Onsager theory: Difference between revisions
		
		
		
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| Carl McBride (talk | contribs)  (New page: Lars Onsager ==References== #L. Onsager "THE EFFECTS OF SHAPE ON THE INTERACTION OF COLLOIDAL PARTICLES", Annals of the New York Academy of Sciences '''51'''  pp. 627- (1949)) | Carl McBride (talk | contribs)  No edit summary | ||
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| [[Lars Onsager]] | The '''Onsager theory''' for the isotropic-[[nematic phase |nematic]] phase transition was developed by [[Lars Onsager]] (Ref. 1). | ||
| In a 3-dimensional gas of [[hard rods]] there are two contributions to the [[entropy]]: a part due to translation and a part due to orientation. These two contributions are coupled. | |||
| ==References== | ==References== | ||
| #L. Onsager "THE EFFECTS OF SHAPE ON THE INTERACTION OF COLLOIDAL PARTICLES", Annals of the New York Academy of Sciences '''51'''  pp. 627- (1949) | #L. Onsager "THE EFFECTS OF SHAPE ON THE INTERACTION OF COLLOIDAL PARTICLES", Annals of the New York Academy of Sciences '''51'''  pp. 627- (1949) | ||
Revision as of 15:26, 23 July 2007
The Onsager theory for the isotropic-nematic phase transition was developed by Lars Onsager (Ref. 1). In a 3-dimensional gas of hard rods there are two contributions to the entropy: a part due to translation and a part due to orientation. These two contributions are coupled.
References
- L. Onsager "THE EFFECTS OF SHAPE ON THE INTERACTION OF COLLOIDAL PARTICLES", Annals of the New York Academy of Sciences 51 pp. 627- (1949)