Atmospheric Radiation: Theoretical Basis

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Oxford University Press, Dec 7, 1995 - Science - 519 pages
A complete revision of Goody's classic 1964 work, this volume offers a systematic discussion of atmospheric radiation processes that today are at the center of worldwide study and concern. It deals with the ways in which incident solar radiation is transformed into scattered and thermal radiation, and the thermodynamic consequences for the Earth's gaseous envelope, identifying aspects of the interaction between radiation and atmospheric motions as the central theme for atmospheric radiation studies. As a complete treatment of physical and mathematical foundations, the text assumes no prior knowledge of atmospheric physics. The theoretical discussion is systematic, and can therefore be applied with minor extension to any planetary atmosphere.

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Contents

1 INTRODUCTION
1
2 THEORY OF RADIATIVE TRANSFER
16
3 VIBRATIONROTATION SPECTRA OF GASEOUS MOLECULES
67
4 BAND MODELS
125
5 ABSORPTION BY ATMOSPHERIC GASES
189
6 RADIATION CALCULATIONS IN A CLEAR ATMOSPHERE
216
7 EXTINCTION BY MOLECULES AND DROPLETS
288
8 RADIATIVE TRANSFER IN A SCATTERING ATMOSPHERE
330
Appendix 2 Spectroscopic units
464
Appendix 3 A model atmosphere
468
Appendix 4 Properties of water vapor
470
Appendix 5 The Planck function
472
Appendix 6 The exponential integrals
475
Appendix 7 The Ladenburg and Reiche function
477
Appendix 8 The Elsasser function
480
Appendix 9 The physical state of the sun
482

9 ATMOSPHERES IN RADIATIVE EQUILIBRIUM
388
10 EVOLUTION OF A THERMAL DISTURBANCE
426
Appendix 1 Physical constants
462
Author Index
497
Subject Index
503
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Page 385 - The formation of absorption bands and the distribution of photon optical paths in a scattering atmosphere, Bull.
Page 75 - We assume that the scattering potential is weak and apply the Born approximation. The scattering probability is proportional to the square of the absolute value of the matrix element O' 1 3f \P> = Sdr%?' exp [-i- (p - /»') • rj Pk = g exp(i* • Rj) . (1.3.3) Here vk is the Fourier transform of v(r) and M = P — p' is the change of the neutron momentum.
Page 490 - ... center about 1,500°K lower than that of the undisturbed photosphere. The fraction of the photosphere covered by spots is never more than 0.2 percent, and their average persistence is about a week. For most of the period for which the observations are available, a sunspot cycle averages 1 1 .04 years. The number of spots is only one characteristic feature of the sun that changes in this rhythmic manner. Just after the minimum, spots first appear near 27° latitude in both hemispheres. As the...
Page 1 - The transformation of the incident solar radiation into scattered and thermal radiation, and the consequent thermodynamic effects on the earth's gaseous envelope, are very complicated phenomena, requiring the most advanced methods of molecular physics and quantum mechanical calculations. Absorption along a real atmospheric path, where pressure, temperature and composition all vary, presents problems...
Page 124 - The collision-induced fundamental and first overtone bands of oxygen and nitrogen,
Page 280 - Goody, RM (1964b). The transmission of radiation through an inhomogeneous atmosphere.

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