kinetic theory of gases and equipartition theorem

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Kinetic Theory of Kinetic Theory of Gases and Gases and Equipartition Theorem Equipartition Theorem

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Page 1: Kinetic Theory of Gases and Equipartition Theorem

Kinetic Theory of Gases and Kinetic Theory of Gases and Equipartition TheoremEquipartition Theorem

Page 2: Kinetic Theory of Gases and Equipartition Theorem

Results of Kinetic TheoryResults of Kinetic Theory

• KE of individual particles is related to the temperature of the gas:

½ mv2 = 3/2 kT

Where v is the average velocity.

Page 3: Kinetic Theory of Gases and Equipartition Theorem

Boltzmann DistributionBoltzmann Distribution

• Demonstrated that there is a wide range of speeds that varies with temperature.

Page 4: Kinetic Theory of Gases and Equipartition Theorem

Equipartition of EnergyEquipartition of EnergyThe Kinetic Theory result tells us that the

average translational KE is proportional to the temperature.

Types of allowed motion are referred to as Degrees of Freedom (DOF)

Linear motion in three directions (x,y,z) is three DOF.

Page 5: Kinetic Theory of Gases and Equipartition Theorem

Equipartition of EnergyEquipartition of Energy

• Each degree of translational freedom takes ½ kT.

KEx +KEy+KEz = ½ kT + ½ kT + ½ kT

KEtotal = 3/2 kT

This is true for single point masses that possess no structure.

Page 6: Kinetic Theory of Gases and Equipartition Theorem

Equipartition of EnergyEquipartition of Energy

For molecules, i.e. multi-atom particles, there are added degrees of freedom.

Page 7: Kinetic Theory of Gases and Equipartition Theorem

Equipartition of EnergyEquipartition of Energy

• Each new DOF requires ½ kT of energy.

Each new DOF contributes ½ kT to the total internal energy of the gas. This is the Equipartition Theorem.

Page 8: Kinetic Theory of Gases and Equipartition Theorem

Internal Energy, UInternal Energy, U

• The internal energy of a gas is the sum of all the kinetic and potential energies.

U = KE + PE.

For an ideal gas we allow no PE of interaction, so U is comprised solely of the various type of kinetic energies, i.e. translational, rotational and vibrational.

Page 9: Kinetic Theory of Gases and Equipartition Theorem

Internal Energy of Di-AtomInternal Energy of Di-Atom

• Three translational DOF + 2 rotational DOF = 5 DOF.

Each DOF contributes ½ kt, so the internal energy of a diatomic gas is,

U = 5/2 NkT,

For a gas of N molecules.