dimensional-analysis

Layer 1 — Physics24 concepts in this subtree

Model-free analysis of physical equations by tracking the units of measurement (M, L, T, Θ, I, N, J) of each variable. Core theorem: Buckingham 1914 π-theorem — a physical relation F(q_1,…,q_n)=0 among n dimensioned quantities with…

Buckingham 1914 π-theorem: n−r independent dimensionless groups
Reynolds-number similarity: laminar ↔ turbulent transition at Re ~ 2300
Rayleigh-Bénard convection onset at dimensionless threshold Ra_c
Pipe-flow π-count: 5 variables, rank 3 → 2 π-groups
Reynolds-number value at reference state and its laminar/turbulent ratio
Rayleigh-Bénard free-free critical Rayleigh number Ra_c = 27π⁴/4
Kolmogorov -5/3 law: E(k) = C_K * epsilon^{2/3} * k^{-5/3} via scaling-group dimensional analysis
Nusselt-Rayleigh scaling law: Nu = C_N * Ra^{1/3} for high-Ra turbulent Rayleigh-Benard convection
Vaschy-Buckingham Pi-theorem: n variables with k independent dimensions reduce to n-k dimensionless groups
Theorem: Kolmogorov E(k) = C_K*epsilon^(2/3)*k^(-5/3) unit check L^3 T^{-2}
Theorem: Nusselt-Rayleigh Nu = C_N*Ra^(1/3) has log-slope d(ln Nu)/d(ln Ra) = 1/3
Theorem: Reynolds number Re = rho*U*L/mu is dimensionless; exponent sums (M,L,T) = (0,0,0)
Buckingham Pi theorem (1914)
Rayleigh method (1899)
Reynolds number (1883)
Planck natural units (1899)
Similitude (Froude / Mach / Weber / Bond)
Anomalous dimensions (RG)
Rayleigh method (1899)
Buckingham π detail (1914)
Reynolds (1883)
Strouhal (1878)
EFT-dimensional (Weinberg 1979)
Sedov-Taylor (1946)
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