Study of Titan's Upper and Lower Atmosphere
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Cassini Update
Cassini Update Dr. Linda Spilker Cassini Project Scientist Outer Planets Assessment Group 22 February 2017 Sols%ce Mission Inclina%on Profile equator Saturn wrt Inclination 22 February 2017 LJS-3 Year 3 Key Flybys Since Aug. 2016 OPAG T124 – Titan flyby (1584 km) • November 13, 2016 • LAST Radio Science flyby • One of only two (cf. T106) ideal bistatic observations capturing Titan’s Northern Seas • First and only bistatic observation of Punga Mare • Western Kraken Mare not explored by RSS before T125 – Titan flyby (3158 km) • November 29, 2016 • LAST Optical Remote Sensing targeted flyby • VIMS high-resolution map of the North Pole looking for variations at and around the seas and lakes. • CIRS last opportunity for vertical profile determination of gases (e.g. water, aerosols) • UVIS limb viewing opportunity at the highest spatial resolution available outside of occultations 22 February 2017 4 Interior of Hexagon Turning “Less Blue” • Bluish to golden haze results from increased production of photochemical hazes as north pole approaches summer solstice. • Hexagon acts as a barrier that prevents haze particles outside hexagon from migrating inward. • 5 Refracting Atmosphere Saturn's• 22unlit February rings appear 2017 to bend as they pass behind the planet’s darkened limb due• 6 to refraction by Saturn's upper atmosphere. (Resolution 5 km/pixel) Dione Harbors A Subsurface Ocean Researchers at the Royal Observatory of Belgium reanalyzed Cassini RSS gravity data• 7 of Dione and predict a crust 100 km thick with a global ocean 10’s of km deep. Titan’s Summer Clouds Pose a Mystery Why would clouds on Titan be visible in VIMS images, but not in ISS images? ISS ISS VIMS High, thin cirrus clouds that are optically thicker than Titan’s atmospheric haze at longer VIMS wavelengths,• 22 February but optically 2017 thinner than the haze at shorter ISS wavelengths, could be• 8 detected by VIMS while simultaneously lost in the haze to ISS. -
Dynamics of Saturn's Small Moons in Coupled First Order Planar Resonances
Dynamics of Saturn's small moons in coupled first order planar resonances Maryame El Moutamid Bruno Sicardy and St´efanRenner LESIA/IMCCE | Paris Observatory 26 juin 2012 Maryame El Moutamid ESLAB-2012 | ESA/ESTEC Noordwijk Saturn system Maryame El Moutamid ESLAB-2012 | ESA/ESTEC Noordwijk Very small moons Maryame El Moutamid ESLAB-2012 | ESA/ESTEC Noordwijk New satellites : Anthe, Methone and Aegaeon (Cooper et al., 2008 ; Hedman et al., 2009, 2010 ; Porco et al., 2005) Very small (0.5 km to 2 km) Vicinity of the Mimas orbit (outside and inside) The aims of the work A better understanding : - of the dynamics of this population of news satellites - of the scenario of capture into mean motion resonances Maryame El Moutamid ESLAB-2012 | ESA/ESTEC Noordwijk Dynamical structure of the system µ µ´ Mp We consider only : - The resonant terms - The secular terms causing the precessions of the orbit When µ ! 0 ) The symmetry is broken ) different kinds of resonances : - Lindblad Resonance - Corotation Resonance D'Alembert rules : 0 0 c = (m + 1)λ − mλ − $ 0 L = (m + 1)λ − mλ − $ Maryame El Moutamid ESLAB-2012 | ESA/ESTEC Noordwijk Corotation Resonance - Aegaeon (7/6) : c = 7λMimas − 6λAegaeon − $Mimas - Methone (14/15) : c = 15λMethone − 14λMimas − $Mimas - Anthe (10/11) : c = 11λAnthe − 10λMimas − $Mimas Maryame El Moutamid ESLAB-2012 | ESA/ESTEC Noordwijk Corotation resonances Mean motion resonance : n1 = m+q n2 m Particular case : Lagrangian Equilibrium Points Maryame El Moutamid ESLAB-2012 | ESA/ESTEC Noordwijk Adam's ring and Galatea Maryame -
Saturn — from the Outside In
