ziad1985
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I have a paramagnatic solid, where the atoms have a spin S=1 , and a magnetic momentum
\mu_{B}
We have a magnetic field:
\vec{B}
Under the influence of B the atoms can take 3 value of energy e,-e,0
e=g.\mu_{B}.B
The solid is maintained at a Temperature T and N number of atoms.
The question are like the following:
1)write the partition function of each atom z, then deduce the one of the whole solid Z.
2)E(T)= ??
Limit of E(T--->0)= ??
Limit of E(T---> Large)= ??
3) same question for the entropy S(T)My work:
1)z=1+2.Cosh(e/KT)
Z=(1+2.Cosh(e/KT))^N
2)E(T)=-N.\frac{2.e.Sinh(e/KT)}{1+2.Cosh(e/KT)}
If T--->0 E(T)---> -N.e
if T--->Large E(T) ---> 0
3)S(T)=K.Ln(Z) +E/T
T---> 0 S(T)=N.K.Ln(2)
T---> Large S(T)=0I feel I messed it all up, anyone to help ?
\mu_{B}
We have a magnetic field:
\vec{B}
Under the influence of B the atoms can take 3 value of energy e,-e,0
e=g.\mu_{B}.B
The solid is maintained at a Temperature T and N number of atoms.
The question are like the following:
1)write the partition function of each atom z, then deduce the one of the whole solid Z.
2)E(T)= ??
Limit of E(T--->0)= ??
Limit of E(T---> Large)= ??
3) same question for the entropy S(T)My work:
1)z=1+2.Cosh(e/KT)
Z=(1+2.Cosh(e/KT))^N
2)E(T)=-N.\frac{2.e.Sinh(e/KT)}{1+2.Cosh(e/KT)}
If T--->0 E(T)---> -N.e
if T--->Large E(T) ---> 0
3)S(T)=K.Ln(Z) +E/T
T---> 0 S(T)=N.K.Ln(2)
T---> Large S(T)=0I feel I messed it all up, anyone to help ?
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