7-129 The top surface of a hot block is to be cooled by forced air. The rate of heat transfer is to be determined for two cases.
Assumptions 1 Steady operating conditions exist. 2 The critical Reynolds number is Recr = 5105. 3 Radiation effects are
negligible. 4 Air is an ideal gas.
Properties The properties k, , cp, and Pr of ideal gases are independent of pressure, while the properties and are
inversely proportional to density and thus pressure. The properties of air at the film temperature of Tf= (Ts+ T
)/2 =(140 +
20)/2 = 80°C and 1 atm pressure are (Table A–15):
k = 0.02953 W/m · K, Pr = 0.7154, @ 1 atm = 2.09710-5 m2/s
The atmospheric pressure in Denver is P = (83.4 kPa)/(101.325
kPa/atm) = 0.823 atm. Then the kinematic viscosity of air in Denver
becomes: = @ 1 atm /P = (2.097 10-5 m2/s)/0.823 = 2.548 10-5 m2/s
Analysis (a) When air flow is parallel to the long side,
we have L= 6 m, andthe Reynolds number at the end of
the plate becomes
6
25 10884.1
/sm 10548.2
)m 6)(m/s 8(
Re =
== −
VL
L
which is greater than the critical Reynolds number.
Thus, we have combinedlaminar and turbulent flow, and
the average Nusselt number for the entire plateis
determined to be
2687)7154.0](871)10884.1(037.0[Pr)871Re037.0(Nu 3/18.063/18.0 =−=−== L
k
hL
K W/m2.13
m 6
K W/m02953.0
)2687(2=
== L
k
Nuh
𝐴𝑠 = wL = (1.5 m)(6 m) = 9 m2
W10 1.43 4
−=−= =C20)(140)m)(9 W/m2.13()( 22 KTThAQss
Note that if we disregarded the laminar region and assumed turbulent flow overthe entire plate, we would get Nu = 3466 from
Eq. 7–22, which is 29 percenthigher than the value calculated above.
(b) When air flow is along the short side, we have L = 1.5 m, and the Reynoldsnumber at the end of the plate becomes