Simulations of stars and gas in spiral galaxies

A new code, DUAL, is developed to model the 2D dynamics of stars and gas in spiral galaxies. DUAL combines grid-based hydrodynamics and N-body techniques. A triaxial model of the bulge of M31 is constructed from its surface brightness profile and shown, using hydrodynamic simulations, to reproduce o...

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Main Author: Berman, Simon Lewis
Published: University of Oxford 2002
Subjects:
520
Online Access:http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.393426
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spelling ndltd-bl.uk-oai-ethos.bl.uk-3934262018-02-06T03:13:32ZSimulations of stars and gas in spiral galaxiesBerman, Simon Lewis2002A new code, DUAL, is developed to model the 2D dynamics of stars and gas in spiral galaxies. DUAL combines grid-based hydrodynamics and N-body techniques. A triaxial model of the bulge of M31 is constructed from its surface brightness profile and shown, using hydrodynamic simulations, to reproduce observations of molecular gas kinemat- ics along the line of nodes of the disk. The bulge model rotates fast, with a pattern speed of 54 km s<sup>-1</sup> kpc<sup>-1</sup>, and a ratio of bulge semi-major axis to corotation radius ℛ = 1.2. The B band mass-to-light ratio is 6.5, the semi-major axis is 3.5 kpc, the bulge mass is 2.3 x 10<sup>10</sup> M<sub>☉</sub> and the angle between the projected minor axis of the bulge and the line of nodes of the disk is 15°. A thick gas disk (HWHM of 200 → 500 pc) is added to account for CO observations parallel to the disk line of nodes. The thickness is minimized if the gas velocity drops by 20% per kpc above the plane. By combining reasonable values of the disk mass-to-light ratio or dynamical friction arguments with the bulge model, M31 is shown to have a maximal disk with a halo mass fraction within 3.5 kpc of just a few percent. In contrast, the Cold Dark Matter theory predicts a fraction of 22% to 30%. The differences between optical and infrared morphologies of spiral galaxies are reproduced using hydrodynamic and N-body simulations of gas and stars. Gaseous spirals have tighter pitch angles than stellar spirals. This phenomenon is attributed to a phase shift between the stellar density and the potential. Gaseous images are more asymmetric, less smooth and more likely to have multiple arms. Morphological decoupling increases as the stellar arm-interarm contrast and Q parameter fall. The flocculence of a galaxy is quantified by decomposing the galaxy images into logarithmic spirals and denning a parameter closely related to the uniformity of the resulting 2D Fourier spectrum. I conclude that a significant amount of morphological decoupling in spiral galaxies is due to the difference in the dynamics of stars and gas, rather than dust, star formation or galaxy interactions.520University of Oxfordhttp://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.393426https://ora.ox.ac.uk/objects/uuid:a368de23-cc46-4726-9903-1b0b72923953Electronic Thesis or Dissertation
collection NDLTD
sources NDLTD
topic 520
spellingShingle 520
Berman, Simon Lewis
Simulations of stars and gas in spiral galaxies
description A new code, DUAL, is developed to model the 2D dynamics of stars and gas in spiral galaxies. DUAL combines grid-based hydrodynamics and N-body techniques. A triaxial model of the bulge of M31 is constructed from its surface brightness profile and shown, using hydrodynamic simulations, to reproduce observations of molecular gas kinemat- ics along the line of nodes of the disk. The bulge model rotates fast, with a pattern speed of 54 km s<sup>-1</sup> kpc<sup>-1</sup>, and a ratio of bulge semi-major axis to corotation radius ℛ = 1.2. The B band mass-to-light ratio is 6.5, the semi-major axis is 3.5 kpc, the bulge mass is 2.3 x 10<sup>10</sup> M<sub>☉</sub> and the angle between the projected minor axis of the bulge and the line of nodes of the disk is 15°. A thick gas disk (HWHM of 200 → 500 pc) is added to account for CO observations parallel to the disk line of nodes. The thickness is minimized if the gas velocity drops by 20% per kpc above the plane. By combining reasonable values of the disk mass-to-light ratio or dynamical friction arguments with the bulge model, M31 is shown to have a maximal disk with a halo mass fraction within 3.5 kpc of just a few percent. In contrast, the Cold Dark Matter theory predicts a fraction of 22% to 30%. The differences between optical and infrared morphologies of spiral galaxies are reproduced using hydrodynamic and N-body simulations of gas and stars. Gaseous spirals have tighter pitch angles than stellar spirals. This phenomenon is attributed to a phase shift between the stellar density and the potential. Gaseous images are more asymmetric, less smooth and more likely to have multiple arms. Morphological decoupling increases as the stellar arm-interarm contrast and Q parameter fall. The flocculence of a galaxy is quantified by decomposing the galaxy images into logarithmic spirals and denning a parameter closely related to the uniformity of the resulting 2D Fourier spectrum. I conclude that a significant amount of morphological decoupling in spiral galaxies is due to the difference in the dynamics of stars and gas, rather than dust, star formation or galaxy interactions.
author Berman, Simon Lewis
author_facet Berman, Simon Lewis
author_sort Berman, Simon Lewis
title Simulations of stars and gas in spiral galaxies
title_short Simulations of stars and gas in spiral galaxies
title_full Simulations of stars and gas in spiral galaxies
title_fullStr Simulations of stars and gas in spiral galaxies
title_full_unstemmed Simulations of stars and gas in spiral galaxies
title_sort simulations of stars and gas in spiral galaxies
publisher University of Oxford
publishDate 2002
url http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.393426
work_keys_str_mv AT bermansimonlewis simulationsofstarsandgasinspiralgalaxies
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