The Ability of Significant Tidal Stress to Initiate Plate Tectonics
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Activity Induced Variation in Spin-Orbit Angles As Derived from Rossiter–Mclaughlin Measurements M
A&A 619, A150 (2018) https://doi.org/10.1051/0004-6361/201833709 Astronomy & © ESO 2018 Astrophysics Activity induced variation in spin-orbit angles as derived from Rossiter–McLaughlin measurements M. Oshagh1,2, A. H. M. J. Triaud3, A. Burdanov4, P. Figueira2,5, A. Reiners1, N. C. Santos2,6, J. Faria2, G. Boue7, R. F. Díaz8,9, S. Dreizler1, S. Boldt1, L. Delrez10, E. Ducrot4, M. Gillon4, A. Guzman Mesa1, E. Jehin4, S. Khalafinejad11,12, S. Kohl11, L. Serrano2, and S. Udry13 1 Institut für Astrophysik, Georg-August Universität Göttingen, Friedrich-Hund-Platz 1, 37077 Göttingen, Germany e-mail: [email protected] 2 Instituto de Astrofísica e Ciências do Espaço, Universidade do Porto, CAUP, Rua das Estrelas, 4150-762 Porto, Portugal 3 University of Birmingham, Edgbaston, Birmingham, B15 2TT, UK 4 Space Sciences, Technologies and Astrophysics Research (STAR) Institute, Université de Liège, Allée du 6 Août 17, Bat. B5C, 4000 Liège, Belgium 5 European Southern Observatory, Alonso de Cordova 3107, Vitacura Casilla 19001, Santiago 19, Chile 6 Departamento de Física e Astronomia, Faculdade de Ciências, Universidade do Porto, Rua do Campo Alegre, 4169-007 Porto, Portugal 7 IMCCE, Observatoire de Paris, UPMC University Paris 6, PSL Research University, Paris, France 8 Universidad de Buenos Aires, Facultad de Ciencias Exactas y Naturales, Buenos Aires 1428, Argentina 9 CONICET – Universidad de Buenos Aires, Instituto de Astronomía y Física del Espacio (IAFE), Buenos Aires 1428, Argentina 10 Astrophysics Group, Cavendish Laboratory, -
Archimedean Proof of the Physical Impossibility of Earth Mantle Convection by J. Marvin Herndon Transdyne Corporation San Diego
Archimedean Proof of the Physical Impossibility of Earth Mantle Convection by J. Marvin Herndon Transdyne Corporation San Diego, CA 92131 USA [email protected] Abstract: Eight decades ago, Arthur Holmes introduced the idea of mantle convection as a mechanism for continental drift. Five decades ago, continental drift was modified to become plate tectonics theory, which included mantle convection as an absolutely critical component. Using the submarine design and operation concept of “neutral buoyancy”, which follows from Archimedes’ discoveries, the concept of mantle convection is proven to be incorrect, concomitantly refuting plate tectonics, refuting all mantle convection models, and refuting all models that depend upon mantle convection. 1 Introduction Discovering the true nature of continental displacement, its underlying mechanism, and its energy source are among the most fundamental geo-science challenges. The seeming continuity of geological structures and fossil life-forms on either side of the Atlantic Ocean and the apparent “fit’ of their opposing coastlines led Antonio Snider-Pellegrini to propose in 1858, as shown in Fig. 1, that the Americas were at one time connected to Europe and Africa and subsequently separated, opening the Atlantic Ocean (Snider-Pellegrini, 1858). Fig. 1 The opening of the Atlantic Ocean, reproduced from (Snider-Pellegrini, 1858). 1 Half a century later, Alfred Wegener promulgated a similar concept, with more detailed justification, that became known as “continental drift” (Wegener, 1912). Another half century later, continental drift theory was modified to become plate tectonics theory (Dietz, 1961;Hess, 1962;Le Pichon, 1968;Vine and Matthews, 1963). Any theory of continental displacement requires a physically realistic mechanism and an adequate energy source. -
(2 Points Each) 1. the Velocity Of
