{[ promptMessage ]}

Bookmark it

{[ promptMessage ]}

# Lecture06A - Partition Functions(17.3 4 5(Believe it or not...

This preview shows pages 1–3. Sign up to view the full content.

Lecture 6 1 Partition Functions (17.3, 4, 5) (Believe it or not) There is more to life than monatomic ideal gases. In Chapter 18 we will derive the details, but for now let’s consider an ideal diatomic molecule (rigid rotor – harmonic oscillator approx.). The molecular partition function has 3 parts: ( ) 3/ 2 2 / 2 2 2 2 8 , 1 hv hv m I e q V V h h e β β π π β β β = Our old friend: translation for an ideal gas molecule of mass m. I = moment of inertia v = harmonic frequency ( ) ( ) , As before: , , ! N q V Q Q N V N β β = = Lecture 6 2 ( ) 2 ln ln ln ! 3 3 2 ln ln ln 1 ln ... 2 2 2 hv Q N q N N hv m N N N e N h β β π β β = = − + + other terms without β , ln 3 2 2 1 hv hv N V Q N N Nhv Nhve E U e β β β β β = − = + + + = / / 3 2 2 1 B B hv k T B B hv k T Nhv Nhve U Nk T Nk T e = + + + A A / / For N=N (1 mole), and N 3 2 2 1 B B B hv k T A A hv k T k R N hv N hve U RT RT e = = + + + Translational energy Rotational energy Zero-point energy Vibrational (beyond zero-point) energy As we might have anticipated, Energy is distributed among the available degrees of freedom.

This preview has intentionally blurred sections. Sign up to view the full version.

View Full Document