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2000 Hook-up Book - Spirax Sarco

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SYSTEM DESIGN<br />

46<br />

Condensate Recovery Systems<br />

have been sized using water volume<br />

only and did not include the<br />

flash steam volume that is present.<br />

The specific volume of water<br />

at 0 psig is .017 cubic feet per<br />

pound, compared to 26.8 cubic<br />

feet per pound for flash steam at<br />

the same pressure. Sizing of condensate<br />

return lines from trap<br />

discharges based totally on water<br />

is a gross error and causes lines<br />

to be drastically undersized for<br />

the flash steam. This causes condensate<br />

lines to become<br />

pressurized, not atmospheric,<br />

which in turn causes a backpressure<br />

to be applied to the trap’s<br />

discharge which can cause<br />

equipment failure and flooding.<br />

This undersizing explains<br />

why the majority of 0 psi atmospheric<br />

condensate return<br />

systems in the United States do<br />

not operate at 0 psig. To take this<br />

thought one step further for those<br />

people who perform temperature<br />

tests on steam traps to determine<br />

if the trap has failed, the instant<br />

we cause a positive pressure to<br />

develop in the condensate return<br />

system by flash steam, the condensate<br />

return line now must<br />

follow the pressure/temperature<br />

relationship of saturated steam.<br />

So, trap testing by temperature<br />

identifies only that we have a<br />

return system at a certain temperature<br />

above 212°F (0 psig)<br />

and we can then determine by<br />

that temperature the system<br />

pressure at which it is operating.<br />

Elevated condensate return temperatures<br />

do not necessarily<br />

mean a trap has failed.<br />

When sizing condensate<br />

return lines, the volume of the<br />

flash steam must be given due<br />

consideration. The chart at Fig.<br />

51 (page 43) allows the lines to<br />

be sized as flash steam lines—<br />

since the volume of the<br />

condensate is so much less than<br />

that of the steam released.<br />

Draining condensate from<br />

traps serving loads at differing<br />

pressures to a common condensate<br />

return line is a concept<br />

which many find difficult. It is<br />

often assumed that the HP “high<br />

pressure” condensate will prevent<br />

the “low pressure” condensate<br />

from passing through the LP<br />

traps and give rise to waterlogging<br />

of the LP system.<br />

However, the terms HP and<br />

LP can only apply to the conditions<br />

on the <strong>up</strong>stream side of the<br />

seats in the traps. At the downstream<br />

or outlet side of the traps,<br />

the pressure must be the common<br />

pressure in the return line.<br />

This return line pressure will be<br />

the sum of at least three components:<br />

1. The pressure at the end of<br />

the return line, either atmospheric<br />

or of the vessel into<br />

which the line discharges.<br />

2. The hydrostatic head needed<br />

to lift the condensate <strong>up</strong> any<br />

risers in the line.<br />

3. The pressure drop needed to<br />

carry the condensate and<br />

any flash steam along the<br />

line.<br />

Item 3 is the only one likely to<br />

give rise to any problems if condensate<br />

from sources at different<br />

pressures enters a common line.<br />

The return should be sufficiently<br />

large to carry all the liquid condensate<br />

and the varying amounts<br />

of flash steam associated with it,<br />

without requiring excessive line<br />

velocity and excessive pressure<br />

drop. If this is accepted, the total<br />

return line cross sectional area<br />

will be the same, whether a single<br />

line is used, or if two or more lines<br />

are fitted, with each taking the<br />

condensate from a single pressure<br />

source.<br />

The return could become<br />

undersized, requiring a high pressure<br />

at the trap discharges and<br />

restricting or preventing discharge<br />

from the LP traps, if it is<br />

forgotten that the pipe has to<br />

carry flash steam as well as water<br />

and that flash steam is released<br />

in appreciable quantity from HP<br />

condensate.<br />

While the percentage, by<br />

weight, of flash steam may be<br />

rather low, its overall volume in<br />

comparison to the liquid is very<br />

large. By determining the quantity<br />

of flash steam and sizing the<br />

return line for velocities between<br />

4,000 and 6,000 ft/min, the twophase<br />

flow within the pipe can be<br />

accommodated. The information<br />

required for sizing is the condensate<br />

load in lb/h, inlet pressure to<br />

steam trap(s) in psig and return<br />

line system pressure.<br />

Example:<br />

Size a condensate return line<br />

from a 160 psig steam trap discharging<br />

to 20 psig. flash tank.<br />

Load is 3,000 lb/h.<br />

1. Determine percent flash<br />

steam produced using Table<br />

12 (page 41). With a steam<br />

pressure of 160 psig and a<br />

flash tank pressure of 20 psig<br />

read a value of 12.4%.<br />

2. Next, multiply the condensate<br />

load by the percent flash from<br />

step #1 to determine the<br />

flowrate, of flash steam produced.<br />

3,000 lb/h x .124 = 372 lb/h.<br />

3. Enter Fig. 51 (page 43) at the<br />

flash steam flowrate of 372<br />

lb/h at “A” and move horizontally<br />

to the right to the flash<br />

tank pressure of 20 psig “B”.<br />

Rise vertically to choose a<br />

condensate return line size<br />

which will give a velocity<br />

between 4,000 and 6,000<br />

ft/min, “C”. In this example, an<br />

1-1/2” schedule 40 pipe with<br />

a velocity of approximately<br />

5,000 ft/min. If schedule 80<br />

pipe is to be used, refer to<br />

table within body of chart.<br />

Multiply the velocity by the<br />

factor to determine whether<br />

the velocity is within acceptable<br />

limits.

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