Survey
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
QuickTime™ and a TIFF (Uncompressed) decompressor are needed to see this picture. Discovering the Complexity of Supernovae through 3D Simulations John M. Blondin NC State University AAS/AAPT January 9, 2007 QuickTime™ and a TIFF (Uncompressed) decompressor are needed to see this picture. AAS/AAPT January 9, 2007 We begin our story in 1572… ``On the 11th day of November in the evening after sunset, I was contemplating the stars in a clear sky. I noticed that a new and unusual star, surpassing the other stars in brilliancy, was shining almost directly above my head.’’ -- Tycho Brahe AAS/AAPT January 9, 2007 Again in 1604… Johannes Kepler observed a “stella nova” that became as bright as Jupiter, but faded away after a couple months. AAS/AAPT January 9, 2007 For 400 years there has not been a supernova in our Galaxy … we are still waiting! But, in a nearby galaxy not long ago (February 1987)… AAS/AAPT January 9, 2007 We can learn even more by looking at what is left hundreds of years later. AAS/AAPT January 9, 2007 Remnants of Supernova Explosions Relic Blastwave AAS/AAPT Spinning Neutron Star January 9, 2007 The iron core contains about 3 times the mass of our Sun, but it is roughly the size of our Earth. This iron core collapses under its own weight until it is small enough to fit inside Puget Sound. At this point the core is as dense as the nucleus of an atom and it cannot compress any further. The rest of the star ‘bounces’ off this hard core and explodes off into space??? AAS/AAPT January 9, 2007 It all starts with core collapse… AAS/AAPT January 9, 2007 The Supernova story has a long history of computational physics… • 1966 Colgate and White Neutrino-Driven prompt explosion • 1985 Bethe and Wilson Shock reheating via neutrino energy deposition • 1992 Herant, Benz, and Colgate Convective instability above neutrino-sphere AAS/AAPT January 9, 2007 The last decade has seen a great deal of interest in multidimensional effects: Convection with the protoneutron star Neutrino-driven convection below the stalled shock Instability of the stalled shock All of these may operate together! AAS/AAPT January 9, 2007 First generation of 2D SN models hinted at a low-order asymmetry in the shock wave at late times (100’s of msec after bounce). Burrows, Hayes & Fryxell 1995 AAS/AAPT January 9, 2007 REU Students, Summer 2000 Christine DeMarino Brett Unks Dana Paquin AAS/AAPT January 9, 2007 To investigate the dynamics of the stalled supernova shock, we consider an idealized problem: QuickTime™ and a TIFF (Uncompressed) decompressor are needed to see this picture. AAS/AAPT January 9, 2007 In One Dimension: Analytical: Houck & Chevalier (1992) presented a linear stability analysis. Numerical: Blondin et al. (2003) perturb SAS and watch the evolution. Radius Pressure Perturbation QuickTime™ and a TIFF (Uncompressed) decompressor are needed to see this picture. Time -> AAS/AAPT January 9, 2007 SN Code Verification Houck and Chevalier 1992 Blondin and Mezzacappa 2005 This post-bounce model provides an opportunity to verify supernova codes against the results of a linear perturbation analysis. AAS/AAPT January 9, 2007 Spherical Accretion Shock Instability Blondin, Mezzacappa, DeMarino 2003, ApJ, 584, 971 QuickTime™ and a YUV420 codec decompressor are needed to see this picture. AAS/AAPT January 9, 2007 The SASI is a global acoustic mode: The spherical accretion shock acts as an acoustic cavity, with a trapped standing wave growing exponentially with time. AAS/AAPT January 9, 2007 QuickTime™ and a YUV420 codec decompressor are needed to see this picture. AAS/AAPT January 9, 2007 Must move to 3D! This initial SASI discovery with axisymmetric 2D simulations pointed to the obvious need for models in full 3D. AAS/AAPT January 9, 2007 Hurdles for Large-Scale 3D Simulation code Not a problem Floating points Thank you DOE Data output It works Data transport Does not work Visualization and analysis I can’t see! AAS/AAPT January 9, 2007 First Results: SASI Exists in 3D • 3D Cartesian grid • 100 Million zones • 100’s of processors QuickTime™ and a TIFF (Uncompressed) decompressor are needed to see this picture. • 100’s of GB in full run Without interactive access to the data, this was science in the dark! AAS/AAPT January 9, 2007 Science Begins with Data Scientific discovery is done with interactive access to data. • • • Must have interactive access on a large-memory computer for analysis and visualization. Must have high bandwidth in accessing the data. Must have sufficient storage to hold data for weeks/months. AAS/AAPT Shared file system Cray X1 Billion-cell simulation in 30 hours generates 4 terabytes Visualization platform January 9, 2007 Interactive Visualization of TB Datasets QuickT ime ™an d a TIFF ( Uncomp res sed) deco mpre ssor ar e need ed to see this pictur e. A commodity linux cluster provides all the ‘must haves.’ Data is sliced into slabs and stored on local disks on the cluster nodes. EnSight Gold provides an easy visualization solution, including remote client-server operation and collaboration. AAS/AAPT January 9, 2007 QuickTime™ and a Animation decompressor are needed to see this picture. AAS/AAPT January 9, 2007 QuickTime™ and a Video decompressor are needed to see this picture. AAS/AAPT January 9, 2007 QuickTime™ and a Video decompressor are needed to see this picture. AAS/AAPT January 9, 2007 QuickTime™ and a Video decompressor are needed to see this picture. AAS/AAPT January 9, 2007 AAS/AAPT January 9, 2007 QuickTime™ and a Video decompressor are needed to see this picture. AAS/AAPT January 9, 2007 QuickTime™ and a YUV420 codec decompressor are needed to see this picture. AAS/AAPT January 9, 2007 AAS/AAPT January 9, 2007 AAS/AAPT January 9, 2007 AAS/AAPT January 9, 2007 QuickTime™ and a Microsoft Video 1 decompressor are needed to see this picture. AAS/AAPT January 9, 2007 SASI A non-rotating, spherically symmetric progenitor star can leave behind a neutron star spinning with a period of tens of milliseconds. AAS/AAPT January 9, 2007 A Million Second Chandra View of Cassiopeia A Hwang et. al. 2004 “These are most likely due to jets of ejecta as opposed to cavities in the circumstellar medium, since we can reject simple models for the latter.” AAS/AAPT January 9, 2007 If the progenitor star possessed an asymmetric stellar wind (e.g., due to rotation), the supernova remnant driven into this relic wind would reflect the asymmetry of the wind. In this 2D simulation, the density in the progenitor wind is four times denser in the equatorial plane than at the poles. AAS/AAPT Forward shock Reverse shock January 9, 2007 QuickTime™ and a Video decompressor are needed to see this picture. AAS/AAPT January 9, 2007 Never believe a jet in 2D… equator pole q equator AAS/AAPT radius January 9, 2007 QuickTime™ and a Video decompressor are needed to see this picture. AAS/AAPT January 9, 2007 A “Jet” from a Spherical Supernova Shocked Ejecta Fast Ejecta Leading Shockwave AAS/AAPT January 9, 2007