Chapter 1 Text
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Chapter 5 Measures of Humidity Phases of Water
Chapter 5 Atmospheric Moisture Measures of Humidity 1. Absolute humidity 2. Specific humidity 3. Actual vapor pressure 4. Saturation vapor pressure 5. Relative humidity 6. Dew point Phases of Water Water Vapor n o su ti b ra li o n m p io d a a at ep t v s o io e en s n d it n io o n c freezing Liquid Water Ice melting 1 Coexistence of Water & Vapor • Even below the boiling point, some water molecules leave the liquid (evaporation). • Similarly, some water molecules from the air enter the liquid (condense). • The behavior happens over ice too (sublimation and condensation). Saturation • If we cap the air over the water, then more and more water molecules will enter the air until saturation is reached. • At saturation there is a balance between the number of water molecules leaving the liquid and entering it. • Saturation can occur over ice too. Hydrologic Cycle 2 Air Parcel • Enclose a volume of air in an imaginary thin elastic container, which we will call an air parcel. • It contains oxygen, nitrogen, water vapor, and other molecules in the air. 1. Absolute Humidity Mass of water vapor Absolute humidity = Volume of air The absolute humidity changes with the volume of the parcel, which can change with temperature or pressure. 2. Specific Humidity Mass of water vapor Specific humidity = Total mass of air The specific humidity does not change with parcel volume. 3 Specific Humidity vs. Latitude • The highest specific humidities are observed in the tropics and the lowest values in the polar regions. -
Insar Water Vapor Data Assimilation Into Mesoscale Model
This article has been accepted for inclusion in a future issue of this journal. Content is final as presented, with the exception of pagination. IEEE JOURNAL OF SELECTED TOPICS IN APPLIED EARTH OBSERVATIONS AND REMOTE SENSING 1 InSAR Water Vapor Data Assimilation into Mesoscale Model MM5: Technique and Pilot Study Emanuela Pichelli, Rossella Ferretti, Domenico Cimini, Giulia Panegrossi, Daniele Perissin, Nazzareno Pierdicca, Senior Member, IEEE, Fabio Rocca, and Bjorn Rommen Abstract—In this study, a technique developed to retrieve inte- an extremely important element of the atmosphere because its grated water vapor from interferometric synthetic aperture radar distribution is related to clouds, precipitation formation, and it (InSAR) data is described, and a three-dimensional variational represents a large proportion of the energy budget in the atmo- assimilation experiment of the retrieved precipitable water vapor into the mesoscale weather prediction model MM5 is carried out. sphere. Its representation inside numerical weather prediction The InSAR measurements were available in the framework of the (NWP) models is critical to improve the weather forecast. It is European Space Agency (ESA) project for the “Mitigation of elec- also very challenging because water vapor is involved in pro- tromagnetic transmission errors induced by atmospheric water cesses over a wide range of spatial and temporal scales. An vapor effects” (METAWAVE), whose goal was to analyze and pos- improvement in atmospheric water vapor monitoring that can sibly predict the phase delay induced by atmospheric water vapor on the spaceborne radar signal. The impact of the assimilation on be assimilated in NWP models would improve the forecast the model forecast is investigated in terms of temperature, water accuracy of precipitation and severe weather [1], [3]. -
ESSENTIALS of METEOROLOGY (7Th Ed.) GLOSSARY
ESSENTIALS OF METEOROLOGY (7th ed.) GLOSSARY Chapter 1 Aerosols Tiny suspended solid particles (dust, smoke, etc.) or liquid droplets that enter the atmosphere from either natural or human (anthropogenic) sources, such as the burning of fossil fuels. Sulfur-containing fossil fuels, such as coal, produce sulfate aerosols. Air density The ratio of the mass of a substance to the volume occupied by it. Air density is usually expressed as g/cm3 or kg/m3. Also See Density. Air pressure The pressure exerted by the mass of air above a given point, usually expressed in millibars (mb), inches of (atmospheric mercury (Hg) or in hectopascals (hPa). pressure) Atmosphere