Estimate the heat, mass, and friction coefficients for a four-row cooling coil that has the geometry of Fig. 14-12 with 12 fins per inch. The face velocity of the air is 600 ft/min and has an entering temperature of 80 F. The air leaves the coil at a temperature of 60 F. The air is at standard barometric pressure.
The correlations of Figs. 14-14 and 14-15 will be used with the parameters JP, FP, J(s), and F(s) computed from Eqs. 14-46 through 14-60. The mass velocity is
∆P_{0i} = K_{i} \frac{G^{2}_{c}}{2ρ_{i}g_{c}} (14-46)
\dot{q}=h _dAη_{ms}Δ i_m (14-60)
G_{c} = \frac{60 (600) 14.5 (144)}{0.54 (53.35) 540} = 4900 lbm/(hr – ft²)
The Reynolds number based on tube diameter is then
\frac{G_{c} D}{μ} = \frac{4900 (0.525/12)}{0.044} = 4870
where data from Fig. 14-12 and Table A-4a are used. To compute the parameter A/A_{t} ,assume a four-row coil, 1 ft in length, with 10 tubes in the face. This coil has a volume of
V = \frac{10(1.25) (12) 4 (1.083)}{1728 } = 0.376 ft^{2}
and a total of 40 tubes. The total outside surface area of the tubes is
A_{t} = 40π, DL = 40π (0.525/12)(1) = 5.498 ft^{2}
From Fig. 14-12, A/V = α = 238 ft²/ft³; then
\frac{A}{A_{t}} = \frac{238(0.376)}{5.498} = 16.28
Using Eq. 14-39,
JP = Re^{-0.4}_{D} \left\lgroup \frac{A}{A_{t}}\right\rgroup ^{-0.15} (14-39)
JP = (4870)^{–0.4} (16.28)^{–0.15} = 0.022
The Reynolds number based on the fin spacing is
Re_{s} = Re_{D} \left\lgroup\frac{s}{D} \right\rgroup = 4870 \left\lgroup\frac{0.0833}{0.525} \right\rgroup = 773
Then
J(s) = 0.84 + (4 × 10^{–5})(773)^{1.25} = 1.003
and
J_{i}(s ) = [0.95 + (4 × 10^{–5}) (773)^{1.25}] \left[\frac{0.0833}{0.0833 – 0.006} \right] ^{2} = 1.293
Then
JP J(s) = 0.0220(1.003) = 0.022
and
JP J_{i}(s) = 0.0220(1.293) = 0.028
Using Fig. 14-14, j = 0.0071 and j_{i } = 0.0088.
From Eq. 14-29,
j = \frac{\bar{h}}{ G c_{p}} Pr^{2/3} (14-29)
h = \frac{j G_{c} c_{p}}{Pr^{2/3}} = \frac{0.0071 (4900) 0.24}{(0.7)^{2/3}} = 10.5 Btu/(hr – ft² – F)
and from Eq. 13-19
j_{m} = \frac{h_d}{\rho_a \overline{V}}Sc^{2/3} (13-19)
h_{d} = \frac{j_{i} G_{c}}{Sc^{2/3}} = \frac{0.0088 (4900)}{(0.6)^{2/3}} = 60.6 Ibma/(ft² – F)
The friction factor will be determined from Fig. 14-15. Using Eqs. 14-44 and 14-45,
FP = Re_{D}^{-0.25} \left\lgroup\frac{D}{D^{*}} \right\rgroup^{0.25} \left[\frac{\chi_{a} – D}{4 (s – y)} \right]^{-0.4} \left[\frac{\chi_{a}}{D^{*}} – 1\right]^{-0.5} (14-44)
D^{*} = \frac{ \left(D \frac{A}{A_{t}}\right)}{1 + \frac{\chi_{a} – D}{s}} (14-45)
D^{*} = \frac{0.525 (16.28)}{1 + (1.25 – 0.525)/0.0833} = 0.881
and
FP = (4870)^{-0.25} \left\lgroup\frac{0.525}{0.881} \right\rgroup ^{0.25} \times \left[\frac{1.25 – 0.525}{4(0.0833 – 0.006)}\right] ^{-0.4} \left[\frac{1.25}{0.881} – 1\right] = 0.116
Using Eq. 14-53,
F (s) = [1 + (Re_{s})^{-0.4}] \left\lgroup\frac{s}{s – y} \right\rgroup ^{1.5} (14-53)
F (s) = (1 + 773^{-0.4}) \left\lgroup\frac{0.0833}{0.0833 – 0.006} \right\rgroup ^{1.5}=1.20
Then
FP F(s) = 0.116(1.20) = 0.14
and from Fig. 14-15, f = 0.031.
Note that the presence of moisture on the surface increases h, h_{d}, and f.