An Introduction to Thermal Physics · Problem 8.24

Systems of Interacting Particles — Daniel Schroeder

Physics — Statistical Mechanics · ising-model-critical-exponents

Problem

In this problem you will use the mean field approximation to analyze the behavior of the Ising model near the critical point. ((a)) Prove that, when x≪1x \ll 1, tanh⁡x≈x−13x3\tanh x \approx x - \frac{1}{3}x^3. ((b)) Use the result of part (a) to find an expression for the magnetization of the Ising model, in the mean field approximation, when TT is very close to the critical temperature. You should find M∝(Tc−T)βM \propto (T_c - T)^\beta, where β\beta (not to be confused with 1/kT1/kT) is a critical exponent, analogous to the β\beta defined for a fluid in Problem 5.55. Onsager's exact solution shows that β=1/8\beta = 1/8 in two dimensions, while experiments and more sophisticated approximations show that β≈1/3\beta \approx 1/3 in three dimensions. The mean field approximation, however, predicts a larger value. ((c)) The magnetic susceptibility χ\chi is defined as χ≡(∂M/∂B)T\chi \equiv (\partial M/\partial B)_T. The behavior of this quantity near the critical point is conventionally written as χ∝(T−Tc)−γ\chi \propto (T - T_c)^{-\gamma}, where γ\gamma is another critical exponent. Find the value of γ\gamma in the mean field approximation, and show that it does not depend on whether TT is slightly above or slightly below TcT_c. (The exact value of γ\gamma in two dimensions turns out to be 7/47/4, while in three dimensions γ≈1.24\gamma \approx 1.24.)

Related theory

Browse the problem library