The origin of the composition and structure of the atmosphere. Earth's atmosphere: history of appearance and structure

The thickness of the atmosphere is about 120 km from the Earth's surface. The total mass of air in the atmosphere is (5.1-5.3) 10 18 kg. Of these, the mass of dry air is 5.1352 ± 0.0003 10 18 kg, the total mass of water vapor is on average 1.27 10 16 kg.

tropopause

The transitional layer from the troposphere to the stratosphere, the layer of the atmosphere in which the decrease in temperature with height stops.

Stratosphere

The layer of the atmosphere located at an altitude of 11 to 50 km. A slight change in temperature in the 11-25 km layer (lower layer of the stratosphere) and its increase in the 25-40 km layer from −56.5 to 0.8 ° (upper stratosphere or inversion region) are typical. Having reached a value of about 273 K (almost 0 °C) at an altitude of about 40 km, the temperature remains constant up to an altitude of about 55 km. This region of constant temperature is called the stratopause and is the boundary between the stratosphere and the mesosphere.

Stratopause

The boundary layer of the atmosphere between the stratosphere and the mesosphere. There is a maximum in the vertical temperature distribution (about 0 °C).

Mesosphere

Earth's atmosphere

Earth's atmosphere boundary

Thermosphere

The upper limit is about 800 km. The temperature rises to altitudes of 200-300 km, where it reaches values ​​of the order of 1500 K, after which it remains almost constant up to high altitudes. Under the influence of ultraviolet and x-ray solar radiation and cosmic radiation, air is ionized ("polar lights") - the main regions of the ionosphere lie inside the thermosphere. At altitudes above 300 km, atomic oxygen predominates. The upper limit of the thermosphere is largely determined by the current activity of the Sun. During periods of low activity - for example, in 2008-2009 - there is a noticeable decrease in the size of this layer.

Thermopause

The region of the atmosphere above the thermosphere. In this region, the absorption of solar radiation is insignificant and the temperature does not actually change with height.

Exosphere (scattering sphere)

Up to a height of 100 km, the atmosphere is a homogeneous, well-mixed mixture of gases. In more high layers the distribution of gases in height depends on their molecular masses, the concentration of heavier gases decreases faster with distance from the Earth's surface. Due to the decrease in gas density, the temperature drops from 0 °C in the stratosphere to −110 °C in the mesosphere. However, the kinetic energy of individual particles at altitudes of 200–250 km corresponds to a temperature of ~150 °C. Above 200 km, significant fluctuations in temperature and gas density are observed in time and space.

At an altitude of about 2000-3500 km, the exosphere gradually passes into the so-called near space vacuum, which is filled with highly rarefied particles of interplanetary gas, mainly hydrogen atoms. But this gas is only part of the interplanetary matter. The other part is composed of dust-like particles of cometary and meteoric origin. In addition to extremely rarefied dust-like particles, electromagnetic and corpuscular radiation of solar and galactic origin penetrates into this space.

The troposphere accounts for about 80% of the mass of the atmosphere, the stratosphere accounts for about 20%; the mass of the mesosphere is no more than 0.3%, the thermosphere is less than 0.05% of the total mass of the atmosphere. Based on the electrical properties in the atmosphere, the neutrosphere and ionosphere are distinguished. It is currently believed that the atmosphere extends to an altitude of 2000-3000 km.

Depending on the composition of the gas in the atmosphere, they emit homosphere and heterosphere. heterosphere- this is an area where gravity affects the separation of gases, since their mixing at such a height is negligible. Hence follows the variable composition of the heterosphere. Below it lies a well-mixed, homogeneous part of the atmosphere, called the homosphere. The boundary between these layers is called turbopause, it lies at an altitude of about 120 km.

Physiological and other properties of the atmosphere

Already at an altitude of 5 km above sea level, an untrained person develops oxygen starvation and, without adaptation, a person's performance is significantly reduced. This is where the physiological zone of the atmosphere ends. Human breathing becomes impossible at an altitude of 9 km, although up to about 115 km the atmosphere contains oxygen.

The atmosphere provides us with the oxygen we need to breathe. However, due to the drop in the total pressure of the atmosphere as you rise to a height, the partial pressure of oxygen also decreases accordingly.

In rarefied layers of air, the propagation of sound is impossible. Up to altitudes of 60-90 km, it is still possible to use air resistance and lift for controlled aerodynamic flight. But starting from altitudes of 100-130 km, the concepts of the M number and the sound barrier familiar to every pilot lose their meaning: there passes the conditional Karman line, beyond which the area of ​​\u200b\u200bpurely ballistic flight begins, which can only be controlled using reactive forces.

At altitudes above 100 km, the atmosphere is also deprived of another remarkable property - the ability to absorb, conduct and transfer thermal energy by convection (i.e., by means of air mixing). This means that various elements of equipment, equipment of the orbital space station will not be able to be cooled from the outside in the way it is usually done on an airplane - with the help of air jets and air radiators. At such a height, as in space in general, the only way to transfer heat is thermal radiation.

History of the formation of the atmosphere

According to the most common theory, the Earth's atmosphere has been in three different compositions over time. Initially, it consisted of light gases (hydrogen and helium) captured from interplanetary space. This so-called primary atmosphere(about four billion years ago). At the next stage, active volcanic activity led to the saturation of the atmosphere with gases other than hydrogen (carbon dioxide, ammonia, water vapor). This is how secondary atmosphere(about three billion years before our days). This atmosphere was restorative. Further, the process of formation of the atmosphere was determined by the following factors:

  • leakage of light gases (hydrogen and helium) into interplanetary space;
  • chemical reactions occurring in the atmosphere under the influence of ultraviolet radiation, lightning discharges and some other factors.

Gradually, these factors led to the formation tertiary atmosphere, characterized by a much lower content of hydrogen and a much higher content of nitrogen and carbon dioxide (formed as a result of chemical reactions from ammonia and hydrocarbons).

Nitrogen

The formation of a large amount of nitrogen N 2 is due to the oxidation of the ammonia-hydrogen atmosphere by molecular oxygen O 2, which began to come from the surface of the planet as a result of photosynthesis, starting from 3 billion years ago. Nitrogen N 2 is also released into the atmosphere as a result of the denitrification of nitrates and other nitrogen-containing compounds. Nitrogen is oxidized by ozone to NO in the upper atmosphere.

Nitrogen N 2 enters into reactions only under specific conditions (for example, during a lightning discharge). Oxidation of molecular nitrogen by ozone during electrical discharges is used in small quantities in the industrial production of nitrogen fertilizers. It can be oxidized with low energy consumption and converted into a biologically active form by cyanobacteria (blue-green algae) and nodule bacteria that form rhizobial symbiosis with legumes, the so-called. green manure.

Oxygen

The composition of the atmosphere began to change radically with the advent of living organisms on Earth, as a result of photosynthesis, accompanied by the release of oxygen and the absorption of carbon dioxide. Initially, oxygen was spent on the oxidation of reduced compounds - ammonia, hydrocarbons, the ferrous form of iron contained in the oceans, etc. At the end of this stage, the oxygen content in the atmosphere began to grow. Gradually, a modern atmosphere with oxidizing properties formed. Since this caused serious and abrupt changes in many processes occurring in the atmosphere, lithosphere and biosphere, this event was called the Oxygen catastrophe.

noble gases

Air pollution

AT recent times man began to influence the evolution of the atmosphere. The result of his activities was a constant significant increase in the content of carbon dioxide in the atmosphere due to the combustion of hydrocarbon fuels accumulated in previous geological epochs. Huge amounts of CO 2 are consumed during photosynthesis and absorbed by the world's oceans. This gas enters the atmosphere due to the decomposition of carbonate rocks and organic substances of plant and animal origin, as well as due to volcanism and human production activities. Over the past 100 years, the content of CO 2 in the atmosphere has increased by 10%, with the main part (360 billion tons) coming from fuel combustion. If the growth rate of fuel combustion continues, then in the next 200-300 years the amount of CO 2 in the atmosphere will double and may lead to global climate change.

Fuel combustion is the main source of polluting gases (СО,, SO 2). Sulfur dioxide is oxidized by atmospheric oxygen to SO 3 in the upper atmosphere, which in turn interacts with water vapor and ammonia, and the resulting sulfuric acid (H 2 SO 4) and ammonium sulfate ((NH 4) 2 SO 4) return to the surface of the Earth in the form of a so-called. acid rain. The use of internal combustion engines leads to significant air pollution with nitrogen oxides, hydrocarbons and lead compounds (tetraethyl lead Pb (CH 3 CH 2) 4)).

Aerosol pollution of the atmosphere is caused both by natural causes (volcanic eruption, dust storms, entrainment of sea water droplets and plant pollen, etc.) and by human economic activity (mining of ores and building materials, fuel combustion, cement production, etc.). Intense large-scale removal of solid particles into the atmosphere is one of the possible causes of climate change on the planet.

see also

  • Jacchia (atmosphere model)

Notes

Links

Literature

  1. V. V. Parin, F. P. Kosmolinsky, B. A. Dushkov"Space biology and medicine" (2nd edition, revised and supplemented), M .: "Prosveshchenie", 1975, 223 pages.
  2. N. V. Gusakova"Chemistry of the environment", Rostov-on-Don: Phoenix, 2004, 192 with ISBN 5-222-05386-5
  3. Sokolov V. A. Geochemistry of natural gases, M., 1971;
  4. McEwen M, Phillips L. Chemistry of the atmosphere, M., 1978;
  5. Wark K., Warner S. Air pollution. Sources and control, trans. from English, M.. 1980;
  6. Monitoring of background pollution of natural environments. in. 1, L., 1982.

Atmosphere(from the Greek atmos - steam and spharia - ball) - the air shell of the Earth, rotating with it. The development of the atmosphere was closely connected with the geological and geochemical processes taking place on our planet, as well as with the activities of living organisms.

The lower boundary of the atmosphere coincides with the surface of the Earth, since air penetrates into the smallest pores in the soil and is dissolved even in water.

The upper limit at an altitude of 2000-3000 km gradually passes into outer space.

Oxygen-rich atmosphere makes life possible on Earth. Atmospheric oxygen is used in the process of breathing by humans, animals, and plants.

If there were no atmosphere, the Earth would be as quiet as the moon. After all, sound is the vibration of air particles. The blue color of the sky is explained by the fact that the sun's rays, passing through the atmosphere, as if through a lens, are decomposed into their component colors. In this case, the rays of blue and blue colors are scattered most of all.

The atmosphere retains most of the ultraviolet radiation from the Sun, which has a detrimental effect on living organisms. It also keeps heat at the surface of the Earth, preventing our planet from cooling.

The structure of the atmosphere

Several layers can be distinguished in the atmosphere, differing in density and density (Fig. 1).

Troposphere

Troposphere- the lowest layer of the atmosphere, whose thickness above the poles is 8-10 km, in temperate latitudes - 10-12 km, and above the equator - 16-18 km.

Rice. 1. The structure of the Earth's atmosphere

The air in the troposphere is heated from the earth's surface, i.e. from land and water. Therefore, the air temperature in this layer decreases with height by an average of 0.6 °C for every 100 m. At the upper boundary of the troposphere, it reaches -55 °C. At the same time, in the region of the equator at the upper boundary of the troposphere, the air temperature is -70 °С, and in the region of the North Pole -65 °С.

About 80% of the mass of the atmosphere is concentrated in the troposphere, almost all water vapor is located, thunderstorms, storms, clouds and precipitation occur, and vertical (convection) and horizontal (wind) air movement occurs.

We can say that the weather is mainly formed in the troposphere.

Stratosphere

Stratosphere- the layer of the atmosphere located above the troposphere at an altitude of 8 to 50 km. The color of the sky in this layer appears purple, which is explained by the rarefaction of the air, due to which the sun's rays almost do not scatter.

The stratosphere contains 20% of the mass of the atmosphere. The air in this layer is rarefied, there is practically no water vapor, and therefore clouds and precipitation are almost not formed. However, stable air currents are observed in the stratosphere, the speed of which reaches 300 km / h.