Saturn — From the Outside In Saturn — From the Outside In Questions, Answers, and Cool Things to Think About Discovering Saturn:The Real Lord of the Rings Saturn — From the Outside In Although no one has ever traveled ing from Saturn’s interior. As gases in from Saturn’s atmosphere to its core, Saturn’s interior warm up, they rise scientists do have an understanding until they reach a level where the tem- of what’s there, based on their knowl- perature is cold enough to freeze them edge of natural forces, chemistry, and into particles of solid ice. Icy ammonia mathematical models. If you were able forms the outermost layer of clouds, to go deep into Saturn, here’s what you which look yellow because ammonia re- trapped in the ammonia ice particles, First, you would enter Saturn’s up- add shades of brown and other col- per atmosphere, which has super-fast ors to the clouds. Methane and water winds. In fact, winds near Saturn’s freeze at higher temperatures, so they equator (the fat middle) can reach turn to ice farther down, below the am- speeds of 1,100 miles per hour. That is monia clouds. Hydrogen and helium rise almost four times as fast as the fast- even higher than the ammonia without est hurricane winds on Earth! These freezing at all. They remain gases above winds get their energy from heat ris- the cloud tops. Saturn — From the Outside In Warm gases are continually rising in Earth’s Layers Saturn’s atmosphere, while icy particles are continually falling back down to the lower depths, where they warm up, turn to gas and rise again. -
Electrons, Life and the Evolution of Earth's Chemical Cycles
Electrons, Life and the Evolution of Earth’s Chemical Cycles OCN 623 – Chemical Oceanography 23 April 2013 Adaption of Brian Glazer lecture (based on Falkowski and Godfrey (2008) Phil. Trans. R. Soc. B, 363: 2705-2716) © 2013 F.J. Sansone Outline Earth’s geological, geochemical and biological co- evolution since formation - Early Earth - Origins of life - The great oxidation event - Linkage between global O and N cycles - Alternate explanations for the great oxidation event - The rise of oxygen and the evolution of life - The Phanerozoic How Does the Earth Work as a Biosphere? All organisms derive energy for growth and maintenance by moving electrons from a substrate to a product All substrates and products must ultimately be recycled All metabolic processes on Earth are prokaryotic and were developed in the Archean and/or Proterozoic Eons Earth’s Geological, Geochemical and Biological Co-evolution Since Formation Earth, ~3.5 Ga Ago • Earth cools to <100˚C • Shallow sea environment – Land covered by low egg- shaped hills and pillow lavas – Silt layers – Scattered volcanic islands and evaporite lagoons • Tides higher – Moon closer to Earth, days shorter • Atmosphere –CO2-rich, no O2 – UV-drenched landscape Faint Sun Paradox High atmospheric CO2 and CH4 important in early Earth -- balanced weak Sun to maintain temp Recycling of Atmospheric CO2 Liquid water on early Earth allowed a hydrologic cycle, carbonate and silicate mineral weathering to develop: 2+ - CaCO3 + CO2 + H2O = Ca + 2HCO3 2+ - CaSiO3 +2CO2 +3H2O = Ca + 2HCO3 + H4SIO4 Uptake -
Application Note 160
APPLICATION NOTE 160 Degas Options for Sample Preparation Introduction A degas study was conducted to determine the effectiveness 1. Inert environment – shift from of flow versus vacuum degas. An amorphous silica- adsorbed phase to inert. alumina and a microporous zeolite were prepared by both techniques and then nitrogen isotherms were collected 2. Heat – increase the rate. for both materials. The resulting isotherms established equivalence between vacuum versus flow degas. Vacuum versus Flowing Degas Methods In the present study we accept that temperature may be controlled by various methods and that commercial temperature controllers provide repeatable performance. Rather than studying temperature control, this document will evaluate the topic of vacuum versus flowing degas. 1. Vacuum degas utilizes mass action as the only method for shifting the chemical equilibrium. An adsorbed molecule has a concentration on the surface, C and a negligible pressure, P=0 in the vapor phase. The pressure is maintained near zero since the sample is in a vacuum. Heating the sample increases the rate of transfer from the adsorbed molecules to the inert environment. 2. Flowing degas also utilizes mass action Theory by constant inert purge. The desorbed molecules are swept from the system Typical degas options include vacuum or flowing degas. The via the continuous inert gas flow and the basic concept of degas is quite simple. The sample material partial pressure of the desorbed molecules is placed in an inert environment. This inert environment in an inert stream approaches zero in a exploits chemical potential and creates a favorable state for manner similar to the vacuum technique. -
Is Extraterrestrial Organic Matter Relevant to the Origin of Life on Earth?
