ML20070P098
| ML20070P098 | |
| Person / Time | |
|---|---|
| Site: | Mcguire |
| Issue date: | 09/28/1982 |
| From: | DUKE POWER CO. |
| To: | |
| Shared Package | |
| ML20070P093 | List: |
| References | |
| NUDOCS 8301260141 | |
| Download: ML20070P098 (191) | |
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INTEGRATED LEAK RATE TEST s CONDUCTED SEPTEMBER 23-28, 1982 i
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TABLE OF CONTENTS Section Dafinition.of Symbols and Abbreviations I Introduction II Test Purpose III Summary IV Test Organization V Test Background Information VI Test Method Calculation Technique Test Activity Flow Chart Test Acceptance Criteria and Test Result Results of Type B & C Leak Rate Tescs Test Equipment VII Instr'anent Specifications Computer Program Instrument Error Analysis Conclusion VIII ILRT F1,ures IX RTD Locations X Appendix A Deviations and Formulas for McGuire Containment Leak Rate Computations B Raw and Processed Data C Minute of Test Events (Test Log)
D Attachments to Test Log
-I-DEFINITION OF SYMBOLS AND ABBREVIATIONS ILRT Integrated Leak Rate Test E Repeatability error e Absolute error I Measurement system error F Temperature, degrees Fahrenheit FOM Figure of Merit L Maximum allowable leakage rate A
L Containment leak rate during 24 hour2.777778e-4 days <br />0.00667 hours <br />3.968254e-5 weeks <br />9.132e-6 months <br /> ILRT (UCL) + Lg L Imposed leak rate for verification O
L C
n a ame ea ra e ur ng ver f cation L Total measured leak rate during 24 hour2.777778e-4 days <br />0.00667 hours <br />3.968254e-5 weeks <br />9.132e-6 months <br /> ILRT OBSRVD L
OBSRVD(95%)
95% Upper Confidence Valve of measured leak rate of the containment vessel = UCL L
UX Leak rate of all penetrations, valves, flanges not exposed to ILRT test pressure LLRT Local leak rate test P Pressure P Design accident pressure psia Absolute pressure psig Gauge pressure R Temperature, degrees Rankine SIT Structural integrity test T Temperature T
dp Dew point temperature t Time V Containment volume, cubic feet
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II INTRODUCTION The purpose of this report is to provide adequate information so that an objec-tiva review of the test can be performed. This will ensure that the test results reflect truly the leakage characteristic of the as-built containment. In confor-mance with the Appendix J of 10CFR50 and all associated ANSI, the absolute method end mass-plot technique which require monitoring the containment vessel tenpara-ture and pressure to determine the change in containment vessel air mass caused by leckage are used as the framework for selecting test equipment, developing test computer programs and test procedures.
The McGuire Unit 2 Containment System consists of a containment vessel and a ssparate reactor building enclosing an annulus. The following containment vessel spzcifications are used as data base for the containment leak rate test.
- Containment Net Free Volume 1,239,759 ft3 (without ice)
- Design pressure 15 PSIG
- Calculated Peak Accident Pressure 14.8 PSIG
- Test Pressure 15.0 PSIG
- Test Temperature Ambient 52 Resistance Temperature Detectors, three (3) Dewpoint hygrometers and 3 pres-sure sensors are installed at predetermined locations in the containment vessal to datermine the weighted averages of containment vessel temperature, vapor pres-sure and pressure. The McGuire containment vessel leak rate test utilizes a fully cutomatic Data Acquisition System. All raw test data is scanned, printed and re-cordcd on Cassette tape automatically to minimize uncontrolled random errors.
Assigned engineers of Duke Power Company were responsible for draf ting and con-ducting the test. Three 8-hour shif t crews which consisted of one shif t coordina-tor and two technicians were utilized to maintain 24 hour2.777778e-4 days <br />0.00667 hours <br />3.968254e-5 weeks <br />9.132e-6 months <br /> test activity.
Pressurization for the McGuire Unit 2 ILRT was accomplished by a portable air conpressor/ dryer rented from Ingersol-Rand. The compressor / dryer was rated at 1800ICFM @ 125 PSIG. This compressor supplied air to the Upper and Lower Compart- -
n:nts only. The Ice Condenser Compartment was pressurized using station Instrument Air through a special -40 F dewpoint dryer. When the test was completed, the containment vessel was depressurized through the Ventilation Evacuation system in ths annulus. Ihe release rate can be controlled if the air is contaiminated.