The envelope of gases that surround a planet and are held to it by the planet's gravitational attraction. The earth's atmosphere is mainly nitrogen and oxygen. Carbon dioxide (CO2) A colorless, odorless gas whose concentration is about 0.039 percent (390 ppm) in a volume of air near sea level. It is a selective absorber of infrared radiation and, consequently, it is important in the earth's atmospheric greenhouse effect. Solid CO2 is called dry ice. Climate The accumulation of daily and seasonal weather events over a long period of time. Front The transition zone between two distinct air masses. Hurricane A tropical cyclone having winds in excess of 64 knots (74 mi/hr). Ionosphere An electrified region of the upper atmosphere where fairly large concentrations of ions and free electrons exist. Lapse rate The rate at which an atmospheric variable (usually temperature) decreases with height. (See Environmental lapse rate.) Mesosphere The atmospheric layer between the stratosphere and the thermosphere. -
Exoplanet Atmospheres and Interiors Types of Planets
Exoplanet Atmospheres and Interiors Types of Planets • Hot Jupiters – Most common, because of observaonal biases – Temperatures ~ 1000K • Neptunes – May resemble the gas giants in our solar system • Super-earths – Rocky? – Water planets? • Terrestrial Atmosphere Basics • Ρ(h) = P(0) e-h/h0 • h0=kT/mg – k = Boltzmann constant – T=temperature – m=mass of par?cle – g=gravitaonal acceleraon • Density falls off exponen?ally with height Atmospheric Complicaons Stars have relavely simple atmospheres • A few diatomic molecules Brown Dwarfs and Planets are more complex • Temperature Inversions (external heang) • Clouds – Probably exist in T dwarfs – precipitaon • Molecules • Chemistry Generalized Thermal Atmosphere • Blue regions are convecve = lapse rate Marley, ARAA, fig 1 Atmospheric Chemistry • Ionizaon equilibrium • Chemical equilibrium High T Low T Low P High P Marley, ARAA, Fig 4 Marley, ARAA, Fig 3 • 2 MJ planet, T=600K, g=10 Marley, ARAA, Fig 5 Condensaon Sequence Transit Photometry Transit widths may reveal high al?tude haze 2 2 Excess eclipse depth δ ≃ ((Rp+ nH)/R∗) – (Rp/R∗) H = pressure scale height n = number of scale heights For typical hot Jupiters, δ ≅ 0.1% Observaons: Photometry • Precision photometry of transi?ng planet can give temperature – Comparison with Teq gives albedo (for Rp) • Inference of Na D1,D2 lines in HD 209458: – Eclipse 0.0002 deeper in lines – Charbonneau et al 2002, ApJ, 568, 377 Observaons: Photometry • Precision photometry of transi?ng planet can give temperature 2 2 – fin = (1-A) L* πRp / 4πd 2 4 – fout = 4πRp σTp – Comparison with Teq gives albedo (for Rp) For A=0: TP=T*√(R*/2d) Hot Jupiters • A is generally small: no clouds • Phase curve -> atmospheric dynamics • Flux variaons -> day to night temperature variaons • Hot Jupiters expected to have jet streams Basic Atmospheric Circulaon – no rotaon (Hadley cells) Jupiter HD 189733b • Temperature: 970-1200K • Peak 30o East • Winds up to 8700 km/h • H atm. -
A Featureless Transmission Spectrum for the Neptune-Mass Exoplanet GJ 436B
A featureless transmission spectrum for the Neptune-mass exoplanet GJ 436b Heather A. Knutson1, Björn Benneke1,2, Drake Deming3, & Derek Homeier4 1Division of Geological and Planetary Sciences, California Institute of Technology, Pasadena, CA 91125, USA. 2Department of Earth, Atmospheric, and Planetary Sciences, Massachusetts Institute of Technology, Cambridge, MA 02139, USA. 3Department of Astronomy, University of Maryland, College Park, MD 20742, USA. 4Centre de Recherche Astrophysique de Lyon, 69364 Lyon, France. GJ 436b is a warm (approximately 800 K) extrasolar planet that periodically eclipses its low-mass (0.5 MSun) host star, and is one of the few Neptune-mass planets that is amenable to detailed characterization. Previous observations1,2,3 have indicated that its atmosphere has a methane-to-CO ratio that is 105 times smaller than predicted by models for hydrogen-dominated atmospheres at these temperatures4,5. A recent study proposed that this unusual chemistry could be explained if the planet’s atmosphere is significantly enhanced in elements heavier than H and He6. In this study we present complementary observations