PPT-Shell-pellet injection modeling and runaway electron pitch-angle scattering effects
Author : sherrill-nordquist | Published Date : 2019-02-06
VA Izzo University of California San Diego PB Parks General Atomics E Hirvijoki Princeton Plasma Physics Laboratory 2017 PPPL Workshop Theory and Simulation
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Shell-pellet injection modeling and runaway electron pitch-angle scattering effects: Transcript
VA Izzo University of California San Diego PB Parks General Atomics E Hirvijoki Princeton Plasma Physics Laboratory 2017 PPPL Workshop Theory and Simulation of Disruptions 18 July 2017. Configuration . for Elements Above Atomic # 18. Electron Shells. Periods on the periodic table are similar because they have the same number of electron shells.. Within these shells there are layers called sublevels', a shell can have between 1 and 4 sublevels.. (status report). Solène. . Lejosne. , Forrest . Mozer. and Oleksiy . Agapitov. . SSL, University of California, Berkeley . solene@ssl.berkeley.edu. Special thanks to the HOPE team. SWG Meeting, 29-31 July 2015, APL. 1 domaindomain= any electron pair, or any double or triple bond is = any electron pair, or any double or triple bond is considered one domain.considered one domain.lone pair 2 domains on central a August. . 18. th. , . 201. 5. Carnegie Mellon University, Pittsburgh. MURI Meeting, 2015. Saransh Singh. Marc . De Graef. 2. Outline. Introduction to . Forward Models in Electron . Scattering. Electron . CM34 @ RAL. Timothy Carlisle. 1. Intro.. MICE performance predicted using the cooling formula (. CF. ):. G4MICE . ≠. CF. (see . prev. CMs). Simulation disagrees with C.F by up to 20%.. MS calc. typically approx.: . Electron Shells. Periods on the periodic table are similar because they have the same number of electron shells.. Within these shells there are layers called sublevels', a shell can have between 1 and 4 sublevels.. Mac . Mestayer. , . Jlab. the discovery of the nucleus - “Rutherford scattering”. method: measure scattering rates vs. angle. the discovery of quarks . evidence that the proton is not a ‘point’ particle. JLEIC simulations status April 3 rd , 2017 Y. Roblin Scope of Simulations Intermediate goal is to arrive at what is needed for a good pre-CDR and subsequently CDR Ion Linac (See talk by Sang- hoon Bremsstrahlung, Photo-emission. Compton scattering . bootcamp. 1. Are you ready?. Q16.1. In the photoelectric effect, how can one increase the kinetic energy of an electron coming out the metal surface?. Scattering from Few-Body Nuclei. Mina Katramatou . and Makis Petratos . Kent State University, Ohio, USA. International Conference on New . Frontiers . in Physics. . Where is optical depth of layer. Optical depth is path length required for attenuation to 1/e of original energy. Depends on attenuation coefficients and density. Transmissivity is proportion of original energy remaining:. EPMA, SEM-EDS. ). Warren Straszheim, PhD. EPMA, Ames Lab, 227 Wilhelm. SEM-EDS, MARL, 23 Town Engineering. wesaia@iastate.edu. 515-294-8187. With acknowledgements to John Donovan of the University of Oregon. Arizona State university. Electron-Electron Interactions. Classification of Scattering Mechanisms. Treatment of the Electron-Electron Interactions. Electron-electron interactions can be treated either in:. Four forces in nature. Gravity. Electromagnetic. Weak. Strong . . . Responsible for binding protons and neutrons together to make . nuclei, holds together. quarks . that make protons and neutrons.
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