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Pythagoras0 (토론 | 기여) (→노트: 새 문단) |
Pythagoras0 (토론 | 기여) (→메타데이터: 새 문단) |
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===소스=== | ===소스=== | ||
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| + | == 메타데이터 == | ||
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| + | ===위키데이터=== | ||
| + | * ID : [https://www.wikidata.org/wiki/Q1077753 Q1077753] | ||
2020년 12월 26일 (토) 06:25 판
노트
- The most practical ensemble is the canonical ensemble with N, V, and T fixed.[1]
- This chapter derives the canonical ensemble, which is arguably the most important concept in quantum statistical mechanics.[2]
- A canonical ensemble does not evolve over time, despite the fact that the underlying system is in constant motion.[3]
- Example of canonical ensemble for a quantum system consisting of one particle in a potential well.[3]
- A canonical ensemble for this system, for the temperature shown.[3]
- Example of canonical ensemble for a classical system consisting of one particle in a potential well.[3]
- The advantage of the canonical ensemble should now be apparent.[4]
- We have derived the properties of the canonical ensemble using a Taylor expansion of the entropy.[5]
- The grand-canonical ensemble is for "open" systems, where the number of particles, , can change.[6]
소스
메타데이터
위키데이터
- ID : Q1077753