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[2003SM/Eval-Test-I]

Node id: 5557page
AK-47's picture 22-07-10 06:07:37 n

[2003SM/Eval-Test-II]

Node id: 5558page
AK-47's picture 22-07-10 06:07:38 n

[2003SM/Eval-Suppl]

Node id: 5556page
AK-47's picture 22-07-10 06:07:37 n

[2003SM/Eval-Suppl]

Node id: 5555page
AK-47's picture 22-07-10 06:07:17 n

[2003SM/Eval-Final01]

Node id: 5554page
AK-47's picture 22-07-10 06:07:53 n

[1998TH/LNP-11] Lecture -11 Work in Thermodynamics

Node id: 5553page
AK-47's picture 22-07-08 07:07:50 n

[1998TH/LNP-10] Lecture -10 Equation of State for non P V systems

Node id: 5552page
AK-47's picture 22-07-08 07:07:10 n

[1998TH/LNP-09] Lecture -9 Equation of State-II

Node id: 5551page
AK-47's picture 22-07-08 07:07:29 n

[1998TH/LNP-08] Lecture -8 Pure Substances

Node id: 5550page
AK-47's picture 22-07-08 07:07:52 n

[1998TH/LNP-07] Lecture -7 Mathematical Preparation

Node id: 5549page
AK-47's picture 22-07-08 07:07:09 n

[1998TH/LNP-06] Lecture -6 Thermodynamic equilibrium

Node id: 5548page
AK-47's picture 22-07-08 07:07:35 n

[1998TH/LNP-05] Lecture -5 Zeroth Law and Temperature

Node id: 5547page
AK-47's picture 22-07-08 07:07:13 n

[1998TH/LNP-04] Lecture -4 Equilibrium

Node id: 5546page
AK-47's picture 22-07-08 07:07:22 n

[1998TH/LNP-03]--Lecture -3 Microscopic vs macroscopic systems

Node id: 5545page
AK-47's picture 22-07-08 07:07:29 n

[1998TH/LNP-02]--Lecture -2 Mechanics vs Thermodynamics

Node id: 5544page
AK-47's picture 22-07-08 07:07:09 n

[2003SM/LNP-18] Lecture-18--Grand Canonical Ensemble — Summary and Applications

Node id: 5543page

The main result for grand canonical ensemble are summarized. The Planck’s law and the Stephan Boltzmann law for black body radiation are derived.

AK-47's picture 22-07-07 07:07:35 n

[2003SM/LNP-17] Lecture-17--Grand Canonical Ensemble

Node id: 5542page

Using the grand canonical ensemble method, the Bose Einstein and Fermi Dirac distribution formula are derived. An expression for the partition function for photons is proved and result on the mean number of particles in terms of grand canonical partition function is obtained

AK-47's picture 22-07-07 07:07:17 n

[2003SM/LNP-16] Lecture-16--Open Systems —Grand Canonical Ensemble

Node id: 5541page
AK-47's picture 22-07-07 07:07:09 n

[2003SM/LNP-15] Lecture-15--Quantum Effects in Statistical Mechanics

Node id: 5540page

Quantum effects in macroscopic systems appear in two ways. The first the energy levels are quantized. The quantization of energy levels does not need any modification in the framework. Secondly identical nature of particles constituting the system. This requires a new approach to enumerating the microstates. The microstates are not labeled by coordinates and momenta as is the case in classical theory. In quantum theory the microstates are specified by giving the number of particles for different levels.

AK-47's picture 22-07-07 07:07:53 n

[2003SM/LNP-14] Lecture-14--Equipartition of Energy

Node id: 5539page

In this lecture we derive law of equipartition of energy under the assumption that the energy is quadratic function of some variable such as coordinates and momenta. The classical theory of specific heat of gases is given and the Einstein model of taking quantum corrections is briefly discussed. A comparison of the classical and quantum model with experiments is given.

AK-47's picture 22-07-07 07:07:20 n

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