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of stock-tank gas is rarely measured in the field. Apparently only one
publication has addressed the problem of estimating the specific
gravities,
γ
gST
, of stock-tank gases.
4
(3.5a)
where
(3.5b)
and
(3.5c)
n
VAR
n
C0
n
C1
n
C2
n
C3
n
C4
n
1
ln
p
SP
-17.275
7.9597
-1.1013
2.7735 x 10
-2
3.2287 x 10
-3
2
ln
R
SP
-0.3354
-0.3346
0.1956
-3.4374 x 10
-2
2.08 x 10
-3
3
API
3.705
-0.4273
1.818 x 10
-2
-3.459 x 10
-4
2.505 x 10
-6
4
γ
gSP
-155.52
629.61
-957.38
647.57
-163.26
5
T
SP
2.085
-7.097 x 10
-2
9.859 x 10
-4
-6.312 x 10
-6
1.4 x 10
-8
Use of equation (3.5) requires knowledge of separator pressures and
temperatures. If this information is not available, equation (3.6) can
be used.
5
(3.6)
Evaluation of proposed correlation equations for weighted-average
surface-gas specific gravities
These two methods were evaluated with the data set described in
table 3-1, and the results are given in table 3-4. Only 618 of the lines
of data could be used because several of the laboratory reports did not
report the stock-tank gas specific gravity.
Table 3-4. Average errors in estimates of weighted-average surface-gas specific gravities are well
within expected experimental error.
Predicted weighted-average surface-gas specific gravities
ARE, %
Correlation
AARE, %
Valko-McCain (2003) equations (3.5), (3.2), and (3.4)
-0.7
2.2
Valko-McCain (2003) equation (3.6)
0.0
3.8
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