User:Tohline/SSC/Structure/LimitingMasses
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==Virial Equilibrium==  ==Virial Equilibrium==  
By examining the [[User:Tohline/SphericallySymmetricConfigurations/Virial#PV_Diagramvirial equilibrium of nonrotating, spherically symmetric configurations that are embedded in an external medium]] of pressure <math>P_e</math>, one can begin to appreciate that there is a mass above which no equilibrium exists if the effective adiabatic exponent of the gas is <math>\gamma_g < 4/3</math>. Assuming uniform density and uniform specific entropy configurations for simplicity, there is an analytic expression for this limiting mass and for the equilibrium radius of that limiting configuration. Specifically,  By examining the [[User:Tohline/SphericallySymmetricConfigurations/Virial#PV_Diagramvirial equilibrium of nonrotating, spherically symmetric configurations that are embedded in an external medium]] of pressure <math>P_e</math>, one can begin to appreciate that there is a mass above which no equilibrium exists if the effective adiabatic exponent of the gas is <math>\gamma_g < 4/3</math>. Assuming uniform density and uniform specific entropy configurations for simplicity, there is an analytic expression for this limiting mass and for the equilibrium radius of that limiting configuration. Specifically,  
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=Related Wikipedia Discussions=  =Related Wikipedia Discussions=  
* [http://en.wikipedia.org/wiki/BonnorEbert)mass BonnorEbert Mass]  * [http://en.wikipedia.org/wiki/BonnorEbert)mass BonnorEbert Mass]  
  
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Revision as of 17:27, 4 November 2012
Contents 
Mass Upper Limits
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Virial Equilibrium
By examining the virial equilibrium of nonrotating, spherically symmetric configurations that are embedded in an external medium of pressure P_{e}, one can begin to appreciate that there is a mass above which no equilibrium exists if the effective adiabatic exponent of the gas is γ_{g} < 4 / 3. Assuming uniform density and uniform specific entropy configurations for simplicity, there is an analytic expression for this limiting mass and for the equilibrium radius of that limiting configuration. Specifically,
and,
Polytropes Embedded in an External Medium
Polytropes embedded in an external medium
Summary of Analytic Results
Example: Specify c_{s}, P_{e} and n (or η = 1 + 1 / n)  

η 
M_{max} 
R_{eq} 

α_{virial} 
α_{DHB} 
scale 
α_{virial} 
α_{DHB} 
scale 


1 

 


 

5 
6/5 




 

BonnorEbert Limiting Mass
Here we will refer to the original works of Ebert (1955, ZA, 37, 217) and Bonnor (1956, MNRAS, 116, 351) .
In his study of the "global gravitational stability [of] onedimensional polytropes," Whitworth (1981, MNRAS, 195, 967) normalizes (or "references") various derived mathematical expressions for configuration radii, R, and for the pressure exerted by an external bounding medium, P_{ex}, to quantities he refers to as, respectively, R_{rf} and P_{rf}. The paragraph from his paper in which these two reference quantities are defined is shown here:
In order to map Whitworth's terminology to ours, we note, first, that he uses M_{0} to represent the spherical configuration's total mass, which we refer to simply as M; and his parameter η is related to our via the relation,
Hence, Whitworth writes the polytropic equation of state as,
whereas, using our standard notation, this same key relation is written as,
;
and his parameter K_{η} is identical to our .
According to the second (bottom) expression identified by the red outlined box drawn above,
and inverting the expression inside the green outlined box gives,
Hence,
or, gathering all factors of P_{rf} to the lefthand side,
Analogously, according to the first (top) expression identified inside the red outlined box,
Related Wikipedia Discussions
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