| name | convection |
| description | Convection heat transfer — forced internal/external, natural convection, boundary layers, Nusselt number correlations (Dittus-Boelter, Churchill-Bernstein, etc.), boiling, condensation. |
| metadata | {"priority":7,"promptSignals":{"phrases":["convection","Nusselt","heat transfer coefficient","forced convection","natural convection","boundary layer","boiling","condensation"],"minScore":4}} |
Convection Heat Transfer — Complete Skill
Key Dimensionless Numbers
Re = ρVL/μ = VL/ν (Reynolds — inertia/viscous)
Nu = hL/k (Nusselt — convection/conduction)
Pr = μc_p/k = ν/α (Prandtl — momentum/thermal diffusivity)
Gr = gβΔTL³/ν² (Grashof — buoyancy/viscous for natural convection)
Ra = Gr·Pr (Rayleigh)
St = Nu/(Re·Pr) = h/(ρVc_p) (Stanton)
Property evaluation: use film temperature T_f = (T_s+T_∞)/2 unless noted
Viscosity correction: (μ/μ_s)^0.14 for liquids with large T variation
External Forced Convection
Flat plate (laminar, Re_L < 5×10⁵):
Local: Nu_x = 0.332·Re_x^0.5·Pr^(1/3) (Pr ≥ 0.6)
Average: Nu_L = 0.664·Re_L^0.5·Pr^(1/3)
δ_thermal = δ_velocity·Pr^(-1/3)
Flat plate (turbulent, Re > 5×10⁵):
Local: Nu_x = 0.0296·Re_x^0.8·Pr^(1/3)
Mixed (transition at Re_c=5×10⁵): Nu_L = (0.037·Re_L^0.8 - 871)·Pr^(1/3)
Cylinder in crossflow (Churchill-Bernstein):
Nu = 0.3 + 0.62·Re^0.5·Pr^(1/3)/(1+(0.4/Pr)^(2/3))^0.25 · (1+(Re/282000)^(5/8))^(4/5)
Valid: Re·Pr > 0.2
Sphere (Whitaker):
Nu = 2 + (0.4·Re^0.5 + 0.06·Re^(2/3))·Pr^0.4·(μ/μ_s)^0.25
Valid: 3.5 ≤ Re ≤ 7.6×10⁴, 0.71 ≤ Pr ≤ 380
Internal Forced Convection (Pipe/Duct)
Entry length:
Hydrodynamic: L_h = 0.05·Re·D (laminar), L_h/D ≈ 10-60 (turbulent)
Thermal: L_t = 0.05·Re·Pr·D (laminar)
Laminar, fully developed:
Constant T_s: Nu = 3.66
Constant q''_s: Nu = 4.36
Combined entry: Nu = 3.66 + 0.0668(D/L·Re·Pr)/(1+0.04(D/L·Re·Pr)^(2/3)) (Hausen)
Turbulent, fully developed (Re > 10,000, 0.6 < Pr < 160):
Nu = 0.023·Re^0.8·Pr^n (Dittus-Boelter): n=0.4 (heating), n=0.3 (cooling)
Nu = (f/8)(Re-1000)Pr / (1+12.7√(f/8)(Pr^(2/3)-1)) (Gnielinski, more accurate)
f = (0.790·ln(Re)-1.64)^(-2) (Petukhov)
Non-circular ducts: Use D_h = 4A_c/P (hydraulic diameter)
Annulus: D_h = D_o - D_i
Temperature rise for constant heat flux:
T_s(x) - T_m(x) = q''_s/h_x [constant for fully developed]
T_m(x) = T_m,in + q''_s·P·x/(ṁ·c_p)
Natural Convection
Vertical plate (Churchill-Chu):
Nu = (0.825 + 0.387·Ra^(1/6)/(1+(0.492/Pr)^(9/16))^(8/27))² [all Ra]
β = 1/T_f [ideal gas], β ≈ 0.00341 K⁻¹ (air at 20°C)
Horizontal cylinder:
Nu = (0.60 + 0.387·Ra^(1/6)/(1+(0.559/Pr)^(9/16))^(8/27))²
Sphere:
Nu = 2 + 0.589·Ra^(1/4)/(1+(0.469/Pr)^(9/16))^(4/9)
Horizontal plate:
Hot side up or cold side down (Ra: 10⁴-10⁷): Nu = 0.54·Ra^(1/4)
Hot side up or cold side down (Ra: 10⁷-10¹¹): Nu = 0.15·Ra^(1/3)
Hot side down or cold side up: Nu = 0.27·Ra^(1/4)
Mixed convection: Gr/Re² >> 1 → natural; << 1 → forced; ~1 → mixed
Nu_combined = (Nu_forced^n ± Nu_natural^n)^(1/n), n=3 (vertical), ± (assist vs. oppose)
Pool Boiling (Nukiyama curve)
Free convection: q'' = h·(T_s-T_sat), h from natural convection
Nucleate boiling (Rohsenow):
q'' = μ_l·h_fg·(g(ρ_l-ρ_v)/σ)^0.5 · (c_pl(T_s-T_sat)/(C_sf·h_fg·Pr_l^n))³
C_sf = surface-fluid constant (0.006 for water-Cu polished)
Critical heat flux (Zuber):
q''_max = 0.131·ρ_v·h_fg·(σ·g(ρ_l-ρ_v)/ρ_v²)^0.25
q''_max ≈ 1.2 MW/m² for water at 1 atm
Minimum heat flux (Berenson):
q''_min = 0.09·ρ_v·h_fg·(σ·g(ρ_l-ρ_v)/(ρ_l+ρ_v)²)^0.25
Film boiling:
Nu_D = 0.62·(ρ_v(ρ_l-ρ_v)g·h''_fg·D³/(μ_v·k_v·(T_s-T_sat)))^0.25
h''_fg = h_fg + 0.80·c_pv·(T_s-T_sat)
Film Condensation (Nusselt Theory)
Vertical plate:
h̄ = 0.943·(ρ_l(ρ_l-ρ_v)g·h'_fg·k_l³/(μ_l·L·(T_sat-T_s)))^0.25
h'_fg = h_fg + 0.68·c_pl·(T_sat-T_s) (modified latent heat)
Horizontal cylinder:
h̄ = 0.725·(ρ_l(ρ_l-ρ_v)g·h'_fg·k_l³/(μ_l·D·(T_sat-T_s)))^0.25
Turbulent condensate (Re_f > 1800):
h = k_l/L·(Re_f/4)^0.4·Pr_l^(-0.4)/(Re_f^0.5 - 5.82×10⁻²)
Output
Provide: Nu, h [W/m²K], q [W], temperature at key locations, correlation used and its validity range.