fundamentals of engineering supplied-reference handbook - Ventech!
fundamentals of engineering supplied-reference handbook - Ventech!
fundamentals of engineering supplied-reference handbook - Ventech!
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Use the cylinder diameter in the evaluation <strong>of</strong> the Nusselt<br />
and Reynolds numbers.<br />
Re n c<br />
1 – 4<br />
4 – 40<br />
40 – 4,000<br />
4,000 – 40,000<br />
40,000 – 250,000<br />
0.330<br />
0.385<br />
0.466<br />
0.618<br />
0.805<br />
0.989<br />
0.911<br />
0.683<br />
0.193<br />
0.0266<br />
For flow past a constant-temperature sphere.<br />
Nu = 2.0 + 0.60Re 0.5 Pr 1/3<br />
(1 < Re < 70,000, 0.6 < Pr < 400)<br />
Use the sphere diameter in the evaluation <strong>of</strong> the Nusselt and<br />
Reynolds numbers.<br />
Conductive Heat Transfer<br />
Steady Conduction with Internal Energy Generation<br />
For one-dimensional steady conduction, the equation is<br />
2<br />
2<br />
d T/dx + Qgen<br />
k = 0 � , where<br />
Qgen � = the heat generation rate per unit volume, and<br />
k = the thermal conductivity.<br />
For a plane wall:<br />
T<br />
Q�<br />
Q�<br />
Q�<br />
L<br />
2<br />
⎛ x<br />
−<br />
⎝<br />
2<br />
⎞<br />
⎛ T − T<br />
⎞⎛<br />
x ⎞<br />
⎛ T + T<br />
gen<br />
( ) ⎜ ⎟ s2<br />
s1<br />
s1<br />
s2<br />
x = 1 + ⎜ ⎟⎜<br />
⎟ + ⎜ ⎟<br />
2k ⎜ 2<br />
L ⎟ 2 ⎝ L ⎠ 2 ⎠<br />
" "<br />
Q Q 2Q L � � � + = , where<br />
1<br />
2<br />
( dT dx)<br />
L<br />
k(<br />
dT dx)<br />
L<br />
"<br />
1 = k −<br />
"<br />
2 = −<br />
⎠<br />
gen<br />
For a long circular cylinder:<br />
⎝<br />
⎠<br />
⎝<br />
⎞<br />
70<br />
1<br />
r<br />
T<br />
d<br />
dr<br />
dT Q�<br />
⎛ ⎞ gen<br />
⎜r<br />
⎟ + = 0<br />
⎝ dr ⎠ k<br />
Q�<br />
2<br />
r ⎛ 2<br />
r ⎞<br />
−<br />
k ⎜ 2 4 r ⎟<br />
⎝ 0 ⎠<br />
gen 0<br />
() r = ⎜1<br />
⎟ + Ts<br />
r Q�<br />
′ = π � , where<br />
2<br />
0 gen Q<br />
HEAT TRANSFER (continued)<br />
Q′ � = the heat-transfer rate from the cylinder per unit<br />
length.<br />
Transient Conduction Using the Lumped Capacitance<br />
Method<br />
If the temperature may be considered uniform within the<br />
body at any time, the change <strong>of</strong> body temperature is given<br />
by<br />
� hA T − T = −ρc<br />
V dT dt<br />
( ) ( )<br />
Q = s ∞ p<br />
The temperature variation with time is<br />
−(<br />
hAs / ρcpV<br />
)t<br />
T – T∞ = (Ti – T∞) e<br />
The total heat transferred up to time t is<br />
Qtotal = ρcPV (Ti – T), where<br />
ρ = density,<br />
V = volume,<br />
cP = heat capacity,<br />
t = time,<br />
As = surface area <strong>of</strong> the body,<br />
T = temperature, and<br />
h = the heat-transfer coefficient.<br />
The lumped capacitance method is valid if<br />
Biot number = Bi = hV/kAs