📊 Ансамблі
Microcanonical
E, V, N fixed. Equal а priori probability: microstates. Entropy S = k_B ln(Ω), де Ω = number of states.
Canonical
T, V, N fixed. Partition function Z = Σ exp(-βE_i), β = 1/(k_B T). F = -k_B T ln(Z).
Grand canonical
T, V, μ fixed. Ξ = Σ exp(-β(E - μN)). Chemical potential μ. Open systems.
Equivalence
Thermodynamic limit N → ∞: ансамблі equivalent. Fluctuations ~ 1/√N. Central limit theorem.
🔬 Больцмана розподіл
Canonical ensemble
P(E_i) = exp(-βE_i)/Z. Boltzmann factor. Partition function: Z = Σ exp(-βE_i).
Maxwell-Boltzmann
f(v) = 4πn(m/(2πk_B T))^(3/2)·v²·exp(-mv²/(2k_B T)). Velocity distribution. Ideal gas.
Ideal gas
P = nk_B T. U = 3/2 Nk_B T. Heat capacities C_V, C_P. Diatomic: rotational, vibrational modes.
Applications
Reaction rates, atmospheric physics. Kinetic theory. Transport phenomena.
⚛️ Фермі-Дірака
Distribution
f(E) = 1/(exp((E-μ)/(k_B T))+1). Pauli exclusion. Fermi energy μ ≈ E_F at T = 0.
Degenerate regime
T < T_F: Fermi degenerate. Step function f(E) at T = 0. Filled up to E_F.
Fermi gas
Metals, white dwarfs, neutron stars. T_F = ℏ²(6π²n)^(2/3)/(2mk_B). High density.
Applications
Electrons in solids, degenerate matter. White dwarfs: electron degeneracy. Chandrasekhar limit.
🌊 Бозе-Ейнштейна
Distribution
n(E) = 1/(exp((E-μ)/(k_B T))-1). Photons, phonons. No exclusion principle.
Condensation
BEC: T < T_c. Macroscopic population lowest state. ¹⁶⁷Rb, ²³Na. 1995 experiments.
Photons
μ = 0 для photons. Planck distribution: n(ν) = 1/(exp(hν/(k_B T))-1). Blackbody radiation.
Phonons
Lattice vibrations. Debye model: C_V ~ T³ для T < Θ_D. Heat capacity, thermal conductivity.
🔄 Phase transitions
Critical phenomena
Order parameter η ~ (T_c - T)^β. Correlation length ξ ~ |T-T_c|^(-ν). Scale invariance.
Symmetry breaking
Spontaneous: ferromagnetic, superconducting. Landau theory: F(η) = aη² + bη⁴.
Renormalization Group
RG flow: coarse-graining. Fixed points: critical, stable. Universality classes.
Applications
Magnetism, superconductivity, liquid-gas. Ising model, XY model, Heisenberg model.
🌊 Transport phenomena
Diffusion
Fick's law: J = -D∇n. D ~ v·l (mean free path l). Random walk: ⟨r²⟩ = 6Dt.
Viscosity
Newtonian: τ = η·(∂v/∂x). η ~ ρvl. Poiseuille flow. Reynolds number Re.
Thermal conduction
Fourier: q = -κ∇T. κ ~ cvl. Wiedemann-Franz: κ/σ ~ T. Metals.
Fluctuation-dissipation
Einstein relation: D = k_B T/(mγ). Langevin equation. Brownian motion.
📊 Графіки та діаграми
Maxwell-Boltzmann
Velocity distribution:
Ideal gas: MB distribution. Most probable, average, RMS speeds. Temperature dependent.
Fermi-Dirac
Occupancy:
Degenerate: T < T_F. Step function at T = 0. Smearing у k_B T at finite T.
f(v) = 4πn(m/(2πk_B T))^(3/2)·v²·exp(-mv²/(2k_B T)) Peak: v_mp = √(2k_B T/m) Average: v_avg = √(8k_B T/(πm)) RMS: v_rms = √(3k_B T/m)
🧪 Практичні приклади
Приклад 1: Ideal gas
Air: P = nk_B T, C_V = 3/2 Nk_B. Maxwell-Boltzmann distribution. Transport coefficients.
Приклад 2: Electron gas
Metals: Fermi energy E_F ~ 1-10 eV. Degenerate T < T_F. Heat capacity C ~ T.
Приклад 3: BEC
¹⁶⁷Rb: T_c ~ 100 nK. Macroscopic condensate. Superfluidity, coherence.
Приклад 4: Ferromagnetic transition
Ising: T_c, β ≈ 1/3. Order parameter, correlations. Critical exponents.
© 2025 Науковий Симулятор. Всі права захищені.
Статистична механіка: колективна поведінка
Try it live
Everything above runs in your browser — open SPH Fluid and change the parameters while it is running. Nothing is installed, nothing is uploaded, the whole model lives in one tab.
▶ Open SPH Fluid simulation