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Radiation, solar, latitude

Most ozone is formed near the equator, where solar radiation is greatest, and transported toward the poles by normal circulation patterns in the stratosphere. Consequendy, the concentration is minimum at the equator and maximum for most of the year at the north pole and about 60°S latitude. The equihbrium ozone concentration also varies with altitude the maximum occurs at about 25 km at the equator and 15—20 km at or near the poles. It also varies seasonally, daily, as well as interaimuaHy. Absorption of solar radiation (200—300 nm) by ozone and heat Hberated in ozone formation and destmction together create a warm layer in the upper atmosphere at 40—50 km, which helps to maintain thermal equihbrium on earth. [Pg.495]

TABLE 12-5 Maximum Expected Solar Radiation at Various North Latitudes ... [Pg.1171]

The chlorine-containing product species (HCl, CIONO2, HOCl) are "inert reservoirs" because they are not directly involved in ozone depletion however, they eventually break down by absorbing solar radiation or by reaction with other free radicals, returning chlorine to its catalytically active form. Ozone is formed fastest in the upper stratosphere at tropical latitudes (by reactions 1 and 2), and in those regions a few percent of the chlorine is in its active "free radical" form the rest is in the "inert reservoir" form (see Figure 3). [Pg.27]

The kinetics of the various reactions have been explored in detail using large-volume chambers that can be used to simulate reactions in the troposphere. They have frequently used hydroxyl radicals formed by photolysis of methyl (or ethyl) nitrite, with the addition of NO to inhibit photolysis of NO2. This would result in the formation of 0( P) atoms, and subsequent reaction with Oj would produce ozone, and hence NO3 radicals from NOj. Nitrate radicals are produced by the thermal decomposition of NjOj, and in experiments with O3, a scavenger for hydroxyl radicals is added. Details of the different experimental procedures for the measurement of absolute and relative rates have been summarized, and attention drawn to the often considerable spread of values for experiments carried out at room temperature (-298 K) (Atkinson 1986). It should be emphasized that in the real troposphere, both the rates—and possibly the products—of transformation will be determined by seasonal differences both in temperature and the intensity of solar radiation. These are determined both by latitude and altitude. [Pg.16]

Significant economies of computation are possible in systems that consist of a one-dimensional chain of identical reservoirs. Chapter 7 describes such a system in which there is just one dependent variable. An illustrative example is the climate system and the calculation of zonally averaged temperature as a function of latitude in an energy balance climate model. In such a model, the surface temperature depends on the balance among solar radiation absorbed, planetary radiation emitted to space, and the transport of energy between latitudes. I present routines that calculate the absorption and reflection of incident solar radiation and the emission of long-wave planetary radiation. I show how much of the computational work can be avoided in a system like this because each reservoir is coupled only to its adjacent reservoirs. I use the simulation to explore the sensitivity of seasonally varying temperatures to such aspects of the climate system as snow and ice cover, cloud cover, amount of carbon dioxide in the atmosphere, and land distribution. [Pg.6]

Fig. 7-8. Solar radiation incident on a horizontal surface (insolation) as a function of time at various latitudes in the Southern Hemisphere. Fig. 7-8. Solar radiation incident on a horizontal surface (insolation) as a function of time at various latitudes in the Southern Hemisphere.
I also applied the revised computational method to calculate zonally averaged temperature as a function of latitude. I introduced an energy balance climate model, which calculates surface temperature for absorbed solar energy, emitted planetary radiation, and the transport of heat between... [Pg.148]

Zerefos, C. S., A. F. Bais, C. Meleti, and I. C. Ziomas, A Note on the Recent Increase of Solar UV-B Radiation over Northern Middle Latitudes, Geophys. Res. Lett., 22, 1245-1247 (1995). [Pg.761]

It has been known for about 50 years4 that the annual variations in ozone do not correspond to these of the solar radiation depending on the latitude and the season. The behavior of ozone is characterized by a maximum in spring and a minimum in autumn also there is more ozone at high than at low latitudes. This behavior shows that the chemical reactions in question are slow, in comparison with transport phenomena, in the lower stratosphere below 25 km. [Pg.67]


See other pages where Radiation, solar, latitude is mentioned: [Pg.8]    [Pg.125]    [Pg.30]    [Pg.249]    [Pg.29]    [Pg.441]    [Pg.212]    [Pg.98]    [Pg.100]    [Pg.137]    [Pg.149]    [Pg.139]    [Pg.222]    [Pg.222]    [Pg.30]    [Pg.161]    [Pg.610]    [Pg.611]    [Pg.66]    [Pg.208]    [Pg.723]    [Pg.992]    [Pg.129]    [Pg.129]    [Pg.814]    [Pg.487]    [Pg.489]    [Pg.627]    [Pg.34]    [Pg.30]    [Pg.108]    [Pg.169]    [Pg.373]    [Pg.375]    [Pg.381]    [Pg.160]    [Pg.174]   
See also in sourсe #XX -- [ Pg.24 ]




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Latitude

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