This layer is concentrated ozone(ozone screen, ozonosphere), a layer that absorbs ultraviolet rays, preventing them from passing to the Earth and thereby protecting living organisms on our planet. Due to ozone, the air temperature at the upper boundary of the stratosphere is in the range from -50 to 4-55 °C.

Between the mesosphere and the stratosphere there is a transitional zone - the stratopause.

Mesosphere

Mesosphere- a layer of the atmosphere located at an altitude of 50-80 km. The air density here is 200 times less than at the surface of the Earth. The color of the sky in the mesosphere appears black, stars are visible during the day. The air temperature drops to -75 (-90)°С.

At an altitude of 80 km begins thermosphere. The air temperature in this layer rises sharply to a height of 250 m, and then becomes constant: at a height of 150 km it reaches 220-240 °C; at an altitude of 500-600 km it exceeds 1500 °C.

In the mesosphere and thermosphere, under the action of cosmic rays, gas molecules break up into charged (ionized) particles of atoms, so this part of the atmosphere is called ionosphere- a layer of very rarefied air, located at an altitude of 50 to 1000 km, consisting mainly of ionized oxygen atoms, nitric oxide molecules and free electrons. This layer is characterized by high electrification, and long and medium radio waves are reflected from it, as from a mirror.

In the ionosphere, auroras arise - the glow of rarefied gases under the influence of electrically charged particles flying from the Sun - and sharp fluctuations in the magnetic field are observed.

Exosphere

Exosphere- the outer layer of the atmosphere, located above 1000 km. This layer is also called the scattering sphere, since gas particles move here at high speed and can be scattered into outer space.

Composition of the atmosphere

The atmosphere is a mixture of gases consisting of nitrogen (78.08%), oxygen (20.95%), carbon dioxide (0.03%), argon (0.93%), a small amount of helium, neon, xenon, krypton (0.01%), ozone and other gases, but their content is negligible (Table 1). The modern composition of the Earth's air was established more than a hundred million years ago, but the sharply increased production activity man nevertheless led to his change. Currently, there is an increase in the content of CO 2 by about 10-12%.

The gases that make up the atmosphere perform various functional roles. However, the main significance of these gases is determined primarily by the fact that they very strongly absorb radiant energy and thus have a significant effect on the temperature regime of the Earth's surface and atmosphere.

Table 1. Chemical composition of dry atmospheric air at the earth's surface

Volume concentration. %

Molecular weight, units

Oxygen

Carbon dioxide

Nitrous oxide

0 to 0.00001

Sulfur dioxide

from 0 to 0.000007 in summer;

0 to 0.000002 in winter

From 0 to 0.000002

46,0055/17,03061

Azog dioxide

Carbon monoxide

Nitrogen, the most common gas in the atmosphere, chemically little active.

Oxygen, unlike nitrogen, is a chemically very active element. The specific function of oxygen is the oxidation of organic matter of heterotrophic organisms, rocks, and incompletely oxidized gases emitted into the atmosphere by volcanoes. Without oxygen, there would be no decomposition of dead organic matter.

The role of carbon dioxide in the atmosphere is exceptionally great. It enters the atmosphere as a result of the processes of combustion, respiration of living organisms, decay and is, first of all, the main building material for the creation of organic matter during photosynthesis. In addition, the property of carbon dioxide to transmit short-wave solar radiation and absorb part of thermal long-wave radiation is of great importance, which will create the so-called greenhouse effect, which will be discussed below.

The influence on atmospheric processes, especially on the thermal regime of the stratosphere, is also exerted by ozone. This gas serves as a natural absorber of solar ultraviolet radiation, and the absorption of solar radiation leads to air heating. The average monthly values ​​of the total ozone content in the atmosphere vary depending on the latitude of the area and the season within 0.23-0.52 cm (this is the thickness of the ozone layer at ground pressure and temperature). There is an increase in the ozone content from the equator to the poles and an annual variation with a minimum in autumn and a maximum in spring.

A characteristic property of the atmosphere can be called the fact that the content of the main gases (nitrogen, oxygen, argon) changes slightly with height: at an altitude of 65 km in the atmosphere, the nitrogen content is 86%, oxygen - 19, argon - 0.91, at an altitude of 95 km - nitrogen 77, oxygen - 21.3, argon - 0.82%. The constancy of the composition of atmospheric air vertically and horizontally is maintained by its mixing.

In addition to gases, air contains water vapor and solid particles. The latter can have both natural and artificial (anthropogenic) origin. These are flower pollen, tiny salt crystals, road dust, aerosol impurities. When the sun's rays penetrate the window, they can be seen with the naked eye.

There are especially many particulate matter in the air of cities and large industrial centers, where emissions of harmful gases and their impurities formed during fuel combustion are added to aerosols.

The concentration of aerosols in the atmosphere determines the transparency of the air, which affects the solar radiation reaching the Earth's surface. The largest aerosols are condensation nuclei (from lat. condensatio- compaction, thickening) - contribute to the transformation of water vapor into water droplets.

The value of water vapor is determined primarily by the fact that it delays the long-wave thermal radiation of the earth's surface; represents the main link of large and small moisture cycles; raises the temperature of the air when the water beds condense.

The amount of water vapor in the atmosphere varies over time and space. Thus, the concentration of water vapor near the earth's surface ranges from 3% in the tropics to 2-10 (15)% in Antarctica.

The average content of water vapor in the vertical column of the atmosphere in temperate latitudes is about 1.6-1.7 cm (the layer of condensed water vapor will have such a thickness). Information about water vapor in different layers of the atmosphere is contradictory. It was assumed, for example, that in the altitude range from 20 to 30 km, the specific humidity strongly increases with height. However, subsequent measurements indicate a greater dryness of the stratosphere. Apparently, the specific humidity in the stratosphere depends little on height and amounts to 2–4 mg/kg.

The variability of water vapor content in the troposphere is determined by the interaction of evaporation, condensation, and horizontal transport. As a result of the condensation of water vapor, clouds form and precipitation occurs in the form of rain, hail and snow.

The processes of phase transitions of water proceed mainly in the troposphere, which is why clouds in the stratosphere (at altitudes of 20-30 km) and mesosphere (near the mesopause), called mother-of-pearl and silver, are observed relatively rarely, while tropospheric clouds often cover about 50% of the entire earth surfaces.

The amount of water vapor that can be contained in the air depends on the temperature of the air.

1 m 3 of air at a temperature of -20 ° C can contain no more than 1 g of water; at 0 °C - no more than 5 g; at +10 °С - no more than 9 g; at +30 °С - no more than 30 g of water.

Conclusion: The higher the air temperature, the more water vapor it can contain.

Air can be rich and not saturated steam. So, if at a temperature of +30 ° C 1 m 3 of air contains 15 g of water vapor, the air is not saturated with water vapor; if 30 g - saturated.

Absolute humidity- this is the amount of water vapor contained in 1 m 3 of air. It is expressed in grams. For example, if they say "absolute humidity is 15", then this means that 1 mL contains 15 g of water vapor.

Relative humidity- this is the ratio (in percent) of the actual content of water vapor in 1 m 3 of air to the amount of water vapor that can be contained in 1 m L at a given temperature. For example, if a weather report is broadcast over the radio that the relative humidity is 70%, this means that the air contains 70% of the water vapor that it can hold at a given temperature.

The greater the relative humidity of the air, t. the closer the air is to saturation, the more likely it is to fall.

Always high (up to 90%) relative humidity is observed in the equatorial zone, since there is a high air temperature throughout the year and there is a large evaporation from the surface of the oceans. The same high relative humidity is in the polar regions, but only because at low temperatures even a small amount of water vapor makes the air saturated or close to saturation. In temperate latitudes, relative humidity varies seasonally - it is higher in winter and lower in summer.

The relative humidity of the air is especially low in deserts: 1 m 1 of air there contains two to three times less than the amount of water vapor possible at a given temperature.

To measure relative humidity, a hygrometer is used (from the Greek hygros - wet and metreco - I measure).

When cooled, saturated air cannot retain the same amount of water vapor in itself, it thickens (condenses), turning into droplets of fog. Fog can be observed in the summer on a clear cool night.

Clouds- this is the same fog, only it is formed not at the earth's surface, but at a certain height. As the air rises, it cools and the water vapor in it condenses. The resulting tiny droplets of water make up the clouds.

involved in the formation of clouds particulate matter suspended in the troposphere.

Clouds can have a different shape, which depends on the conditions of their formation (Table 14).

The lowest and heaviest clouds are stratus. They are located at an altitude of 2 km from the earth's surface. At an altitude of 2 to 8 km, more picturesque cumulus clouds can be observed. The highest and lightest are cirrus clouds. They are located at an altitude of 8 to 18 km above the earth's surface.

families

Kinds of clouds

Appearance

A. Upper clouds - above 6 km

I. Pinnate

Threadlike, fibrous, white

II. cirrocumulus

Layers and ridges of small flakes and curls, white

III. Cirrostratus

Transparent whitish veil

B. Clouds of the middle layer - above 2 km

IV. Altocumulus

Layers and ridges of white and gray

V. Altostratified

Smooth veil of milky gray color

B. Lower clouds - up to 2 km

VI. Nimbostratus

Solid shapeless gray layer

VII. Stratocumulus

Opaque layers and ridges of gray

VIII. layered

Illuminated gray veil

D. Clouds of vertical development - from the lower to the upper tier

IX. Cumulus

Clubs and domes bright white, with torn edges in the wind

X. Cumulonimbus

Powerful cumulus-shaped masses of dark lead color

Atmospheric protection

The main sources are industrial enterprises and automobiles. In large cities, the problem of gas contamination of the main transport routes is very acute. That is why in many large cities of the world, including our country, environmental control car exhaust toxicity. According to experts, smoke and dust in the air can halve the flow of solar energy to the earth's surface, which will lead to a change in natural conditions.

ATMOSPHERE
gaseous envelope surrounding a celestial body. Its characteristics depend on the size, mass, temperature, rotation speed and chemical composition of a given celestial body, and are also determined by the history of its formation from the moment of its birth. Earth's atmosphere is made up of a mixture of gases called air. Its main constituents are nitrogen and oxygen in a ratio of approximately 4:1. A person is affected mainly by the state of the lower 15-25 km of the atmosphere, since it is in this lower layer that the bulk of the air is concentrated. The science that studies the atmosphere is called meteorology, although the subject of this science is also the weather and its effect on humans. The state of the upper layers of the atmosphere, located at altitudes from 60 to 300 and even 1000 km from the Earth's surface, is also changing. Strong winds, storms develop here, and such amazing electrical phenomena as auroras appear. Many of these phenomena are associated with fluxes of solar radiation, cosmic radiation, and the Earth's magnetic field. The high layers of the atmosphere are also a chemical laboratory, since there, under conditions close to vacuum, some atmospheric gases, under the influence of a powerful flow of solar energy, enter into chemical reactions. The science that studies these interrelated phenomena and processes is called the physics of the high layers of the atmosphere.
GENERAL CHARACTERISTICS OF THE EARTH'S ATMOSPHERE
Dimensions. Until sounding rockets and artificial satellites explored the outer layers of the atmosphere at distances several times greater than the radius of the Earth, it was believed that as you move away from the earth's surface, the atmosphere gradually becomes more rarefied and smoothly passes into interplanetary space. It has now been established that energy flows from the deep layers of the Sun penetrate into outer space far beyond the Earth's orbit, up to the outer limits of the Solar System. This so-called. sunny wind flows around the Earth's magnetic field, forming an elongated "cavity", inside which the Earth's atmosphere is concentrated. The Earth's magnetic field is noticeably narrowed on the day side facing the Sun and forms a long tongue, probably extending beyond the orbit of the Moon, on the opposite, night side. The boundary of the Earth's magnetic field is called the magnetopause. On the day side, this boundary passes at a distance of about seven Earth radii from the surface, but during periods of increased solar activity it is even closer to the Earth's surface. The magnetopause is also the boundary of the earth's atmosphere, the outer shell of which is also called the magnetosphere, since it contains charged particles (ions), whose movement is due to the earth's magnetic field. The total weight of atmospheric gases is approximately 4.5*1015 tons. Thus, the "weight" of the atmosphere per unit area, or atmospheric pressure, is approximately 11 tons/m2 at sea level.
Significance for life. It follows from the above that the Earth is separated from interplanetary space by a powerful protective layer. Outer space is permeated with powerful ultraviolet and X-ray radiation from the Sun and even harder cosmic radiation, and these types of radiation are detrimental to all living things. At the outer edge of the atmosphere, the radiation intensity is lethal, but a significant part of it is retained by the atmosphere far from the Earth's surface. The absorption of this radiation explains many properties of the high layers of the atmosphere, and especially the electrical phenomena that occur there. The lowest, surface layer of the atmosphere is especially important for a person who lives at the point of contact of the solid, liquid and gaseous shells of the Earth. The upper shell of the "solid" Earth is called the lithosphere. About 72% of the Earth's surface is covered by the waters of the oceans, which make up most of the hydrosphere. The atmosphere borders both the lithosphere and the hydrosphere. Man lives at the bottom of the air ocean and near or above the level of the water ocean. The interaction of these oceans is one of the important factors that determine the state of the atmosphere.
Compound. The lower layers of the atmosphere consist of a mixture of gases (see table). In addition to those listed in the table, other gases are also present in the form of small impurities in the air: ozone, methane, substances such as carbon monoxide (CO), nitrogen and sulfur oxides, ammonia.

