average ionization rates for October 27 and 28 before the SPE, and the average ionization rates for October 28 and 29 during the main SPE phase. The ionization rates for the extreme event are about 1-2 orders of magnitude higher compared to the Halloween SPE main phase due to the presence of protons with energies up to a few GeV.
read more
3. What is the 1D model ExoTIC based on?
The 1D model ExoTIC is based on the UBIC model developed by Winkler et al. (2009) for terrestrial middle atmosphere ion-chemistry and the SLIMCAT model by Chipperfield (1999) for neutral chemistry. It simulates a neutral atmosphere with 106 charged and 58 neutral species interacting through various reactions. The model uses 2.7 km boxes in height and is calculated iteratively with the neutral chemistry model feeding volume mixing ratios to the ion-chemistry model. The ion-chemistry is calculated in equilibrium state, with the highest level being 1 (207.4 km) and the lowest level being 53 (25.4 km). The model also computes net effective production or loss rates of neutral species due to primary ionization and ion-chemistry, which can be used as a parameterization for global chemistry-climate models.
read more
4. How are primary positive charges distributed in full-ion chemistry?
In full-ion chemistry, primary positive charges are distributed onto N2, N, O2, and O, balanced with electrons. This distribution is driven by prescribed ionization rates and photo-ionization of NO, as described by Sinnhuber et al. (2012). The ionization cross-sections used for calculating these rates are based on research by Rusch et al. (1981) and Jones and Rees (1973). Additionally, dissociation and dissociative ionization of O2 and N2, as well as ionization of O2, N2, and O, contribute to the formation of excited states of N, O, N+2, N+, and NO+. These processes and their reaction rates are detailed in Sinnhuber et al. (2012) and updated in Herbst et al. (2022).
read more