Re = ρvL/μ · flat-plate BL: laminar Re < 2×10⁵, turbulent > 5×10⁵, fully turbulent > 10⁷.
a = √(γRT), Ma = v/a · incompressible OK to Ma ≈ 0.3; subsonic <0.8, transonic 0.8–1.2, supersonic 1.2–5, hypersonic >5.
q = ½ρv² (dynamic pressure) · f = St·v/L (vortex shedding) · Kn = λ/L (continuum <0.01, slip 0.01–0.1, transitional 0.1–10, free-molecular >10).
AR = b²/S · 3-D lift slope a = a₀/(1 + a₀/(πe·AR)) · C_L = a·(α − α₀) [rad].
L = ½ρv²S·C_L · induced C_Di = C_L²/(πe·AR) · C_D = C_D0 + C_Di · D = ½ρv²S·C_D · L/D = C_L/C_D.
Thin symmetric airfoil: C_L = 2πα. Stall at the critical angle (~15–20°) — this linear model does not capture it. Elliptic e=1, tapered ≈0.9, rectangular ≈0.8.
Re_x = ρUx/μ · transition at x_tr = Re_x,tr·μ/(ρU).
Laminar (Blasius): δ = 5x/√Re_x, δ* = 1.721x/√Re_x, θ = 0.664x/√Re_x, c_f = 0.664/√Re_x.
Turbulent (1/7-power): δ = 0.37x/Re_x^0.2, c_f = 0.0592/Re_x^0.2, δ* ≈ δ/8.
Wall shear τ_w = c_f·½ρU². Turbulent BL has higher friction but resists separation (fuller profile — the golf-ball-dimple effect).