COMPOSITION OF THE ATMOSPHERE


In the high layers of the atmosphere, the composition of the air changes under the influence of hard radiation from the Sun, which leads to the breakdown of oxygen molecules into atoms. Atomic oxygen is the main component of the high layers of the atmosphere. Finally, in the most distant layers of the atmosphere from the surface of the Earth, the lightest gases, hydrogen and helium, become the main components. Since the bulk of matter is concentrated in the lower 30 km, changes in air composition at altitudes above 100 km do not have a noticeable effect on the overall composition of the atmosphere.
Energy exchange. The sun is the main source of energy coming to the Earth. Being at a distance of approx. 150 million km from the Sun, the Earth receives about one two billionth of the energy it radiates, mainly in the visible part of the spectrum, which man calls "light". Most of this energy is absorbed by the atmosphere and lithosphere. The earth also radiates energy, mostly in the form of far infrared radiation. Thus, a balance is established between the energy received from the Sun, the heating of the Earth and the atmosphere, and the reverse flow of thermal energy radiated into space. The mechanism of this balance is extremely complex. Dust and gas molecules scatter light, partially reflecting it into the world space. Clouds reflect even more of the incoming radiation. Part of the energy is absorbed directly by gas molecules, but mostly by rocks, vegetation and surface waters. Water vapor and carbon dioxide present in the atmosphere transmit visible radiation but absorb infrared radiation. Thermal energy accumulates mainly in the lower layers of the atmosphere. A similar effect occurs in a greenhouse when the glass lets light in and the soil heats up. Since glass is relatively opaque to infrared radiation, heat accumulates in the greenhouse. The heating of the lower atmosphere due to the presence of water vapor and carbon dioxide is often referred to as the greenhouse effect. Cloudiness plays a significant role in the conservation of heat in the lower layers of the atmosphere. If the clouds dissipate or the transparency of the air masses increases, the temperature will inevitably decrease as the surface of the Earth freely radiates thermal energy into the surrounding space. Water on the surface of the Earth absorbs solar energy and evaporates, turning into a gas - water vapor, which carries a huge amount of energy into the lower atmosphere. When water vapor condenses and forms clouds or fog, this energy is released in the form of heat. About half of the solar energy reaching the earth's surface is spent on the evaporation of water and enters the lower atmosphere. Thus, due to the greenhouse effect and the evaporation of water, the atmosphere warms up from below. This partly explains the high activity of its circulation in comparison with the circulation of the World Ocean, which warms up only from above and is therefore much more stable than the atmosphere.
See also METEOROLOGY AND CLIMATOLOGY. In addition to the general heating of the atmosphere by solar "light", significant heating of some of its layers occurs due to ultraviolet and X-ray radiation from the Sun. Structure. Compared to liquids and solids, in gaseous substances, the force of attraction between molecules is minimal. As the distance between molecules increases, gases are able to expand indefinitely if nothing prevents them. The lower boundary of the atmosphere is the surface of the Earth. Strictly speaking, this barrier is impenetrable, since gas exchange occurs between air and water and even between air and rocks, but in this case these factors can be neglected. Since the atmosphere is a spherical shell, it has no side boundaries, but only a lower boundary and an upper (outer) boundary open from the side of interplanetary space. Through the outer boundary, some neutral gases leak out, as well as the flow of matter from the surrounding outer space. Most of the charged particles, with the exception of high-energy cosmic rays, are either captured by the magnetosphere or repelled by it. The atmosphere is also affected by the force of gravity, which keeps the air shell at the surface of the Earth. Atmospheric gases are compressed by their own weight. This compression is maximum at the lower boundary of the atmosphere, and therefore the air density is the highest here. At any height above the earth's surface, the degree of air compression depends on the mass of the overlying air column, so the air density decreases with height. The pressure, equal to the mass of the overlying air column per unit area, is directly related to the density and, therefore, also decreases with height. If the atmosphere were an "ideal gas" with a constant composition independent of height, a constant temperature, and a constant force of gravity acting on it, then the pressure would decrease by a factor of 10 for every 20 km of altitude. The real atmosphere slightly differs from the ideal gas up to about 100 km, and then the pressure decreases more slowly with height, as the composition of the air changes. Small changes in the described model are also introduced by a decrease in the force of gravity with distance from the center of the Earth, amounting to approx. 3% for every 100 km of altitude. Unlike atmospheric pressure, temperature does not decrease continuously with altitude. As shown in fig. 1, it decreases to approximately 10 km and then begins to rise again. This occurs when oxygen absorbs ultraviolet solar radiation. In this case, ozone gas is formed, the molecules of which consist of three oxygen atoms (O3). It also absorbs ultraviolet radiation, and therefore this layer of the atmosphere, called the ozonosphere, heats up. Higher, the temperature drops again, since there are much fewer gas molecules, and the energy absorption is correspondingly reduced. In even higher layers, the temperature rises again due to the absorption of the shortest wavelength ultraviolet and X-ray radiation from the Sun by the atmosphere. Under the influence of this powerful radiation, the atmosphere is ionized, i.e. A gas molecule loses an electron and acquires a positive electric charge. Such molecules become positively charged ions. Due to the presence of free electrons and ions, this layer of the atmosphere acquires the properties of an electrical conductor. It is believed that the temperature continues to rise to heights where the rarefied atmosphere passes into interplanetary space. At a distance of several thousand kilometers from the surface of the Earth, temperatures from 5,000° to 10,000° C probably prevail. Although molecules and atoms have very high speeds of movement, and therefore a high temperature, this rarefied gas is not "hot" in the usual sense. . Due to the meager number of molecules at high altitudes, their total thermal energy is very small. Thus, the atmosphere consists of separate layers (i.e., a series of concentric shells, or spheres), the selection of which depends on which property is of greatest interest. Based on the average temperature distribution, meteorologists have developed a scheme for the structure of an ideal "middle atmosphere" (see Fig. 1).

Troposphere - the lower layer of the atmosphere, extending to the first thermal minimum (the so-called tropopause). The upper limit of the troposphere depends on the geographical latitude (in the tropics - 18-20 km, in temperate latitudes - about 10 km) and the time of year. The US National Weather Service conducted soundings near the South Pole and revealed seasonal changes in the height of the tropopause. In March, the tropopause is at an altitude of approx. 7.5 km. From March to August or September there is a steady cooling of the troposphere, and its boundary rises for a short period in August or September to a height of approximately 11.5 km. Then from September to December it drops rapidly and reaches its lowest position - 7.5 km, where it remains until March, fluctuating within only 0.5 km. It is in the troposphere that the weather is mainly formed, which determines the conditions for human existence. Most of the atmospheric water vapor is concentrated in the troposphere, and therefore clouds form mainly here, although some of them, consisting of ice crystals, are also found in the higher layers. The troposphere is characterized by turbulence and powerful air currents (winds) and storms. In the upper troposphere, there are strong air currents of a strictly defined direction. Turbulent eddies, like small whirlpools, are formed under the influence of friction and dynamic interaction between slow and fast moving air masses. Since there is usually no cloud cover in these high layers, this turbulence is referred to as "clear air turbulence".
Stratosphere. The upper layer of the atmosphere is often erroneously described as a layer with relatively constant temperatures, where the winds blow more or less steadily and where the meteorological elements change little. The upper layers of the stratosphere heat up as oxygen and ozone absorb solar ultraviolet radiation. The upper boundary of the stratosphere (stratopause) is drawn where the temperature rises slightly, reaching an intermediate maximum, which is often comparable to the temperature of the surface air layer. Based on observations made with airplanes and balloons adapted to fly at a constant altitude, turbulent disturbances and strong winds blowing in different directions have been established in the stratosphere. As in the troposphere, powerful air vortices are noted, which are especially dangerous for high-speed aircraft. Strong winds, called jet streams, blow in narrow zones along the borders of temperate latitudes facing the poles. However, these zones can shift, disappear and reappear. Jet streams usually penetrate the tropopause and appear in the upper troposphere, but their speed decreases rapidly with decreasing altitude. It is possible that part of the energy entering the stratosphere (mainly spent on the formation of ozone) affects the processes in the troposphere. Particularly active mixing is associated with atmospheric fronts, where extensive flows of stratospheric air were recorded significantly below the tropopause, and tropospheric air was drawn into the lower layers of the stratosphere. Significant progress has been made in the study of the vertical structure of the lower layers of the atmosphere in connection with the improvement of the technique of launching radiosondes to altitudes of 25-30 km. The mesosphere, located above the stratosphere, is a shell in which, up to a height of 80-85 km, the temperature drops to the minimum for the atmosphere as a whole. Record low temperatures down to -110°C were recorded by meteorological rockets launched from the US-Canadian installation at Fort Churchill (Canada). The upper limit of the mesosphere (mesopause) approximately coincides with the lower limit of the region of active absorption of the X-ray and the shortest wavelength ultraviolet radiation of the Sun, which is accompanied by heating and ionization of the gas. In the polar regions in summer, cloud systems often appear in the mesopause, which occupy a large area, but have little vertical development. Such clouds glowing at night often make it possible to detect large-scale undulating air movements in the mesosphere. The composition of these clouds, sources of moisture and condensation nuclei, dynamics and relationship with meteorological factors are still insufficiently studied. The thermosphere is a layer of the atmosphere in which the temperature rises continuously. Its power can reach 600 km. The pressure and, consequently, the density of a gas constantly decrease with height. Near the earth's surface, 1 m3 of air contains approx. 2.5x1025 molecules, at a height of approx. 100 km, in the lower layers of the thermosphere - approximately 1019, at an altitude of 200 km, in the ionosphere - 5 * 10 15 and, according to calculations, at an altitude of approx. 850 km - approximately 1012 molecules. In interplanetary space, the concentration of molecules is 10 8-10 9 per 1 m3. At a height of approx. 100 km, the number of molecules is small, and they rarely collide with each other. The average distance traveled by a randomly moving molecule before colliding with another similar molecule is called its mean free path. The layer in which this value increases so much that the probability of intermolecular or interatomic collisions can be neglected is located on the boundary between the thermosphere and the overlying shell (exosphere) and is called the thermal pause. The thermopause is located approximately 650 km from the earth's surface. At a certain temperature, the speed of a molecule's movement depends on its mass: lighter molecules move faster than heavy ones. In the lower atmosphere, where the free path is very short, there is no noticeable separation of gases according to their molecular weight, but it is expressed above 100 km. In addition, under the influence of ultraviolet and X-ray radiation from the Sun, oxygen molecules break up into atoms, the mass of which is half the mass of the molecule. Therefore, as we move away from the Earth's surface, atomic oxygen becomes increasingly important in the composition of the atmosphere and at an altitude of approx. 200 km becomes its main component. Higher, at a distance of about 1200 km from the Earth's surface, light gases - helium and hydrogen - predominate. They are the outer layer of the atmosphere. This separation by weight, called diffuse separation, resembles the separation of mixtures using a centrifuge. The exosphere is the outer layer of the atmosphere, which is isolated on the basis of changes in temperature and the properties of neutral gas. Molecules and atoms in the exosphere revolve around the Earth in ballistic orbits under the influence of gravity. Some of these orbits are parabolic and similar to the trajectories of projectiles. Molecules can revolve around the Earth and in elliptical orbits, like satellites. Some molecules, mainly hydrogen and helium, have open trajectories and escape into outer space (Fig. 2).



