statistical mechanics Flashcards

(51 cards)

1
Q

How to find heat capacity

equipartition theorem

A
  1. each T / R =1/2kT
  2. each V = kT
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2
Q

Heat capacity of monotonic

A

3* Trans =3/2kT

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3
Q

Heat capacity of diatomic

A

3T + 2R + 1V

= 7/2kT

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4
Q

How to find no. of modes of vibration

for equipartition

A

3N-6 for non-linear
3N-5 for linear

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5
Q

Three modes of vibration

A
  1. Assymetrical
  2. Symetrical
  3. Bending
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6
Q

What does the boltzman’s distribution tells you

A

The ratio of population between two energy level

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7
Q

How to find the population (in mols) at a specific energy level

if we know N, total population

partition function

A
  1. use eq. - set j to ground state
  2. hence find sum of population as a submation
  3. then replace the N0 in the submation
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8
Q

What can we analysis from the partition function

A

kT = currency of the molecule
ΔE = object to access

if kT needs to be sufficient to buy ΔE

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9
Q

What are the most probable speed, mean speed, and root mean square speed?

A

most probable - largest population
mean speed - avg from the graph
Crms - from avg KE

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10
Q

When does degeneracy in boltzman’s distribution apply

A

rotational energy level

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11
Q

When is vibrational and rotational modes accessible

A

when temp. > threshold temp

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12
Q

what does Cv,m and Cr,m
mean

A

vibration/rotational molar heat capacity contribution

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13
Q

Describle Cv graph

A
  1. at low temp, only translational motion
  2. rotational then vibration modes are accessible as it passes each threshold temp
  3. high temp may then cause molecule to dissociate
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14
Q

How to find heat capacity

A
  1. find the no. of modes (T,R,V)
  2. estimate the θv and θr
  3. if T > θr = find rotational Cm,r
  4. if T> θv = find vibrational Cm,v
  5. add up all three contributional

(compare with equapartition theoerm-depending on mode accessible)

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15
Q

Assumptions of
kinetic theory of gas

A
  1. translation is not quantised
  2. KE is conserved
    (elastic collision)
  3. rigid, point masses
  4. random infrequent motion
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16
Q

Consider 1D - derive

Maxwell boltzman distrubution

along a 1 dimension

A
  1. E of molecule = KE
  2. integrate the partition func. using gaussian integral
  3. complete for all 3 dimension
  4. cube root for solution
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17
Q

What does the maxwell-boltzman distribution show

A

The probability of a molecule at a certain Crms/energy

Crms = root mean sq speed

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18
Q

How to find avg. KE

from maxwell-boltzman

A

via rms speed

  1. find mean sq speed from boltzman function
    [integrate v × f(v) , proability]
    +require gaussian integral
  2. then use 1/2 mv^2
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19
Q

Define collision rate

A

no. of collision per sec.

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20
Q

Define mean free path

A

Avg. dist. travelled before collision

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21
Q

How to derive diffusivity/viscosity, thermal conductivity

A
  1. Using eq of flux
  2. set up three windows at -l, 0, l
  3. find flux at -l and l
  4. do balance to relate to flux eq. (gradient of quantity)
22
Q

how to find quantity transfered from flux

A

flux * time * area of window

23
Q

Derivation of ideal gas eq.

from kinetic theory model

A
  1. find force, i.e. change in momentum in collision
    (assume elastic)
  2. find pressure from area of wall
  3. use the definiton of rms speed from M-B distribution
24
Q

When does ideal gas eq. fails

A

At VLE, i.e. phase change

25
What are the 2 modified assumption of the VDW eq.
1. point masses -> finite size sphere 2. introduce potential energy
26
What can we find from the maxwell contruction
VLE line = line bounding the two Maxwell loop with equal area
27
how to find the most favoured seperation from the Lennard-Jones potential
find dV/dr = 0 (where the potential is minimum)
28
what is g(r) | Intermolecular potential
the likelihood to finding a particle at different seperation
29
What happen to g(r) when V increase
More WD needed to reach seperation less likely to find molecule hence dec.
30
4 step developing Lennard-Jones g(r)
1. for ideal gas - potential is same everywhere 2. but now infinite potential when r< radius of sphere 3. now include attractive and repulsive forces (weakens over seperation) 4. line needs to be continuous
31
Explain the g(r) of solid
1. kT cannot access the energy well 2. can only be at the position of lowest potential 3. hence fixed positions
32
Explain g(r) for gas
1. energy well is << kT 2. not quantised 3. potential is same everywhere
33
Explain g(r) of liquid
1. kT around energy well 2. can occasionally overcome hence +local order +closely packed
34
Explain activation energy in terms of energy well
Energy required to jump from one well to another
35
How does temperature affect diffusion and viscosity
As temp inc. 1. Diffusion inc. 2. viscosity dec.
36
Define polytypes
Identical 2D structure differ in 3D
37
2 rules for solid crystaline structure
1. fill up as much as possible 2. overall charge = 0
38
Define coordination number
No. of neighbours each molecule has
39
packing order expression
vol. taken by particle/vol. of cube
40
How to find heat capacity of solid lattice ? (using Boltzman's distribution)
**particle can only oscillate on the spot** 1. ΔE = 1/2ℏω 2. form partiton function 3. sum of E,energy × N,population = U, internal energy 3. total energy = inf. series (x^n = 1/1-x) 4.Cv = dU/DT
41
What does point imperfection mean | in crystal defects
maybe: 1. missing atom 2. chemcial impurity
42
43
Why does the viscosity of liquid decrease with temperature?
For liquid: inc. kT to overcome attraction For liquid: inc. collision between molecules
44
Unit cell
smallest repeatable unit of the lattice
45
Primitive cell
smallest possible unit of unit cell - containing one lattice point (min. volume)
46
What is the difference between simple, body centred, face-centred
simple -containing a quarter each body-centred (bcc) - a particle in the centre face centred - no particle in the centre but each has face has a half on
47
hat was the weakness of Einstein’s model and how did Debye improve this?
Einstein - assumed all vibrate at one frq fails at low temp Debye considers a spectrum of frq.
48
What effects does defects have on crystal
May lead to: 1. reduced strength, conductivity 2. increased diffusion coefficient
49
Why is L-J not suitable for solid ionic lattice
1. as prescence of electrostatic force, attraction and repulsion present between different molecule 2. instead a geometric series of potential generated instead
50
What is the boltzman's constant, k
k = R/Na | Na = avogadro constant = no. of molecules per mol
51
How to find number of molecules
1 mol = Na no. of molecules N= n* Na | N = no. of molecules Na = avogadro constant n = moles