GG 101, Spring 2006 Name_________________________ Exam 2, March 9, 2006 A. Fill in the blank (2 points each) 1. The velocity of an S-wave is ______lower_________ than the velocity of a P-wave. 2. What type of seismic wave is being recorded by the above diagram? A __P__ wave. 3. The most voluminous layer of Earth is the ___mantle_________. 4. The rigid layer of Earth which consists of the crust and uppermost mantle is called the __ lithosphere__________. 5. Which of the major subdivisions of Earth's interior is thought to be liquid? ____outer core________. 6. When the giant ice sheets in the northern hemisphere melted after the last ice age, the Earth's crust ____rebounded____ because a large weight was removed. Name _______________________________ GG 101 Exam 2 Page 2 7. The process described in question 6 is an example of ___isostasy____. 8. Earth's dense core is thought to consist predominantly of ____iron________. 9. The island of Hawaii experiences volcanism because it is located above a(n) ___hot spot_________. 10. The Himalaya Mountains were caused by ___collision__ between ___India__________ and Asia. 11. ___Folds____ are the most common ductile response to stress on rocks in the earth’s crust. 12. ___Faults___ are the most common brittle response to stress on rocks in the earth’s crust. 13. What types of faults are depicted in the cross section shown above? ___thrust_______ faults. Name _______________________________ GG 101 Exam 2 Page 3 14. The structure shown in the above diagram is a(n) ____anticline_____. 15. The name of a fold that occurs in an area of intense deformation where one limb of the fold has been tilted beyond the vertical is called a(n) ____overturned____ fold. -
The Relation Between Mantle Dynamics and Plate Tectonics
The History and Dynamics of Global Plate Motions, GEOPHYSICAL MONOGRAPH 121, M. Richards, R. Gordon and R. van der Hilst, eds., American Geophysical Union, pp5–46, 2000 The Relation Between Mantle Dynamics and Plate Tectonics: A Primer David Bercovici , Yanick Ricard Laboratoire des Sciences de la Terre, Ecole Normale Superieure´ de Lyon, France Mark A. Richards Department of Geology and Geophysics, University of California, Berkeley Abstract. We present an overview of the relation between mantle dynam- ics and plate tectonics, adopting the perspective that the plates are the surface manifestation, i.e., the top thermal boundary layer, of mantle convection. We review how simple convection pertains to plate formation, regarding the aspect ratio of convection cells; the forces that drive convection; and how internal heating and temperature-dependent viscosity affect convection. We examine how well basic convection explains plate tectonics, arguing that basic plate forces, slab pull and ridge push, are convective forces; that sea-floor struc- ture is characteristic of thermal boundary layers; that slab-like downwellings are common in simple convective flow; and that slab and plume fluxes agree with models of internally heated convection. Temperature-dependent vis- cosity, or an internal resistive boundary (e.g., a viscosity jump and/or phase transition at 660km depth) can also lead to large, plate sized convection cells. Finally, we survey the aspects of plate tectonics that are poorly explained by simple convection theory, and the progress being made in accounting for them. We examine non-convective plate forces; dynamic topography; the deviations of seafloor structure from that of a thermal boundary layer; and abrupt plate- motion changes. -
Geothermal Gradient - Wikipedia 1 of 5
Geothermal gradient - Wikipedia 1 of 5 Geothermal gradient Geothermal gradient is the rate of increasing temperature with respect to increasing depth in the Earth's interior. Away from tectonic plate boundaries, it is about 25–30 °C/km (72-87 °F/mi) of depth near the surface in most of the world.[1] Strictly speaking, geo-thermal necessarily refers to the Earth but the concept may be applied to other planets. The Earth's internal heat comes from a combination of residual heat from planetary accretion, heat produced through radioactive decay, latent heat from core crystallization, and possibly heat from other sources. The major heat-producing isotopes in the Earth are potassium-40, uranium-238, uranium-235, and thorium-232.[2] At the center of the planet, the temperature may be up to 7,000 K and the pressure could reach 360 GPa (3.6 million atm).[3] Because much of the heat is provided by radioactive decay, scientists believe that early in Earth history, before isotopes with short half- lives had been depleted, Earth's heat production would have been much Temperature profile of the inner Earth, higher. Heat production was twice that of present-day at approximately schematic view (estimated). 3 billion years ago,[4] resulting in larger temperature gradients within the Earth, larger rates of mantle convection and plate tectonics, allowing the production of igneous rocks such as komatiites that are no longer formed.[5] Contents Heat sources Heat flow Direct application Variations See also References Heat sources Temperature within the Earth -