Section IX, Figures 2 and 3 show the pressurization and depressurization path used in this test.
III Test Purpose The purpose of the Preoperational Containment Integrated Leak Rate Test is to datarmine the leak rate of the containment vessel under controlled test condi-tions; to verify that there were no unidentified openings in the containment vessel due to incomplete construction; and to evaluate the possibility of ac-curetely measuring the containment leak rate in a shorter period of time.
Tha containment vessel was preconditioned to provide test conditions which satisfy the following:
- The vessel is under calculated accident pressure, 14.8 psig.
- Air temperature and pressure are stable to avoid biasing the leakage characteristics
- The contaimment vessel and all penetrations are lined up as close as possible to the predicted post-accident condition; i.e., those portions .
of the fluid system that are part of the reactor coolant pressure boundary and are opened directly to the containment atmosphere under post-accident conditions and become an extension of the bound-ary of the containment shall be opened or vented to the containment atmosphere prior to and during the test.
The test utilized highly accurate sensors and an automatic data system te assure tha accuracy and quality of the test data.
Statistical and error propagation analysis are performed on the test data to en-sure that the test results are reliable and accurate.
IV Summary "THE CONTAINMENT VESSEL IN'rEGRATED LEAK RATE AND STRUCTURAL INTEGRITY TEST" was initiated on 9/23/82 and completed on 9/28/82. It was conducted in compliance with tha McGuire FSAR and Title 10, Code of Federal Regulations, Part 50, Appendix J, which states that the containment vessel is subject to a test to assure that an ac-captable upper limit of leakage of radioactive material is not exceeded under dssign accident basis.
The vessel was initially pressurized up to 16.970 PSIG for the Structural Integ-i rity Test. Pressure was then reduced to 15.0 PSIG and the Integrated Leak Rate Test begun at 0245 (Run 1 ) on 9/26/82 af ter a > 4 hour4.62963e-5 days <br />0.00111 hours <br />6.613757e-6 weeks <br />1.522e-6 months <br /> stabilization period. The tsat result was evaluated acceptable at 1445 on 9/27/82 af ter a 36 hour4.166667e-4 days <br />0.01 hours <br />5.952381e-5 weeks <br />1.3698e-5 months <br /> test run. At Run 143 computer printout indicated:
The containment vessel leak rate (observed) = 0.0770901% per day The containment vessel leak rate upper limit (95% UCL) = 0.0876706% per day The containment vessel leak rate lower limit = 0.0665096% per day Tha 95% upper confidence limit of the leakage rate was less than the acceptance criteria which is 0.15% per day.
Tha verification test to demonstrate the sensitivity and accuracy of test equip-mant started at Run 148 and attained acceptable measured value of 0.3496252% per day at Run 186.
Bassd on the low value of the measured leakage rate compared with the acceptance criteria and the analysis of aAl graphical data, the Containment Vessel leak rate test for McGuire Nuclear Station Unit 2 was declared successfully completed and tsrminated at 0130 on 9/28/82. This test was conducted per test proceddr-TP/.!/A/l:00/29, Containment Initial Integrated Leak Rate Test and Structural Intsgrity Test.
Problems were encountered with the ILRT computer af ter initiation of the 24 hour2.777778e-4 days <br />0.00667 hours <br />3.968254e-5 weeks <br />9.132e-6 months <br /> test and were not cleared up until about 35 hours4.050926e-4 days <br />0.00972 hours <br />5.787037e-5 weeks <br />1.33175e-5 months <br /> later. From this data we chose our 24 hour2.777778e-4 days <br />0.00667 hours <br />3.968254e-5 weeks <br />9.132e-6 months <br /> limits (Readings48-143) . However, because of these problems and etne bsing essential, the leak rate was considered initial at Reading #1. So our leak rate included leakage from Readings #1-47. Later analysis showed that at an ini-tistion point at Reading #48, the leak rate could have been red : ed to L.026685%/
Day observed and L , (95%) to 0.0429875%/ Day. This would also affect the limits i
IV Pcg3 2 for the supplemental verification test equation. We would now have .0469402%/ Day
< .05%/ Day; still within the acceptance criteria.
