Lecture 19 - for , can neither be neglected nor Strongly...

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Unformatted text preview: for , can neither be neglected nor Strongly deg approximated enerate B-E 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 ?...
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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.

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Lecture 19 - for , can neither be neglected nor Strongly...

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