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5. Stratospheric Ozone: An Introduction to Its Study

About: The article was published on 2014-03-03 and is currently open access. It has received None citations till now. The article focuses on the topics: Ozone layer.

Summary (3 min read)

REACTIONS IN A HYDROGEN-OXYGEN ATMOSPHèRE

  • When an analysis of the various reaction rates is made, a certain number of them can be ignored, and for several years it was assumed [e.g.. Fig. 2 . Observed and calculated ozone profiles.
  • Hunt. 1966; Leovy. 1969] that the reactions of OH and HO2 radicals with O and Oj were the essential reactions explaining the aeronomic behavior of stratospheric ozone.
  • The normal photodissociation process (a,3) H2O + hv neS) + OH{Xm) (30) which can still occur in the stratosphère, is less important than the reaction process (29).
  • This reaction may be introduced into the aeronomic chemistry of molecular hydrogen.
  • The rate coefficient «20 should be of the same order of magnitude as 13,5, but no acceptable value has been found.

REACTIONS AFTER OXIDATION OF MéTHANE

  • Methyl radicals, which are produced by oxidation processes of CH,, may react rapidly with atomic oxygen (c) CH, + O -H + HjCO + 67 Iccal (63û) with u rate coefficient [Slagle et al..
  • According to Levy [1972] , CH,0,H either reacts with OH or is subject to photodissociation (c") CH,0,H + hv ^ CH,0 + OH (78) Finally, if methylperoxynitrite and methylperoxynitrate are formed, the photodissociation should be considered to be and (Oo) EQUATION Reactions of CH,, CH3O, and CHjO, with ozone have also been considered [Simonaitis and Heicklen, 1975a] .

ATMOSPHèRE

  • The présence of nitrogen oxides in the upper atmosphère requires the production of atomic nitrogen [Nicolei.
  • From this analysis of the various reactions of nitrogen trioxide, it is not clear if NO, can play a major rôle in stratospheric aeronomy.
  • Among the various dissociation processes, the authors may consider the following: Cl, + hv{\ < 483 nm) -2CI (159a) is photodissociated in the stratosphère and troposphère by radiation of X > 300 nm [Seery and Britton.

and

  • Thus the addition of nitrogen oxides NO and NO,, which destroy odd oxygen by various reactions involving ozone and atomic oxygen, must be considered with its counterpart, the photodissociation of NO, NO,, and NO, and the N formation, as production processes in addition to the photodissociation of molecular oxygen.
  • Furthermore, the differential équation for nitric oxide must be written as foilows:.
  • Thus the nitrogen oxide concentrations, and particularly those of HNOs, NO, and NO2, must dépend on atmospheric conditions in the lower stratosphère [Brasseur and Nicolet, 1973] , and their behavior will be related to the variation of the tropopause.

SOLAR RADIATION

  • The authors knowledge of solar radiation in the ultraviolet which plays a rôle in the photodissociation of molecular oxygen is due to rocket and balloon data.
  • The percentages are given for the spectral range AK = 500 cm"'; standard conditions prevail.
  • There is therefore no doubt that the stratospheric ozone below its concentration peak is essentially due to a downward transport from the production régions Figure 20 is another illustration of this distribution of the ozone formation resulting from the atomic oxygen production with a peak in the upper stratosphère between 40 and 50 km even for overhead sun conditions.
  • The température-altitude profiles indicate that the important différences occur between 10 and 20 km; they are related to the hcight of the tropopause and have therefore an effect on the rate coefficients in the lower stratosphère.

PHOTODISSOCIATION IN THE TROPOSPHèRE AND STRATOSPHèRE AND ITS EFFECTS

  • The photodissociation in the lower régions of the terrestrial atmosphère is of particular interest, since it is the necessary process to start various chemical reactions.
  • The ozone photolysis (see for example, Welge [1974] for a récent analysis of the photolysis of O», Hd, COj, and SO, compounds) occurs in the visible région in the spectral range of the Chappuis bands with production of oxygen molécules and atoms in their normal States.
  • Its concentration dépends on the exchange processes between the stratosphère and troposphère.
  • The absorption cross section of nitrous oxide varies within very low values less than 10"" cm^ between 310 and 250 nm, and its photodissociation coefficient is not greater than 10"' s"' at the stratopause and reaches only values less than 10"' S"' in the low stratosphère.
  • The photodissociation rates are relatively small, and departures from photochemical equilibrium conditions are aiways the rule.

FINAL INTRODUCTORY REMARKS

  • The authors have seen that it is aiways possible to résolve the theoretical problem of stratospheric ozone with the introduc-PHOTOOI SSOCIAT ION COEFFICIENT I sec"'l Fig. 37 . 1972] . tion of correct aeronomic équations and with the adoption oi the principal atmospheric parameters.
  • The boundary conditions, which are used in stratospheric models, are not aiways adopted to varying atmospheric conditions.
  • Seiler, 1974; Seiler and Schmidi, 1974] il may be pointed out that the CO concentration must be known with précision in the lower stratosphère in order to détermine the ratio n(OH)/«(H02).
  • In the same way, the tropospheric ozone problem requires more attention, since a photochemical theory has been proposed by Chameides and Walker [1973.

CONCENTRATION Icm"'')

  • Récent measurements by Schmidt [1974] and Seller and Schmidt [1974] lead to an almost constant mixing ratio ofO.55 ppm for tropospheric molecular hydrogen which can be taken as the normal mixing ratio above the tropopause level.
  • Sampling [Ehhall, 1974] in the stratosphère at various latitudes is required in order to obtain enough vertical profiles to compare with the calculated vertical distributions of méthane and molecular hydrogen.
  • It is not yet clear how the vertical and horizontal transports play their rôle [Wofsy et ai. 1967] , and even spécial sources [Deuser et al., 1973] .
  • Récent measurements at ground level of HNO2 by Nash [1974] lead to mixing ratios from 1 to 10 ppb which must be explained by its various reactions with nitrogen oxides and hydroxyl and hydroperoxyl radicals.