SOLAR-TERRESTRIAL RELATIONSHIPS AND THEIR INFLUENCE ON THE ATMOSPHERE
atmospheric tides. The attraction of the Sun and the Moon causes tides in the atmosphere, similar to the terrestrial and sea tides. But atmospheric tides have a significant difference: the atmosphere reacts most strongly to the attraction of the Sun, while the earth's crust and ocean - to the attraction of the Moon. This is explained by the fact that the atmosphere is heated by the Sun and, in addition to the gravitational tide, a powerful thermal tide arises. In general, the mechanisms of formation of atmospheric and sea tides are similar, except that in order to predict the reaction of air to gravitational and thermal effects, it is necessary to take into account its compressibility and temperature distribution. It is not entirely clear why semidiurnal (12-hour) solar tides in the atmosphere predominate over diurnal solar and semidiurnal lunar tides, although the driving forces of the latter two processes are much more powerful. Previously, it was believed that a resonance occurs in the atmosphere, which amplifies precisely the oscillations with a 12-hour period. However, observations carried out with the help of geophysical rockets indicate that there are no temperature reasons for such a resonance. In solving this problem, one should probably take into account all the hydrodynamic and thermal features of the atmosphere. At the earth's surface near the equator, where the influence of tidal fluctuations is maximum, it provides a change in atmospheric pressure by 0.1%. The speed of the tidal winds is approx. 0.3 km/h. Due to the complex thermal structure of the atmosphere (especially the presence of a temperature minimum in the mesopause), tidal air currents intensify, and, for example, at an altitude of 70 km their speed is about 160 times higher than at the earth's surface, which has important geophysical consequences. It is believed that in the lower part of the ionosphere (layer E) tidal oscillations move the ionized gas vertically in the Earth's magnetic field, and therefore, electric currents arise here. These constantly emerging systems of currents on the surface of the Earth are established by perturbations of the magnetic field. The diurnal variations of the magnetic field are in good agreement with the calculated values, which convincingly testifies in favor of the theory of tidal mechanisms of the "atmospheric dynamo". Electric currents arising in the lower part of the ionosphere (layer E) must move somewhere, and, therefore, the circuit must be closed. The analogy with the dynamo becomes complete if we consider the oncoming movement as the work of the engine. It is assumed that the reverse circulation of the electric current is carried out in a higher layer of the ionosphere (F), and this counter flow can explain some of the peculiar features of this layer. Finally, the tidal effect must also generate horizontal currents in the E layer and hence in the F layer.
Ionosphere. Trying to explain the mechanism of the occurrence of auroras, scientists of the 19th century. suggested that in the atmosphere there is a zone with electrically charged particles. In the 20th century Convincing evidence was obtained experimentally for the existence of a layer reflecting radio waves at altitudes from 85 to 400 km. It is now known that its electrical properties are the result of atmospheric gas ionization. Therefore, this layer is usually called the ionosphere. The impact on radio waves is mainly due to the presence of free electrons in the ionosphere, although the propagation mechanism of radio waves is associated with the presence of large ions. The latter are also of interest in the study chemical properties atmosphere, because they are more active than neutral atoms and molecules. Chemical reactions occurring in the ionosphere play an important role in its energy and electrical balance.
normal ionosphere. Observations carried out with the help of geophysical rockets and satellites have given a lot of new information, indicating that the ionization of the atmosphere occurs under the influence of broad-spectrum solar radiation. Its main part (more than 90%) is concentrated in the visible part of the spectrum. Ultraviolet radiation with a shorter wavelength and more energy than violet light rays is emitted by hydrogen in the inner part of the Sun's atmosphere (chromosphere), and X-ray radiation, which has even higher energy, is emitted by gases in the Sun's outer shell (corona). The normal (average) state of the ionosphere is due to constant powerful radiation. Regular changes occur in the normal ionosphere under the influence of the daily rotation of the Earth and seasonal differences in the angle of incidence of the sun's rays at noon, but unpredictable and abrupt changes in the state of the ionosphere also occur.
Disturbances in the ionosphere. As is known, powerful cyclically repeating perturbations arise on the Sun, which reach a maximum every 11 years. Observations under the program of the International Geophysical Year (IGY) coincided with the period of the highest solar activity for the entire period of systematic meteorological observations, i.e. from the beginning of the 18th century During periods of high activity, some areas on the Sun increase in brightness several times, and they send out powerful pulses of ultraviolet and X-ray radiation. Such phenomena are called solar flares. They last from several minutes to one or two hours. During a flare, solar gas (mostly protons and electrons) erupts, and elementary particles rush into outer space. The electromagnetic and corpuscular radiation of the Sun at the moments of such flares has a strong effect on the Earth's atmosphere. The initial reaction is observed 8 minutes after the flash, when intense ultraviolet and X-ray radiation reaches the Earth. As a result, ionization sharply increases; x-rays penetrate the atmosphere to the lower boundary of the ionosphere; the number of electrons in these layers increases so much that the radio signals are almost completely absorbed ("extinguished"). Additional absorption of radiation causes heating of the gas, which contributes to the development of winds. Ionized gas is an electrical conductor, and when it moves in the Earth's magnetic field, the dynamo effect appears and arises electricity. Such currents can, in turn, cause noticeable perturbations of the magnetic field and manifest themselves in the form of magnetic storms. This initial phase takes only a short time, corresponding to the duration of a solar flare. During powerful flashes on the Sun, a stream of accelerated particles rushes into outer space. When it is directed towards the Earth, the second phase begins, which has a great influence on the state of the atmosphere. Many natural phenomena, among which the auroras are best known, indicate that a significant number of charged particles reach the Earth (see also POLAR LIGHTS). Nevertheless, the processes of separation of these particles from the Sun, their trajectories in interplanetary space, and the mechanisms of interaction with the Earth's magnetic field and the magnetosphere are still insufficiently studied. The problem became more complicated after the discovery in 1958 by James Van Allen of shells held by the geomagnetic field, consisting of charged particles. These particles move from one hemisphere to another, rotating in spirals around the magnetic field lines. Near the Earth, at a height depending on the shape of the lines of force and on the energy of the particles, there are "points of reflection", in which the particles change their direction of motion to the opposite (Fig. 3). Since the strength of the magnetic field decreases with distance from the Earth, the orbits along which these particles move are somewhat distorted: electrons deviate to the east, and protons to the west. Therefore, they are distributed in the form of belts around the globe.



Some consequences of the heating of the atmosphere by the Sun. Solar energy affects the entire atmosphere. We have already mentioned the belts formed by charged particles in the Earth's magnetic field and revolving around it. These belts are closest to the earth's surface in the circumpolar regions (see Fig. 3), where auroras are observed. Figure 1 shows that the auroral regions in Canada have significantly higher thermospheric temperatures than those in the US Southwest. It is likely that the captured particles give up some of their energy to the atmosphere, especially when colliding with gas molecules near the reflection points, and leave their former orbits. This is how the high layers of the atmosphere are heated in the aurora zone. Another important discovery was made while studying the orbits of artificial satellites. Luigi Iacchia, an astronomer at the Smithsonian Astrophysical Observatory, believes that the small deviations of these orbits are due to changes in the density of the atmosphere as it is heated by the Sun. He suggested the existence of a maximum electron density in the ionosphere at an altitude of more than 200 km, which does not correspond to solar noon, but under the influence of friction forces lags behind it by about two hours. At this time, the values ​​of the atmospheric density, typical for an altitude of 600 km, are observed at a level of approx. 950 km. In addition, the maximum electron concentration experiences irregular fluctuations due to short-term flashes of ultraviolet and X-ray radiation from the Sun. L. Yakkia also discovered short-term fluctuations in air density, corresponding to solar flares and magnetic field disturbances. These phenomena are explained by the intrusion of particles of solar origin into the Earth's atmosphere and the heating of those layers where satellites orbit.
ATMOSPHERIC ELECTRICITY
In the surface layer of the atmosphere, a small part of the molecules undergo ionization under the influence of cosmic rays, radiation from radioactive rocks and decay products of radium (mainly radon) in the air itself. In the process of ionization, an atom loses an electron and acquires a positive charge. A free electron quickly combines with another atom, forming a negatively charged ion. These paired positive and negative ions have molecular sizes. Molecules in the atmosphere tend to cluster around these ions. Several molecules combined with an ion form a complex commonly referred to as a "light ion". The atmosphere also contains complexes of molecules, known in meteorology as condensation nuclei, around which, when the air is saturated with moisture, the condensation process begins. These nuclei are particles of salt and dust, as well as pollutants released into the air from industrial and other sources. Light ions often attach to such nuclei to form "heavy ions". Under the influence of an electric field, light and heavy ions move from one area of ​​the atmosphere to another, transferring electric charges. Although the atmosphere is not generally considered to be an electrically conductive medium, it does have a small amount of conductivity. Therefore, a charged body left in the air slowly loses its charge. The conductivity of the atmosphere increases with height due to an increase in the intensity of cosmic radiation, a decrease in ion losses under conditions of more low pressure (and therefore with a larger mean free path) and also because of the smaller number of heavy nuclei. The conductivity of the atmosphere reaches its maximum value at a height of approx. 50 km, so-called. "compensation level". It is known that between the Earth's surface and the "compensation level" there is always a potential difference of several hundred kilovolts, i.e. constant electric field. It turned out that the potential difference between a certain point in the air at a height of several meters and the Earth's surface is very large - more than 100 V. The atmosphere has a positive charge, and the earth's surface is negatively charged. Since the electric field is an area, at each point of which there is a certain potential value, we can talk about a potential gradient. In clear weather, within the lower few meters, the electric field strength of the atmosphere is almost constant. Due to differences in the electrical conductivity of air in the surface layer, the potential gradient is subject to diurnal fluctuations, the course of which varies significantly from place to place. In the absence of local sources of air pollution - over the oceans, high in the mountains or in the polar regions - the daily course of the potential gradient in clear weather is the same. The magnitude of the gradient depends on the universal, or Greenwich Mean, Time (UT) and reaches a maximum at 19:00 E. Appleton suggested that this maximum electrical conductivity probably coincides with the greatest thunderstorm activity on a planetary scale. Lightning discharges during thunderstorms carry a negative charge to the Earth's surface, since the bases of the most active cumulonimbus thunderclouds have a significant negative charge. The tops of thunderclouds have a positive charge, which, according to the calculations of Holzer and Saxon, flows from their tops during thunderstorms. Without constant replenishment, the charge on the earth's surface would be neutralized by the conductivity of the atmosphere. The assumption that the potential difference between the earth's surface and the "compensation level" is maintained due to thunderstorms is supported by statistical data. For example, the maximum number of thunderstorms is observed in the valley of the river. Amazons. Most often, thunderstorms occur there at the end of the day, i.e. OK. 19:00 Greenwich Mean Time, when the potential gradient is at its maximum anywhere in the world. Moreover, the seasonal variations in the shape of the curves of the diurnal variation of the potential gradient are also in full agreement with the data on the global distribution of thunderstorms. Some researchers argue that the source of the Earth's electric field may be of external origin, since electric fields are believed to exist in the ionosphere and magnetosphere. This circumstance probably explains the appearance of very narrow elongated forms of auroras, similar to backstage and arches.
(see also POLAR LIGHTS). Due to the potential gradient and conductivity of the atmosphere between the "compensation level" and the Earth's surface, charged particles begin to move: positively charged ions - towards the earth's surface, and negatively charged - upwards from it. This current is approx. 1800 A. Although this value seems large, it must be remembered that it is distributed over the entire surface of the Earth. The current strength in an air column with a base area of ​​1 m2 is only 4 * 10 -12 A. On the other hand, the current strength during a lightning discharge can reach several amperes, although, of course, such a discharge has a short duration - from fractions of a second to a whole second or a little more with repeated discharges. Lightning is of great interest not only as a peculiar phenomenon of nature. It makes it possible to observe an electric discharge in a gaseous medium at a voltage of several hundred million volts and a distance between the electrodes of several kilometers. In 1750, B. Franklin proposed to the Royal Society of London that they experiment with an iron rod fixed on an insulating base and mounted on a high tower. He expected that when a thundercloud approaches the tower, a charge of the opposite sign will be concentrated at the upper end of the initially neutral rod, and a charge of the same sign as at the base of the cloud will be concentrated at the lower end. If the strength of the electric field during a lightning discharge increases sufficiently, the charge from the upper end of the rod will partially drain into the air, and the rod will acquire a charge of the same sign as the base of the cloud. The experiment proposed by Franklin was not carried out in England, but it was set up in 1752 in Marly near Paris by the French physicist Jean d'Alembert. He used an iron rod 12 m long inserted into a glass bottle (which served as an insulator), but did not place it on the tower. May 10 his assistant reported that when a thundercloud was over a rod, sparks were generated when a grounded wire was brought to it.Franklin himself, unaware of the successful experience realized in France, in June of that year conducted his famous experiment with a kite and observed electric sparks at the end of a wire tied to it.The next year, while studying the charges collected from a rod, Franklin found that the bases of thunderclouds are usually negatively charged.More detailed studies of lightning became possible in the late 19th century due to improvements in photographic methods, especially after the invention of the device with rotating lenses, which made it possible to fix rapidly developing processes. Such a camera was widely used in the study of spark discharges. It was found that there are several types of lightning, with the most common being linear, flat (intra-cloud) and globular (air discharges). Linear lightning is a spark discharge between a cloud and the earth's surface, following a channel with downward branches. Flat lightning occurs inside a thundercloud and looks like flashes of scattered light. Air discharges of ball lightning, starting from a thundercloud, are often directed horizontally and do not reach the earth's surface.