Mantle Convection in Terrestrial Planets
MANTLE CONVECTION IN TERRESTRIAL PLANETS Elvira Mulyukova & David Bercovici Department of Geology & Geophysics Yale University New Haven, Connecticut 06520-8109, USA E-mail: [email protected] May 15, 2019 Summary surfaces do not participate in convective circu- lation, they deform in response to the underly- All the rocky planets in our Solar System, in- ing mantle currents, forming geological features cluding the Earth, initially formed much hot- such as coronae, volcanic lava flows and wrin- ter than their surroundings and have since been kle ridges. Moreover, the exchange of mate- cooling to space for billions of years. The result- rial between the interior and surface, for exam- ing heat released from planetary interiors pow- ple through melting and volcanism, is a conse- ers convective flow in the mantle. The man- quence of mantle circulation, and continuously tle is often the most voluminous and/or stiffest modifies the composition of the mantle and the part of a planet, and therefore acts as the bottle- overlying crust. Mantle convection governs the neck for heat transport, thus dictating the rate at geological activity and the thermal and chemical which a planet cools. Mantle flow drives geo- evolution of terrestrial planets, and understand- logical activity that modifies planetary surfaces ing the physical processes of convection helps through processes such as volcanism, orogene- us reconstruct histories of planets over billions sis, and rifting. On Earth, the major convective of years after their formation. currents in the mantle are identified as hot up- wellings like mantle plumes, cold sinking slabs and the motion of tectonic plates at the surface. -
Greeting Fellow Naturalists. As of This Writing, We Have Come Back To
Hawk Watch Team by John Wright Galveston Bay Area Chapter - Texas Master Naturalists June 2018 Table of Contents President’s Corner by George Kyame, President 2018 Wetland Wanderings 2 Prairie Ponderings 2 Greeting Fellow Naturalists. Dire Diseases in 3 As of this writing, we have come back to reality after an interesting spring. The mercury Deer, Part 2 finally hit 90, and won't be changing soon. Of course this means we must properly AT: iNaturalist 4 prepare for all of our outdoor stewardship. Please remember the big three: hydration, AT: Gems of the Gulf 5 sun protective clothing, and SPF 30 and above. A cooler beginning to 2018 was nice, although it was accompanied by a rather rainy season, which brings me to my next Heritage Book Study - 6 point. Review The Big Picture - 6 Ah, Beach and Bay. Last year's record attendance would be hard to beat even without Ocean Worlds and the wind and rain that was visited upon us! Impressive was the number of attendees Our World’s Oceans that did come out, and, with our dedicated volunteers, braved the elements! Alas, we Another Botany 8 shut down a little early, but not before our participants got some extra hands-on Question attention. Thank you all for the hard work. AT: The Big Thicket 8 The City Nature Challenge wrapped up 96 hours of species observation on April 30. So 2018 Class Fun and 10 how did the Houston Metro fare? In the Most Species category (my favorite), Houston Adventures placed 2nd. We were 1st last year. -
SPECULOOS Search for Habitable Planets Eclipsing Ultra-Cool Stars
SPECULOOS Search for habitable Planets EClipsing ULtra-cOOl Stars M. Gillon ([email protected]), E. Jehin, L. Delrez, P. Magain, C. Opitom, S. Sohy Department of Astrophysics, Geophysics and Oceanography (AGO), University of Liège, Belgium Transiting planets: treasures in the sky TRAPPIST/UCDTS : the prototype Among the hundreds of planets detected outside our solar system, the ones No existing transit survey is optimized for detecting Earth-size planets transiting the that transit their parent star are genuine Rosetta Stones for the study of nearest ultra-cool stars. Extensive simulations show us that robotic 1m-class exoplanets, because they can be studied in greatest detail. Indeed, their orbital telescopes equipped with modern CCD cameras highly sensitive in near-IR, operating parameters, mass and radius can be precisely measured, and their atmosphere from an exquisite astronomical