V TEST ORGANIZATION In order to assure that the test is conducted in a safe and efficient manner, as-signed personnel are organized as shown and their responsibility defined.
TEST INSTRUMENTATION
^
TEST SUPPORT COORDINATOR GROUPS I I ASSISTANT TEST COORDINATOR l l SHIFT SHIFT SHIFT COORDINATOR COORDINATOR COORDINATOR DATA '
DATA DATA SPECIALIST SPECIALIST SPECIALIST
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DATA DATA DATA TAKER TAKER TAKER Test Coordinator: His lead responsibility is to provide overall planning and efficient execution of the test.
Aesistant Test Coordinator: His lead responsibility is to assume test coordinator responsibilities during his 12 hour1.388889e-4 days <br />0.00333 hours <br />1.984127e-5 weeks <br />4.566e-6 months <br /> shif t. Only Test and Assistant Test Coordina-tors are on 12 hour1.388889e-4 days <br />0.00333 hours <br />1.984127e-5 weeks <br />4.566e-6 months <br /> shifts.
Instrument Coordinator: His responsibility is to provide test equipment maintenance support to Test Coordinator.
Test Support: Their responsibilities are to furnish technical support to Test Per-sonnel as required in conducting the ILRT, solving test problems, and minimizing schedule delays, Shift Coordinator: Assume general responsibility for ILRT execution on a shif t basis.
Data Specialist: His lead responsibility is to process and edit raw data.
Data Taker: Record data accurately at correct intervals.
VI TLST 3ACT. GROUND INFOR'uTION TEST METHOD AND CALCULATION TECHNIQUE (DETAIL IN APPENDIX A)
TEST y.ETHOD,: The absolute method of leakage rate testing is used for the McGuire test. This requires the determination and calculation of air losses by the containment vessel leakage over a stated period cf time by the means of direct pressure, temperature and humidity observations during the period of the test.
Sensors are properly located to provide an average value of the containment vessel temperature and pressure. The effect of the partial pressure of water vapor is measured and compensated.
e Upon completion of the 24 hour2.777778e-4 days <br />0.00667 hours <br />3.968254e-5 weeks <br />9.132e-6 months <br /> leak rate test, a test is perfomed to verify the accuracy of the leak rate test. This requires superimposing a controlled and measurable leak on the containment vessel and the composite leakage of both the containment vessel leaks and the superimposed leak is measured. The difference between the result of the leakage measurement obtained prior to the introduction of the superimposed leak and that of the composite leak determines the accuracy of the leak rate test.
The test enviroment is simulated as close to that of designed accident basis as possible. All portions of the fluid systems that are postulated as opening directly to the containment or cutside atmosphere under post-accident conditions are openad or vented during the test except systems required to maintain the plant in saf e conditions during the test.
The test pressure is the calculated design basis accident pressure of 14.8 PSIG.
CALCULATICS TECHNIQUE: Mass of the contair. ment vessel air volume is calculated by the Ideal Gas Law for 24 consecutive hours and plotted against time. The leak rete is obtained by a linear least square fit to the mass plot graph. The 95%
confidence upper limit of the leak rate is calculated by applying the Student T Distribution Test on the leak rate test result. This upper limit is compared with th2 acceptance criteria to determine the completion of the test.
TEST ACTI'lITY FLOW CHART: Figure 1, Test Pressure versus Time Curve, provides an overall look of the test activities. This provides critical information for test planning and test execution.
i
VI Pzga 2 TEST ACCEPTANCE CRITERIA AND TEST RESULTS:
Acceptance Criteria 24 Hour Leak Test: The total Containment Vessel Leak Rate (Lg)
- Lg < .75 Lg
's than .75 L where LA = .20% of the Containment Vessel air mass per day.
Now Lg
=L OBSRVD (' }+b AUX where L OBSRVD (95%) Upper Confidence Value of measured leak rate of the containment vessel.
L AUX
= Leak Rate of all penetrations, valves, flanges which cannot be exposed to test pressure due to system operation.
