170 CHEMICAL ENGINEERING VOLUME 1 SOLUTIONS
Forconvectionfrom the pipe, the heat loss:
qcDhcA
TsT
D 1. 65
443 2900.^25 ð 1. 131
443 290 D 1. 866
443 2901.^25 D1004 W
and the total lossD2718 W or 2.71 kW
For the insulated pipe
The heat conducted through the laggingqlmust equal the heat lost from the surface
qrCqc.
Mean diameter of the laggingD[
0. 060 C 2 ð 0. 050 C 0 .060]/ 2 D 0 .110 m
at which the areaD
$ð 0. 110 ð 6. 0 D 2 .07 m^2
and in equation 9.12:qlD 0. 07 ð 2. 07
443 Ts/ 0. 050 D
1280 2. 90 Ts W
whereTsis the surface temperature.
The outside areaD$
0. 060 C 2 ð 0. 050 ð 6. 0 D 3 .016 m^2
and from equation 9.119 :qrD
5. 67 ð 10 ^8 ð 0. 85 ð 3. 016
T^4 s 2904
D 1. 456 ð 10 ^7 T^4 sD1030 W
and: qcD 1. 65
Ts 2900.^25 ð 3. 016
Ts 290
D 4. 976
Ts 2901.^25 W
Making a heat balance:
1280 2. 90 Ts D
1. 456 ð 10 ^7 T^4 s 1030 C 4. 976
Ts 2901.^25
or: 4. 976
Ts 2901.^25 C
- 456 ð 10 ^7 T^4 s C 2. 90 TsD 2310
Solving by trial and error:TsD305 K
and hence the heat lostD
1280 2. 90 ð 305 D396 W.
The heat saved by lagging the pipeD
2712 396 D2317 W or 2.317 kW.
At 800 kN/m^2 , the latent heat of steam is 2050 kJ/kg
and the reduction in the amount of steam condensedD
2. 317 / 2050 D 0 .00113 kg/s
or:
0. 00113 ð 3600 ð 24 ð 365 D 35 ,643 kg/year
∴ annual savingD
35 , 643 ð 0. 5 / 100 D£178/year
It may be noted that arithmetic mean radius should only be used with thin walled tubes,
which is not the case here. If a logarithmic mean radius is used in applying equation 9.8,
TsD 305 .7 K and the difference is, in this case, negligible.