A lightning discharge usually consists of three or more repeated discharges - impulses following the same path. The intervals between successive pulses are very short, from 1/100 to 1/10 s (this is what causes lightning to flicker). In general, the flash lasts about a second or less. A typical lightning development process can be described as follows. First, a weakly luminous discharge-leader rushes from above to the earth's surface. When he reaches it, a brightly glowing reverse, or main, discharge passes from the earth up the channel laid by the leader. The discharge-leader, as a rule, moves in a zigzag manner. The speed of its propagation ranges from one hundred to several hundred kilometers per second. On its way, it ionizes air molecules, creating a channel with increased conductivity, through which the reverse discharge moves upward at a speed of about a hundred times greater than that of the leader discharge. It is difficult to determine the size of the channel, but the diameter of the leader discharge is estimated at 1–10 m, and that of the reverse discharge, several centimeters. Lightning discharges create radio interference by emitting radio waves in a wide range - from 30 kHz to ultra-low frequencies. The greatest radiation of radio waves is probably in the range from 5 to 10 kHz. Such low-frequency radio interference is "concentrated" in the space between the lower boundary of the ionosphere and the earth's surface and is capable of propagating to distances of thousands of kilometers from the source.
CHANGES IN THE ATMOSPHERE
Impact of meteors and meteorites. Although sometimes meteor showers make a deep impression with their lighting effects, individual meteors are rarely seen. Far more numerous are invisible meteors, too small to be seen at the moment they are swallowed up by the atmosphere. Some of the smallest meteors probably do not heat up at all, but are only captured by the atmosphere. These small particles ranging in size from a few millimeters to ten-thousandths of a millimeter are called micrometeorites. The amount of meteoric matter entering the atmosphere every day is from 100 to 10,000 tons, with most of this matter being micrometeorites. Since meteoric matter partially burns up in the atmosphere, its gas composition is replenished with traces of various chemical elements. For example, stone meteors bring lithium into the atmosphere. The combustion of metallic meteors leads to the formation of tiny spherical iron, iron-nickel and other droplets that pass through the atmosphere and are deposited on the earth's surface. They can be found in Greenland and Antarctica, where ice sheets remain almost unchanged for years. Oceanologists find them in bottom ocean sediments. Most of the meteor particles entering the atmosphere are deposited within approximately 30 days. Some scientists believe that this cosmic dust plays an important role in the formation of atmospheric phenomena such as rain, as it serves as the nuclei of water vapor condensation. Therefore, it is assumed that precipitation is statistically associated with large meteor showers. However, some experts believe that since the total input of meteoric matter is many tens of times greater than even with the largest meteor shower, the change in the total amount of this material that occurs as a result of one such shower can be neglected. However, there is no doubt that the largest micrometeorites and, of course, visible meteorites leave long traces of ionization in the high layers of the atmosphere, mainly in the ionosphere. Such traces can be used for long-distance radio communications, as they reflect high-frequency radio waves. The energy of meteors entering the atmosphere is spent mainly, and perhaps completely, on its heating. This is one of the minor components of the heat balance of the atmosphere.
Carbon dioxide of industrial origin. In the Carboniferous period, woody vegetation was widespread on Earth. Most of the carbon dioxide absorbed by plants at that time was accumulated in coal deposits and in oil-bearing deposits. People have learned to use the huge reserves of these minerals as a source of energy and are now rapidly returning carbon dioxide to the circulation of substances. The fossil is probably ca. 4*10 13 tons of carbon. Over the past century, mankind has burned so much fossil fuel that approximately 4 * 10 11 tons of carbon has again entered the atmosphere. There are currently approx. 2 * 10 12 tons of carbon, and in the next hundred years this figure may double due to the burning of fossil fuels. However, not all carbon will remain in the atmosphere: some of it will dissolve in the waters of the ocean, some will be absorbed by plants, and some will be bound in the process of weathering of rocks. It is not yet possible to predict how much carbon dioxide will be in the atmosphere or what effect it will have on the world's climate. Nevertheless, it is believed that any increase in its content will cause warming, although it is not at all necessary that any warming will significantly affect the climate. The concentration of carbon dioxide in the atmosphere, according to the results of measurements, is noticeably increasing, albeit at a slow pace. Climate data for Svalbard and Little America Station on the Ross Ice Shelf in Antarctica indicate an increase in average annual temperatures over a period of approximately 50 years by 5° and 2.5°C, respectively.
The impact of cosmic radiation. When high-energy cosmic rays interact with individual components of the atmosphere, radioactive isotopes are formed. Among them, the 14C carbon isotope, which accumulates in plant and animal tissues, stands out. By measuring the radioactivity of organic substances that have not exchanged carbon with the environment for a long time, their age can be determined. The radiocarbon method has established itself as the most reliable method for dating fossil organisms and objects of material culture, the age of which does not exceed 50 thousand years. Other radioactive isotopes with long half-lives could be used to date materials that are hundreds of thousands of years old if the fundamental problem of measuring extremely low levels of radioactivity is solved.
(see also RADIOCARBON DATING).
ORIGIN OF THE EARTH'S ATMOSPHERE
The history of the formation of the atmosphere has not yet been restored absolutely reliably. Nevertheless, some probable changes in its composition have been identified. The formation of the atmosphere began immediately after the formation of the Earth. There are quite good reasons to believe that in the process of the evolution of the Pra-Earth and its acquisition of close to modern sizes and mass, it has almost completely lost its original atmosphere. It is believed that at an early stage the Earth was in a molten state and ca. 4.5 billion years ago, it took shape in a solid body. This milestone is taken as the beginning of the geological chronology. Since that time there has been a slow evolution of the atmosphere. Some geological processes, such as eruptions of lava during volcanic eruptions, were accompanied by the release of gases from the bowels of the Earth. They probably included nitrogen, ammonia, methane, water vapor, carbon monoxide and carbon dioxide. Under the influence of solar ultraviolet radiation, water vapor decomposed into hydrogen and oxygen, but the released oxygen reacted with carbon monoxide to form carbon dioxide. Ammonia decomposed into nitrogen and hydrogen. Hydrogen in the process of diffusion rose up and left the atmosphere, while heavier nitrogen could not escape and gradually accumulated, becoming its main component, although some of it was bound during chemical reactions. Under the influence of ultraviolet rays and electrical discharges, a mixture of gases, probably present in the original atmosphere of the Earth, entered into chemical reactions, as a result of which organic substances, in particular amino acids, were formed. Consequently, life could originate in an atmosphere fundamentally different from the modern one. With the advent of primitive plants, the process of photosynthesis began (see also PHOTOSYNTHESIS), accompanied by the release of free oxygen. This gas, especially after diffusion into the upper atmosphere, began to protect its lower layers and the Earth's surface from life-threatening ultraviolet and X-ray radiation. It is estimated that the presence of as little as 0.00004 of today's volume of oxygen could lead to the formation of a layer with half the current ozone concentration, which nevertheless provided very significant protection from ultraviolet rays. It is also likely that the primary atmosphere contained a lot of carbon dioxide. It was consumed during photosynthesis, and its concentration must have decreased as the plant world evolved, and also due to absorption during some geological processes. Since the greenhouse effect is associated with the presence of carbon dioxide in the atmosphere, some scientists believe that fluctuations in its concentration are one of the important causes of large-scale climatic changes in the history of the Earth, such as ice ages. The helium present in the modern atmosphere is probably for the most part is a product of the radioactive decay of uranium, thorium and radium. These radioactive elements emit alpha particles, which are the nuclei of helium atoms. Since no electrical charge is created or destroyed during radioactive decay, there are two electrons for every alpha particle. As a result, it combines with them, forming neutral helium atoms. Radioactive elements are contained in minerals dispersed in the thickness of rocks, so a significant part of the helium formed as a result of radioactive decay is stored in them, volatilizing very slowly into the atmosphere. A certain amount of helium rises up into the exosphere due to diffusion, but due to the constant influx from the earth's surface, the volume of this gas in the atmosphere is unchanged. Based on the spectral analysis of starlight and the study of meteorites, it is possible to estimate the relative abundance of various chemical elements in the Universe. The concentration of neon in space is about ten billion times higher than on Earth, krypton - ten million times, and xenon - a million times. It follows that the concentration of these inert gases, which were originally present in the Earth's atmosphere and were not replenished in the course of chemical reactions, greatly decreased, probably even at the stage when the Earth lost its primary atmosphere. An exception is the inert gas argon, since it is still formed in the form of the 40Ar isotope in the process of radioactive decay of the potassium isotope.
OPTICAL PHENOMENA
The variety of optical phenomena in the atmosphere is due to various reasons. The most common phenomena include lightning (see above) and the very picturesque aurora borealis and aurora borealis (see also POLAR LIGHTS). In addition, the rainbow, gal, parhelion (false sun) and arcs, crown, halos and ghosts of Brocken, mirages, St. Elmo's fires, luminous clouds, green and twilight rays are of particular interest. Rainbow is the most beautiful atmospheric phenomenon. Usually this is a huge arch, consisting of multi-colored stripes, observed when the Sun illuminates only part of the sky, and the air is saturated with water droplets, for example, during rain. The multi-colored arcs are arranged in a spectrum sequence (red, orange, yellow, green, cyan, indigo, violet), but the colors are almost never pure because the bands overlap. As a rule, the physical characteristics of rainbows vary significantly, and therefore they are very diverse in appearance. Their common feature is that the center of the arc is always located on a straight line drawn from the Sun to the observer. The main rainbow is an arc consisting of the brightest colors - red on the outside and purple on the inside. Sometimes only one arc is visible, but often a secondary one appears on the outside of the main rainbow. It has not as bright colors as the first one, and the red and purple stripes in it change places: red is located on the inside. The formation of the main rainbow is explained by double refraction (see also OPTICS) and single internal reflection of sunlight rays (see Fig. 5). Penetrating inside a drop of water (A), a ray of light is refracted and decomposed, as when passing through a prism. Then it reaches the opposite surface of the drop (B), is reflected from it and exits the drop to the outside (C). In this case, the beam of light, before reaching the observer, is refracted a second time. The initial white beam is decomposed into rays of different colors with a divergence angle of 2°. When a secondary rainbow is formed, double refraction and double reflection of the sun's rays occur (see Fig. 6). In this case, the light is refracted, penetrating inside the drop through its lower part (A), and is reflected from the inner surface of the drop, first at point B, then at point C. At point D, the light is refracted, leaving the drop towards the observer.





