Groundbased observations 1988 – 2001 and post-2003 –Two distinct populations of brightness –Brightenings occur periodically Between 2001 and 2003 –Single.

Slides:



Advertisements
Similar presentations
The scaling of LWFA in the ultra-relativistic blowout regime: Generation of Gev to TeV monoenergetic electron beams W.Lu, M.Tzoufras, F.S.Tsung, C. Joshi,
Advertisements

Section 18.1 Volcanoes Types of Volcanoes
Thermoforming Process
The Radial Variation of Interplanetary Shocks C.T. Russell, H.R. Lai, L.K. Jian, J.G. Luhmann, A. Wennmacher STEREO SWG Lake Winnepesaukee New Hampshire.
Proposed Experimental Method to Determine the Radiant Influence of CO 2 in the Night Sky Brian G Valentine US Department of Energy Washington, DC March.
Non-Equilibrium Ionization Modeling of the Current Sheet in a Simulated Solar Eruption Chengcai Shen Co-authors: K. K. Reeves, J. C. Raymond, N. A. Murphy,
The Seasonal Behavior of Water Ice Clouds in the Tharsis and Valles Marineris Regions of Mars: Mars Obiter Camera Observations J. Benson, B. Bonev, P.
RHESSI/GOES Observations of the Non-flaring Sun from 2002 to J. McTiernan SSL/UCB.
The Seasonal Behavior of Water Ice Clouds in the Tharsis and Valles Marineris Regions of Mars: Mars Obiter Camera Observations J. Benson, B. Bonev, P.
Ionization, Resonance excitation, fluorescence, and lasers The ground state of an atom is the state where all electrons are in the lowest available energy.
T21C-1981 Estimating Earth's Heat Flux Will Gosnold, Department of Geology and Geological Engineering University of North Dakota
Yalin Fan and Isaac Ginis GSO, University of Rhode Island Effects of surface waves on air- sea momentum and energy fluxes and ocean response to hurricanes.
Magma Ocean Solidification: Oldest Lunar Zircon COSMOCHEMISTRY iLLUSTRATED Time to Solidify an Ocean of Magma The Moon melted when it formed. How long.
1 “A Post Galileo view of Io’s Interior” Keszthelyi et al. Icarus 169 (2004) Raquel Fraga-Encinas Dec 7, 2004UMD TERPS Conference.
Two Simple Models of Thermal Stress Voller-Guzina-Stelson
A Warm South Pole? Yes, on Neptune! A&A 473, L5 – L8 (2007) "Evidence for Methane Escape and Strong Seasonal and Dynamical Perturbations of Neptune's Atmospheric.
Vulcanian fountain collapse mechanisms revealed by multiphase numerical simulations: Influence of volatile leakage on eruptive style and particle-size.
Loki Spectra Update Robert R. Howell University of Wyoming with help from Jani and Jason while on sabbatical at UA Fall 2005 and calibrated C10 images.
Prometheus Lava-Frost Interaction Robert R. Howell University of Wyoming.
Lens Galaxy Environments Neal Dalal (IAS), Casey R. Watson (Ohio State) astro-ph/ Who cares? 2.What to do 3.Results 4.Problems! 5.The future.
Io. Io Overview Innermost Galilean Moon 4 th largest moon in the solar system with a diameter of 2,263 miles Most geologically active object in the solar.
What stellar properties can be learnt from planetary transits Adriana Válio Roque da Silva CRAAM/Mackenzie.
Lecture 5 Historical Interest Rate Movements. Term Structure Shapes Normal upward sloping Inverted Level Humped.
Multiwavelength Continuum Survey of Protostellar Disks in Ophiuchus Left: Submillimeter Array (SMA) aperture synthesis images of 870 μm (350 GHz) continuum.
Experimental determination of motor model parameters ETEC6419.
Speed-Current Relation in Lightning Return Strokes Ryan Evans, Student - Mostafa Hemmati, Advisor Department of Physical Sciences Arkansas Tech University.
Multiwavelength observations of a partially occulted solar flare Laura Bone, John C.Brown, Lyndsay Fletcher.
The study of MARFE during long pulse discharges in the HT-7 tokamak W.Gao, X.Gao, M.Asif, Z.W.Wu, B.L.Ling, and J.G.Li Institute of Plasma Physics, Chinese.
Where is Coronal Plasma Heated? James A. Klimchuk NASA Goddard Space Flight Center, USA Stephen J. Bradshaw Rice University, USA Spiros Patsourakos University.
1 Determination of CME 3D Trajectories using COR Stereoscopy + Analysis of HI1 CME Tracks P. C. Liewer, E. M. DeJong, J. R. Hall, JPL/Caltech; N. Sheeley,
ACM #8102. Tuesday, 15 July 2008 Velocities and relative amounts of material ejected after the collision of DI impactor with comet Tempel 1 Sergei.
