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Solar and Stellar Convection

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dc.contributor.author Narasimha, D
dc.date.accessioned 2005-01-08T05:06:11Z
dc.date.available 2005-01-08T05:06:11Z
dc.date.issued 1988
dc.identifier.citation Kodaikanal Observatory Bulletins Series A, Vol. 9. pp. 33-54 en
dc.identifier.issn 0374-3632
dc.identifier.uri http://hdl.handle.net/2248/184
dc.description.abstract The flow field in stellar convection zones, characterised by high Rayleigh number, low Prandtl number and large Reynolds number, is time dependent and turbulent, consisting of eddies having a range of scale-lengths upto the size of the convection zone. The mixing lengths approximation has been the most widely used formalism to model such a flow, in spite of all its shortcomings. It is possible to test the consistency of this approach as well as to get a good estimate of the mixing-length in the framework of linear stability analysis. The salient features of stellar convection distinguishing it from the laboratory flows are discussed. The underlying physical ideas behind the local and non-local mixing-lenght theories and tests of the resultant models are outlined. Some of the results from other attempts to treat stellar convection using truncated modal analysis and finite difference schemes are briefly summarised. en
dc.format.extent 882704 bytes
dc.format.mimetype application/pdf
dc.language.iso en
dc.publisher Indian Institute of Astrophysics, Bangalore en
dc.subject Solar Convection en
dc.subject Stellar Convection en
dc.title Solar and Stellar Convection en
dc.type Article en


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