Statistical Mechanics Mean Field Model

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SUMMARY

The discussion focuses on the mean field model in statistical mechanics, specifically addressing the relationship between magnetization (M), magnetic field (H), and temperature (T). It establishes that M is proportional to H1/3 at the critical temperature (Tc) and that at zero magnetic field (H=0), M is proportional to (Tc - T)1/2. The equations discussed include M = N/V gμbS(x - x3/3) and the critical temperature equation Tc = λN(gμbS)2/VK. The conversation highlights the necessity of using higher-order terms in the Taylor series expansion of tanh(x) for accurate calculations.

PREREQUISITES
  • Understanding of statistical mechanics concepts, particularly mean field theory.
  • Familiarity with Taylor series expansions and their applications in physics.
  • Knowledge of magnetization equations and their dependence on temperature and magnetic field.
  • Proficiency in using variables such as N (number of particles), V (volume), and gμb (magnetic moment).
NEXT STEPS
  • Study the derivation of the mean field model equations in statistical mechanics.
  • Learn about the implications of higher-order terms in Taylor series expansions.
  • Explore the relationship between critical temperature and magnetization in various materials.
  • Investigate the applications of mean field theory in phase transitions and critical phenomena.
USEFUL FOR

Students and researchers in physics, particularly those focusing on statistical mechanics, phase transitions, and magnetic properties of materials.

Chris B
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I don't think I've fully grasped the underlying ideas of this class, so at the moment I'm just sort of flailing for equations to plug stuff into...

Homework Statement



Show that in the mean field model, M is proportional to H1/3 at T=Tc and that at H=0, M is proportional to (Tc - T)1/2

Homework Equations



It'll take me forever to write it out here, but M equals some coefficients times tanh(x) where x depends on H, M, and T

The Attempt at a Solution



In class we approximated M at T=0 by taking the first term in the Taylor series expansion of tanh(x) which turns out to just be x. We were given the hint that we need to take the next term in the series (why?) to do this problem. The next term in the series is -x3/3 so the whole thing is
M=N/V gμbS(x-x3/3)
where x = gμbS(H+λM)/kT
I also know that Tc = λN(gμbS)2/VK
I plugged Tc in for T and by rearranging got something that was proportional to H1/3 minus H/λ
For the next part I'm not sure what to do. If I plug in zero for H the whole thing is zero. I don't see how I'm going to get (Tc - T)1/2 if I'm substituting Tc for T.
 
Physics news on Phys.org
These are two different scenarios. In part A, you assume T=Tc. In part B, the only assumption is that H=0.
 

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