Jökull

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Jökull - 01.12.1966, Qupperneq 33

Jökull - 01.12.1966, Qupperneq 33
diagram in which G’/X was plotted against LXý/G’, the quantities having the definitions given in the nomenclature. Baker recognized more sub-divisions in the flow patterns than did Kozlov, adding regions for “wave”, “strati- fied” and “plug” types. It should be emphasiz- ed, however, that for both diagrams the lines dividing adjacent flow regions are ficticious in the sense that there is no sudden change of regime from one type into the other as the nominal boundary is crossed, only a gradual transition. The Ivozlov diagram is shown in Fig. 2 and the Baker diagram in Fig. 3. On each diagram state point loci are shown for the following data. (A) Data from Iceland (Hveragerdi, Well G-7, Run 8) Mass flux 356,000 lb/hr., Exit pressure 40 psia, Base Temperature 421° F, Exit mass flow dryness fraction 0.174. (B) Data frorn New Zealand (J. H. Srnith (1958); Run 1) Mass flux 347,000 lb/hr., Exit pressure 335 psia; Base temperature 508° F, Exit mass flow dryness fraction 0.089. It will be observed that there is broad agree- ment between the two diagrams. In each case and for both wells the flow pattern changes from one of slug flow to annular dispersed or fully dispersed (mist) flow. Since the slip is unknown for both cases, A and B, it has been necessary to base the Kozlov diagram ordinates on the assumption of homogeneous flow, and the placing of the loci will be to some extent in error, particularlv towards the duct exit. (b) Methods of Evaluating Discharge (i) Method due to R.James (1962) James separated the phases at the well head and subsequently remixed them in controlled proportions before discharging the mixture to atmosphere. He obtained values of the mass flow G over a range of stagnation enthalpies 230—1200 Btu/lb for critical pressures measur- ed at the pipe exit of 14—64 psia. Pipes 3", 6" and 8" in diameter were employed. James was able, by observation of the free jet after discharge to affirm the existence of mist flow or of annular dispersed flow. Fle found he was able to correlate his results to an error of less JÖKULL 187
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