Physics and Chemistry in Space Vol. 13 Edited by L. J. Lanzerotti, Murray Hill Vladimir A. Krasnopolsky Photochemistry of the Atmospheres of Mars and Venus Technical Editor UlfvonZahn With 209 Figures Springer-Verlag Berlin Heidelberg New York Tokyo ~----J Professor Dr. VLADIMIR A. KRASNOPOLSKY Space Research Institute Academy of Sciences Profsojusnaja, 84/32 117810 Moscow, USSR Technical Editor: Professor Dr. ULF VON ZAHN Rheinische Friedrich-Wilhelms-Universitat Bonn Physikalisches Institut NuJ3allee 12 5300 Bonn, FRG Title of the original Russian edition: Fotokhimia atmosfer marsa i veneri © by Nauka, Moscow 1982 ISBN-13 978-3-642-70403-1 e-ISBN-13: 978-3-642-70401-7 DOl: 10.1007/978-3-642-70401-7 Library of Congress Cataloging-in-Publication Data. Krasnopol'skiI, V. A. (Vla dimir Anatol'evich), 1938- Photochemistry of the atmosphere of Mars and Venus. (Physics and chemistry in space ; v. 13) Translation of: Fotokhimiia atmosfer Marsa i Venery. Bibliography: p. Includes index. I. Mars (Planet) - Atmosphere. 2. Venus (Planet) - Atmosphere. 3. Photochemistry. 4. Cosmo chemistry. I. Title. II. Series. QC80l.P46 vol. 13 530'.0919 s 85-25008 [QB6411 [551.5'0999'231 This work is subject to copyright. All rights are reserved, whether the whole or part of the material is concerned, specifically those of translation, reprinting, re use of illustrations, broadcasting, reproduction by photocopying machine or similar means, and storage in data banks. Under § 54 of the German Copy right Law, where copies are made for other than private use, a fee is payable to "Verwertungsgesellschaft Wort", Munich. © by Springer-Verlag Berlin Heidelberg 1986 Softcover reprint of the hardcover I st edition 1986 The use of registered names, trademarks, etc. in this publication does not imply, even in the absence of a specific statement, that such names are exempt from the relevant protective laws and regulations and therefore free for general use. 2131/3130-543210 Preface Spacecraft study of the Solar system is one of humanity's most outstanding achievements. Thanks to this study, our present knowledge of properties of and conditions on the planets exceeds many-fold that of 20 years ago: planets have been rediscovered. This is especially the case for planetary atmospheres, whose properties were for the most part either not at all or only erroneously known. Much research has been invested in the study of the atmospheres of Mars and Venus, and their chemical composition and photochemistry are basic problems in these studies. In the present publication I have tried to summarize all findings in this field. The English version of the book includes new data in the field from the last 3 years since the book was published in Russian. I wish to thank U. von Zahn, who initiated my talks with Springer-Verlag and acted as technical editor. December 2, 1985 V. A. KRASNOPOLSKY Contents Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1 1 Chemical Composition and Structure of the Martian Atmosphere 4 1.1 Carbon Dioxide and Atmospheric Pressure . . . . . . . . . . . . . . . . . . . 4 1.2 CO and O2 Mixing Ratios . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8 1.3 Ozone. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 10 1.4 Water Vapor ............................................ 18 1.5 Composition of the Upper Atmosphere as Determined from Airglow Spectroscopy . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 23 1.6 Mass Spectrometric Measurements of the Atmospheric Composition ............................................ 31 1.7 Ionospheric Composition . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 34 1.8 Temperature Profile of the Lower Atmosphere. . . . . . . . . . . . . . . . 36 1.9 Temperature of the Upper Atmosphere ...................... 40 1.10 Eddy Diffusion Coefficient ................................ 42 2 Photochemistry of the Martian Atmosphere .................. 46 2.1 Ionosphere. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 46 2.2 Photochemistry of Nitrogen ............................... 53 2.3 H2 Dissociation and Escape of Atomic Hydrogen . . . . . . . . . . . . . . 58 2.4 Nonthermal Escape and Isotopic Composition of Oxygen and Nitrogen ................................................ 61 2.5 Dissociation of CO2: Atomic Carbon in the Upper Atmosphere. . 65 2.6 Diffusion and Photolysis of Water Vapor .................... 69 2.7 Photochemistry of the Lower Atmosphere (Global Average Conditions) ............................................. 74 2.8 Diurnal Variations of Minor Components in the Low Latitude Atmosphere ............................................. 84 2.9 Latitudinal Distribution of Ozone in Different Seasons ......... 85 2.10 Seasonal Variations of Atmospheric Composition at a Latitude of 65°N ................................................... 91 VIII Contents 3 Chemical Composition and Structure of the Venusian Atmosphere and Cloud Layer ............................. . 99 3.1 Properties of Aerosol in the Upper Part of the Cloud Layer Deduced from Polarization Measurements .................. . 99 3.2 Interpretation of Spectroscopic Measurements of Escaping Radiation ............................................. ,. 102 3.3 Spectroscopy in Visible and Infrared Ranges ................. . 105 3.4 Remote Sounding of Water Vapor and Carbon Monoxide in Far Infrared and Microwave Regions. Radio Spectrum ........... . 110 3.5 Optical Measurements in the 0.45 -1.2 J.Lm Range from Venera Landers ................................................ . 