Supplemental Verification Test: The difference between the supplemental verifica-tion and the total measured leak rate is within .25 L A (L C ~
0
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< .25 L OBSRVD A where LC = Total measured leak rate during supplemental test LO= Imposed Known leakage L =
a measured leak rate during 24 hour2.777778e-4 days <br />0.00667 hours <br />3.968254e-5 weeks <br />9.132e-6 months <br /> test OBSRVD Tant Results The following are results of McGuire Unit. 2 Preoperatianal ILRT completed on September 28, 1982:
24-Hour Test Results -
L OBSRVD
= .0770901 % per day L "
OBSRVD(95%)
Now Ventilation Instrument Air penetration M-359 (2VI) was not exposed to ILRT test conditions because this penetration needed to be available to provide air to the inner seal of the Upper Personnel Air Lock Reactor Door for entry into the pressurized vessel if necessary. This was the only Thru Line Leak Class 2 penetration not exposed to test conditions. It was, however, tested immediately af ter ILRT on 10/1/82 and the resuAting leakage was 0.00028% per day.
So Lg
=LOBSRVD(95%) + L and Lg = 0.0876706%/ Day + 0.00028%/ Day
~
Lgg = 0.0879506%/ Day '
VI Pags 3 Varification Test Results L = 0.3496252%/ Day C
LO= 0.276%/ Day L = 0.0770901%/ Day OBSRVD (0.3496252%/ Day - 0.276%/ Day) - 0.0770901%/ Day < .05%/ Day
. 0034649%/ Day < .05%/ Day, well within the acceptance critaria.
NOTE: Some questions have been raised concerning inlet pressure measurements for the turbine flowmeter during the supplemental verification test.
See Appendix D Attachment #3.
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RESULTS OF TYPE B AND C LEAK RATE TESTS: 1 Test Final Conservative Test Results TP/2/A/1200/16, Isolation 1452.61 scen Velves Leak Rate Test = 4.2199819 x 10 -6 %/ Day TP/2/A/1200/15, Mechanical 1900.0 seem Psnstrations Leak Rate Test = 3.4549135 x 10 ~0 %/ Day TP/2/A/1200/18, Upper Con-
- tsinment Personnel Air Lock Lcck Rate Test TP/2/A/1200/19, Lower Con-tainment Personnel Air Lock Lh k Rate Test TP/2/A/1200/17, Fuel Transfer 0.2 seem Tubs Leak Rate Test -10 %/ Day
= 5.8102063x 10 TP/2/A/1200/20, Equipment 90.0 seem -
7 Hatch Leak Rate Test = 2.6145928x 10 %/ Day TP/2/A/1350/24, Electrical 3.974 seem Penstration 0-Ring Leak Rate = 1.154488 x 10-8 %/ Day Tent Formula Used for Conversion:
S
(%/D y) = 100% x where Sg = Measured leakage of TP in question (lbm/ Day) i my = Mass containment vessel at start of 24 hr. test.(lba).
(%/ Day) = 100% P 2 2 = 100 P 2 2 Ty ; where P2 = Test pressure of B or C test (PSIA)
R T 2 Py V1 T2 2 = Final leakage results (SCFM)
Py V1 Ty = Temp of Vessel at start of 24 Hour Test R T 2
= 546.17 R P y = Pressure of Vessel at start of 24 Hr. Tes SCFM = SCCM x (3.5314667 x 10-5) = 29.355 PSIA 3
V = Volume of Vessel = 1,239,759 ft 1
T2= Use 80 F (540 R) as standard for B & C test temperatures
- Thsze tests cannot be completed by due date of this report. When test is completed, results will be submitted to the Nr.C.
-- -- - , - am
VII Pggn 1 TEST EQUIPMENT The ILRT instrumentation system is designed to accurately record test parameters.
The system consists of a central data acquisition system with a remote scanner /
multiplexer unit and individual temperature, pressure, and dewpoint sensors. All RTD's are wired to the remote scanner / multiplexer unit located inside containment.
Tha signals are then multiplexed and sent to the central data acquisition facility.
All other sensors are wired directly to the data acquisition facility located out-sids containment in a test van.
Instrument Specifications e
Precision Pressure Gauges are Ruska model 6000-801-40 PSIA gauges.
Range: 0 to 40 PSIA Repeatability - 24 Hr: i .0008 PSI; 90 Day: 1 0016 PSI Accuracy: + (.008% Full Scale + .012% Reading) or better, traceable to NBS Output: Direct digital output plus BCD parallel signal for recording.
Tha Dawpoint Temperature Analyzers are General Eastern system 1200 AP sensors with modal 700 aspirators.