3rd International Conference LUBRICANTS RUSSIA Diesel Particulate Filter Regeneration Strategy and its Influence on Engine Oil Characteristics Luca.
Volcanoes Chapter 15 Section 2.
CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing January 2012.
Arrival time of halo coronal mass ejections In the vicinity of the Earth G. Michalek, N. Gopalswamy, A. Lara, and P.K. Manoharan A&A 423, (2004)
2-D FEM MODELING OF MICROWAVE HEATING OF COAL PARTICLES EGEE 520 SEMESTER PRESENTATION by Ojogbane M. Achimugu May 3 rd 2007.
Terrestrial atmospheres. Overview Most of the planets, and three large moons (Io, Titan and Triton), have atmospheres Mars Very thin Mostly CO 2 Some.
The Dilemma of RESOLUTION: How Good is Good Enough: A Case Study from Greenland James L Fastook University of Maine We thank the NSF, which has supported.
Modelling the radiative signature of turbulent heating in coronal loops. S. Parenti 1, E. Buchlin 2, S. Galtier 1 and J-C. Vial 1, P. J. Cargill 3 1. IAS,
Thermal evolution of an early magma ocean in interaction with the atmosphere T. Lebrun 1, H. Massol 1, E. Chassefière 1, A. Davaille 2, E. Marcq 3, P.
Astronomical Seeing. The Project Students will be introduced to the concept of astronomical seeing and how it affects the quality of astronomical images.
The impact of He II reionisation on the H I Ly-  forest Jamie Bolton Peng Oh (UCSB), Steve Furlanetto (UCLA)
Physical Fluid Dynamics by D. J. Tritton What is Fluid Dynamics? Fluid dynamics is the study of the aforementioned phenomenon. The purpose.
Games Development 2 Entity Update & Rendering CO3301 Week 2, Part 1.
Warm-Up Kinematics: the study of motion Take out a sheet of paper and answer the following questions. How do you define “motion”? What do we need to know.
Numerical simulations of optical properties of nonspherical dust aerosols using the T-matrix method Hyung-Jin Choi School.
COMPARATIVE TEMPERATURE RETRIEVALS BASED ON VIRTIS/VEX AND PMV/VENERA-15 RADIATION MEASUREMENTS OVER THE NORTHERN HEMISPHERE OF VENUS R. Haus (1), G. Arnold.
TIPS - Oct 13, 2005 M. Sirianni Temperature change for ACS CCDs: initial study on scientific performance M. Sirianni, T. Wheeler, C.Cox, M. Mutchler, A.
Infrasound Technology WS – Bermuda, November 6 th, Microbarom signals recorded in Antarctica - a measure for sudden stratospheric warming? L. Ceranna,
Travis Metcalfe Space Science Institute + Stellar Astrophysics Centre Probing Stellar Activity with Kepler.
The Sun: Part 2. Temperature at surface = 5800 K => yellow (Wien’s Law) Temperature at center = 15,000,000 K Average density = 1.4 g/cm 3 Density at center.
Top Down Emission Analyses Theme 17 th GEIA Conference Nov. 19, 2015 Alex Guenther Department of Earth System Science University of California, Irvine.
Centre for Astrophysics Space- and time-dependent heating of solar coronal loops S. W. Higgins & R. W. Walsh
Implications of Errors in Density Response Time Delay on Satellite Prediction Error Rodney L. Anderson and Christian P. Guignet October 28, 2010, NADIR.
+ Quintessence and Gravitational Waves Peng Zhou, Daniel Chung UW-Madison Physics Dept.
2011 DSMC Workshop Workshop 2011 DSMC Workshop Workshop William McDoniel Modeling Gas and Dust Flow in Io’s Pele Plume William McDoniel D. B. Goldstein,
Study of the HTS Insert Quench Protection M. Sorbi and A. Stenvall 1 HFM-EuCARD, ESAC meeting, WP 7.4.1CEA Saclay 28 feb. 2013,
Volcanoes Chapter 7. Volcanoes Volcano is a weak spot in crust where molten material comes to the surface Magma is a molten mixture of rock-forming.
FISHERIES POSTER SESSION
Thermoforming Process
Solar Flare Energy Partition into Energetic Particle Acceleration
The Big Bang The Big Bang
Active volcanism on Venus?
EART193 Planetary Capstone
Observations of Magnetic Waves in the Voyager Data Set Marios Socrates Dimitriadis, Charles Smith Introduction Solar wind consists of highly energetic.
Phillip Hess Jie Zhang, Dusan Odstrcil
The spectral evolution of impulsive solar X-ray flares
The Big Bang The Big Bang
PANDA solenoid quench calculations
Temporal and Azimuthal Variability in the Io Plasma Torus
Presentation transcript:

