partition function applications of partition function what

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Statistical thermodynamics 2012-04-24 Partition function Applications of Partition function What is Temperature? 1

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Page 1: Partition function Applications of Partition function What

Statistical thermodynamics 2012-04-24

• Partition function

• Applications of Partition function

• What is Temperature?

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Why does energy exchange? (Economists suggest maximizing a utility function.)

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Polymer chain

• The system is one four-bead chain, that has two energy levels.

• Each of the five configurations is called a microstate, to distinguish it from a state or macrostate, which is a collection of microstates.

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Boltzmann distribution

• The Boltzmann distribution says that more particles will have low energies and fewer particles will have high energies.

• Fundamentally, all energy levels are equivalent. Rather, there are more arrangements of the system that way.

• It is extremely unlikely that one particle would have such a high energy that it would leave all the others no energy.

• There are far more arrangements in which most particles have energies that are relatively low, but nonzero. If each particle takes only a small fraction of the total energy, it leaves a great many more ways for the other particles to distribute the remaining energy.

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What Does a Partition Function Tell You?

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Computing the Internal Energy from the Partition Function

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Computing the Entropy Energy from the Partition Function

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An unfolding or denaturation profile for a protein

• For the four-bead chain, there is one compact conformation and four open conformations .

• The density of states is W(0)=1 and W(ε0) =4.

• Since W is the number of microstates per level, the partition function can be expressed as a sum over the two levels (open and compact, in this case), rather than over the five microstates:

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Curie’s law of paramagnetism, a two-level system.

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Peptide loop on a protein molecule

We probe the loop with fluorescence spectroscopy, which measures a distance l from a point on the loop to a point on the protein.

4A 2A 1A

1.7kCal mol-1 1 0

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Partition function

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Molecular partition function

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Translational energy (Particle in a box)

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Partition function contributed by 1-dimensional translation

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Partition function contributed by 3-dimensional translation

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Partition function contributed by 3-dimensional translation

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Partition function by rotation of a nonlinear molecule

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Partition function by rotation of a nonlinear molecule

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Partition function by rotation of a nonlinear molecule

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Partition function contributed by the rotation of a nonlinear molecule

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Partition function by vibration

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Overall Partition function

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Mean translational energy

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Mean rotational energy

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Mean vibrational energy

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Heat capacity

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Heat capacity of diatomic molecule

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Partition Functions for Independent and Distinguishable Particles

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Partition Functions for Independent and Indistinguishable Particles

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Ideal gas law

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Schottky two-state model

• a system that has N distinguishable particles with two energy levels for each particle

• a ground state with energy zero and an excited state with energy ε = ε0 > 0.

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Average energy of two-state model

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Heat capacity of two-state model

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A two-state system with N particles

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What is (1/Temperature)?

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What is Temperature?

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What is Negative Temperature?

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1/T

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Driving force

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Driving force

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Temperature is related with the population density

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What drives heat exchange?

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Summary

• 1/T is the driving force for the uptake of energy. For two bodies A and B in thermal contact, energy will flow from one to the other until the driving forces are equal: 1/TA = 1/TB .

• Thermal equilibrium is not a tendency of high-energy objects to unload their energy to low-energy object.

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