Two State Paramagnet Flashcards

1
Q

The Two Level Paramagnet

Description

A
  • paramagnetic salts with one unpaired electron have only two possible quantum states
  • the magnetic moment of the electron can be either +μ or -μ
  • in an external magnetic field the spins prefer to line up with the field, but entropy randomises the spins to increase multiplicity
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2
Q

The Two Level Paramagnet

Microstates

A

-a microstate is specified if the directions of all spins of the unpaired electron in every atom is specified

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3
Q

The Two Level Paramagnet

Macrostates

A

-a macrostate is specified by the total number of dipoles that point up (Nu) and the total number of dipoles that point down (Nd)

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4
Q

The Two Level Paramagnet

N

A

N = Nu + Nd

-the total number of dipoles in the body

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5
Q

The Two Level Paramagnet

μ

A

-the magnetic moment of an individual dipole

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6
Q

The Two Level Paramagnet

Energy Per Dipole in the Field

A

-for dipoles lined up parallel to |B:
-μB
-for dipoles lined up antiparallel to |B:
+μB

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7
Q

The Two Level Paramagnet

Total Magnetic Moment

A

|M = |μ( Nu - Nd )
-and since Nd=N-Nu,
|M = |μ (2Nu - N)

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8
Q

The Two Level Paramagnet

Energy of a Macrostate

A

E = μB (Nd - Nu) = μB (N-2Nu)

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9
Q

How many microstates do two spins have?

A
-two spins have 4 possible microstates:
uu, ud, du, dd
-this corresponds to three macrostates
-for the two microstates ud and du, M=0
-for the microstate uu, M=2μ
-for the microstate dd, M=-2μ
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10
Q

How many macrostates do two spins have?

A
  • the macrostates can be classified by their moment M, and their multiplicity
  • there are three macrostates, M= 0, +2μ, -2μ
  • for M=0, Ω=2
  • for M=+2μ , Ω=1
  • for M=-2μ , Ω=1
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11
Q

How many microstates and macrostates do three spins etc. have?

A
  • the number of microstates is given by 2^N where N is the number of spins (so for three spins there are 8 microstates)
  • the number of macrostates is (N+1), so for three spins there are 4 macrostates
  • the multiplicity of each macrostate is given by the lines of pascals triangle so for N=3, the multiplicities are 1, 3, 3, 1
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12
Q

The Two Level Paramagnet

Calculating Number of Microstates, Probability of Being in a Particular Microstate, Multiplicity

A

number of equally probable microstates = 2^N
probability of being in a particular microstate = 1/(2^N)
multiplicity of a two-state paramagnet:
Ω(N,Nu) = N! / (Nu! Nd!)
= N! / (Nu! (N-Nu)!)

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13
Q

The Two Level Paramagnet

Effect of B

A

-for B=0 the energy of each macrostate is the same

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14
Q

How does the energy of a state effect its probability?

A

-the higher energy the state is the lower the probability it will be occupied

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15
Q

Boltzmann Factor

General Definition

A
  • a Boltzmann factor is an exponential function

- the Boltzmann factor gives the fraction of atoms in one energy state compared to another

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16
Q

Boltzmann Factor

Nu / Nd

A

Nu/Nd = exp (2μB/kT)

17
Q

Boltzmann Distribution

General Definition

A

-gives the distribution between states of different energies

18
Q

Boltzmann Factor

Nd

A

Nd = exp (-μB/kT)

19
Q

Boltzmann Factor

Nu

A

Nu = exp (μB/kT)

20
Q

Boltzmann Factor

N

A

N = exp (μB/kT) + exp (-μB/kT)

21
Q

Boltzmann Factor

General Formula

A

-the boltzmann factor for a particular energy state is given by:

exp (-ε/kT)

-where ε is the energy of the state

22
Q

Single Particle Partition Function

General Definition

A
  • it is the Boltzmann factor associated with each state added together
  • in principle a partition function can be written for any system provided all of the energy states are known
  • the number of terms in the partition function is equal to the number of energy states in the system
  • the symbol for partition function is Z1
23
Q

The Two Level Paramagnet

The Single Particle Partition Function

A

Z1 = exp(-μB/kT) + exp(μB/kT)

24
Q

Occupational Probability of a Two-State Paramagnet With Temperature

A

-at lower temperatures, the lower energy state is
occupied
-as temperature increases, the two states become more equally occupied
-at very high temperatures the two states become equally populated
-these trend are seen in all systems not just the two state

25
Internal Energy of the Two-State Paramagnet With Temperature
- asymptotically approaches zero - increases towards a maximum value - there is a temperature at which the maximum rate of change of states occurs - heat capacity would follow the gradient of this graph
26
Two-State Paramagnet | Entropy Equation
S = Nk [ ln(2cosh(μB/kT) - μB/kT tanh(μB/kT) ]
27
Two-State Paramagnet | Entropy as a Function of Temperature
- follows the same shape as internal energy - lower magnetic field results in higher entropy at every temperature - because the field causes alignment so a weaker field means more disorder and therefore higher entropy
28
Two-State Paramagnet | Heat Capacity and Temperature
- at low temperatures heat capacity is small because kT<<2μB, thermal fluctuations are rare and it is hard for the system to absorb thermal energy, this is universal for systems with energy quantisation - at high temperatures, Nu~Nd and it is hard for the system to absorb thermal energy, this is not universal behaviour, it occurs if the system's energy spectrum occupies a finite interval of energies
29
Two-State Paramagnet | Internal Energy Equation (and Magnetic Moment)
E = -NμB tanh(μB/kT) = -MB -where M = Nμ tanh(μB/kT) is the total magnetic moment
30
Magnetic Moment - High Temperature Limit | Curie's Law
M = Nμ tanh(μB/kT) -for x<<1 , tanh(x) -> x -so in the high temperature limit T->∞ => 1/T->0 : M = Nμ * μB/kT = Nμ²B/kT -increasing B orders spin and increase M -increasing T disorders spin and decreases M