Range: -40 to +120 F Dewpoint Repeatability - 1 05 F Accuracy: 1 4 F dewpoint, tracable to NES Output: Direct digital readout plus 0-50 my signal recording The Resistance Temperature Detectors are Leeds & Northup Catalog number 178055 Range: -100 to +250 F Repeatability - 1 035% Span Accuracy: 1 07 F (32 F and 77 F) 0-120 F = 1 042 F 1 10 F ( ct 120 F)
Element: Copper Resistance: 100 ohms at 77 F Section IX, Figure 6 shows placement of RTD while Section X, Table 1 gives their general locations.
The Turbine Flowmeter is a Flow Technology model FTC-8C5.0-GJS Flocapsule with model PRI-402A Flow Rate Monitor.
Range: 0.5 to 5 ACFM Repeatability - 1 25% FS Accuracy: +0.2%, traceable to NBS. 1 0125 ACFM Output: Visual display plus 0-5 VDC signal for recording Tha Data Acquisition Facility is a Leeds and Northup catalog Number 70072-409-4999-6-000000-0600-00-001-301-099 Digital Data Surveillance Facility with the following features:
~
- Numation Numeric Display Scanner / Programmer
a VII Pega 2 Digital Printer
- Digital Clock
- Cassette tape recorder Section IX, Figure 4 shows the test instrumentation set-up.
COMPUTER PROGRAM To provide on-line data analysis, a computer program is developed using formulas and methods specified in Appendix A. The Leak Rate Test Program (LRT) reads in-strument readings from a magnetic tape cassette taken from the data recorder on ths Digital Data Surveillance Facility (DDSF). The raw data from the tape are calibrated using quadratic curve fits. These calibrated data are then checked for validity. Using the mass plot analysis method, the calibrated verified data are j processed to yield a normalized weight which is the ratio of the mass of air in tha containment at the present tbne to that which was initially present when the test began. Linear regression and confidence interval calculations are then parformed to determine whether the results have converged sufficiently to yield an accurate indication of the actual containment leak rate.
Using the terminal procedures detailed in the user documentation, the test ad-ministrator can run the program from any teletype-compatible terminal device having magnetic tape cassette capability. The program is desinged for inter- .
4 active processing so that at each step the user will be queried as to how he wishss the work to be accomplished. Instrument parameters and readings can both entet into the computer system either automatically from cassette or atnually from the terminal keyboard. If any errors are detected in the data, than the user will have the option of correcting the specific error on the co:puter instead of re~ entering all of the data.
-- - - - - . . - - , - - , - . _ - + _ , - - _ - , , _ _ . - , _ _ , _ _ _ _ , , _ _ _ _ _ . . - _ _ ,
VII Pega 3 All data stored in the computer is protected by a password selected at the begin-ning of the test and must be specified each time the program is run to gain access to the data. This provides some measure of protection against inadvertent intru-sion during the conduct of the test. At the conclusion of the test all of the stored data, from raw instrument readings through intermediate results to the final results, will be copied to an archival storage medium to satisfy long-term re-tcntion requirements of regulatory agencies. The archives can be placed on active storage at any time to verify calculations or generate reports.
- Instrument Error Analysis (Equations used in this section can be found in ANS N274, Draf t Revision 3, November 15, 1978)
Symbols:
FOM = Instrument figure of merit (%/ day) t = Test duration (hr.)
p = Test pressare (PSIA)
P = Vapor presnure at test time (PSIA) y T = Cont. weighed average absolute test temp. ( F) e = Error associated with measurement of change E = Sensor erro.- (Sensitivity)
E = Measurement system error excluding sensor
- 1. Pressure:
No. of sensor = 3 Range 0 - 40 PSIA Sensor Error (E ) = 10.008%FS = 0.0032 PSIA Measurement system rupeatability error (Ip) = 10.002%FS = 0.0008 PSIA (Ep ) + (E p) -
e =1' = 10.0019044 PSIA No. of sensors
- 2. Vapor Pressure:
No. of senser = 3 Range -40 F to 120 F Sensor Error E = 10.40 F or 1 001268 PSIA
- Measurement System Error (I) = 10.05 F or 10001585 PSIA
- E (.001268,2 <,ooo13gs,2- 8 epy =
= 1 0007378 PSIA
VII PJgs 4
- At dewpoint of 36 F, the rate of vapor pressure change per 1 F is .00317 PSIA / F
- 3. Temperature No. of Sensor = 52 Sensor Error = 1 042 F or 1 042 R Measurement System Error = 1. 15 F or .15 R
_(.042 R)2 + ( .15 R)2~
e T 3 =
1 0216013 R 52
- 4. FOM (Figure of Merit)
-t 2400 feT
[ep FOM = +- t 2
P)+2i\P/+2 \T, ,
, (
2400 I 2f 0019044' I.0007378\ +
24
\ 29.27 29.27 / (I.0216013) 536.3/ ;
- 1 0080566% per day This FOM value indicates that test instrument repeatabi.lity is adequate to provide a precision measurement of maximum allowable leak rate of 0.20%/ day.