IS EXTRATERRESTRIAL ORGANIC MATTER RELEVANT TO THE ORIGIN OF LIFE ON EARTH? D. C. B. WHITTET Department of Physics, Applied Physics and Astronomy, Rensselaer Polytechnic Institute, Troy, NY 12180, U.S.A. (Received 19 August 1996) Abstract. I review the relative importance of internal and external sources of prebiotic molecules on Earth at the time of life's origin 3.7 Gyr ago. The ef®ciency of synthesis in the Earth's atmosphere was critically dependent on its oxidation state. If the early atmosphere was non-reducing and CO2- dominated, external delivery might have been the dominant source. Interplanetary dust grains and micrometeorites currently deliver carbonaceous matter to the Earth's surface at a rate of 3 5 7 10 kg/yr (equivalent to a biomass in 2 Gyr), but this may have been as high as 5 10 kg/yr (a biomass in only 10 Myr) during the epoch of late bombardment. Much of the incoming material is in the form of chemically inactive kerogens and amorphous carbon; but if the Earth once had a dense (10-bar) atmosphere, small comets rich in a variety of prebiotic molecules may have been suf®ciently air-braked to land non-destructively. Lingering uncertainties regarding the impact history of the Earth and the density and composition of its early atmosphere limit our ability to draw ®rm conclusions. 1. Introduction In at least one sense, a connection between the Universe at large and life in our small corner of it is inevitable. The hydrogen, carbon, nitrogen, oxygen, and other elements that make up our bodies and other living things were created billions of years ago in the interiors of stars and, in the case of hydrogen, in the the Big Bang itself (see Trimble, 1997, in this volume for an eloquent review). -
Titan and the Moons of Saturn Telesto Titan
The Icy Moons and the Extended Habitable Zone Europa Interior Models Other Types of Habitable Zones Water requires heat and pressure to remain stable as a liquid Extended Habitable Zones • You do not need sunlight. • You do need liquid water • You do need an energy source. Saturn and its Satellites • Saturn is nearly twice as far from the Sun as Jupiter • Saturn gets ~30% of Jupiter’s sunlight: It is commensurately colder Prometheus • Saturn has 82 known satellites (plus the rings) • 7 major • 27 regular • 4 Trojan • 55 irregular • Others in rings Titan • Titan is nearly as large as Ganymede Titan and the Moons of Saturn Telesto Titan Prometheus Dione Titan Janus Pandora Enceladus Mimas Rhea Pan • . • . Titan The second-largest moon in the Solar System The only moon with a substantial atmosphere 90% N2 + CH4, Ar, C2H6, C3H8, C2H2, HCN, CO2 Equilibrium Temperatures 2 1/4 Recall that TEQ ~ (L*/d ) Planet Distance (au) TEQ (K) Mercury 0.38 400 Venus 0.72 291 Earth 1.00 247 Mars 1.52 200 Jupiter 5.20 108 Saturn 9.53 80 Uranus 19.2 56 Neptune 30.1 45 The Atmosphere of Titan Pressure: 1.5 bars Temperature: 95 K Condensation sequence: • Jovian Moons: H2O ice • Saturnian Moons: NH3, CH4 2NH3 + sunlight è N2 + 3H2 CH4 + sunlight è CH, CH2 Implications of Methane Free CH4 requires replenishment • Liquid methane on the surface? Hazy atmosphere/clouds may suggest methane/ ethane precipitation. The freezing points of CH4 and C2H6 are 91 and 92K, respectively. (Titan has a mean temperature of 95K) (Liquid natural gas anyone?) This atmosphere may resemble the primordial terrestrial atmosphere. -
Life in the Outer Solar System Jupiter
Life in the Outer Solar System Jupiter Big R = 11R⊕ Massive M = 300 M⊕ = 2.5 all the rest Thick Atmosphere Mostly H2, He But also more complex molecules Colors, storms Like Miller - Urey Life in Jupiter Atmosphere? Sagan-Salpeter, etc. Sinkers (Plankton) Floaters (Fish) Hunters (Fish) Galileo Results on Jupiter Reached Jupiter Dec. 1995 Sent probe into Jupiter’s atmosphere at 100,000 mile/hour Decelerated at 230 g Lasted for 57 min. Found: Strong winds Turbulence, little lightning Life less likely? Surprise: Little or no H2O May have entered in an unusual place (fewer clouds) Europa (Moon of Jupiter) Surface: Fractured Ice