Starting from the partition function, calculate the average energy of the one-dimensional Ising model, to verify equation 8.44. Sketch the average energy as a function of temperature.

Short Answer

Expert verified

The average energy =-Nεtanhβε

Sketch for the average energy as function of temperature

Step by step solution

01

Step 1. Given information

The partition function of the system:

Z=se-εi/r

Z=se-εi/r

02

Step 2. To find the expression for average energy 

We substituteβfor1/τ

Z=se-εnβ

The average energy of the system is,

U=ε

=1Zsεse-βcs

=-1Zεsse-βss

Substituting the value of dZdβ=εsse-βcs

U=-1ZdZdβ

=-β(lnZ)

The expression for partition function for final sum of Ndipole is,

Z=(2coshβε)

lnZ=ln(2coshβε)

U=-1ZdZdβ

=-β(ln(2coshβε))

=1(2coshβε)((2sinhβε))α

=-Nεtanhβε

The average energy ==-Nεtanhβε

03

Step 3. Sketch for the following function

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Most popular questions from this chapter

Modify the ising program to simulate a one-dimensional Ising model.

(a) For a lattice size of 100, observe the sequence of states generated at various temperatures and discuss the results. According to the exact solution (for an infinite lattice), we expect this system to magnetise only as the temperature goes to zero; is the behaviour of your program consistent with this prediction? How does the typical cluster size depend on temperature?

(b) Modify your program to compute the average energy as in Problem 8.27. Plot the energy and heat capacity vs. temperature and compare to the exact result for an infinite lattice.

(c) Modify your program to compute the magnetisation as in Problem 8.28. Determine the most likely magnetisation for various temperatures and sketch a graph of this quantity. Discuss.

Consider a gas of molecules whose interaction energy u(r)u is infinite for r<r0and negative for r>r0, with a minimum value of -u0. Suppose further that kTu0, so you can approximate the Boltzmann factor forr>r0using ex1+x. Show that under these conditions the second virial coefficient has the form B(T)=b-(a/kT), the same as what you found for a van der Waals gas in Problem 1.17. Write the van der Waals constants aand b in terms of r0and u(r), and discuss the results briefly.

Consider an Ising model of 100 elementary dipoles. Suppose you wish to calculate the partition function for this system, using a computer that can compute one billion terms of the partition function per second. How long must you wait for the answer?

Problem 8.10. Use a computer to calculate and plot the second virial coefficient for a gas of molecules interacting via the Lennard-Jones potential, for values of kT/u0 ranging from 1to 7. On the same graph, plot the data for nitrogen given in Problem 1.17, choosing the parameters r0 and u0so as to obtain a good fit.

Draw all the connected diagrams containing four dots. There are six diagrams in total; be careful to avoid drawing two diagrams that look superficially different but are actually the same. Which of the diagrams would remain connected if any single dot were removed?

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