This preview shows pages 1–4. Sign up to view the full content.
This preview has intentionally blurred sections. Sign up to view the full version.
View Full DocumentThis preview has intentionally blurred sections. Sign up to view the full version.
View Full Document
Unformatted text preview: for , can neither be neglected nor Strongly deg approximated enerate BE g by an expan ases sion  = starting with , we obtained the density 1 k k k e N e ( 29 = + Z 3 2 2 2 1 mkT V h l 3 2 l =1 l ( 29  = for the weakly degenerate case, 1 1 V < = where 1 (for a 0) o to find the equation of state ( 29  =  ln 1 k k pV kT e ( 29  = + 3 3 2 1 g V we first have to find from ( 29 = = + + + 2 3 3 2 ... 2 3 g l 3 3 3 2 2 2 l =1 l + + + + = 2 3 4 5 6 0.3536 0.1925 0.125 0.089 +0.068 +... ( 29 ( 29 = = = = = Z ] n where we looked in a table for the Riemann zeta f 3 2 3 2 for 0 for 1 1 2.612 g g ( 29 g 1 2.612 = = 3 2 2 3 for a given T, constant 2 h mkT ( 29 3 2 we can plo g t vs 1 2.612 ( 29 ( 29 + 3 3 2 and g 1 vs V ( 29  3 1 vs V  3 since V is large, 0 1 only for 1 V what is the value for a given ?...
View
Full
Document
This note was uploaded on 05/29/2011 for the course CHM 6461 taught by Professor Bowers during the Spring '08 term at University of Florida.
 Spring '08
 Bowers

Click to edit the document details