94 ENGINEERING THERMODYNAMICSDharm
\M-therm/th3-2.p65which now has a higher dryness fraction, is passed through the throttling calorimeter. With the
combined separating and throttling calorimeter it is necessary to condense the steam after throt-
tling and measure the amount of condensate (ms). If a throttling calorimeter only is sufficient,
there is no need to measure condensate, the pressure and temperature measurements at exit being
sufficient.
Separating
calorimeterOutletCooling water
inlet
msThrottle
valvep,h 33p , x , h 222T 3
Steam p, x 11
main
xp 1 PressuremwFig. 3.17. Separating and throttling calorimeter.
Dryness fraction at 2 is x 2 , therefore, the mass of dry steam leaving the separating calorim-
eter is equal to x 2 ms and this must be the mass of dry vapour in the sample drawn from the main
at state 1.
Hence fraction in main, x xm
mms
ws1 ==^2 +Mass of dry vapour
Total mass.
The dryness fraction, x 2 , can be determined as follows :
*hhh xh 32 f 2 fg
== + 22 at p 2 [()]
*hh h cT T p
3 =+ +f 33 fg pssup 33 −s at pressure 3or xhh
hf(^2) fg
(^32)
2
−
The values of hf 2 and hfg 2 are read from steam tables at pressure p 2. The pressure in the
separator is small so that p 1 is approximately equal to p 2.
Example 3.27. The following observations were taken with a separating and a throttling
calorimeter arranged in series :
Water separated = 2 kg, steam discharged from the throttling calorimeter = 20.5 kg, tem-
perature of steam after throttling = 110°C, initial pressure = 12 bar abs., barometer = 760 mm of
Hg, final pressure = 5 mm of Hg.
Estimate the quality of steam supplied.
Solution. Quantity of water separated out, mw = 2 kg
Steam (condensate) discharged from the throttling calorimeter, ms = 20.5 kg
Temperature of steam after throttling, tsup = 110°C
Initial pressure of steam, p 1 = 12 bar abs.