Random errors on test results were analyzed under 95% confidence analysis and in-corporated into the test results for acceptance verification.
Tha test method also underwent a required accuracy test at the end of the 24 hour2.777778e-4 days <br />0.00667 hours <br />3.968254e-5 weeks <br />9.132e-6 months <br /> ILRT. It met the Acceptance Criteria (See test result). '
1
UIII CONCLUSION With all conservative factors built in the test results analysis, the following conclusions were made on the McGuire Unit 2 ILRT:
- 1. McGuire Unit 2 Containment Vessel is capable of saf ely Containing fission products under designed accident conditions.
- 2. With a properly controlled test environment, test acceptance .:ould be attained much earlier than the
, 24 hour2.777778e-4 days <br />0.00667 hours <br />3.968254e-5 weeks <br />9.132e-6 months <br /> minimum required time for a 24-hour test.
The supplemental test could be achieved in about 6.5 hours5.787037e-5 days <br />0.00139 hours <br />8.267196e-6 weeks <br />1.9025e-6 months <br />.
- 3. No identified opening in the McGuire Unit 2 Containment vessel exist due to incomplete construction.
XX ILRT FIGURES
- 1) Pressure vs Time
- 2) Depressurization Path
- 3) Pressurization Path
- 4) Test Instrumentation System
- 5) Sectional View of Containment Vessel
- 6) RTD Locations i
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'D pe ee E T wS rS M R e P N D I A
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HEMISPHERICAL DOME EL 894'+3" o
dg.
7 u
'o 9k .%
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c o _ _
EL 83Ef-9" o
1 I3 80" _
'm
@ [ VERTICAL CYLINDER
~ ~ 0.7j TH'K I
EL.737'5 *
~
- 1.dTH'K m < ; EL. 72 3'+0' -
A N
O.26TH'K- -
FLAT LINER PLATE R ~
o EL.69 4'+ 4's
=
252" _
Figure 5 Sectional View of Containment Vessel 1
Figure 6 RTD LOCATIONS ,
7 N -
ORTD 36 RTD370 RTD 4-35
_ .. t OarD RTD 38-42 4 3-4 7___ bTD32 RTD33O O O ~
RTD RTD 11,12 10 gHumdity Sensor I 28-29 RTD 30- -
lumdity -
- ensor
~~
1 \" / 2 t \l /
- UO -
i RTD 23-24 n RTD 22,50 O- -DTD48-49
. JJ 52 -'
OTD 14-15 RTD' 7'16-A ORTD 2's RTD 19 -20 OTD 18, 2 O O 3 RTD 26 y' -E -
,8 T RTD 2-3 ,
Humdity ;
Sensor
.T ) 6-7 RTD 8-S - b
, 1 -
~
L J ,
RTD 1 i
I
X Pags 1 TABLE 1 RTD LOCATIONS LOWER CONTAINMENT (COMPARTMENT VOLUME FRACTION = .297)
RTD # GENERAL LOCATION COMPARTMENT VOLUME FRACTIONS 1 Wall mounced in incore inst. .0417 area 2 S.G. D lower support structure .0566 el. 745' 3 S.G. A lower support structure .0566 J
el. 745' 4 S.G. B lower support structure .0566 el. 745' 5 S.G. C lower support structure .0566 el. 745' 6 Wall mounted in tunnel area .0297 7 Wall mounted in tunnel area .0297 8 Wall mounced in tunnel area .0297 9 Wall mounted in tunnel area .0297 10 On top of S.G. 2D .0378 11 On top of S.G. 2C .0378 12 On top of S.G. 2B .0378 13 On top of S.G. 2A .0378 14 On top of RC pump 2D .0377 15 On top of RC pump 2A .0566 16 On top of RC pump 23 .0566 17 On top of RC pump 2C .0377 18 In accumulator room 2D ,
.0117 19 In accumulator room 2C .0099 20 In accumulator room 2B .0112 21 In accumulator room 2A .0112 22 Wall mounted in room with air .0345 return fans 23 Mounced on ladder support in .0438 reactor cavity
^ -
^7 -
Page 2 TABLE 1 (Cont.)
