Geometry Forced, flat plate Conditions π ππΏ < 5 × 105 ππ > 0.6 Correlation Μ Μ Μ Μ Μ Μ ππ’πΏ = 0.664 π ππΏ0.5 ππ1/3 [none] π +π Μ Μ Μ Μ Μ Μ ππ’πΏ = 0.036ππ1/3 (π ππΏ0.8 − 23200) 5 × 105 < π ππΏ < 108 0.6 < ππ < 60 Forced, cylinder Notes Zukauskas ππ 0.25 π π Μ Μ Μ Μ Μ Μ ππ’π· = πΆ π ππ· ππ ( ) πππ -Properties at ππ = π ∞ 2 -Laminar flow π +π -Properties at ππ = π ∞ 2 -Mixed correlation -Properties at π∞ except πππ at ππ - πΆ, π dependent on π ππ· ππ < 10: π = 0.37 ππ > 10: π = 0.36 Forced, sphere Forced, bundle of tubes Liquid or gas 3.5 < π ππ· < 7.6 × 104 0.7 < ππ < 380 Whitaker Μ Μ Μ Μ Μ Μ ππ’π· = 2 + (0.4π ππ·0.5 -Properties at π∞ except ππ at ππ Liquid metal 3.6 × 104 < π ππ· < 2 × 105 Witte -Properties at ππ = 1 < π ππ· < 100 0.7 < ππ < 500 103 < π ππ· < 2 × 105 0.7 < ππ < 500 π 0.25 + 0.06π ππ·0.67 )ππ 0.4 ( ) ππ Μ Μ Μ Μ Μ Μ ππ’π· = 2 + 0.386(π ππ· ππ)0.5 Zukauskas-in-line tubes 0.25 ππ Μ Μ Μ Μ Μ Μ ππ’π· = 0.81 π ππ·0.4 ππ 0.36 ( ) πππ Zukauskas-staggered tubes ππ 0.25 Μ Μ Μ Μ Μ Μ ππ’π· = 0.9 π ππ·0.4 ππ 0.36 ( ) πππ Zukauskas-in-line tubes ππ ≥ 0.7: ππΏ ππ 0.25 Μ Μ Μ Μ Μ Μ ππ’π· = 0.27 π ππ·0.63 ππ 0.36 ( ) πππ Zukauskas-staggered tubes ππ < 2: ππΏ ππ 0.2 ππ 0.25 Μ Μ Μ Μ Μ Μ ππ’π· = 0.35 ( ) π ππ·0.6 ππ 0.36 ( ) ππΏ πππ ππ ≥ 2: π πΏ -Properties at πΜ = at ππ -Laminar regime ππ +π∞ 2 πππ +πππ’π‘ 2 except πππ π +π -Properties at πΜ = ππ 2 ππ’π‘ except πππ at ππ -Transition regime π -ππ < 0.7 is not an effective heat πΏ exchanger for in-line tubes Μ Μ Μ Μ Μ Μ ππ’π· = 0.40 π ππ·0.6 ππ 0.36 ( π ππ· > 2 × 105 0.7 < ππ < 500 Internal, tubes πΏ/π· > 0.05 π ππ· ππ π ππ· < 2300 πΏ/π· < 0.05 π ππ· ππ ππ = ππππ π‘ ππ > 5 π ππ· > 104 0.6 < ππ < 160 πΏ ≥ 10 π· πΊπ§π·−1 = Natural, vertical plate πΊππΏ ππ = π ππΏ < 108 π ππΏ > 1010 Natural, horizontal plat 105 < π ππΏπ < 107 Upper surface hot, lower surface cool 107 < π ππΏπ < 1010 Upper surface hot, lower surface cool 105 < π ππΏπ < 1010 Lower surface hot, upper surface cool ππ 0.25 ) πππ Zukauskas-in-line tubes 0.25 ππ Μ Μ Μ Μ Μ Μ ππ’π· = 0.021 π ππ·0.84 ππ 0.36 ( ) πππ Zukauskas-staggered tubes ππ > 1: ππ 0.25 0.84 0.36 Μ Μ Μ Μ Μ Μ ππ’π· = 0.022 π ππ· ππ ( ) πππ ππ = 0.7: Μ Μ Μ Μ Μ Μ ππ’π· = 0.019 π ππ·0.84 ππ ′′ = ππππ π‘.: Μ Μ Μ Μ Μ Μ ππ’π· = 4.36 ππ = ππππ π‘: Μ Μ Μ Μ Μ Μ ππ’π· = 3.66 Hausen 0.0668πΊπ§π· Μ Μ Μ Μ Μ Μ ππ’π· = 3.66 + 2/3 1 + 0.04 πΊπ§π· Dittus-Boelter Μ Μ Μ Μ Μ Μ ππ’π· = 0.023π ππ·0.8 ππ π Μ Μ Μ Μ Μ Μ ππ’πΏ = 0.68 ππ 0.5 πΊππΏ0.25 (0.952 + ππ)0.25 Μ Μ Μ Μ Μ Μ ππ’πΏ = 0.13 π ππΏ 1/3 Μ Μ Μ Μ Μ Μ Μ ππ’πΏπ = 0.54 π ππΏπ 1/4 -Properties at πΜ = at ππ -Turbulent regime -Properties at Μ Μ Μ Μ ππ = -Laminar, developed 2 π +ππ,π π +ππ,π -Properties at Μ Μ Μ Μ ππ = π,π 2 -max 25% error -π = 0.3 for ππ < ππ π = 0.4 for ππ > ππ π +π -Properties at ππ = π 2 ∞ -Laminar regime π +π -Properties at ππ = π ∞ 2 -Turbulent regime π +π -Properties at ππ = π ∞ ππ’πππππ ππππ πππππππ‘ππ -Properties at ππ = -πΏπ = Μ Μ Μ Μ Μ Μ Μ ππ’πΏπ = 0.27 π ππΏπ 1/4 ππ,π +ππ,π -Properties at Μ Μ Μ Μ ππ = π,π 2 -Thermal entry length -πΏπ = Μ Μ Μ Μ Μ Μ Μ ππ’πΏπ = 0.15 π ππΏπ 1/3 πππ +πππ’π‘ except 2 ππ’πππππ ππππ πππππππ‘ππ -Properties at ππ = -πΏπ = ππ’πππππ ππππ πππππππ‘ππ 2 ππ +π∞ 2 ππ +π∞ 2 πππ