Completely or Strongly Deg. Fermi Gas - Edubirdie

University:
Santa Fe College
Course:
PHY 2048 | General Physics 1 with Calculus
Academic year:

2024
Views:

208

Pages:

3
Author:

Jabin F.

Completely or strongly deg. fermi Gas. 3-D (ηλ² = ∞, T= 0) fle) = {o 0 ECM = EF 1g(E) = ge , EM = EF 2πV (2m) 43 no. of fermione. N= EF 0 N= [gle) de Ef N= 63 E2 de 129 Non-Rel., E=m 3/2 EF 2TV 88 (27) 3/2 3/2 3/2 3/2 4TVgs (2m) EF N = 343 3/2 EF 3/2 = 23 3N (2m) 3/2 4TVgs, h² 3N 2 EF= m (mg)/3 2m for e-, 8= 8 = 25+1 = 2 EF= 2 h² 2m 3N 8TV 2/3 EF = PF 2m = L 2m 3N PF = 8 PF VF = FF m EF = KBTF EF KF = Pf m TF = KB : # Total energy of the system at T=0 = Ground state energy of the system. E. = U 00 Efle) g(t) de N Sof(e) 8(4) de U= = EF Eg(e) de () (2 de Ef(t) de... = Ep2/5/2 = EF E2/3/2 Average energy per partiicle. 0 Ef 12 de -NEF = Eo #: E = AP, d-dimensim. √2 (E) 2(E)/ =) S= = KB/1ηνα + InE) = JE d (KB) SE PA ne se d KB SE = KB Va P= () from epm (1) d= 3, 8 = 2 2 E. P= 3 V = 3 3 NEF 5 V P=÷(₩) EFX/5/3 V 3 Poan 5/3 130

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