119 3.6 Mass Spectrometric and Gas Chromatographic Measurements in the Lower Atmosphere .. , .............................. . 125 3.7 Physical Characteristics of the Cloud Layer ................. . 131 3.8 Ultraviolet Absorption in the Cloud Layer .................. . 143 3.9 Investigation of a Cloud Layer Elemental Composition by X-Ray Fluorescent Spectroscopy in the Region of 1 to 20 A (0.6-13 keY) ........................................... . 159 3.10 Summary of the Data on the Tropospheric and Cloud Layer Composition ........................................... . 162 3.11 The Upper Atmosphere .................................. . 172 3.12 Ionosphere ............................................. . 189 3.13 Temperature, Eddy Mixing, Atmospheric Dynamics, and Lightning .......................................... . 196 4 Photochemistry of the Venusian Atmosphere ................ . 205 4.1 Day Side Ionosphere ..................................... . 205 4.2 Nighttime Ionosphere .................................... . 209 4.3 Metastable Species in the Venusian Ionosphere. Nitric Oxide, Atomic Nitrogen, and Atomic Carbon ...................... . 215 4.4 Light Components of the Upper Atmosphere (H, H2, He). "Hot" Atoms and Nonthermal Escape of H, He, and 0 ....... . 220 4.5 Thermospheric Models ................................... . 229 4.6 Lightning and Lower Atmospheric Chemistry. Nitric Oxide in the Lower Atmosphere ...................... . 232 4.7 Lower Atmospheric and Surface Rock Compositions (0 - 50 km) 236 4.8 Neutral Atmospheric Photochemistry Above 50 km. Main Problems, Previous Results, Main Chemical Reactions ........ . 246 4.9 Radiative Transfer and Aerosol Transport in the Cloud Layer .. . 255 4.10 Boundary Conditions .................................... . 258 4.11 Atmospheric Composition at 50 to 200 km (Results of Calculations) ........................................... . 260 4.12 0 1.27 J.Lm and OeD) 630 nm Airglow. Photolytic Rates ...... . 270 2 Contents IX 4.13 The Influence of Some Reaction Rate Coefficients on the Results of Calculations .......................................... 274 4.14 Photochemistry of the Venusian Mesosphere as Considered by Winick and Stewart (1980) ................................. 275 4.15 Analysis of Atmospheric Photochemistry on Venus by Yung and DeMore (1982) . .. . . . . . . . . . ... .. . . . . . . . . . . . . . . . . . . . . . .. . . . 277 4.16 Loss of Water from Venus and Its Atmospheric Evolution ...... 295 4.17 Conclusions............................................. 310 References ................................................... 315 Subject Index. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 331 Introduction The main aim of this book is to present experimental and theoretical results achieved over the last decade on the chemical composition and structure of the atmospheres of Mars and Venus, processes defining the properties of the at mospheres, and other related phenomena. Three basic aims for studies of an atmosphere exist: chemical composi tion, thermal regime, and dynamics. The chemical composition of an atmo sphere is determined by its origin and evolution, processes of gas exchange be tween the atmosphere and the planetary body and space, and by chemical and physical processes inside the atmosphere. The latter processes are defined in the science of aeronomy, and this book is concerned primarily with findings in this field. However, a planetary atmosphere is a single entity and all its com ponents are interrelated, e.g., its chemical composition determines thermal regime and the latter, in turn, affects its dynamics. Therefore, this book provides a brief description of these problems as well. Ample space is given to experimental results and their interpretation. For theoretical findings, I will try to give an idea of a method or an interpretation, followed by the results obtained. The advantages or speculative aspects of some approaches are also considered. Unfortunately, in many cases I had no possibility to discuss the papers described with their authors, thus, this may have led sometimes to errors in my evaluations. Therefore, I would greatly appreciate receiving some response from readers. Of similar importance to experimental results are theoretical models which describe the transformations of atmospheric constituents by photochemical processes in the presence of transport. If these models are in accord with the scope of experimental data, then they demonstrate the adequacy of our knowledge of the intimate properties of the atmosphere. A photochemical ap proach may be of use in the case of controversial experimental data. Besides, model calculations yield the amounts and vertical profiles of components which have been undetected or measured in a limited altitude range. Important aspects of the space programs of the USSR and USA over the last two decades include investigations of Mars and Venus. The structures of these programs were different. The Soviet program from the beginning of the 1960's was directed toward the designing of space vehicles with descent probes, while in the United States spacecraft with more and more complicated functions were developed: flyby systems for short-term observations from a distance of _104 km, orbiters, and descent probes. 