At sunrise and sunset, the observer sees the rainbow in the form of an arc equal to half a circle, since the axis of the rainbow is parallel to the horizon. If the Sun is higher above the horizon, the arc of the rainbow is less than half a circle. When the Sun rises above 42° above the horizon, the rainbow disappears. Everywhere, except at high latitudes, a rainbow cannot appear at noon when the Sun is too high. It is interesting to estimate the distance to the rainbow. Although it seems that the multi-colored arc is located in the same plane, this is an illusion. In fact, the rainbow has great depth, and it can be represented as the surface of a hollow cone, at the top of which is the observer. The axis of the cone connects the Sun, the observer and the center of the rainbow. The observer looks, as it were, along the surface of this cone. Two people can never see exactly the same rainbow. Of course, one can observe the same effect in general, but the two rainbows are in different positions and are formed by different water droplets. When rain or mist forms a rainbow, the full optical effect is achieved by the combined effect of all the water droplets crossing the surface of the rainbow's cone with the observer at the apex. The role of each drop is fleeting. The surface of the rainbow cone consists of several layers. Quickly crossing them and passing through a series of critical points, each drop instantly decomposes the sun's ray into the entire spectrum in a strictly defined sequence - from red to purple. Many drops cross the surface of the cone in the same way, so that the rainbow appears to the observer as continuous both along and across its arc. Halo - white or iridescent light arcs and circles around the disk of the Sun or Moon. They are caused by the refraction or reflection of light by ice or snow crystals in the atmosphere. The crystals that form the halo are located on the surface of an imaginary cone with the axis directed from the observer (from the top of the cone) to the Sun. Under certain conditions, the atmosphere is saturated with small crystals, many of whose faces form a right angle with the plane passing through the Sun, the observer, and these crystals. Such facets reflect the incoming light rays with a deviation of 22 °, forming a halo that is reddish on the inside, but it can also consist of all colors of the spectrum. Less common is a halo with an angular radius of 46°, located concentrically around a 22-degree halo. Its inner side also has a reddish tint. The reason for this is also the refraction of light, which occurs in this case on the crystal faces that form right angles. The ring width of such a halo exceeds 2.5°. Both 46-degree and 22-degree halos tend to be brightest at the top and bottom of the ring. The rare 90-degree halo is a faintly luminous, almost colorless ring that has a common center with the other two halos. If it is colored, it has a red color on the outside of the ring. The mechanism of the appearance of this type of halo has not been fully elucidated (Fig. 7).



Parhelia and arcs. Parhelic circle (or circle of false suns) - a white ring centered at the zenith point, passing through the Sun parallel to the horizon. The reason for its formation is the reflection of sunlight from the edges of the surfaces of ice crystals. If the crystals are sufficiently evenly distributed in the air, a full circle becomes visible. Parhelia, or false suns, are brightly luminous spots resembling the Sun, which form at the points of intersection of the parhelic circle with the halo, having angular radii of 22°, 46° and 90°. The most frequently formed and brightest parhelion forms at the intersection with a 22-degree halo, usually colored in almost all colors of the rainbow. False suns at intersections with 46- and 90-degree halos are observed much less frequently. Parhelia that occur at intersections with 90-degree halos are called paranthelia, or false countersuns. Sometimes an antelium (counter-sun) is also visible - a bright spot located on the parhelion ring exactly opposite the Sun. It is assumed that the cause of this phenomenon is the double internal reflection of sunlight. The reflected beam follows the same path as the incident beam, but in the opposite direction. The circumzenithal arc, sometimes incorrectly referred to as the upper tangent arc of the 46-degree halo, is an arc of 90° or less centered on the zenith point and approximately 46° above the Sun. It is rarely visible and only for a few minutes, has bright colors, and the red color is confined to the outer side of the arc. The circumzenithal arc is notable for its coloration, brightness, and clear outlines. Another curious and very rare optical effect of the halo type is the Lovitz arc. They arise as a continuation of parhelia at the intersection with the 22-degree halo, pass from the outer side of the halo and are slightly concave towards the Sun. Pillars of whitish light, as well as various crosses, are sometimes seen at dawn or dusk, especially in the polar regions, and can accompany both the Sun and the Moon. At times, lunar halos and other effects similar to those described above are observed, with the most common lunar halo (ring around the Moon) having an angular radius of 22°. Like false suns, false moons can arise. Crowns, or crowns, are small concentric colored rings around the Sun, Moon or other bright objects that are observed from time to time when the light source is behind translucent clouds. The corona radius is smaller than the halo radius and is approx. 1-5°, the blue or violet ring is closest to the Sun. A corona is formed when light is scattered by small water droplets of water that form a cloud. Sometimes the crown looks like a luminous spot (or halo) surrounding the Sun (or Moon), which ends with a reddish ring. In other cases, at least two concentric rings of larger diameter, very weakly colored, are visible outside the halo. This phenomenon is accompanied by iridescent clouds. Sometimes the edges of very high clouds are painted in bright colors.
Gloria (halos). Under special conditions, unusual atmospheric phenomena occur. If the Sun is behind the observer, and its shadow is projected onto nearby clouds or a curtain of fog, under a certain state of the atmosphere around the shadow of a person's head, you can see a colored luminous circle - a halo. Usually such a halo is formed due to the reflection of light by dew drops on a grassy lawn. Glorias are also quite common to be found around the shadow that the plane casts on the underlying clouds.
Ghosts of the Brocken. In some regions of the globe, when the shadow of an observer on a hill at sunrise or sunset falls behind him on clouds located at a short distance, a striking effect is revealed: the shadow acquires colossal dimensions. This is due to the reflection and refraction of light by the smallest water droplets in the fog. The described phenomenon is called the "ghost of the Brocken" after the peak in the Harz mountains in Germany.
Mirages- an optical effect caused by the refraction of light when passing through layers of air of different densities and is expressed in the appearance of a virtual image. In this case, distant objects may turn out to be raised or lowered relative to their actual position, and may also be distorted and acquire irregular, fantastic shapes. Mirages are often observed in hot climates, such as over sandy plains. Inferior mirages are common, when the distant, almost flat desert surface takes on the appearance of open water, especially when viewed from a slight elevation or simply above a layer of heated air. A similar illusion usually occurs on a heated paved road that looks like a water surface far ahead. In reality, this surface is a reflection of the sky. Below eye level, objects, usually upside down, may appear in this "water". An "air puff cake" is formed above the heated land surface, and the layer closest to the earth is the most heated and so rarefied that light waves passing through it are distorted, since their propagation speed varies depending on the density of the medium. Superior mirages are less common and more scenic than inferior mirages. Distant objects (often below the sea horizon) appear upside down in the sky, and sometimes a direct image of the same object also appears above. This phenomenon is typical for cold regions, especially when there is a significant temperature inversion, when a warmer layer of air is above the colder layer. This optical effect is manifested as a result of complex patterns of propagation of the front of light waves in air layers with a non-uniform density. Very unusual mirages occur from time to time, especially in the polar regions. When mirages occur on land, trees and other landscape components are upside down. In all cases, objects in the upper mirages are more clearly visible than in the lower ones. When the boundary of two air masses is a vertical plane, side mirages are sometimes observed.
Saint Elmo's fire. Some optical phenomena in the atmosphere (for example, glow and the most common meteorological phenomenon - lightning) are electrical in nature. Much less common are the fires of St. Elmo - luminous pale blue or purple brushes from 30 cm to 1 m or more in length, usually on the tops of masts or the ends of the yards of ships at sea. Sometimes it seems that the entire rigging of the ship is covered with phosphorus and glows. Elmo's fires sometimes appear on mountain peaks, as well as on spiers and sharp corners of tall buildings. This phenomenon is brush electric discharges at the ends of electrical conductors, when the electric field strength is greatly increased in the atmosphere around them. Will-o'-the-wisps are a faint bluish or greenish glow that is sometimes seen in swamps, cemeteries, and crypts. They often appear as a calmly burning, non-heating, candle flame raised about 30 cm above the ground, hovering over the object for a moment. The light seems to be completely elusive and, as the observer approaches, it seems to move to another place. The reason for this phenomenon is the decomposition of organic residues and the spontaneous combustion of swamp gas methane (CH4) or phosphine (PH3). Wandering lights have a different shape, sometimes even spherical. Green beam - a flash of emerald green sunlight at the moment when the last ray of the Sun disappears below the horizon. The red component of sunlight disappears first, all the others follow in order, and the emerald green remains last. This phenomenon occurs only when only the very edge of the solar disk remains above the horizon, otherwise there is a mixture of colors. Crepuscular rays are diverging beams of sunlight that become visible when they illuminate dust in the high atmosphere. Shadows from the clouds form dark bands, and rays propagate between them. This effect occurs when the Sun is low on the horizon before dawn or after sunset.

At sea level 1013.25 hPa (about 760 mmHg). The average global air temperature at the Earth's surface is 15°C, while the temperature varies from about 57°C in subtropical deserts to -89°C in Antarctica. Air density and pressure decrease with height according to a law close to exponential.

The structure of the atmosphere. Vertically, the atmosphere has a layered structure, determined mainly by the features of the vertical temperature distribution (figure), which depends on the geographical location, season, time of day, and so on. The lower layer of the atmosphere - the troposphere - is characterized by a drop in temperature with height (by about 6 ° C per 1 km), its height is from 8-10 km in polar latitudes to 16-18 km in the tropics. Due to the rapid decrease in air density with height, about 80% of the total mass of the atmosphere is in the troposphere. Above the troposphere is the stratosphere - a layer that is characterized in general by an increase in temperature with height. The transition layer between the troposphere and stratosphere is called the tropopause. In the lower stratosphere, up to a level of about 20 km, the temperature changes little with height (the so-called isothermal region) and often even slightly decreases. Higher, the temperature rises due to the absorption of solar UV radiation by ozone, slowly at first, and faster from a level of 34-36 km. The upper boundary of the stratosphere - the stratopause - is located at an altitude of 50-55 km, corresponding to the maximum temperature (260-270 K). The layer of the atmosphere, located at an altitude of 55-85 km, where the temperature again falls with height, is called the mesosphere, at its upper boundary - the mesopause - the temperature reaches 150-160 K in summer, and 200-230 K in winter. Above the mesopause, the thermosphere begins - a layer, characterized by a rapid increase in temperature, reaching values ​​of 800-1200 K at an altitude of 250 km. The corpuscular and X-ray radiation of the Sun is absorbed in the thermosphere, meteors are slowed down and burned out, so it performs the function of the Earth's protective layer. Even higher is the exosphere, from where atmospheric gases are dissipated into world space due to dissipation and where a gradual transition from the atmosphere to interplanetary space takes place.

Composition of the atmosphere. Up to an altitude of about 100 km, the atmosphere is practically homogeneous in chemical composition and the average molecular mass air (about 29) in it is constant. Near the Earth's surface, the atmosphere consists of nitrogen (about 78.1% by volume) and oxygen (about 20.9%), and also contains small amounts of argon, carbon dioxide (carbon dioxide), neon, and other constant and variable components (see Air ).

In addition, the atmosphere contains small amounts of ozone, nitrogen oxides, ammonia, radon, etc. The relative content of the main components of the air is constant over time and uniform in different geographical areas. The content of water vapor and ozone is variable in space and time; despite the low content, their role in atmospheric processes is very significant.

