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1.3. Equipartition Of Energy Per Molecule And Its Constituent Parts

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Presentation on theme: "1.3. Equipartition Of Energy Per Molecule And Its Constituent Parts"— Presentation transcript:

1 1.3. Equipartition Of Energy Per Molecule And Its Constituent Parts
 A Fundamental Problem

2 Gas molecules composed of several atoms
Equipartition theorem (see Part III) Each quadratic term in H contributes kT /2 to <ε> For each atom <ε> = 3kT /2. For each molecule <K.E.>C.M. = 3kT /2. Ideal gas law: PV = NkT = 2E / f. E = total energy = N f kT /2 f = effective degrees of freedom of each molecule

3 Proof of (2) : <K.E.>C.M. = 3kT /2
From (1): Hence:

4 vcm and vrel are independent:

5 Proof of (3): PV = NkT = 2E / f
Elastic collisions: For r atoms: Adiabatic process: See Exercise 1.8

6

7 Rotations and vibrations of a triatomic molecule
DoF = 33 = 9 Translation: 3 Rotation: 3 Vibration: 3

8 Heat Capacity Problem Experiment (Theory): For He,   1.660
For O2 ,   1.4  f  5 (6)

9 Heat Capacity Problem  Failure of the Equipartition Theorem
Atom = ( Protons + Neutrons ) + electrons  f  Z Hadrons = Quarks f not known exactly Explanation: States are quantized  Degree of freedom is “frozen” if Excitation energy >> Thermal energy

10 Diatomic Gas Low T Experiment: High T Experiment:  f  5  f  7
Theory: K.E. + Vvib f = = 7 Theory: K.E. + Vvib f = 5 + (1+1) = 5


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