Partition Function, Entropy, Distinguishability, Planck Distribution, Heat Capacity of Platinum

   

Added on  2023-06-12

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Running Head: PVB 301 1
PVB 301 Assignment 2
Student’s name
University affiliation
Partition Function, Entropy, Distinguishability, Planck Distribution, Heat Capacity of Platinum_1
PVB 301 2
1. PARTITION FUNCTION OF A 2D GAS
The partition equation for a system of particles that obeys Boltzmann statistics has a
definition (Harris, 2012).
Z=
j
g j eε j/ kBT
....................................... (1)
Where there are ∆G j energy states within the macro level then
Z=
j
G j eε j/ kB T
......................................... (2) And ε j= h2 A1
8 m n j
2
......................................................... (3) For single particle in a box using the
principle of quantum mechanics. For a gas confined in a 2D area;
G j= 1
4 π n j
2....................................................... (4)
G j= 1
2 π nj n j substituting G j in the second equation;
Z= π
2
j
n j nj eε j /kB T
............................... (5)
Substituting ε jin equation (3) into equation (5);
Z= π
2
j
n j nj e¿ h2 A1
8 mk B T nj
2 ¿
Integrating from 0 to ; Z= π
2
0

nj exp (h2 A1
8 mk B T nj
2
)d n j;
Z=A ( 2 πm kB T
h2 )
2
2 = A
( h2
2 πm kB T )
= A
λth
2 Where λth= h
(2 πmk B T )
2. ENTROPY AND DISTINGUISHABILITY
Partition Function, Entropy, Distinguishability, Planck Distribution, Heat Capacity of Platinum_2
PVB 301 3
a) Probability density for distributing N1 particles in a sub volume V1, and N2 in
V2, is given by the binomial distribution (Santos, Dorini, & Cunha, 2008);
W = N !
N1 ! N2 ! (V 1
V )N1
( V 2
V )N2
¿ W =¿ Ωc ( V 1 N1 ) +¿ Ωc ( V 2 N 2 ) ¿ Ωc ( V 1 N ) Ωc(V , N )=( V N
N ! )
Entire entropy;Ωp (U , N )=
( (2 πmU )
3 N
2
(3 N
2 )! )
Assuming N>>1 Ωp ( U , V , N ) =
( Ωc (V , N)Ωp (U , N )
h3 N )
Substituting : S=kInΩ ( U ,V , N )This gives the same Sackur-Tetrode equation for distinguishable
particles as for indistinguishable ones.
b) Helmholtz energy: F=U – TS
dA=SdT pdV =SdT pdV +
j
u j dN j
Where N j=no of particles
u j=corresponding chemical potentials
dA=SdT
i
ui dNi +
j
u j dN jCITATION Vid 08 ¿ 1033(Vidal , 2008)
Probability to find the system in some energy Eigen state r
Pr = eβEr
Z Where β= 1
kT , Z=
r
e βr
U = E =
r
Pr Xr= 1
β
logz
x
Partition Function, Entropy, Distinguishability, Planck Distribution, Heat Capacity of Platinum_3

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