of GJ 436b’s atmosphere obtained during transit. Our observations indicate that the planet’s transmission spectrum is effectively featureless, ruling out cloud-free, hydrogen-dominated atmosphere models with a significance of 48σ. The measured spectrum is consistent with either a high cloud or haze layer located at a pressure of approximately 1 mbar or with a relatively hydrogen-poor (3% H/He mass fraction) atmospheric composition7,8,9. We observed four transits of the Neptune-mass planet GJ 436b on UT Oct 26, Nov 29, and Dec 10 2012, and Jan 2 2013 using the red grism (1.2-1.6 µm) on the Hubble Space Telescope (HST) Wide Field Camera 3 instrument. -
TABLE A-2 Properties of Saturated Water (Liquid–Vapor): Temperature Table Specific Volume Internal Energy Enthalpy Entropy # M3/Kg Kj/Kg Kj/Kg Kj/Kg K Sat
720 Tables in SI Units TABLE A-2 Properties of Saturated Water (Liquid–Vapor): Temperature Table Specific Volume Internal Energy Enthalpy Entropy # m3/kg kJ/kg kJ/kg kJ/kg K Sat. Sat. Sat. Sat. Sat. Sat. Sat. Sat. Temp. Press. Liquid Vapor Liquid Vapor Liquid Evap. Vapor Liquid Vapor Temp. Њ v ϫ 3 v Њ C bar f 10 g uf ug hf hfg hg sf sg C O 2 .01 0.00611 1.0002 206.136 0.00 2375.3 0.01 2501.3 2501.4 0.0000 9.1562 .01 H 4 0.00813 1.0001 157.232 16.77 2380.9 16.78 2491.9 2508.7 0.0610 9.0514 4 5 0.00872 1.0001 147.120 20.97 2382.3 20.98 2489.6 2510.6 0.0761 9.0257 5 6 0.00935 1.0001 137.734 25.19 2383.6 25.20 2487.2 2512.4 0.0912 9.0003 6 8 0.01072 1.0002 120.917 33.59 2386.4 33.60 2482.5 2516.1 0.1212 8.9501 8 10 0.01228 1.0004 106.379 42.00 2389.2 42.01 2477.7 2519.8 0.1510 8.9008 10 11 0.01312 1.0004 99.857 46.20 2390.5 46.20 2475.4 2521.6 0.1658 8.8765 11 12 0.01402 1.0005 93.784 50.41 2391.9 50.41 2473.0 2523.4 0.1806 8.8524 12 13 0.01497 1.0007 88.124 54.60 2393.3 54.60 2470.7 2525.3 0.1953 8.8285 13 14 0.01598 1.0008 82.848 58.79 2394.7 58.80 2468.3 2527.1 0.2099 8.8048 14 15 0.01705 1.0009 77.926 62.99 2396.1 62.99 2465.9 2528.9 0.2245 8.7814 15 16 0.01818 1.0011 73.333 67.18 2397.4 67.19 2463.6 2530.8 0.2390 8.7582 16 17 0.01938 1.0012 69.044 71.38 2398.8 71.38 2461.2 2532.6 0.2535 8.7351 17 18 0.02064 1.0014 65.038 75.57 2400.2 75.58 2458.8 2534.4 0.2679 8.7123 18 19 0.02198 1.0016 61.293 79.76 2401.6 79.77 2456.5 2536.2 0.2823 8.6897 19 20 0.02339 1.0018 57.791 83.95 2402.9 83.96 2454.1 2538.1 0.2966 8.6672 20 21 0.02487 1.0020 -
REVIEW Doi:10.1038/Nature13782
REVIEW doi:10.1038/nature13782 Highlights in the study of exoplanet atmospheres Adam S. Burrows1 Exoplanets are now being discovered in profusion. To understand their character, however, we require spectral models and data. These elements of remote sensing can yield temperatures, compositions and even weather patterns, but only if significant improvements in both the parameter retrieval process and measurements are made. Despite heroic efforts to garner constraining data on exoplanet atmospheres and dynamics, reliable interpretation has frequently lagged behind ambition. I summarize the most productive, and at times novel, methods used to probe exoplanet atmospheres; highlight some of the most interesting results obtained; and suggest various broad theoretical topics in which further work could pay significant dividends. he modern era of exoplanet research started in 1995 with the Earth-like planet requires the ability to measure transit depths 100 times discovery of the planet 51 Pegasi b1, when astronomers detected more precisely. It was not long before many hundreds of gas giants were the periodic radial-velocity Doppler wobble in its star, 51 Peg, detected both in transit and by the radial-velocity method, the former Tinduced by the planet’s nearly circular orbit. With these data, and requiring modest equipment and the latter requiring larger telescopes knowledge of the star, the orbital period (P) and semi-major axis (a) with state-of-the-art spectrometers with which to measure the small could be derived, and the planet’s mass constrained. However, the incli- stellar wobbles. Both techniques favour close-in giants, so for many nation of the planet’s orbit was unknown and, therefore, only a lower years these objects dominated the bestiary of known exoplanets. -
Cold Plasma Diagnostics in the Jovian System