Groundbased observations 1988 – 2001 and post-2003 –Two distinct populations of brightness –Brightenings occur periodically Between 2001 and 2003 –Single brightness population –Lower maximum brightness

October 1999 February 2000 Galileo Voyager Propagation direction

Quantification of model Unroll to make a simple rectangular lava lake Age determined as function of time and length Temperature calculated using cooling model of Davies, 2005 Total brightness calculated assuming blackbody emission Two input parameters: –Raft size Doesn’t affect results –Propagation speed, which influences Duration of event Maximum brightness reached: 3.5 micron brightness (in GW/μm/str) = speed (in km/day) x km 390 km raft WE

Model results What if Loki was a sulfur lake? –Used analytic cooling model of Howell (1997) altering the parameters for Sulfur –Doesn’t match A typical event lasts ~225 days To last 225 days, propagation speed must be 1.7 km/day The model predicts an average active brightness of 55 GW/μm/str Matches observed average active brightness of ~ 60 GW/μm/str

Matching data from Best three- year period of data Matched by simple variations of velocity with time

1998 position data Brightness and position of hot spots on 7/12 and 8/4 measured by MacIntosh et al. (2003) using speckle imaging Ran previous model and calculated 2.2 micron brightness – matches measurements Used velocity as a function of time to predict position of hot front during observations – matches measurements

data Remained at approximately average brightness (~35 GW/micron/str) for days A speed of 0.9 km/day gives –maximum brightness of 29 GW/μm/str –takes ~450 days to overturn entire patera Adaptive optics brightness measurements at 2.2, 3.8, and 4.3 microns (Marchis et al., 2005) –Data taken close together in time (December 18 th, 20 th, and 28 th ) –Velocity of 0.5 km/day matches the average data value With a velocity of 0.5 km/day, it takes 780 days to overturn the entire patera If the westernmost rafts begin to overturn after 540 days, 2 fronts will be present for part of the time Maximum brightness ~ 33 GW/μm/str –Compare to 17 GW/μm/str

Conclusions Model can match all data with simple changes in velocity of overturn propagation Changes in velocity imply that the age at which the rafts sinks also changes over time Age of raft when it sinks d epends on 1.The density of the magma 2.Initial density (especially porosity) of the crust 3.Other factors (e.g. the behavior of neighboring slabs) We use porosity profile from Peck et al. and a simple Stefan model of solidification to calculate the density of the solidified crust as a function of time Density remains remarkably constant between ~400 and 800 days (~1% difference) Small differences in porosity profile used will similarly lead to large differences in age at which the raft sinks Small changes in magma volatile content can produce large variations in sinking time (via effects 1 and 2) and thus propagation speed of the sinking front