Volume 2 Greenhouse Gas Emissions |
Table D1. Overlap of Absorption Bands of Greenhouse Gases (Micrometers) | |
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Greenhouse Gases | Greenhouse Gases' Absorption Bands |
H2O | 0.5 - 2.0 |
H2O, CO, and CO2 | 2.0 - 3.0 |
H2O and CH4 | 3.0 - 4.0 |
CO and CO2 | 4.0 - 5.0 |
H2O | 5.0 - 7.0 |
N2O and CH4 | 7.0 - 8.0 |
O3 | 8.0 - 10.0 |
CO2, CH4, and O3 | 13.7 - 14.7 |
CO2 | 14.7 - 16.5 |
N2O | 16.5 - 46.0 |
CH4 = Methane. CO = Carbon monoxide.
CO2 = Carbon dioxide. H2O = Water vapor. N2O
= Nitrous oxide. O3 = Ozone. Notes: Carbon dioxide absorbs infrared radiation at wavelengths of 2.69 micrometers (µm), 2.76 µm, 4.25 µm, 14 µm, and 15 µm. Carbon monoxide absorbs at 2.3 µm, and 4.7 µm. Water vapor absorbs at 0.6 µm, 0.72 µm, 0.82 µm, 0.94 µm, 1.10 µm, 1.38 µm, 1.87 µm, 2.70 µm, 3.20 µm, and 6.30 µm. Methane absorbs at 3.4 µm, 7.4 µm, 7.58 µm, and 7.87 µm. Nitrous oxide absorbs at 7.83 µm, 16.98 µm, and 44.9 µm. Ozone absorbs at 9.0 µm, 9.6 µm, and 14.2 µm. Sources: Snell-Ettre, Encyclopedia of Industrial Chemical Analysis, Vol. 8, p. 252; and N.V. Sidgewick, The Chemical Elements and Their Compounds, Vol. 11 (Oxford, United Kingdom: Clarendon Press, 1950), pp. 859-863. |
Current global warming calculations and some climate models include infrared absorption characteristics of GHGs to a moderate extent [101], [102] [103]. The infrared absorption spectrum of atmospheric greenhouse gases is very complex. The monochromaticity (radiation of one wavelength) of most of its absorption bands of individual GHGs is lost due to pressure, temperature, aggregation, emission, and other factors. Mathematical and statistical models are used to deconvolute the polychromatic (radiation of more than one wavelength) infrared absorption spectrum of atmospheric GHGs, and this brings a certain amount of uncertainty into the data. In addition, uncertainty in the proper treatment of the water vapor continuum in the infrared spectrum of atmospheric GHGs still poses a challenge for line-by-line models to provide an absolute reference for evaluating less detailed model calculations [104]. The infrared absorption spectrum of atmospheric GHGs may also depend on latitude/longitude and altitude locations since GHG distributions other than carbon dioxide are not uniform.
Partly because the infrared absorption bands of the various components of the atmosphere overlap, the contributions from individual absorbers do not add linearly. Clouds trap only 14 percent of the radiation with all other major species present, but would trap 50 percent if all other absorbers were removed [105] (Table D2 and Figure D1). Carbon dioxide adds 12 percent to radiation trapping, which is less than the contribution from either water vapor or clouds. By itself, however, carbon dioxide is capable of trapping three times as much radiation as it actually does in the Earth's atmosphere. Freidenreich and colleagues [106] have reported the overlap of carbon dioxide and water absorption bands in the infrared region. Given the present composition of the atmosphere, the contribution to the total heating rate in the troposphere is around 5 percent from carbon dioxide and around 95 percent from water vapor. In the stratosphere, the contribution is about 80 percent from carbon dioxide and about 20 percent from water vapor. It is important to remember, however, that it is currently believed that the impact of water vapor produced from surface sources such as fuel combustion on the atmospheric water vapor concentrations is minimal.
Table D2. Efficiency of Heat Trapping by Greenhouse Gases and Clouds | ||
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Species Removed | Percentage Heat Trapped | Percentage Heat Not Trapped |
Alla | 0 | 100 |
H2O, CO2, O3 | 50 | 50 |
H2O | 64 | 36 |
Clouds | 86 | 14 |
CO2 | 88 | 12 |
O3 | 97 | 3 |
None | 100 | 0 |
CO2 = Carbon dioxide. H2O
= Water vapor. O3 = Ozone. aIncludes clouds. Source: V. Ramanathan and J.A. Coakley, Jr., Climate Modeling Through Radiative-Convective Models, Review of Geophysics & Space Physics 16 (1978):465. |