Phase Transitions
Phase transitions occur when a system undergoes a qualitative change in its macroscopic properties. First-order transitions involve latent heat; second-order (continuous) transitions are characterized by order parameters and critical exponents near the critical point.
Key Concepts
- Order parameter: quantifies degree of order (e.g., magnetization M)
- First-order: discontinuous order parameter (e.g., liquid-gas)
- Second-order: continuous order parameter, diverging correlation length
- Ising model: spins ±1 with nearest-neighbor coupling J
- Mean-field critical temperature: T_c = zJ/k_B (z = coordination number)
Key Equations
Example Problem
A 2D square Ising model has J=0.1 eV, coordination z=4. Estimate the mean-field T_c in K.
T_c = zJ/k_B = 4×0.1×1.6×10⁻¹⁹/1.38×10⁻²³ = 4640 K. (Exact 2D Ising: T_c = 2J/(k_B ln(1+√2)) ≈ 2.27J/k_B = 2630 K.)
Exercises
7 problemsA 1D Ising chain has J=0.02 eV per bond. What is the mean-field T_c in K for z=2?
The Curie-Weiss susceptibility has C=1.0 (SI) and T_c=300 K. Find χ at T=350 K.
Near T_c, the order parameter scales as M ∝ (T_c-T)^β with β=1/2 (mean field). If M=0.5 at T=T_c-4 K, find M at T=T_c-1 K.
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Upgrade to Pro →Water at 100°C has latent heat L=2260 J/g. Find the entropy change per gram on vaporization in J/(g·K).
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Upgrade to Pro →In a mean-field Ising model at T = 2T_c, find the susceptibility χ = ∂M/∂h|_{h=0}. For T > T_c in mean field: χ = 1/(k_BT - zJ) ∝ 1/(T-T_c). With T=2T_c, k_BT_c=zJ, find χ in units of 1/(zJ).
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Upgrade to Pro →The specific heat of a material shows a jump ΔC = 1.5 Nk_B at the mean-field transition. For 1 mole, find ΔC in J/K.
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Upgrade to Pro →The correlation length ξ ∝ |T-T_c|^{-ν} with ν=1/2 (MF). At T-T_c=0.01 K (close to T_c), ξ=100 nm. At T-T_c=0.04 K, find ξ in nm.
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Upgrade to Pro →Key Takeaways
- Phase transitions are classified by continuity of the order parameter
- Mean-field theory gives T_c = zJ/k_B but neglects fluctuations
- Critical exponents characterize the universal behavior near phase transitions
- The correlation length diverges at the critical point