Subsurface Oceans? (Heated from Inside) Close-up of “ice floes” Galileo - Jupiter’s Moons http://www.jpl.nasa.gov/galileo/index.html Europa has a (THIN!) atmosphere UV H H H O=O T hin O O2 H2O ATM Pressure ~ 10–11 Earth More evidence for resurfacing along cracks by “ice geysers” fluid ice or liquid water Organic molecules on Callisto & Ganymede, maybe Europa? Saturn • Big (9.4 R⊕) • Massive (95 M⊕) • Year 29.5 years • Day 0.43 days • Composition similar to Jupiter Titan • Moon of Saturn • Diameter ~0.4 Earth • Atmospheric Pressure = 1.5 × Earth • 85% Nitrogen BUT • Cold (~90 K) • Reducing atmosphere • Haze • Lab for prebiotic chemistry The Cassini-Huygens Mission • Launched 10/13/97 • Arrived Saturn 7/2004 • Cassini studies – Saturn – Moons • Huygens – Dropped onto Titan – Study atmosphere – Surface CASSINI SPACECRAFT Huygens Probe • Released from Cassini • Slowed by heat shield • Parachute deploys • Soft landing • Sample -
Degas Backfill Gas Selection for Micromeritics Gas Adsorption Instruments
Application Note 73 Degas Backfill Gas Selection for Micromeritics Gas Adsorption Instruments Introduction adsorbed gas is one type of contaminant that you Specific surface areas and pore volume distribu- wish to remove during degassing, using nitrogen tions are often determined using gas adsorption as the backfill gas partially defeats the purpose of techniques. Prior to analysis, any adsorbed gas or degassing. Obviously, nitrogen is not a true inert vapor phase (such as water or other volatiles) gas when it comes to microporous materials. should be removed from the sample. This process is often referred to as degassing the sample. Therefore, for materials which tend to adsorb nitrogen, helium is a better choice as the backfill Degassing usually involves either heating the gas. Helium adsorption at room temperature is sample or flowing an inert gas across the sample negligible, even in the high energy pores of most during evacuation. In either case, molecules being microporous samples. desorbed from the surface of the sample are removed from the sample tube. After degassing, There are some highly microporous materials in the sample tube can be sealed and removed in one which helium (if used as the backfill gas) is ex- of the following conditions: tremely difficult to remove due to diffusion. Complete removal requires great care as well as • Under vacuum using the TranSealTM, an appa- time-consuming tasks. Otherwise its presence can ratus which is inserted into the sample tube. It severely distort an adsorption isotherm. is designed to close when removed from the degassing port and open automatically when For samples where neither nitrogen nor helium are installed on the sample port, maintaining a ideal, a vacuum-sealed transfer is the most vacuum-tight seal. -
Computer Simulation Applied to Studying Continuous Spirit Distillation and Product Quality Control
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Food Control 22 (2011) 1592e1603 Contents lists available at ScienceDirect Food Control journal homepage: www.elsevier.com/locate/foodcont Computer simulation applied to studying continuous spirit distillation and product quality control Fabio R.M. Batista, Antonio J.A. Meirelles* Laboratory EXTRAE, Department of Food Engineering, Faculty of Food Engineering, University of Campinas e UNICAMP, Campinas, Brazil article info abstract Article history: This work aims to study continuous spirit distillation by computational simulation, presenting some Received 7 June 2010 strategies of process control to regulate the volatile content. The commercial simulator Aspen (Plus and Received in revised form dynamics) was selected. A standard solution containing ethanol, water and 10 minor components rep- 2 March 2011 resented the wine to be distilled. A careful investigation of the vaporeliquid equilibrium was performed Accepted 8 March 2011 for the simulation of two different industrial plants. The simulation procedure was validated against experimental results collected from an industrial plant for bioethanol distillation. The simulations were Keywords: conducted with and without the presence of a degassing system, in order to evaluate the efficiency of Spirits fi Distillation this system in the control of the volatile content. To improve the ef ciency of the degassing system, fl Simulation a control loop based on a feedback controller was developed. The results showed that re ux ratio and Aspen Plus product flow rate have an important influence on the spirit composition. High reflux ratios and spirit Degassing flow rates allow for better control of spirit contamination. -