Above 100-110 km, the dissociation of oxygen, carbon dioxide and water vapor molecules occurs, so the molecular weight of air decreases. At an altitude of about 1000 km, light gases - helium and hydrogen - begin to predominate, and even higher, the Earth's atmosphere gradually turns into interplanetary gas.

The most important variable component of the atmosphere is water vapor, which enters the atmosphere through evaporation from the surface of water and moist soil, as well as through transpiration by plants. The relative content of water vapor varies near the earth's surface from 2.6% in the tropics to 0.2% in the polar latitudes. With height, it quickly falls, decreasing by half already at a height of 1.5-2 km. The vertical column of the atmosphere at temperate latitudes contains about 1.7 cm of the “precipitated water layer”. When water vapor condenses, clouds form, from which atmospheric precipitation falls in the form of rain, hail, and snow.

An important component of atmospheric air is ozone, 90% concentrated in the stratosphere (between 10 and 50 km), about 10% of it is in the troposphere. Ozone provides absorption of hard UV radiation (with a wavelength of less than 290 nm), and this is its protective role for the biosphere. The values ​​of the total ozone content vary depending on the latitude and season, ranging from 0.22 to 0.45 cm (the thickness of the ozone layer at a pressure of p= 1 atm and a temperature of T = 0°C). AT ozone holes, observed in the spring in Antarctica since the early 1980s, the ozone content can drop to 0.07 cm. latitudes. An essential variable component of the atmosphere is carbon dioxide, the content of which in the atmosphere has increased by 35% over the past 200 years, which is mainly explained by the anthropogenic factor. Its latitudinal and seasonal variability associated with plant photosynthesis and solubility in sea ​​water(according to Henry's law, the solubility of a gas in water decreases with increasing temperature).

An important role in the formation of the planet's climate is played by atmospheric aerosol - solid and liquid particles suspended in the air ranging in size from several nm to tens of microns. There are aerosols of natural and anthropogenic origin. Aerosol is formed in the process of gas-phase reactions from the products of plant life and human economic activity, volcanic eruptions, as a result of dust being lifted by the wind from the surface of the planet, especially from its desert regions, and is also formed from cosmic dust entering the upper atmosphere. Most of the aerosol is concentrated in the troposphere; aerosol from volcanic eruptions forms the so-called Junge layer at an altitude of about 20 km. The largest amount of anthropogenic aerosol enters the atmosphere as a result of the operation of vehicles and thermal power plants, chemical industries, fuel combustion, etc. Therefore, in some areas the composition of the atmosphere differs markedly from ordinary air, which required the creation of a special service for monitoring and controlling the level of atmospheric air pollution.

Atmospheric evolution. The modern atmosphere seems to be of secondary origin: it was formed from gases released by the solid shell of the Earth after the formation of the planet was completed about 4.5 billion years ago. During the geological history of the Earth, the atmosphere has undergone significant changes in its composition under the influence of a number of factors: dissipation (volatilization) of gases, mainly lighter ones, into outer space; release of gases from the lithosphere as a result of volcanic activity; chemical reactions between the components of the atmosphere and the rocks that make up the earth's crust; photochemical reactions in the atmosphere itself under the influence of solar UV radiation; accretion (capture) of the matter of the interplanetary medium (for example, meteoric matter). The development of the atmosphere is closely connected with geological and geochemical processes, and for the last 3-4 billion years also with the activity of the biosphere. A significant part of the gases that make up the modern atmosphere (nitrogen, carbon dioxide, water vapor) arose during volcanic activity and intrusion, which carried them out of the depths of the Earth. Oxygen appeared in appreciable quantities about 2 billion years ago as a result of the activity of photosynthetic organisms that originally originated in the surface waters of the ocean.

Based on the data on the chemical composition of carbonate deposits, estimates of the amount of carbon dioxide and oxygen in the atmosphere of the geological past were obtained. Throughout the Phanerozoic (the last 570 million years of Earth's history), the amount of carbon dioxide in the atmosphere varied widely, in accordance with the level of volcanic activity, ocean temperature, and photosynthesis. Most of this time, the concentration of carbon dioxide in the atmosphere was significantly higher than the current one (up to 10 times). The amount of oxygen in the atmosphere of the Phanerozoic changed significantly, and the tendency to increase it prevailed. In the Precambrian atmosphere, the mass of carbon dioxide was, as a rule, greater, and the mass of oxygen, less than in the atmosphere of the Phanerozoic. Fluctuations in the amount of carbon dioxide have had a significant impact on the climate in the past, increasing the greenhouse effect with an increase in the concentration of carbon dioxide, due to which the climate during the main part of the Phanerozoic was much warmer than in the modern era.

atmosphere and life. Without an atmosphere, Earth would be a dead planet. Organic life proceeds in close interaction with the atmosphere and its associated climate and weather. Insignificant in mass compared to the planet as a whole (about a millionth part), the atmosphere is a sine qua non for all life forms. Oxygen, nitrogen, water vapor, carbon dioxide, and ozone are the most important atmospheric gases for the life of organisms. When carbon dioxide is absorbed by photosynthetic plants, organic matter is created that is used as an energy source by the vast majority of living beings, including humans. Oxygen is necessary for the existence of aerobic organisms, for which the energy supply is provided by the oxidation reactions of organic matter. Nitrogen, assimilated by some microorganisms (nitrogen fixers), is necessary for the mineral nutrition of plants. Ozone, which absorbs the Sun's harsh UV radiation, significantly attenuates this life-threatening portion of the sun's radiation. Condensation of water vapor in the atmosphere, the formation of clouds and the subsequent precipitation of precipitation supply water to land, without which no form of life is possible. The vital activity of organisms in the hydrosphere is largely determined by the amount and chemical composition of atmospheric gases dissolved in water. Since the chemical composition of the atmosphere significantly depends on the activity of organisms, the biosphere and atmosphere can be considered as part of a single system, the maintenance and evolution of which (see Biogeochemical cycles) was of great importance for changing the composition of the atmosphere throughout the history of the Earth as a planet.

Radiation, heat and water balances of the atmosphere. Solar radiation is practically the only source of energy for all physical processes in the atmosphere. The main feature of the radiation regime of the atmosphere is the so-called greenhouse effect: the atmosphere transmits solar radiation to the earth's surface quite well, but actively absorbs the thermal long-wave radiation of the earth's surface, part of which returns to the surface in the form of counter radiation that compensates for the radiative heat loss of the earth's surface (see Atmospheric radiation ). In the absence of an atmosphere, the average temperature of the earth's surface would be -18°C, in reality it is 15°C. Incoming solar radiation is partially (about 20%) absorbed into the atmosphere (mainly by water vapor, water droplets, carbon dioxide, ozone and aerosols), and is also scattered (about 7%) by aerosol particles and density fluctuations (Rayleigh scattering). The total radiation, reaching the earth's surface, is partially (about 23%) reflected from it. The reflectance is determined by the reflectivity of the underlying surface, the so-called albedo. On average, the Earth's albedo for the integral solar radiation flux is close to 30%. It varies from a few percent (dry soil and black soil) to 70-90% for freshly fallen snow. The radiative heat exchange between the earth's surface and the atmosphere essentially depends on the albedo and is determined by the effective radiation of the earth's surface and the counter-radiation of the atmosphere absorbed by it. The algebraic sum of radiation fluxes entering the earth's atmosphere from outer space and leaving it back is called the radiation balance.

Transformations of solar radiation after its absorption by the atmosphere and the earth's surface determine the heat balance of the Earth as a planet. The main source of heat for the atmosphere is the earth's surface; heat from it is transferred not only in the form of long-wave radiation, but also by convection, and is also released during the condensation of water vapor. The shares of these heat inflows are on average 20%, 7% and 23%, respectively. About 20% of heat is also added here due to the absorption of direct solar radiation. The flux of solar radiation per unit of time through a single area perpendicular to the sun's rays and located outside the atmosphere at an average distance from the Earth to the Sun (the so-called solar constant) is 1367 W / m 2, the changes are 1-2 W / m 2 depending on cycle of solar activity. With a planetary albedo of about 30%, the time-average global influx of solar energy to the planet is 239 W/m 2 . Since the Earth as a planet emits the same amount of energy into space on average, then, according to the Stefan-Boltzmann law, the effective temperature of the outgoing thermal long-wave radiation is 255 K (-18°C). At the same time, the average temperature of the earth's surface is 15°C. The 33°C difference is due to the greenhouse effect.

The water balance of the atmosphere as a whole corresponds to the equality of the amount of moisture evaporated from the surface of the Earth, the amount of precipitation falling on the earth's surface. The atmosphere over the oceans receives more moisture from evaporation processes than over land, and loses 90% in the form of precipitation. Excess water vapor over the oceans is carried to the continents by air currents. The amount of water vapor transported into the atmosphere from the oceans to the continents is equal to the volume of river flow that flows into the oceans.

air movement. The Earth has a spherical shape, so much less solar radiation comes to its high latitudes than to the tropics. As a result, large temperature contrasts arise between latitudes. The relative position of the oceans and continents also significantly affects the distribution of temperature. Due to the large mass of ocean waters and the high heat capacity of water, seasonal fluctuations in ocean surface temperature are much less than those of land. In this regard, in the middle and high latitudes, the air temperature over the oceans is noticeably lower in summer than over the continents, and higher in winter.

The uneven heating of the atmosphere in different regions of the globe causes a distribution of atmospheric pressure that is not uniform in space. At sea level, the pressure distribution is characterized by relatively low values ​​near the equator, an increase in the subtropics (high pressure belts), and a decrease in middle and high latitudes. At the same time, over the continents of extratropical latitudes, the pressure is usually increased in winter, and lowered in summer, which is associated with the temperature distribution. Under the action of a pressure gradient, the air experiences an acceleration directed from areas of high pressure to areas of low pressure, which leads to the movement of air masses. The moving air masses are also affected by the deflecting force of the Earth's rotation (the Coriolis force), the friction force, which decreases with height, and in the case of curvilinear trajectories, the centrifugal force. Of great importance is the turbulent mixing of air (see Turbulence in the atmosphere).

A complex system of air currents (general circulation of the atmosphere) is associated with the planetary distribution of pressure. In the meridional plane, on average, two or three meridional circulation cells are traced. Near the equator, heated air rises and falls in the subtropics, forming a Hadley cell. The air of the reverse Ferrell cell also descends there. At high latitudes, a direct polar cell is often traced. Meridional circulation velocities are on the order of 1 m/s or less. Due to the action of the Coriolis force, westerly winds are observed in most of the atmosphere with speeds in the middle troposphere of about 15 m/s. There are relatively stable wind systems. These include trade winds - winds blowing from high pressure belts in the subtropics to the equator with a noticeable eastern component (from east to west). Monsoons are quite stable - air currents that have a clearly pronounced seasonal character: they blow from the ocean to the mainland in summer and in the opposite direction in winter. The monsoons of the Indian Ocean are especially regular. In middle latitudes, the movement of air masses is mainly western (from west to east). This is a zone of atmospheric fronts, on which large eddies arise - cyclones and anticyclones, covering many hundreds and even thousands of kilometers. Cyclones also occur in the tropics; here they differ in smaller sizes, but very high wind speeds, reaching hurricane force (33 m/s or more), the so-called tropical cyclones. In the Atlantic and eastern Pacific they are called hurricanes, and in the western Pacific they are called typhoons. In the upper troposphere and lower stratosphere, in the areas separating the direct cell of the meridional Hadley circulation and the reverse Ferrell cell, relatively narrow, hundreds of kilometers wide, jet streams with sharply defined boundaries are often observed, within which the wind reaches 100-150 and even 200 m/ With.

Climate and weather. The difference in the amount of solar radiation coming at different latitudes to the earth's surface, which is diverse in physical properties, determines the diversity of the Earth's climates. From the equator to tropical latitudes, the air temperature near the earth's surface averages 25-30 ° C and changes little during the year. In the equatorial zone, a lot of precipitation usually falls, which creates conditions for excessive moisture there. In tropical zones, the amount of precipitation decreases and in some areas becomes very small. Here are the vast deserts of the Earth.

