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 Methodology of Thermodynamics and Statistical Mechanics
 Thermodynamics
study of the relationships between macroscopic properties
Volume, pressure, compressibility, …
Statistical Mechanics (Statistical Thermodynamics)
how the various macroscopic properties arise as a
consequence of the microscopic nature of the system
Position and momenta of individual molecules (mechanical
variables)
 Statistical Thermodynamics (or Statistical Mechanics) is a
link between microscopic properties and bulk (macroscopic)
properties
 A collection of particles - system
 A collection systemts – ensembles
 The systems may have same
macroscopic proterties and
may have different
microscopic properties.
Ensembles
Canonical
Ensembles
Grand
Canonical
Ensembles
Micro
Canonical
Ensembles
 represents states of a mechanical system in
thermal equilibrium with a heat bath at a
fixed temperature.
 system can exchange energy with the heat
bath, so that the states of the system with
differ in total energy.
Canonical Ensemble
Large reservoir (constant T)
All the ensemble members have
the same (n, V, T)
Energy can be exchanged but
particles cannot
Number of Systems : N
N  ∞
Grand Canonical Ensembles
 represents the possible states of a mechanical
system of particles that are in thermo-dynamic
equilibrium (thermal & chemical) with a reservoir.
 system is said to be open in sense that the
system can exchange energy and particles with a
reservoir.
So that the system can differ in bath their total
energy and total no. of particles.
Large reservoir (constant T )
All the ensemble members have
the same (V, T, mi )
Energy and particles can be exchanged
Number of Systems : N
N  ∞
Micro canonical ensembles
 represents the possible states of a
mechanical system whose total energy is
exactly specified.
 System is assumed to be isolated in the sense
the energy of the system does not change
with time.
Micro Canonical Ensembles
EVN EVN EVN
impermeable
All the ensemble members have
the same (E, V, N)
there is no transfer of Energy
and mass
isolated
 Gibbs,Josiah willard(1902). Elementary
principles in Statistical Mechanics.New York:
Charles Scribner’s Sons.
 Cercignani,Carlo,(1998). Ludwig Boltzmann:
The Man Who Trusted Atoms. Oxford
University Press. IsBN 9780198501541.
 Huang, Kerson(1967). Statistical Mechanics.
John Wiley & Sons.
 Srivastava, R.K; Ashok, J.(2005). Statistical
Mechanics. New Delhi: PHI Learning Pvt.Ltd.
ISBN 9788120327825.
Thank you

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Statistical ensembles-b.subha

  • 1.
  • 2.  Methodology of Thermodynamics and Statistical Mechanics  Thermodynamics study of the relationships between macroscopic properties Volume, pressure, compressibility, … Statistical Mechanics (Statistical Thermodynamics) how the various macroscopic properties arise as a consequence of the microscopic nature of the system Position and momenta of individual molecules (mechanical variables)  Statistical Thermodynamics (or Statistical Mechanics) is a link between microscopic properties and bulk (macroscopic) properties
  • 3.  A collection of particles - system  A collection systemts – ensembles  The systems may have same macroscopic proterties and may have different microscopic properties.
  • 5.  represents states of a mechanical system in thermal equilibrium with a heat bath at a fixed temperature.  system can exchange energy with the heat bath, so that the states of the system with differ in total energy.
  • 6. Canonical Ensemble Large reservoir (constant T) All the ensemble members have the same (n, V, T) Energy can be exchanged but particles cannot Number of Systems : N N  ∞
  • 7. Grand Canonical Ensembles  represents the possible states of a mechanical system of particles that are in thermo-dynamic equilibrium (thermal & chemical) with a reservoir.  system is said to be open in sense that the system can exchange energy and particles with a reservoir. So that the system can differ in bath their total energy and total no. of particles.
  • 8. Large reservoir (constant T ) All the ensemble members have the same (V, T, mi ) Energy and particles can be exchanged Number of Systems : N N  ∞
  • 9. Micro canonical ensembles  represents the possible states of a mechanical system whose total energy is exactly specified.  System is assumed to be isolated in the sense the energy of the system does not change with time.
  • 10. Micro Canonical Ensembles EVN EVN EVN impermeable All the ensemble members have the same (E, V, N) there is no transfer of Energy and mass isolated
  • 11.  Gibbs,Josiah willard(1902). Elementary principles in Statistical Mechanics.New York: Charles Scribner’s Sons.  Cercignani,Carlo,(1998). Ludwig Boltzmann: The Man Who Trusted Atoms. Oxford University Press. IsBN 9780198501541.  Huang, Kerson(1967). Statistical Mechanics. John Wiley & Sons.  Srivastava, R.K; Ashok, J.(2005). Statistical Mechanics. New Delhi: PHI Learning Pvt.Ltd. ISBN 9788120327825.