341 COLD PLASMA DIAGNOSTICS IN THE JOVIAN SYSTEM: BRIEF SCIENTIFIC CASE AND INSTRUMENTATION OVERVIEW J.-E. Wahlund(1), L. G. Blomberg(2), M. Morooka(1), M. André(1), A.I. Eriksson(1), J.A. Cumnock(2,3), G.T. Marklund(2), P.-A. Lindqvist(2) (1)Swedish Institute of Space Physics, SE-751 21 Uppsala, Sweden, E-mail: [email protected], [email protected], mats.andré@irfu.se, [email protected] (2)Alfvén Laboratory, Royal Institute of Technology, SE-100 44 Stockholm, Sweden, E-mail: [email protected], [email protected], [email protected], per- [email protected] (3)also at Center for Space Sciences, University of Texas at Dallas, U.S.A. ABSTRACT times for their atmospheres are of the order of a few The Jovian magnetosphere equatorial region is filled days at most. These atmospheres can therefore rightly with cold dense plasma that in a broad sense co-rotate with its magnetic field. The volcanic moon Io, which be termed exospheres, and their corresponding ionized expels sodium, sulphur and oxygen containing species, parts can be termed exo-ionospheres. dominates as a source for this cold plasma. The three Observations indicate that the exospheres of the three icy Galilean moons (Callisto, Ganymede, and Europa) icy Galilean moons (Europa, Ganymede and Callisto) also contribute with water group and oxygen ions. are oxygen rich [1, 2]. Several authors have also All the Galilean moons have thin atmospheres with modelled these exospheres [3, 4, 5], and the oxygen was residence times of a few days at most. -
4.4 Atmospheres of Solar System Planets
4.4. ATMOSPHERES OF SOLAR SYSTEM PLANETS 87 4.4 Atmospheres of solar system planets For spectroscopic studies of planets one needs to understand the net emission of the radiation from the surface or the atmosphere. Radiative transfer in planetary atmosphere is therefore a very important topic for the analysis of solar system objects but also for direct observations of extra-solar planets. In this section we discuss some basic properties of planetary atmospheres. 4.4.1 Hydrostatic structure of atmospheres The planet structure equation from Section 3.2 apply also for planetary atmospheres. One can often make the following simplifications: – the atmosphere can be calculated in a plane-parallel geometry considering only a vertical or height dependence z, – the vertical dependence of the gravitational acceleration can often be neglected for the pressure range 10 bar – 0.01 bar and one can just use g(z)=g(z = 0) = g(R)= 2 g = GMP /RP . – the equation of state can be described by the ideal gas law ⇢kT µP P (⇢)= or ⇢(P )= , µ kT where µ is the mean particle mass (in [kg] or [g]), – a mean particle mass which is constant with height µ(z)=µ can often be used in a first approximation, – a temperature which is constant with height T (z)=T can often be used as first approximation. Pressure structure. The di↵erential equation for the pressure gradient is: dP (z) µ(z)P (z) = g(z)⇢(z)= g(z) dz − − kT(z) which yields the general solution: z 1/H (z)dz kT(z) P (z)=P e− 0 P with H (z)= . -
Lecture.1.Introduction.Pdf
Lecture 1: Introduction to the Climate System Earth’s Climate System Solar forcing T mass (& radiation) The ultimate driving T & mass relation in vertical mass (& energy, weather..) Atmosphere force to Earth’s climate system is the heating from Energy T vertical stability vertical motion thunderstorm the Sun. Ocean Land The solar energy drives What are included in Earth’s climate system? Solid Earth three major cycles (energy, water, and biogeochemisty) What are the general properties of the Atmosphere? Energy, Water, and in the climate system. How about the ocean, cryosphere, and land surface? Biogeochemistry Cycles ESS200 ESS200 Prof. Jin-Yi Yu Prof. Jin-Yi Yu Thickness of the Atmosphere (from Meteorology Today) The thickness of the atmosphere is only about 2% 90% of Earth’s thickness (Earth’s 70% radius = ~6400km). Most of the atmospheric mass is confined in the lowest 100 km above the sea level. tmosphere Because of the shallowness of the atmosphere, its motions over large A areas are primarily horizontal. Typically, horizontal wind speeds are a thousands time greater than vertical wind speeds. (But the small vertical displacements of air have an important impact on ESS200 the state of the atmosphere.) ESS200 Prof. Jin-Yi Yu Prof. Jin-Yi Yu 1 Vertical Structure of the Atmosphere Composition of the Atmosphere (inside the DRY homosphere) composition temperature electricity Water vapor (0-0.25%) 80km (from Meteorology Today) ESS200 (from The Blue Planet) ESS200 Prof. Jin-Yi Yu Prof. Jin-Yi Yu Origins of the Atmosphere What Happened to H2O? When the Earth was formed 4.6 billion years ago, Earth’s atmosphere was probably mostly hydrogen (H) and helium (He) plus hydrogen The atmosphere can only hold small fraction of the mass of compounds, such as methane (CH4) and ammonia (NH3). -