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TL;DR: In this paper, present and anticipated future sources of GCl are described and an estimate of their stratospheric source strength is derived, and the mean source strengths are estimated to be, respectively, 4 x 10 10, 1 x 10 11, and 5 x 10 9 g GCl yr -1, the last figure representing a projection of anthropogenic emissions to include 50 space shuttle flights per year.
Abstract: Interest in atmospheric gaseous chlorine (GCl) has been generated by its increasing anthropogenic introduction coupled with its reactivity with ozone. Present and anticipated future sources of GCl are described and an estimate of their stratospheric source strength is derived. The stratospheric sources are transport of tropospheric GCl across the tropopause, direct stratospheric introduction by major volcanic eruptions, and anthropogenic emissions in the stratosphere. The mean source strengths are estimated to be, respectively, 4 x 10 10, 1 x 10 11, and 5 x 10 9 g GCl yr -1, the last figure representing a projection of anthropogenic emissions to include 50 space shuttle flights per year. Whereas the first source introduces GCl only at the base of the stratosphere, the other two can supply GCl directly to altitudes up to approximately 50 km. The dominant, volcanic, source is highly variable, it being estimated that as much as 3 x 10 13 g GCl can enter the stratosphere from a single eruption. Although major volcanic eruptions are indicated to be the dominant source, few ''hard'' data are currently available.

28 citations

Journal ArticleDOI
T. Nash1
01 Feb 1974-Tellus A
TL;DR: In this article, low concentrations of nitrous acid in air were estimated by a differential absorption method, and the highest proportion of acid was found in air which had passed over the industrial regions of W. Europe.
Abstract: Low concentrations of nitrous acid in air were estimated by a differential absorption method. Over a three-month period, atmospheric concentrations at one location in southern England varied between 0.4 and 11 ppb while those of nitrogen dioxide varied between 4 and 21 ppb. The highest proportion of acid was found in air which had passed over the industrial regions of W. Europe. In the laboratory, concentrations of about 1 ppm of nitrous acid with less than 0.03 ppm of nitrogen dioxide were produced by blowing air over a shallow layer of very dilute acidified nitrite solution. Exposure of the vapour to the light from a pyrex-shielded mercury arc caused decomposition, with production of nitrogen dioxide. This decomposition was apparently prevented by some olefins. The experiments did not support the view that nitrous acid is a source of hydroxyl radicals in the atmosphere. DOI: 10.1111/j.2153-3490.1974.tb01964.x

28 citations

Journal ArticleDOI
TL;DR: In this paper, the authors derived an expression for the number of ozone molecules as a function of height, in terms respectively of a numerical constant, the concentration of oxygen and of total air molecules.
Abstract: The paper consists of a calculation of the distribution of ozone with height as it would be in an undisturbed photochemical steady state under the influence of solar radiation considered as that of a black body at a temperature of 6000°K. An expression is derived for the number of ozone molecules as a function of height, in terms respectively of a numerical constant, the concentration of oxygen and of total air molecules as a function of height, and the number of quanta absorbed by oxygen and by ozone as a function of height. The latter two quantities are in principle integrals over frequency-ranges, and they are evaluated by summing over finite frequency-strips. Moreover, the number of quanta absorbed by ozone at any height depends of course upon the concentration of the ozone itself. The complete expression is, therefore, evaluated by the method of successive approximations for a series of heights, the available intensity of the radiation absorbed by ozone being derived as the remainder from the last greater height. The ozone concentration, once evaluated for a particular height, is assumed constant over the interval of which this is the midpoint in evaluating the depletion of the radiation in this interval; then, by deduction, the remaining radiation available for the next lower interval is determined. The numerical constant is perhaps best looked upon as evaluated from the known total atmospheric ozone path, though its order of magnitude is indicated by the facts of experimental photochemistry. In this way a distribution of ozone is found which resembles rather closely that which from observation is now known approximately to obtain in the atmosphere. The values of the absorption-coefficient of ozone and oxygen in the region where the two absorptions meet, that is, about 2200A, prove to be very important, two possible sets of values being used in this narrow interval for illustration.

27 citations

Journal ArticleDOI
TL;DR: In this article, it was shown that the vertical distribution of nitrogen atoms cannot be determined by a dissociation equilibrium, since it is subject to dynamical effects such as diffusion and atmospheric mixing.

27 citations

Journal ArticleDOI
TL;DR: In this paper, the authors have shown that if atmospheric ozone is considered as existing in a photochemical steady state depending on solar radiation, calculations involving certain assumptions regarding the absorption-coefficients yield a distribution of the ozone with height which is sufficiently similar to the distribution that is deduced from experimental observations to suggest that the photochemical picture is adequate to account for atmospheric ozone.
Abstract: In two earlier articles the authors have shown that if atmospheric ozone is considered as existing in a photochemical steady state depending on solar radiation, calculations involving certain assumptions regarding the absorption-coefficients yield a distribution of the ozone with height which is sufficiently similar to the distribution that is deduced from experimental observations to suggest that the photochemical picture is adequate to account for atmospheric ozone. At the end of the first paper the disturbance of the steady state by atmospheric circulation was briefly discussed, and it was pointed out that the known variations in the existing vertical ozone path over any point on the Earth's surface might be explained as due to such disturbance. In order to estimate the quantitative importance of circulation in the photochemical picture, it is necessary to have some idea of the rates at which the steady state is maintained at the various heights. It is one of the purposes of the present paper to estimate the approximate values of these rates.

26 citations