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4.2 JET PUMP APPLICATIONS 4.47
TABLE 10 Steam consumption of steam-jet siphons, lb/h
a
Siphon
Operating steam pressure, lb/in
2
(bar) gage
size, in Capacity 40 50 60 80 100 120 160 240
(mm) ratio (2.8) (3.4) (4.1) (5.5) (6.9) (8.3) (11.0) (16.5)
(12.7) 0.125 40 47 54 69 83 97 126 84
(19.1) 0.222 70 83 96 122 147 173 222 322
1 (25.4) 0.346 110 130 150 190 230 270 350 510
1 (38.1) 1.000 318 376 434 550 665 780 1,012 1,475
2 (50.8) 1.38 440 520 600 761 920 1,080 1,400 2,040
2 (63.5) 2.0 635 750 865 1,100 1,329 1,558 2,020 2,940
3 (76.2) 3.11 990 1,170 1,350 1,710 2,065 2,425 3,145 4,590
4 (102) 5.54 1,760 2,085 2,400 3,045 3,685 4,320 5,500 8,170
6 (152) 12.45 3,960 4,680 5,400 6,850 8,280 9,710 12,600 18,360
a
Lb/h 0.454 kg/h
Source: Schutte and Koerting.
1
2
1
2
3
4
1
2
TABLE 11 Relative capacities of annular siphons
Capacity of standard 3-in (76.2-mm) siphon,
water temperature 100°F (37.8°C), 0 suction lift
Steam pressure, lb/in
2
(bar) 50 (3.45) 75 (5.17) 100 (6.90) 125 (8.62)
gage
Steam consumption, lb/h 1180 (535) 1620 (735) 2060 (934) 2490 (1130)
(kg/h)
Max back pressure, lb/in
2
(bar) 12 (0.83) 18 (1.24) 22 (1.52) 35 (2.41)
gage at zero flow
Suction capacity, gpm (m
3
/h) 140 (31.8) 130 (29.5) 120 (27.2) 110 (25)
Discharge pressure, lb/in
2
5 (0.34) 8 (0.55) 12 (0.83) 30 (2.07)
(bar) gage
Relative capacities of standard sizes
Size, in 1 1 2 2 3 4 6 8
(mm) (31.8) (38.1) (50.8) (63.5) (76.2) (102) (152) (203)
Capacity
ratio 0.13 0.21 0.30 0.60 1.00 1.85 4.0 7.1
Source: Schutte and Koerting.
1
2
1
2
1
4
Small units (less than 1 gpm, 0.23 m
3
/h) can be supplied for limited discharge pres-
sures, as indicated by Figure 21.With air as the motive fluid, the suction liquid can be very
close to its boiling point and only a very slight NPSH is required.
When air is used as a motive fluid, the smaller sizes operate more efficiently because
the air is more intimately mixed with a suction fluid. In larger sizes, the tendency is for
the fluid to be discharged in slugs because intimate mixing does not readily occur. This
has a detrimental effect on the performance and especially on available discharge head.
Air-Lift Eductors Air-lift pumps are frequently used for difficult pumping operations.
Compressed air is forced into the bottom of a pipe submerged in the liquid to be pumped.
The expanding air, as it rises up the pipe, entrains the suction fluid.
If compressed air is not available, it is possible to lift water higher than 34 ft (10 m)
with the use of an eductor-air-lift combination. Figure 22 illustrates the suction capacity