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INDUSTRIES
PPG INDUSTRIES, INC.
INDUSTRIAL CHEMICAL DIVISION
P. 0. BOX 1000
LAKE CHARLES, LA. 70601
October 19, 1971
Mr. Dick Churns Continental Oil Company P. O. Box 37 Westlake, Louisiana 70669
Dear Mr. Churns:
Attached is a tabulation of manual versus computer calculations of chlorine delivery for the month of July. In August we stopped hand calculations.
I hope that this will answer your questions. If you need any other information, please call us.
Very truly yours.
AMC :edh Attachment
CCR 000038710
f f **33-670077 E2V0E/2E0ASSEUFP
CHLORINE TO CONOCO
............ ............ ..
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Manual
Computer
Calculation Calculat ion
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CCR 000038713
* INDUSTRIES
SEND COPRcSPONDtNCE TO. PPG INDUSTRIES, INC . P O 30a ! 000, IA.XE CHARLES, LA 7060 I
in;p^?SNo
'Customer ord?r no
J11` S1'i = F=0
700653C
S!CCNTI:JE:4TAL oil CO DIV 713753 B0X 197, PURCHASING DEPT ^HOUSTON, TEXAS 77001
! elste--`h :o:c
1837200
NY-2134
\ Cl AS) j 7n,/,,
1 net 30
AUGUST-C 8-791 23801 3-31-71
sCCNTIllENTAL OIL CO "WESTLAKE, LOUISIANA
PIPELINE
lOfST'^A- .:n ;
|507017001
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LC
03 LC
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Gaseous Chlorine delivered
through pipe line for the month of August, 1971
30,971,700#
USS DIAMOND EXCHANGE
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Barges
5,545,^00#
Tank Cars
3,740,000#
OJC -O
21,636,300# 40.00 433,726.00 1 NT
Plus 2.00NT Handling Charge for Unloading 1692.7 Tons
3,385.40
'(
437,111.40
o 4 * -( .
j
1
CCR 00387l4
x INVOICE COPY
We hereby certify that these goods were produced m compliance with oil applicable requirement! of section* 6, 7, and 1 2 ot *he Foir Labor Standard! Act, a* emended, and of reg^ioT;on> and orders of the United State* Deportment of Labor issued under section 14 thereof
ALL CLAIMS MUST BE SUPPORTED BY BILL OF LADING AND FREIGHT BILL SEE REVERSE SIDE
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CALCULATE;;-; SHEET
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CONTINENTAL OIL COMPANY :: A L. C U A A T j o N S MEET
Job No . ..Si ^te
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Calculations for Steam, Vapor, or Gas
' 351
SPECIFIC WEIGHTS OF GASES AND VAPORS
Compressibility. No gas or vapor follows the simple laws of Boyle and Charles exactly. The deviation from these laws is called compressibility.
A number of formulae based on theoretical considerations have been developed to supplant Boyle's and Charles' laws at high, pressure, but all are cumbersome to use and none gives an exact result over a wide range of conditions for all gases and vapors.
The theorem of corresponding states correlates the deviation from Boyle's and Charles' laws with the ratios of temperature and pressure to pseudocritical temperature and pressure This correla tion is defined by the value of Z shown in Figures B-2519 to B-2524, pages 355-60 inclusive. These Z values substituted in Eq. 47 will give a more accurate value for y/ the specific weight at flowing conditions.
For gases of known molecular weight, mv the specific weight can be computed from the formula
7/ " 10.73T/Z/
^Eq- 47J
in which pf is the flowing pressure, psia; 7/ is flowing absolute temperature R. F. + 460; and Z/ is the compressibility ratio at flowing conditions.
When measuring gar in volume units, both base and flowing conditions must be correcled when usin? combressibihty ratio data. On wet gas, Zb the compressibility ratio at base conditions may be appreciably less than 1.0. The combined correction factor is Fav. (See pp. 402,' 403, and 411.)
If a specific gravity. G,, calculated from the known m- of the gas as is common when measuring some industrial gases[ is sub stituted for G in the gas flow equations,
51)
The specific gravity of natural gas is usually determined by test. Hence, G includes any effect of compressibility at test conditions and m,, * 29GZ*. Substituting in Eq. 47,
29pjGZh 2J02pfGZb 7/ " 10.73 7/Z/ " T,Zj
(Eq. 50)
352 Steam Flow Measurement
Since yj is a half power term in the flow equation (see Eq. 78, p. 406), the supercompressibility factor when using an experimen tally determined specific gravity is
(Eq. 51a)
CHARTS USED TO DETERMINE Z
Figure B-2518, page 353, is a chart based on the average char acteristics of refinery gas. It permits the quick reading of an estimated value of reduced pressure (pr) and reduced temperature, { Tr) for the use of the compressibility curves, if the flowing fluid is a refinery gas. Follow up the abscissa corresponding to the flowing temperature to the diagonal line corresponding to the molecular weight of the gas or vapor, and read from the ordinate the value of Tr. Determine p, in a similar manner. Refer these values to the compressibility curve of the most readable reduced pressure range and read the value of Zf for use in Eq. 47, page 351.