site, and monitoring individually nearby ultra-cool can be probed during and outside eclipses, bringing strong constraints on their stars, should be able to probe eficiently their habitable zone for terrestrial planets. actual nature (Winn 2010). Within the last two decades, more than three hundred transiting exoplanets have been detected. This large harvest includes many gas giants, but also a steeply growing fraction of terrestrial planets. In parallel to this galore of detections, many projects aiming to characterize giant exoplanets have been successful, bringing notably a Eirst glimpse at their atmospheric properties (Seager & Deming 2010). Fig. 3. Actual TRAPPIST/UCDTS light curves for three ultra-cool stars, aer injecBon of a fake transit of an habitable Earth-size planet. The best-fit transit models are overimposed in red. -
Présentation Powerpoint
Hunting for habitable exoplanets around the nearest very-low-mass stars Michaël Gillon (University of Liège, Belgium) CERN– 17 Jan 2019 Is our blue world unique? Credit: NASA Earth: a rocky planet hosting a complex surface biosphere Credit: NASA Earth: a rocky planet with surface liquid water « Habitable » planet Credits: Howard Perlman, USGS The « habitable zone » of the Sun Credits: NASA No little green men on Mars Credits: NASA We must search beyond our solar system Credits: Ryan Sullivan 1995: beginning of the exoplanet era A giant planet in very short orbit around a Sun-like star Didier Queloz Michel Mayor The exoplanet revolution 51 Peg b 9 Planets everywhere Credits: ESO/M. Kornmesser The diversity of planetary systems Compact Hot Jupiters systems Very eccentric Free-floating orbits planets Credits: NASA/JPL-Caltech; Northwestern University; SETI Institute 11 A few dozen possible biospheres A few dozen BILLIONS in the whole Milky Way! 12 A few exoplanets have been imaged Spectroscopy of terrestrial planets Best spectral range for the detection of molecules is infrared Infrared spectroscopy of potentially habitable exoplanets Spectroscopy of exoplanets Imaging planets around other stars Imaging planets around other stars Planetary transit Transit of exoplanet Credits: Deeg & Garrido Atmospheric study of a transiting exoplanet Credits: C. Daniloff/MIT, J. de Wit 20 Atmospheric study of a transiting exoplanet Credits: E. Sedaghati et al. 2018 21 Atmospheric study of a transiting exoplanet Credits: NASA/JPL 22 Atmospheric study of a transiting exoplanet Credits: Grillmair et al. 2008 23 The smaller the star, the better Low-mass stars are small and cold Credits: ESO The habitable zone of hot and cold stars Credits: NASA 26 Most stars are smaller and colder than the Sun 27 Search for habitable Planets EClipsing ULtra-cOOl Stars Search for habitable Planets EClipsing ULtra-cOOl Stars What are « ultra-cool stars »? Ultracool dwarfs: Teff < 2700K, (Kirckpatrick erSun al. -
SPECULOOS: Ultracool Dwarf Transit Survey Target List and Strategy?
A&A 645, A100 (2021) Astronomy https://doi.org/10.1051/0004-6361/202038827 & c ESO 2021 Astrophysics SPECULOOS: Ultracool dwarf transit survey Target list and strategy? D. Sebastian1, M. Gillon1, E. Ducrot1, F. J. Pozuelos1,3, L. J. Garcia1, M. N. Günther4, L. Delrez1,3,5 , D. Queloz2, B. O. Demory6, A. H. M. J. Triaud7, A. Burgasser8, J. de Wit4, A. Burdanov4, G. Dransfield7, E. Jehin3, J. McCormac9, C. A. Murray2, P. Niraula4, P. P. Pedersen2, B. V. Rackham4, S. Sohy3, S. Thompson2, and V. Van Grootel3 1 Astrobiology Research Unit, University of Liège, Allée du 6 Août, 19, 4000 Liège, Sart-Tilman, Belgium e-mail: [email protected] 2 Cavendish Laboratory, JJ Thomson Avenue, Cambridge CB3 0HE, UK 3 Space Sciences, Technologies and Astrophysics Research (STAR) Institute, Université de Liège, Allée du 6 Août 19C, 4000 Liège, Belgium 4 Department of Earth, Atmospheric and Planetary Sciences, MIT, 77 Massachusetts Avenue, Cambridge, MA 02139, USA 5 Observatoire de l’Université de Genéve, Chemin des Maillettes 51, Versoix 1290, Switzerland 6 University of Bern, Center for Space and Habitability, Gesellschaftsstrasse 6, 3012 Bern, Switzerland 7 School of Physics & Astronomy, University of Birmingham, Edgbaston, Birmingham B15 2TT, UK 8 University of California San Diego, 9500 Gilman Drive, La Jolla, CA 92093, USA 9 Department of Physics, University of Warwick, Coventry CV4 7AL, UK Received 2 July 2020 / Accepted 27 October 2020 ABSTRACT Context. One of the most promising avenues for the detailed study of temperate Earth-sized exoplanets is the detection of such planets in transit in front of stars that are small and near enough to make it possible to carry out a thorough atmospheric characterisation with next-generation telescopes, such as the James Webb Space telescope (JWST) or Extremely Large Telescope (ELT). -