In subtropical and middle latitudes, air temperature varies significantly throughout the year, and the difference between summer and winter temperatures is especially large in areas of the continents remote from the oceans. Thus, in some areas of Eastern Siberia, the annual amplitude of air temperature reaches 65°С. Humidification conditions in these latitudes are very diverse, depend mainly on the regime of the general circulation of the atmosphere, and vary significantly from year to year.

In the polar latitudes, the temperature remains low throughout the year, even if there is a noticeable seasonal variation. This contributes to the widespread distribution of ice cover on the oceans and land and permafrost, occupying over 65% of Russia's area, mainly in Siberia.

Over the past decades, changes in the global climate have become more and more noticeable. The temperature rises more at high latitudes than at low latitudes; more in winter than in summer; more at night than during the day. Over the 20th century, the average annual air temperature near the earth's surface in Russia increased by 1.5-2 ° C, and in some regions of Siberia an increase of several degrees is observed. This is associated with an increase in the greenhouse effect due to an increase in the concentration of small gaseous impurities.

The weather is determined by the conditions of atmospheric circulation and the geographical location of the area, it is most stable in the tropics and most changeable in the middle and high latitudes. Most of all, the weather changes in the zones of change of air masses, due to the passage of atmospheric fronts, cyclones and anticyclones, carrying precipitation and increasing wind. Data for weather forecasting is collected from ground-based weather stations, ships and aircraft, and meteorological satellites. See also meteorology.

Optical, acoustic and electrical phenomena in the atmosphere. When electromagnetic radiation propagates in the atmosphere, as a result of refraction, absorption and scattering of light by air and various particles (aerosol, ice crystals, water drops), various optical phenomena arise: rainbow, crowns, halo, mirage, etc. Light scattering determines the apparent height of the firmament and blue color of the sky. The visibility range of objects is determined by the conditions of light propagation in the atmosphere (see Atmospheric visibility). The transparency of the atmosphere at different wavelengths determines the communication range and the possibility of detecting objects with instruments, including the possibility of astronomical observations from the Earth's surface. For studies of optical inhomogeneities in the stratosphere and mesosphere, the phenomenon of twilight plays an important role. For example, photographing twilight with spacecraft allows detection of aerosol layers. Features of the propagation of electromagnetic radiation in the atmosphere determine the accuracy of methods for remote sensing of its parameters. All these questions, like many others, are studied by atmospheric optics. Refraction and scattering of radio waves determine the possibilities of radio reception (see Propagation of radio waves).

The propagation of sound in the atmosphere depends on the spatial distribution of temperature and wind speed (see Atmospheric acoustics). It is of interest for remote sensing of the atmosphere. Explosions of charges launched by rockets in upper atmosphere, gave a wealth of information about wind systems and the course of temperature in the stratosphere and mesosphere. In a stably stratified atmosphere, when the temperature falls with height more slowly than the adiabatic gradient (9.8 K/km), so-called internal waves arise. These waves can propagate upward into the stratosphere and even into the mesosphere, where they attenuate, contributing to increased wind and turbulence.

The negative charge of the Earth and the electric field caused by it, the atmosphere, together with the electrically charged ionosphere and magnetosphere, create a global electrical circuit. An important role is played by the formation of clouds and lightning electricity. The danger of lightning discharges necessitated the development of methods for lightning protection of buildings, structures, power lines and communications. This phenomenon is of particular danger to aviation. Lightning discharges cause atmospheric radio interference, called atmospherics (see Whistling atmospherics). During a sharp increase in the strength of the electric field, luminous discharges are observed that arise on the points and sharp corners of objects protruding above the earth's surface, on individual peaks in the mountains, etc. (Elma lights). The atmosphere always contains a number of light and heavy ions, which vary greatly depending on the specific conditions, which determine the electrical conductivity of the atmosphere. The main air ionizers near the earth's surface are the radiation of radioactive substances contained in the earth's crust and in the atmosphere, as well as cosmic rays. See also atmospheric electricity.

Human influence on the atmosphere. Over the past centuries, there has been an increase in the concentration of greenhouse gases in the atmosphere due to human activities. Percentage carbon dioxide increased from 2.8-10 2 two hundred years ago to 3.8-10 2 in 2005, methane content - from 0.7-10 1 about 300-400 years ago to 1.8-10 -4 21st century; about 20% of the increase in the greenhouse effect over the past century was given by freons, which practically did not exist in the atmosphere until the middle of the 20th century. These substances are recognized as stratospheric ozone depleters and their production is prohibited by the 1987 Montreal Protocol. The increase in carbon dioxide concentration in the atmosphere is caused by the burning of ever-increasing amounts of coal, oil, gas and other carbon fuels, as well as the deforestation, resulting in a decrease in the absorption of carbon dioxide through photosynthesis. The concentration of methane increases with the growth of oil and gas production (due to its losses), as well as with the expansion of rice crops and an increase in the number of cattle. All this contributes to climate warming.

To change the weather, methods of active influence on atmospheric processes have been developed. They are used to protect agricultural plants from hail damage by dispersing special reagents in thunderclouds. There are also methods for dispelling fog at airports, protecting plants from frost, influencing clouds to increase rainfall in the right places, or to disperse clouds during public events.

Study of the atmosphere. Information about the physical processes in the atmosphere is obtained primarily from meteorological observations, which are carried out by a global network of permanent meteorological stations and posts located on all continents and on many islands. Daily observations provide information about air temperature and humidity, atmospheric pressure and precipitation, cloudiness, wind, etc. Observations of solar radiation and its transformations are carried out at actinometric stations. Of great importance for the study of the atmosphere are the networks of aerological stations, where meteorological measurements are made with the help of radiosondes up to a height of 30-35 km. At a number of stations, observations are made of atmospheric ozone, electrical phenomena in the atmosphere, and the chemical composition of the air.

Data from ground stations are supplemented by observations on the oceans, where "weather ships" operate, permanently located in certain areas of the World Ocean, as well as meteorological information received from research and other ships.

In recent decades, an increasing amount of information about the atmosphere has been obtained with the help of meteorological satellites, on which instruments are installed for photographing clouds and measuring the fluxes of ultraviolet, infrared, and microwave radiation from the Sun. Satellites make it possible to obtain information about vertical temperature profiles, cloudiness and its water content, elements of the atmospheric radiation balance, ocean surface temperature, etc. Using measurements of the refraction of radio signals from a system of navigation satellites, it is possible to determine vertical profiles of density, pressure and temperature, as well as moisture content in the atmosphere . With the help of satellites, it became possible to clarify the value of the solar constant and planetary albedo of the Earth, build maps of the radiation balance of the Earth-atmosphere system, measure the content and variability of small atmospheric impurities, and solve many other problems of atmospheric physics and environmental monitoring.

Lit .: Budyko M. I. Climate in the past and future. L., 1980; Matveev L. T. Course of general meteorology. Physics of the atmosphere. 2nd ed. L., 1984; Budyko M. I., Ronov A. B., Yanshin A. L. History of the atmosphere. L., 1985; Khrgian A.Kh. Atmospheric Physics. M., 1986; Atmosphere: A Handbook. L., 1991; Khromov S. P., Petrosyants M. A. Meteorology and climatology. 5th ed. M., 2001.

G. S. Golitsyn, N. A. Zaitseva.

The formation of the Earth's atmosphere began in ancient times - in the protoplanetary stage of the Earth's development, during the active period with the release of a huge amount of gases. Later, when the biosphere appeared on Earth, the formation of the atmosphere continued due to gas exchange between water, plants, animals and their decomposition products.

Throughout geological history, the Earth's atmosphere has undergone a series of profound transformations.

Earth's primary atmosphere. Recovery.

Part Earth's primary atmosphere at the protoplanetary stage of the development of the Earth (more than 4.2 billion years ago), methane, ammonia, and carbon dioxide were predominantly included. Then, as a result of degassing and continuous weathering processes on the earth's surface, the composition of the Earth's primary atmosphere was enriched with water vapor, carbon compounds (CO 2, CO) and sulfur, as well as strong halogen acids (HCI, HF, HI) and boric acid. The initial atmosphere was very thin.

Earth's secondary atmosphere. Oxidative.

Subsequently, the primary atmosphere began to transform into a secondary one. This happened as a result of the same weathering processes that took place on the surface of the earth, volcanic and solar activity, as well as due to the vital activity of cyanobacteria and blue-green algae.

The result of the transformation was the decomposition of methane into hydrogen and carbon dioxide, ammonia - into nitrogen and hydrogen. Carbon dioxide and nitrogen began to accumulate in the Earth's atmosphere.

Blue-green algae through photosynthesis began to produce oxygen, which was almost all spent on the oxidation of other gases and rocks. As a result, ammonia was oxidized to molecular nitrogen, methane and carbon monoxide - to carbon dioxide, sulfur and hydrogen sulfide - to SO 2 and SO 3.

Thus, the atmosphere gradually turned from a reducing atmosphere into an oxidizing one.

Formation and evolution of carbon dioxide in the primary and secondary atmosphere.

Sources of carbon dioxide in the early stages of atmospheric formation:

  • Methane oxidation,
  • Degassing of the Earth's mantle,
  • Weathering of rocks.

At the turn of the Proterozoic and Paleozoic (about 600 million years ago), the content of carbon dioxide in the atmosphere decreased and amounted to only tenths of a percent of the total volume of gases in the atmosphere.

The current level of carbon dioxide content in the atmosphere reached only 10-20 million years ago.

Formation and evolution of oxygen in the primary and secondary atmosphere.

Sources of oxygen early stages of atmospheric formation :

  • Degassing of the Earth's mantle - almost all oxygen was spent on oxidative processes.
  • Photodissociation of water (decomposition into hydrogen and oxygen molecules) in the atmosphere under the action of ultraviolet radiation - as a result, free oxygen molecules appeared in the atmosphere.
  • Processing of carbon dioxide into oxygen by eukaryotes. The appearance of free oxygen in the atmosphere led to the death of prokaryotes (adapted to life in reducing conditions) and the emergence of eukaryotes (adapted to live in an oxidizing environment).

Change in the concentration of oxygen in the atmosphere.

Archean - first half of the Proterozoic - oxygen concentration 0.01% of the current level (Urey point). Almost all of the resulting oxygen was spent on the oxidation of iron and sulfur. This continued until all the ferrous iron on the surface of the earth was oxidized. Since then, oxygen began to accumulate in the atmosphere.

The second half of the Proterozoic - the end of the early Vendian - the concentration of oxygen in the atmosphere is 0.1% of the current level (Pasteur point).

Late Vendian - Silurian period. Free oxygen stimulated the development of life - the anaerobic fermentation process was replaced by an energetically more promising and progressive oxygen metabolism. Since then, the accumulation of oxygen in the atmosphere has been quite fast. The emergence of plants from the sea to land (450 million years ago) led to the stabilization of the oxygen level in the atmosphere.

Mid Cretaceous . The final stabilization of the oxygen concentration in the atmosphere is associated with the appearance of flowering plants (100 million years ago).

Formation and evolution of nitrogen in the primary and secondary atmosphere.

Nitrogen was formed in the early stages of the development of the Earth due to the decomposition of ammonia. The binding of atmospheric nitrogen and its burial in marine sediments began with the advent of organisms. After the release of living organisms on land, nitrogen began to be buried in continental sediments. The process of nitrogen fixation was especially intensified with the advent of terrestrial plants.

Thus, the composition of the Earth's atmosphere determined the characteristics of the life of organisms, contributed to their evolution, development and settlement on the surface of the earth. But in the history of the Earth there were sometimes failures in the distribution of the gas composition. The reason for this was various catastrophes that occurred more than once during the Cryptozoic and Phanerozoic. These failures led to mass extinctions of the organic world.

The composition of the ancient and modern atmosphere in percentage terms is shown in Table 1.

Table 1. Composition of the Earth's primary and modern atmosphere.

gases

The composition of the earth's atmosphere

Primary atmosphere, %

Modern atmosphere, %

Oxygen O 2

Carbon dioxide CO 2

Carbon monoxide CO

water vapor