Modelling of 2D radiative transfer in quiescent prominences

Slides:



Advertisements
Similar presentations
Estimate of physical parameters of molecular clouds Observables: T MB (or F ν ), ν, Ω S Unknowns: V, T K, N X, M H 2, n H 2 –V velocity field –T K kinetic.
Advertisements

Determination of 3D structure, avg density, total mass and plasma properties of an EUV filament observed by SoHO/CDS, SoHO/SUMER and VTT/MSDP Pavol Schwartz.
EXAMPLE DATA: Beam: K - ; E = 4,2 GeV ; m K =m p /2 Target: Hydrogen atoms; R nucleus =10 -5 R atom me = mp/2000.
1 Plasma flows during solar flares A. Berlicki Observatoire de Paris, Section de Meudon, LESIA (Astronomical Institute of the Wrocław University, Poland)
Stability of MHD Buoyancy Driven Flows Presented by Naveen Vetcha (UCLA) With contribution from: Sergey Smolentsev (UCLA) Rene Moreau (Prof., Lab. EPM,
Dynamics of a Continuous Model for Flocking Ed Ott in collaboration with Tom Antonsen Parvez Guzdar Nicholas Mecholsky.
A Relativistic Magnetohydrodynamic (RMHD) Code Based on an Upwind Scheme Hanbyul Jang, Dongsu Ryu Chungnam National University, Korea HEDLA 2012 April.
Microphysics of the radiative transfer. Numerical integration of RT in a simplest case Local Thermodynamical Equilibrium (LTE, all microprocesses are.
Solar Radiation Physical Modeling (SRPM) J. Fontenla June 30, 2005a.
PCTR Physics and “Chewy Nougats*” SSL, UC Berkeley * This nomenclature due either to Greg Slater or Sam Freeland, SXT data pioneers (most likely Greg)
Observational Evidence for Cross-field Diffusion of Neutral Filament Material Holly Gilbert & Gary Kilper Rice University 10/29/07.
Transformation of MHD waves in sunspots and simulation of HMI level1 data Konstantin Parchevsky, Sebastien Couvidat, Richard Wachter, Alexander Kosovichev.
Superhot DEM (or DF?) RHESSI continuum with TRACE or EIT FeXXIV, SUMER FeXXI, GOES, or whatever.
Interstellar Turbulence and hierarchical structuring Nicolas Décamp (Univ. della Calabria) Jacques Le Bourlot (Obs. de Paris)
An Enthalpy Based Scheme for Simulating Dendritic Growth V.R. Voller 4d o (blue) 3.25d o (black) 2.5d o (red) Dendrite shape with 3 grid sizes shows reasonable.
Antennas Hertzian Dipole –Current Density –Vector Magnetic Potential –Electric and Magnetic Fields –Antenna Characteristics.
MHD Modeling of the Large Scale Solar Corona & Progress Toward Coupling with the Heliospheric Model.
Stellar Atmospheres: Solution Strategies 1 Solution Strategies.
Coronal Heating of an Active Region Observed by XRT on May 5, 2010 A Look at Quasi-static vs Alfven Wave Heating of Coronal Loops Amanda Persichetti Aad.
Modeling of Two-Phase Flow in RH Vacuum Degassing Vessel With the Effect of Rotating Magnetic field Baokuan Li Northeastern University, China Fumitaka.
Turbulent AU Structures Revealed by H 2 O and CH 3 OH Masers V. Strelnitski Maria Mitchell Observatory In collaboration with: J. Alexander, S. Gezari,
Evolution of the 2012 July 12 CME from the Sun to the Earth: Data- Constrained Three-Dimensional MHD Simulations F. Shen 1, C. Shen 2, J. Zhang 3, P. Hess.
Galaxy Evolution in the Virgo Cluster Bernd Vollmer CDS, Observatoire de Strasbourg, France In collaboration with: P. Amram, C. Balkowski, R. Beck, A.
Title: SHAPE OPTIMIZATION OF AXISYMMETRIC CAVITATOR IN PARTIALY CAVITATING FLOW Department of Mechanical Engineering Ferdowsi University of Mashhad Presented.
Max-Planck-Institut für Plasmaphysik, EURATOM Association Different numerical approaches to 3D transport modelling of fusion devices Alexander Kalentyev.
M. Onofri, F. Malara, P. Veltri Compressible magnetohydrodynamics simulations of the RFP with anisotropic thermal conductivity Dipartimento di Fisica,
A multiline LTE inversion using PCA Marian Martínez González.
On the Structure of Magnetic Field and Radioemission of Sunspot-related Source in Solar Active Region T. I. Kaltman, V. M. Bogod St. Petersburg branch.
Emission measure distribution in loops impulsively heated at the footpoints Paola Testa, Giovanni Peres, Fabio Reale Universita’ di Palermo Solar Coronal.
Photospheric MHD simulation of solar pores Robert Cameron Alexander Vögler Vasily Zakharov Manfred Schüssler Max-Planck-Institut für Sonnensystemforschung.
FREE CONVECTION 7.1 Introduction Solar collectors Pipes Ducts Electronic packages Walls and windows 7.2 Features and Parameters of Free Convection (1)
Acoustic wave propagation in the solar subphotosphere S. Shelyag, R. Erdélyi, M.J. Thompson Solar Physics and upper Atmosphere Research Group, Department.
Constant magnetic field LL2 section 43. Electrons in atoms and circuits all perform finite motion. This creates magnetic fields that are constant when.
Organization and Evolution of Solar Magnetic Field Serena Criscuoli INAF,OAR In Collaboration with Ilaria Ermolli, Mauro Centrone, Fabrizio Giorgi and.
Ergodic heat transport analysis in non-aligned coordinate systems S. Günter, K. Lackner, Q. Yu IPP Garching Problems with non-aligned coordinates? Description.
Formulations of Longitudinal Dispersion Coefficient A Review:
Measurement of magnetic field by Hanle effect in Na I D 2 T. Anan (Kyoto univ.) 1, review of Holzreuter et al , Hanle effect of Na D2.
Saturn Magnetosphere Plasma Model J. Yoshii, D. Shemansky, X. Liu SET-PSSD 06/26/11.
Cosmic Fireworks: When Stars Explode Alisha Humphries, Naomi Pequette, Charee Peters Advisor: Dr. Jennifer Hoffman Department of Physics and Astronomy.
Preliminary analysis of a 16 T sc dipole with cos-theta lay-out INFN team October 2015.
Magnetic Reconnection in Solar Flares
P.Zacharias1, S. Bingert2 & H. Peter2 1ISSI, Bern, Switzerland
Hertzian Dipole Current Density Vector Magnetic Potential
Numerical Simulations of Solar Magneto-Convection
Date of download: 10/16/2017 Copyright © ASME. All rights reserved.
Lecture Objectives: Review - Heat transfer Convection Conduction
MDI Level 1.8 Magnetograms
Finite difference code for 3D edge modelling
Lecture 3 Radiative Transfer
Master Thesis Lefteris Benos
Non-LTE Models for Hot Stars
Accelerated Lambda Iteration
Radiative Field (Hubeny & Mihalas Chapter 3)
Multi-fluid modeling of ion-neutral interactions in the solar chromosphere with ionization and recombination effects.
Saturn upper atmosphere structure
Numerical Model Atmospheres (Hubeny & Mihalas 16, 17)
Experiment Experiment: thing ferromagnetic films
Observations of Magnetic Waves in the Voyager Data Set Marios Socrates Dimitriadis, Charles Smith Introduction Solar wind consists of highly energetic.
Frictional Heating During an Earthquake
STAAR Review DAY 3 MATTER AND ENERGY TEKS 8.5E (R), 8.5F (S)
Bogdan Rosa1, Marcin Kurowski1, Damian Wójcik1,
Understanding solar flares from optical observations Heinzel, P
PROMINENCES AND EUV FILAMENTS B.Schmieder
P. Heinzel Astronomical Institute, Czech Academy of Sciences
-Short Talk- The soft X-ray characteristics of solar flares, both with and without associated CMEs Kay H.R.M., Harra L.K., Matthews S.A., Culhane J.L.,
PANDA solenoid quench calculations
Comparing the results of 1D and 2D modelling of prominence thread
Time harmonic excitation magnetic field intensity H
Contents Introduction to the inversion code
Presentation transcript:

Modelling of 2D radiative transfer in quiescent prominences

Structure of the presentation Modelling of prominences Grid of models Contribution functions Results and analyses Conclusion

Two dimensional Kippenhahn-Schlüter model

Two dimensional Kippenhahn-Schlüter model

Kuperus-Raadu model

2D radiative transfer equation

Modelling of 2D radiative transfer in quiescent prominences Heasley a Mihalas (1976) – non-LTE model with inclusion of MHS and radiative transfer Mihalas et al. (1978) – the first 2D model Heinzel et al. (1987) – inclusion of PRD Fontenla et al. (1996) – multi-threat model Anzer a Heinzel (1999) – inclusion of PCTR Heinzel a Anzer (2001) – generalisation of MHS for 2D

2D models of the quiescent prominences Motivation – the different orientation of the magnetic field lines towards the observer (Heinzel et al. 2001) Model – 12-level Hydrogen atom – MHS equations of 2D K-S type – numerical solution of radiative transfer by ALI method (Auer and Paletou 1994) with usage of SC (Kunasz and Auer 1988)

Short Characteristics method (SC)

Two-dimensional magnetic dip model

The temperature structure

The magnetic dip The density structure

Grid of models Constant parameters

The geometrical shape of the prominence threats of each model

The dependence of profiles on magnetic field orientation

Contribution functions

Contribution functions – A1 Lb

Conclusion Multi-threat model Inclusion of the velocity field Creation of 3D code Comparison of synthetic profiles with observed profiles on SOHO

Who says that Solar Physics is boring ?