Activity Induced Variation in Spin-Orbit Angles As Derived from Rossiter-Mclaughlin Measurements? M
Astronomy & Astrophysics manuscript no. RM-VARIATION-ARXIV c ESO 2018 September 5, 2018 Activity induced variation in spin-orbit angles as derived from Rossiter-McLaughlin measurements? M. Oshagh1;2, A. H. M. J. Triaud3, A. Burdanov4, P. Figueira2;5, A. Reiners1, N. C. Santos2;6, J. Faria2, G. Boue7, R. F. D´ıaz8;9, S. Dreizler1, S. Boldt1, L. Delrez10, E. Ducrot4, M. Gillon4, A. Guzman Mesa1, E. Jehin4, S. Khalafinejad11;12, S. Kohl11, L. Serrano2, S. Udry13 1 Institut f¨urAstrophysik, Georg-August Universit¨atG¨ottingen,Friedrich-Hund-Platz 1, 37077 G¨ottingen,Germany 2 Instituto de Astrof´ısicae Ci^enciasdo Espa¸co,Universidade do Porto, CAUP, Rua das Estrelas, PT4150-762 Porto, Portugal 3 University of Birmingham, Edgbaston, Birmingham, B15 2TT, UK 4 Space sciences, Technologies and Astrophysics Research (STAR) Institute, Universit´ede Li`ege, All´eedu 6 Ao^ut17, Bat. B5C, 4000 Li`ege,Belgium 5 European Southern Observatory, Alonso de Cordova 3107, Vitacura Casilla 19001, Santiago 19, Chile 6 Departamento de F´ısicae Astronomia, Faculdade de Ci^encias,Universidade do Porto,Rua do Campo Alegre, 4169- 007 Porto, Portugal 7 IMCCE, Observatoire de Paris, UPMC Univ. Paris 6, PSL Research University, Paris, France 8 Universidad de Buenos Aires, Facultad de Ciencias Exactas y Naturales, Buenos Aires, 1428, Argentina 9 CONICET - Universidad de Buenos Aires, Instituto de Astronoma y F´ısicadel Espacio (IAFE), Buenos Aires, 1428, Argentina 10 Astrophysics Group, Cavendish Laboratory, J. J. Thomson Avenue, Cambridge, CB3 0HE, UK 11 Hamburg Observatory, Hamburg University, Gojenbergsweg 112, 21029, Hamburg, Germany 12 Max Planck Institute for Astronomy, K¨onigstuhl17, 69117 Heidelberg, Germany 13 Observatoire de Gen`eve, Universit´ede Gen`eve, 51 chemin des Maillettes, 1290 Versoix, Switzerland Received XXX; accepted XXX ABSTRACT One of the most powerful methods used to estimate sky-projected spin-orbit angles of exoplanetary systems is through a spectroscopic transit observation known as the RossiterMcLaughlin (RM) effect. -
Geodynamic Modelling Using Ellipsis
GEOS3104-3804: GEOPHYSICAL METHODS Geodynamic modelling using Ellipsis Patrice F. Rey GEOS-3104 Computational Geodynamics Computational tectonics/geodynamics provides a robust plat- form for hypotheses testing and exploring coupled tectonic and geodynamic processes. It delivers the unexpected by re- vealing previously unknown behaviors. 1 SECTION 1 The rise of computer science During the mid-19th century, the laws of thermody- tle convection, and plate tectonic processes which also namics - which describe the relation between heat and involves the flow - brittle or ductile - of rocks. 21st cen- forces between contiguous bodies - and fluid dynam- tury computers have now the capability to compute in ics - which describes the flow of fluids in relation to four dimensions the flow of complex fluid with com- pressure gradients - reached maturity. Both theories plex rheologies and contrasting physical properties we underpin our understanding of many natural proc- typically encounter on Earth. For geosciences, this is a esses from atmospheric and oceanic circulation, man- significant shift. 2 Computational tectonics and geodynamics: There is a revolution Navier-Stokes equations: Written in Georges G. Stokes (1819-1903) unfolding at the moment in all corners of science, engineering, and the 1850’s, the Navier-Stokes equations other disciplines like economy and social sciences. This revolution are the set of differential equations that is driven by the growing availability of increasingly powerful describe the motion of fluid and associ- high-performance computers (HPC), and the growing availability ated heat exchanges. They relate veloc- of free global datasets and open source data processing tools (Py- ity gradients to pressure gradients and thon, R, Paraview, QGIS-GRASS, etc).