2 Introduction The first successful experiments for the study of Mars were carried out by the American flybys Mariner 4 (1965) and Mariner 6, 7 (1969). The first orbiters were in 1971: Soviet Mars 2 and 3 and U.S. Mariner 9. That year, the first descent probe, Mars 3, was launched into the Martian atmosphere to measure its properties. Though the descent and landing proceeded normally, information transmission ceased soon after it started, probably as a result of extremely strong winds of a global dust storm on the planet which could have led to the disturbance of the antenna's operation. In 1974, four Soviet probes, i.e., two flybys (Mars 4 and 7), one orbiter (Mars 5), and one descent probe (Mars 6), investigated the planet. The most extensive research program of Mars was carried out by Viking 1 and 2 (1976 until 1981), which incorporated long-lived landers and orbiters. The first space studies of Venus were made by the American flybys Mariner 2 (1962) and Mariner 5 (1967). The latter was accompanied by the successful descent of the Soviet Venera 4. Then, a series of first generation Soviet descent probes followed (Veneras 5 to 8, 1969-1972). In 1974, Mariner 10 flew by Venus and Mercury. The second generation of Soviet spacecraft to study Venus was started in 1975 by Veneras 9 and 10, each in cluding a descent probe and an orbiter. At the end of 1978 the U.S. Pioneer Venus spacecraft arrived at Venus, which incorporated four descent probes intended to operate at different locations (low and high latitudes, day and night sides), an entry probe (bus) for measurements down to 130 km, and an orbiter with a pericenter at 150 km. At the same time, Soviet Veneras 11 and 12 operated. Since then, studies of Venus were continued by Veneras 13, 14 lander probes (1982) and Veneras 15, 16 orbiters (1983 -1984). Results obtained by the spacecraft, supplemented by some ground-based observations, especially high resolution spectroscopy in infrared and micro wave regions, form the foundation of our modern knowledge of both planets. Studies of the solar system, which may seem at first glance to be far removed from the needs and concerns of humanity, are of great cognitive and philosophical value, especially the problem of the origin and evolution of the solar system. However, it is our deep belief that atmospheric photochemistry will find ever increasing use. Human activity influences the environment negatively, in particular, leads to air pollution. Effective methods to maintain the existing properties of the atmosphere might be developed in the future. One significant problem is to study the atmospheric resilience to influences which might result in some irreversible consequences in definite conditions. For example, the atmospheric temperature depends on abundances of water vapor and carbon dioxide and the area of clouds reflecting solar radiation. The situation when high atmospheric temperature could be maintained by the amount of increased atmospheric water vapor does not seem totally im probable. Another apt example widely discussed in the last decade is the nega tive consequences of reduced amounts of ozone in the atmosphere as a result of enhanced delivery of chlorfluormethanes and nitrogen oxides, which act as catalysts in the process of destroying the ozone layer. Introduction 3 The mathematical background of photochemical modeling is a system of continuity equations for every component under consideration: onj - --+ V¢Jj= Pj-njLj ot where nj is the number density, V = i ~ + j ~ + k ~ is the differential op- oX oy oz fPj erator, P and L are the production and loss rates by chemical reactions, is j j the flux of the component which can be given by -(K OT] (K ¢Jj = +Dj) [onj +~(1 + aj) -nj + Dj) oz oz T H H j for one-dimensional models and in the approximation of the minor component nj ~ L nj. Here, K is the eddy mixing coefficient, Dj is the j molecular diffusion coefficient, Hand H are the mean atmospheric scale j heights and that of the i component, T is the temperature, and aj is the ther mal diffusion factor. In a physical sense, the continuity equation implies that changes in the density of a component number are due to chemical reactions or transport from or to other atmospheric regions. Since altitude variations of atmospheric composition as a rule greatly ex ceed horizontal variations, derivatives with respect to horizontal coordinates are much less than those with respect to height and may be neglected. This ap proximation gives one-dimensional models. When diurnal and other temporal variations are not taken into consideration, time independent models are used which simplify the system of partial differential equations to that of ordinary differential equations. In some cases, e.g., for ionospheric calculations, when photochemical lifetimes, Tc = L -1, are much less than transport time con stants, Tm = H2/(K + D), transport effects can be neglected, and one gets a system of algebraic equations, Pj = njLj. In most cases these systems of equations need a special computation tech nique, the description of which is beyond the scope of our book. Boundary and (in the case of time-dependent problems) initial conditions should be introduced. The usual form of boundary conditions is number den sities or fluxes at both (upper and lower) boundaries. Below, some widespread cases are given: ¢Jj = 0 at the upper boundary implies diffusive equilibrium of the component nj, its altitude distribution having a scale height H = ~ j mjg above the upper boundary. The same at the lower boundary implies that inter actions with the low lying atmosphere or surface are negligible (chemically passive surface). A condition of photochemical equilibrium at the boundary, nj = P;lL is a partial case of the boundary condition for a component j, number density. This book is based on data published up to the beginning of 1984.