The Sun's Dynamic Atmosphere
Lecture 16 The Sun’s Dynamic Atmosphere Jiong Qiu, MSU Physics Department Guiding Questions 1. What is the temperature and density structure of the Sun’s atmosphere? Does the atmosphere cool off farther away from the Sun’s center? 2. What intrinsic properties of the Sun are reflected in the photospheric observations of limb darkening and granulation? 3. What are major observational signatures in the dynamic chromosphere? 4. What might cause the heating of the upper atmosphere? Can Sound waves heat the upper atmosphere of the Sun? 5. Where does the solar wind come from? 15.1 Introduction The Sun’s atmosphere is composed of three major layers, the photosphere, chromosphere, and corona. The different layers have different temperatures, densities, and distinctive features, and are observed at different wavelengths. Structure of the Sun 15.2 Photosphere The photosphere is the thin (~500 km) bottom layer in the Sun’s atmosphere, where the atmosphere is optically thin, so that photons make their way out and travel unimpeded. Ex.1: the mean free path of photons in the photosphere and the radiative zone. The photosphere is seen in visible light continuum (so- called white light). Observable features on the photosphere include: • Limb darkening: from the disk center to the limb, the brightness fades. • Sun spots: dark areas of magnetic field concentration in low-mid latitudes. • Granulation: convection cells appearing as light patches divided by dark boundaries. Q: does the full moon exhibit limb darkening? Limb Darkening: limb darkening phenomenon indicates that temperature decreases with altitude in the photosphere. Modeling the limb darkening profile tells us the structure of the stellar atmosphere. -
Our Atmosphere Greece Sicily Athens
National Aeronautics and Space Administration Sardinia Italy Turkey Our Atmosphere Greece Sicily Athens he atmosphere is a life-giving blanket of air that surrounds our Crete T Tunisia Earth; it is composed of gases that protect us from the Sun’s intense ultraviolet Gulf of Gables radiation, allowing life to flourish. Greenhouse gases like carbon dioxide, Mediterranean Sea ozone, and methane are steadily increasing from year to year. These gases trap infrared radiation (heat) emitted from Earth’s surface and atmosphere, Gulf of causing the atmosphere to warm. Conversely, clouds as well as many tiny Sidra suspended liquid or solid particles in the air such as dust, smoke, and Egypt Libya pollution—called aerosols—reflect the Sun’s radiative energy, which leads N to cooling. This delicate balance of incoming and reflected solar radiation 200 km and emitted infrared energy is critical in maintaining the Earth’s climate Turkey Greece and sustaining life. Research using computer models and satellite data from NASA’s Earth Sicily Observing System enhances our understanding of the physical processes Athens affecting trends in temperature, humidity, clouds, and aerosols and helps us assess the impact of a changing atmosphere on the global climate. Crete Tunisia Gulf of Gables Mediterranean Sea September 17, 1979 Gulf of Sidra October 6, 1986 September 20, 1993 Egypt Libya September 10, 2000 Aerosol Index low high September 24, 2006 On August 26, 2007, wildfires in southern Greece stretched along the southwest coast of the Peloponnese producing Total Ozone (Dobson Units) plumes of smoke that drifted across the Mediterranean Sea as far as Libya along Africa’s north coast.