chapter 6 boltzmann statistics. boltzmann factor & partition functions u r, s r u, s huge...

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Chapter 6 Boltzmann Statistics

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Page 1: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Chapter 6

Boltzmann Statistics

Page 2: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Boltzmann Factor & Partition Functions

UR, SR

U, S

Huge reservoir

System

Changes in energy of the reservoir are very small compared to its total energy.

Say the system has 5 atoms and 2 units of energy.

)!1(!

!1),(

Nq

NqqN

Page 3: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Boltzmann Factor & Partition FunctionsSay the system has 5 atoms and 2 units of energy.

)!1(!

!1),(

Nq

NqqNtotal

Atom 1 Atom 2 Atom 3 Atom 4 Atom 5

2 0 0 0 0

0 2 0 0 0

0 0 2 0 0

0 0 0 2 0

0 0 0 0 2

1 1 0 0 0

1 0 1 0 0

1 0 0 1 0

1 0 0 0 1

0 1 1 0 0

0 1 0 1 0

0 1 0 0 1

0 0 1 1 0

0 0 1 0 1

0 0 0 1 1

)0(

)1(

)2(

P

P

P

What is the probability of finding a particular atom with 2, 1, or 0 units of energy?

Page 4: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Boltzmann Factor & Partition FunctionsSay the system has 10 atoms and 4 units of energy.

715

)!1(!

!1),(

Nq

NqqNtotal

692.0715/495)0(

231.0715/165)1(

0629.0715/45)2(

0126.0715/9)3(

00140.0715/1)4(

P

P

P

P

P

What is the probability of finding a particular atom with 4, 3, 2, 1, or 0 units of energy?

UR, SR

U, S

Huge reservoir

System

Page 5: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Boltzmann Factor & Partition FunctionsSay the system has 10 atoms and 4 units of energy.

715

)!1(!

!1),(

Nq

NqqNtotal

692.0715/495)0(

231.0715/165)1(

0629.0715/45)2(

0126.0715/9)3(

00140.0715/1)4(

P

P

P

P

P

What is the probability of finding a particular atom with 4, 3, 2, 1, or 0 units of energy?

UR, SR

U, S

Huge reservoir

System

Page 6: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Boltzmann Factor & Partition FunctionsSay the system has 10 atoms and 4 units of energy.

715

)!1(!

!1),(

Nq

NqqNtotal

692.0715/495)0(

231.0715/165)1(

0629.0715/45)2(

0126.0715/9)3(

00140.0715/1)4(

P

P

P

P

P

What is the probability of finding a particular atom with 4, 3, 2, 1, or 0 units of energy?

Page 7: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Boltzmann Factor & Partition FunctionsSay the system has 10 atoms and 4 units of energy.

715

)!1(!

!1),(

Nq

NqqNtotal

n

eP

n

TkZ

total

nn

Bn

/1)(

What is the probability of finding a particular atom with 4, 3, 2, 1, or 0 units of energy?

Page 8: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Boltzmann Factor & Partition Functions

Tk

Tk

n

TkZn

Bn

Bn

Bn

e

eZ

eP

/

/

/1)(

Boltzmann Factors

Partition Function

Boltzmann or Canonical Distribution

Page 9: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Boltzmann, Entropy, & Gibbs

)(ln)(

)( /1

nnB

TkZ

total

nn

PPkS

eP Bn

Page 10: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Boltzmann, Entropy, & Gibbs

)(ln)(

)( /1

nnB

TkZ

total

nn

PPkS

eP Bn

Page 11: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Boltzmann, Entropy, & Gibbs

)(ln)(

)( /1

nnB

TkZ

total

nn

PPkS

eP Bn

Page 12: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Boltzmann, Entropy, & Gibbs

)(ln)(

)( /1

nnB

TkZ

total

nn

PPkS

eP Bn

Page 13: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Partition Functions & Hydrogen AtomWhat’s the energy of the electron on a hydrogen atom?

Solution to Rydberg or Bohr Model can be used.

Page 14: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Partition Functions & Hydrogen AtomWhat’s the energy of the electron on a hydrogen atom?

Solution to Rydberg or Bohr Model can be used.

Page 15: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Hydrogen Atom @ 300K

Page 16: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Hydrogen Atom on Sun

Page 17: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Hydrogen Atom on Sun

Page 18: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

A System with Smaller Energies

Page 19: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

A System with Smaller Energies

0 0.1 0.2 0.3 0.4 0.5 0.60

0.2

0.4

0.6

0.8

1

Energy (eV)

Pro

ba

bil

ity

Page 20: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

A System with Smaller Energies

0 0.1 0.2 0.3 0.4 0.5 0.60

0.10.20.30.40.50.60.70.80.9

Energy (eV)

Pro

ba

bil

ity

Page 21: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Average ValuesSay the system has 10 atoms and 4 units of energy.

What is the average energy of the system if4 atoms have n=03 atoms have n=12 atoms have n=21 atom has n=30 atoms have n=4?

Page 22: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Averages Values

Be careful about using the proper probability when computing averages.

Page 23: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Rotation of Diatomic Molecules

Page 24: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Rotation of Diatomic Molecules

Page 25: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Rotation of Diatomic Molecules

0

/)(

0

/)1( 2

1212j

Tkjj

j

Tkjjrot

BB ejejZ

This can be calculated as an integral if dj is small compared to kBT/e (high temperature limit).

djejZ Tkjjrot

B 0

/)( 2

12

Page 26: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Rotation of Diatomic MoleculesA simplified partition function in the high temperature limit.

Page 27: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Rotation of Diatomic MoleculesHCl rotations

Page 28: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Rotation of Diatomic MoleculesAverage energy and heat capacity.

Page 29: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very
Page 30: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Rotational Partition Function• For diatoms with unlike atoms

• For diatoms with like atoms

Tk

ejZ B

j

Tkjjrot

B

0

/)1()12(

20

/)1(2)12( TkeZ B

j

Tkjjjrot

B

Unlike atomsdistinguishable

like atomsIndistinguishable

Bol

tzm

ann

Fac

tors

Page 31: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Rotational Partition FunctionB

oltz

man

n F

acto

rs

Bol

tzm

ann

Fac

tors

Page 32: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Rotational Energies

Unlike atomsdistinguishable

like atomsIndistinguishable

BV

V

B

B

NkT

UC

TNkU

TkE

Page 33: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Maxwell Speed Distribution

vx

vy

vz

v

For continuous variables, we talk about probability density function or probability distribution function (pdf).

Page 34: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Maxwell Speed DistributionWhat is Z?

Page 35: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Maxwell Speed Distribution

What is maximum probability speed?

The Maxwell Speed Distribution

Page 36: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Maxwell Speed DistributionWhat is the average speed?

Page 37: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Maxwell Speed Distribution

Page 38: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Example: Nitrogen @ 300KFor Monday:

(a) Show the maximum probability speed is 517 m/s.

(b) Show the average speed is 476 m/s.

(c) Show the rms speed is 422 m/s.

(d) Calculate the probability of a molecule moving faster than 1000 m/s. (Need Maple or Mathematica)

Page 39: Chapter 6 Boltzmann Statistics. Boltzmann Factor & Partition Functions U R, S R U, S Huge reservoir System Changes in energy of the reservoir are very

Nitrogen Speed Distribution