If the composition of the gas is known, the pseudocritical ab solute temperature (Tca) and the pseudocritical absolute pressure (pe) should be estimated from a weighted average of the critical constants on a volumetric or mol fraction basis .
(Eq. 28)
A-S
(Eq. 27)
Figures B-2519 to B-2524, pages 355-60 inclusive, show the aver age correlation according to the theorem of corresponding states of the 30 gases and vapors listed in Table 28, page 354, except as listed. From the correlations, it would appear that these curves could be used with reasonable accuracy for most gases. The exceptions listed under the titles should be observed.
More accurate correlations for some conditions may be obtained from plots based on kinetic parameters. If interested in further study of the subject, see Reference No. 30, page 537.
Figures B-2519, B-2520, B-2521, B-2522, B-2523, and B-2524, pages 355-60, are the Compressibility Charts 6f Nelson and Obert, Northwestern Technological Institute, Evanston, III.
VIII. GRAVITY CORRECTION FACTOR,
In the chlorine supply contract It is stated that "The gravity correction factor. F^, will be the calculated ideal specific gravity using molecular weights and calculated daily from the gas composition.11"-
Therefore, subroutine'"FACTG" computes Fq by the equation
(5)
= Vol. fraction of component i by daily analysis Mj = Molecular weight of component i When xi does not equal 1, the balance is assumed to be air.
IX. SUPERCOMPRESSIBILITY FACTOR, Fpv By definition, the supercompressibility factor ?s
(6)
Where Zg is the compressibility factor of the metered gas at standard conditions (60F. and 14.73 PSIA), and Zp Is the compressibility factor at actual flow temperature and pressure.
Subroutine "FACTZ" contains a table of components compressibility factors at 60F. and 14.73 PSIA. They are:
Chlorine Carbon Dioxide Nitrogen Oxygen Hydrogen Carbon Monoxide Air
h == 0.98790 Z2 0.99536 Z3 = 0.99922 *4 a 0.99892 Z5 1.00068 z6 - 0.99906 z7 a 0.99917
Calculation starts by computing Zg
z,, *
5* z>
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-8-
000038726 ^CCR
Then the compressibility factors at actual flow temperature and pressure are calculated by calling two special subprograms. They are
*ZCHLR" for compressibility factor of Cl2 "ZINER" for compressibility factors of all other components
Then the value of Zp f$ computed by
ZF =
Zx,.ZF1
(8)
And Fpy ts calculated by Equation 6.
X. COMPRESSIBILITY FACTOR OF CHLORINE
According to the chlorine supply contract, the compressibility ciT chlorine is
calculated as ?n Kapoor-Martin Thermodynamic Proeerties of Chlorine, University of Michigan Press, 1957. In this kook the gaseous volumes are calculated by the
Martin-Hou equat?on-of-state.
T
5 4r
-K Tc -|
3
P(V-b) - RT(V-bf -A2 + B2T +C2 e C I (V-b) -
- [*3 + V +C3e`KTc ] (V-b) - A4 (V-b) -
* [V + V '^J = 0
Special subroutine "ZCHLR" solves Equation 9 by a trial-and-error method based upon Newton-Raphson Algorithm. Since Equation 9 is of the fifth order for V, it has five roots. In order to avoid that the solution may diverge toward an un wanted root,provision is introduced so that the solution be in the range of compressi bility 0.275 (critical point) to 1.5.
The constants for Equation 9, as given by Hapoor-Martin, are as follows:
A2 = 0.46496772246 . . B2 = 2.129865506x 10 C2 = 0.098636526 A3 = 8.8856032387 x10"3 B3 = 0.35635855479 x 10"5 C3 = 2.252937606 x 1 O'3 A4 = 6.60499557 x 10*5 B5 = 0.3692381884 x 10-9
C5 = 0.45521856137 x 10"^ R * 0.010296 (ATM)(CuFt.)/(Lb)(-dR) b = 0.00608353
K = 2.3 Tc * 750.9 R
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