Constraining Exoplanet Mass from Transmission Spectroscopy Arxiv
Constraining Exoplanet Mass from Transmission Spectroscopy? Julien de Wit1∗ and Sara Seager1;2 ?This is the author’s version of the work. It is posted here by permission of the AAAS for personal use, not for redistribution. The definitive version was published in Science (Vol. 342, pp. 1473, 20 December 2013), DOI: 10.1126/science.1245450. 1Department of Earth, Atmospheric and Planetary Sciences, Massachusetts Institute of Technology, 77 Massachusetts Avenue, Cambridge, MA 02139, USA. 2Department of Physics, Massachusetts Institute of Technology, 77 Massachusetts Avenue, Cambridge, MA 02139, USA. ∗To whom correspondence should be addressed; E-mail: [email protected]. Determination of an exoplanet’s mass is a key to understanding its basic prop- erties, including its potential for supporting life. To date, mass constraints for exoplanets are predominantly based on radial velocity (RV) measurements, which are not suited for planets with low masses, large semi-major axes, or those orbiting faint or active stars. Here, we present a method to extract an exoplanet’s mass solely from its transmission spectrum. We find good agree- ment between the mass retrieved for the hot Jupiter HD 189733b from trans- arXiv:1401.6181v1 [astro-ph.EP] 23 Jan 2014 mission spectroscopy with that from RV measurements. Our method will be able to retrieve the masses of Earth-sized and super-Earth planets using data from future space telescopes that were initially designed for atmospheric char- acterization. 1 1 Introduction With over 900 confirmed exoplanets (1) and over 2300 planetary candidates known (2), research priorities are moving from planet detection to planet characterization. In this context, a planet’s mass is a fundamental parameter because it is connected to a planet’s internal and atmospheric structure and it affects basic planetary processes such as the cooling of a planet, its plate tec- tonics (3), magnetic field generation, outgassing, and atmospheric escape. -
Humidity, Condensation, and Clouds-I
Humidity, Condensation, and Clouds-I GEOL 1350: Introduction To Meteorology 1 Overview • Water Circulation in the Atmosphere • Properties of Water • Measures of Water Vapor in the Atmosphere (Vapor Pressure, Absolute Humidity, Specific Humidity, Mixing Ratio, Relative Humidity, Dew Point) 2 Where does the moisture in the atmosphere come from ? Major Source Major sink Evaporation from ocean Precipitation 3 Earth’s Water Distribution 4 Fresh vs. salt water • Most of the earth’s water is found in the oceans • Only 3% is fresh water and 3/4 of that is ice • The atmosphere contains only ~ 1 week supply of precipitation! 5 Properties of Water • Physical States only substance that are present naturally in three states • Density liquid : ~ 1.0 g / cm3 , solid: ~ 0.9 g / cm3 , vapor: ~10-5 g / cm3 6 Properties of Water (cont’) • Radiative Properties – transparent to visible wavelengths – virtually opaque to many infrared wavelengths – large range of albedo possible • water 10 % (daily average) • Ice 30 to 40% • Snow 20 to 95% • Cloud 30 to 90% 7 Three phases of water • Evaporation liquid to vapor • Condensation vapor to liquid • Sublimation solid to vapor • Deposition vapor to solid • Melting solid to liquid • Freezing liquid to solid 8 Heat exchange with environment during phase change As water moves toward vapor it absorbs latent heat to keep the molecules in rapid mo9ti on Energy associated with phase change Sublimation Deposition 10 Sublimation – evaporate ice directly to water vapor Take one gram of ice at zero degrees centigrade Energy required