Sign on

SAO/NASA ADS Astronomy Abstract Service


· Find Similar Abstracts (with default settings below)
· Electronic Refereed Journal Article (HTML)
· Full Refereed Journal Article (PDF/Postscript)
· Full Refereed Scanned Article (GIF)
· References in the article
· Citations to the Article (8) (Citation History)
· Refereed Citations to the Article
· Also-Read Articles (Reads History)
·
· Translate This Page
Title:
A numerical simulation of supersonic turbulent convection relating to the formation of the Solar system
Authors:
Prentice, A. J. R.; Dyt, C. P.
Affiliation:
AA(School of Mathematical Sciences, Box 28M, Monash University, Victoria 3800, Australia; Jet Propulsion Laboratory, California Institute of Technology, Pasadena, California, 91109 USA), AB(School of Mathematical Sciences, Box 28M, Monash University, Victoria 3800, Australia)
Publication:
Monthly Notice of the Royal Astronomical Society, Volume 341, Issue 2, pp. 644-656. (MNRAS Homepage)
Publication Date:
05/2003
Origin:
MNRAS
MNRAS Keywords:
convection, turbulence, Sun: atmospheric motions, Solar system: formation
DOI:
10.1046/j.1365-8711.2003.06454.x
Bibliographic Code:
2003MNRAS.341..644P

Abstract

A flux-corrected transport scheme due to Zalesak is used to carry out a numerical simulation of thermal convection in a two-dimensional layer of ideal, diatomic gas, which is heated from below and stratified gravitationally across many pressure scaleheights. The purpose of this calculation is to mimic the physical conditions in the outer layers of the protosolar cloud (PSC) from which the Solar system formed. The temperature T0 at the top boundary (z= 0) and the dimensionless temperature gradient θ= (d/T0)∂T/∂z at the base of the layer of thickness d are kept fixed, with θ= 10. The initial atmosphere is uniformly superadiabatic, having polytropic index min= 1. Because the Reynolds number of the real atmosphere is so large, a subgrid-scale (SGS) turbulence approximation due to Smagorinsky is used to model the influence of motions with length-scale less than the computational grid size.

The flow soon evolves to a network of giant convective cells, which span the whole layer. At cell boundaries the downflows are spatially concentrated and rapid while the upflows are broad and sluggish. The peak downflow Mach number is at depth z= 0.55d. The descent of the cold gas eliminates much of the initial superadiabatic structure of the atmosphere for z>~ 0.1d, thereby reducing the long-term mean temperature gradient and causing a net shift of mass towards the base.

In the top 10 per cent of depth, SGS modelling causes to increase sharply. A steep density inversion occurs with the long-term mean density at the top boundary rising to 3.5 times the initial density ρ0 there. This result gives new credibility to the modern Laplacian theory (MLT) of Solar system origin. Here a postulated 35-fold density increase at the surface of the PSC causes the shedding of discrete gas rings at the observed mean orbital spacings of the planets. Even so, further numerical simulations, corresponding to higher values of θ, which may yield values and , are required before the MLT can be considered to be valid.


Printing Options

Send high resolution image to Level 2 Postscript Printer
Send low resolution image to Level 2 Postscript Printer
Send low resolution image to Level 1 Postscript Printer
Get high resolution PDF image
Get low resolution PDF
Send 300 dpi image to PCL Printer
Send 150 dpi image to PCL Printer


More Article Retrieval Options

HELP for Article Retrieval


Bibtex entry for this abstract   Preferred format for this abstract (see Preferences)

   

Find Similar Abstracts:

Use: Authors
Title
Keywords (in text query field)
Abstract Text
Return: Query Results Return    items starting with number
Query Form
Database: Astronomy
Physics
arXiv e-prints