Lecture 3 Flashcards

1
Q

What is the molecular partition function?

A

Sum(i)e^-Bie

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2
Q

What formula describes the energy from each type of energy system? (comes from the partition function)

A

Ei = ei(translational) + ei (rotational) + ei(vibrational) + ei(electronic)

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3
Q

How are the different energy states separated?

A

-Assumption that electronic states are always in the ground state
-Based on the born-Oppenheimer approx
-The rot is independent of the vib state

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4
Q

How is the formula of energies put into the partition function?

A

q = Sum(i)e^-Bie
ei = eiT + eiR + eV + eiE
Gives over all
q = qTqRqVqE

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5
Q

What is the partition function for translational for a molecule moving only 1 direction?

A

-Approximate that its only moving a single direction (X) in a box with fixed volume
The energy levels are
En = n^2h^2/8mX^2

When q is subbed into this
qx = (2pim)/h^2B))^1/2 all times by X (the direction)

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6
Q

What is the MPF for a molecule moving in all directions for translational?

A

In all directions (X,Y and Z) the total energy is
ei = eXn1 + eYn2 + xZn3

This is subbed into q and since e^(a+b+c) is equal to e^a x e^b x e^c then it becomes q = qxqyqz (where x,y and z are a,b and c)

The formula is therefor
qx = (2pim/h^2B)^3/2 x XYZ
XYZ = the volume of the box and simplifies to V

So q simplifies too
q = V/TW^3

TW = h/SQRT(2pikmT) and has units of m

m = kg
h = J s
V = m3
k = J K-1

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7
Q

How is cm3 converted too m3?

A

By dividing by E6

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8
Q

What are the units of thermal wavelength and therefor q?

A

TW = m
Volume = m3
q = V/TM^3
q = unitless

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9
Q

What are the main conclusions on translational partition function?

A

-The gap between trans energy levels in small (due to q being large)
-At room temp a large amount of states are occupied (as q is large)
-A continuum at room temp

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10
Q

How do we get the vibrational partition function?

A

Use the harmonic oscillator approx, where e = hcv

c = SOF
v = frequency of wavenumebers

As the parition function (q) is equal to 1/1-e^-Bev for HO and using equation for e above

qV = 1/1-e-Bhcv

To find B = hcv/kT

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11
Q

What does a small q mean for vib?

A

That only ground and first excited states are occupied at that temperature

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12
Q

How is speed of light converted to fit the equation?

A

Times by 100 to give cm

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13
Q

What is the equation for rotational energy levels?

A

ej = hc”B”J(J+1)

Where this B is equal to a rot constant.
J = rot quantum number

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14
Q

How are rot energy levels separated?
(Degeneracy increases by 2 each time)

A

By 2J + 1
The first level has 1 energy state, then the next has 3 and so on.

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15
Q

What is the PF for rot?

A

The degenracy, gj = 2J + 1, and the energy equation, ej = hc”B”J(J+1) are subsitiuted into

Sum(gj)e-Be

gives qR = Sum(i)(2J+1)e^-Bhc”B”J(J+1)

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16
Q

What trends does the rot partition function show?

A

That q for increasing energy levels will increase then drop rapidly. This is due to the Boltzmann factor contribution (due to the exponential), that energy levels that get higher aren’t favoured at RT as there’s not enough energy.

17
Q

How do we use the rot PF?

A

Each energy level is calculated separately then added up (to give total qR), it will keep decreasing as the level goes up, so eventually the no will be so small that it doesn’t contribute.

18
Q

How is the MPF done for a rotational energy levels of a LINEAR molecule? (This is a more updated version that above, both are for linear)

A

qR = kT/sigma x hc”B”

Approximation only right is T&raquo_space; hc”B”/k

19
Q

What is the symmetry number for symmetrical and non-sym linear molecules?

A

Sym is 2
Non sym is 1

20
Q

What is the rot MPF for non-linear molecules?

A

qR = (1/sigma)x(kT/hc)^3/2 x (pi/ABC*)^1/2

A, B and C are rot constants
sigma is the sym number (from tells stuff) - how many time it can turn to look the same

21
Q

What is the MPF of electronic states?

A

Ground electronic states usually have a lot less energy that excited states, and its assumed that only the GS is occupied. So, qE = g0E, the degeneracy of the ground state.

22
Q

What can q be used for? (when considering weak interactions!!)

A

-To find the mean energy, which can be used to find other thermodynamic processes

23
Q

How is the MPF of mean energy derived?

A

Using the MPF (from boltzman) and the fact that the E = sum(i)niei

[e] = E/N = 1/q sum(i)energyi e^-Bei

Using derivatives, this simplifies to -1/q x dp/dB

24
Q

What is the mean energy of a two-state system?

A

MPF is q = 1 + e^-Be
So [e] = e(energy state)/1+e^Benergy

25
Q

How does mean energy change with temp?

A

As T goes to 0, ME goes to 0.
As T goes to infinity, ME is equal half the energy of the system.

26
Q

How do we correct for the real mean energy?

A

As assumed, e0 = 0 so we need to add the energy of the ground state to the ME calculated to get the real one.

27
Q

How else should this ME be expressed?

A

Usually depends on something, for example volume.

[e] = -1/q (delq/del B) V
[e] = - (del ln(q)/delB) V

28
Q

What is the mean trans energy?

A

Given same as above except a T is in it.
Sub with the MPF to give
[eT]=3/2kT

29
Q

What is the mean vib energy?

A

Given same as above but with a v, and using the MPF of vib energy.
[eV] =hcv/(e^Bhcv -1)