Publication detail
Multi-Wavelength Eclipse Observations of a Quiescent Prominence Multi-Wavelength Eclipse Observations of a Quiescent Prominence Multi-Wavelength Eclipse Observations of a Quiescent Prominence
JEJCIC, S. PETR HEINZEL, P. ZAPIOR, M. DRUCKMÜLLER, M. STANISLAV, G. KOTRČ, P.
Czech title
Multi-Wavelength Eclipse Observations of a Quiescent Prominence
English title
Multi-Wavelength Eclipse Observations of a Quiescent Prominence Multi-Wavelength Eclipse Observations of a Quiescent Prominence Multi-Wavelength Eclipse Observations of a Quiescent Prominence
Type
journal article in Web of Science
Language
en
Original abstract
We construct the maps of temperatures, geometrical thicknesses, electron densities and gas pressures in a quiescent prominence. For this we use the RGB signal of the prominence visible-light emission detected during the total solar eclipse of 1 August 2008 in Mongolia and quasi-simultaneous H alpha spectra taken at OndA (TM) ejov Observatory. The method of disentangling the electron density and geometrical (effective) thickness was described by Jeji and Heinzel (Solar Phys. 254, 89 -aEuro parts per thousand 100, 2009) and is used here for the first time to analyse the spatial variations of prominence parameters. For the studied prominence we obtained the following range of parameters: temperature 6000 -aEuro parts per thousand 15 000 K, effective thickness 200 -aEuro parts per thousand 15000 km, electron density 5x10(9) -aEuro parts per thousand 10(11) cm(-3) and gas pressure 0.02 -aEuro parts per thousand 0.2 dyn cm(-2) (assuming a fixed ionisation degree n (p)/n (H)=0.5). The electron density increases towards the bottom of the prominence, which we explain by an enhanced photoionisation due to the incident solar radiation. To confirm this, we construct a two-dimensional radiative-transfer model with realistic prominence illumination.
Czech abstract
We construct the maps of temperatures, geometrical thicknesses, electron densities and gas pressures in a quiescent prominence. For this we use the RGB signal of the prominence visible-light emission detected during the total solar eclipse of 1 August 2008 in Mongolia and quasi-simultaneous H alpha spectra taken at OndA (TM) ejov Observatory. The method of disentangling the electron density and geometrical (effective) thickness was described by Jeji and Heinzel (Solar Phys. 254, 89 -aEuro parts per thousand 100, 2009) and is used here for the first time to analyse the spatial variations of prominence parameters. For the studied prominence we obtained the following range of parameters: temperature 6000 -aEuro parts per thousand 15 000 K, effective thickness 200 -aEuro parts per thousand 15000 km, electron density 5x10(9) -aEuro parts per thousand 10(11) cm(-3) and gas pressure 0.02 -aEuro parts per thousand 0.2 dyn cm(-2) (assuming a fixed ionisation degree n (p)/n (H)=0.5). The electron density increases towards the bottom of the prominence, which we explain by an enhanced photoionisation due to the incident solar radiation. To confirm this, we construct a two-dimensional radiative-transfer model with realistic prominence illumination.
English abstract
We construct the maps of temperatures, geometrical thicknesses, electron densities and gas pressures in a quiescent prominence. For this we use the RGB signal of the prominence visible-light emission detected during the total solar eclipse of 1 August 2008 in Mongolia and quasi-simultaneous H alpha spectra taken at OndA (TM) ejov Observatory. The method of disentangling the electron density and geometrical (effective) thickness was described by Jeji and Heinzel (Solar Phys. 254, 89 -aEuro parts per thousand 100, 2009) and is used here for the first time to analyse the spatial variations of prominence parameters. For the studied prominence we obtained the following range of parameters: temperature 6000 -aEuro parts per thousand 15 000 K, effective thickness 200 -aEuro parts per thousand 15000 km, electron density 5x10(9) -aEuro parts per thousand 10(11) cm(-3) and gas pressure 0.02 -aEuro parts per thousand 0.2 dyn cm(-2) (assuming a fixed ionisation degree n (p)/n (H)=0.5). The electron density increases towards the bottom of the prominence, which we explain by an enhanced photoionisation due to the incident solar radiation. To confirm this, we construct a two-dimensional radiative-transfer model with realistic prominence illumination.
Keywords in Czech
Eclipse observations, Prominences, quiescent, Spectral line, intensity and diagnostics
Keywords in English
Sun, prominence
RIV year
2014
Released
01.07.2014
ISSN
0038-0938
Volume
2014 (289)
Number
7
Pages from–to
2487–2501
Pages count
14
BIBTEX
@article{BUT107604,
author="Sonja {Jejcic} and Petr {Heinzel} and Maciej {Zapior} and Miloslav {Druckmüller} and Gunár {Stanislav} and Pavel {Kotrč},
title="Multi-Wavelength Eclipse Observations of a Quiescent Prominence Multi-Wavelength Eclipse Observations of a Quiescent Prominence Multi-Wavelength Eclipse Observations of a Quiescent Prominence",
year="2014",
volume="2014 (289)",
number="7",
month="July",
pages="2487--2501",
issn="0038-0938"
}