RTD # GENERAL LOCATION CCMPARTMENT VOLUME FRACTIONS 24 Mounced on ladder support in .0377 reactor internals storage area 25 Column mounted in incore .0321 insertr.scation area 26 Column mounted near lower con- .0406 tain==at vent. Unit 2 D 27 Column mounted near lower con- .0406 tainment vent. Unit 2 B UPPER CONTAINMENT (COMPARTMENT VOL1)ME FRACTION = .541) e RTD # GENERAL LOCATION COMPARTMENT VOLUME FRACTIONS 28 On concrete housing for S.G. .0763 2D 29 On concrete housing for S.G. .0763 2A 30 On concrete housing for S.G. .0763 23 31 On concrete housing for S.C. .0763 2C 32 on wall between S.G. 2.A & 2 D .0847 33 On wall between S.G. 2 B & 2 C .0847 34 On wall below crane track .1356
- el. 838' 35 On wall below crane track .1356 el. 838' 36 On cont. spray piping 31'6" west .1271 of center el. 875' t
37 On cont. spray piping 31'6" east .1271 i
of center el. 875' ICE CONDENSER (COMPARTMENT VOLUME FRACTION = .162)
RTD # GENERAL LOCATION COMPARTMENT VOLUME FRACTIONS 38-47 Evenly spaced around the upper .0557
- plenum area el. 835' 48-52 Evenly spaced around the lower .0886 plenum area el. 773' l
t
h APPENDIX A DERIVATIONS AND FORMUI.AS FOR MCGUIRE CONTAINMENT LEAK RATE COMPUTATIONS This appendix presents derivations of formuiss used to develop McGuire leak rate computer program.
I Pzgo 1 )
A.1 DEFINITION OF SYMBOLS P = Absolute pressure in the Containment Vessel (PSIA)
T = Weighted average absolute temperature of the Containment Vessel air compartment ( R) l Normalized mass of containment vessel air at i Wg =
data point (dimension less)
Pv = Partial pressure of water vapor (PSIA) t = time (min.)
V = Assigned volume fraction of keh sensor (Fraction of volume) k T = Recorded temperature of k* sensor ( R) k W =
Estimated value of Wg in the least square fit calculation b = Slope of the least square fit lina (fraction / min.)
L " *""" **
- OBSRVD[9h) .'L OBSRVD L
OBSRVD
= easured conta h ent lea b ge rate M ay) a = y intercept of the least square fit line (dimension less)
S g = the variance of W g S = the variance of b b
A.2 SUBSCRIPTS u = upper containment compartment L =
lower containment compartment I = Ice Condsnser compartment v = vapor 1 = data point at start of test i = 1* data point (i = 1 to N)
N = Final data point of a given set k = keh ,,,,,,
A.3 MASS PLOT CALCULATION AND STATISTICAL TREATMENT OF LEAK RATE DATA Normalized Containment Vessel Air Mass The air mass of the Containment Vessel is calculated using ideal gas law compensated for partial water vapor pressure. Air mass of 3 compartments (lower, upper, Ice) are determined separately and combined to yield the whole Containment Vessel to simplify the calculation. Normalization of Wg is applied by taking the ratio of the i value and that of the initial value.
l Pags 2 The values 0.541, 0.297, 0.162 are the assigned volume fraction for upper, lower, and Ice Compartment.
The average temperature T at each compartment is calculated as the sum of the volume weighed recorded temperatures.
IP-P* Y IP-P' '
/P-P*
+ 0.29 7 + .162 0.541(T /u L T )g (T )7 f
i (p .\1 [p,p 31 p,,
il 0.541 '} + 0.297' (T )g
+ .162' (T )g (T /u T=Ekk k = 1 to 27 for lower compartment k = 28 to 37 for upper compartment k
- 39 to 52 fer ice condenser See attached Table 1 for volume fraction of each sensor.
Leakage Rate of the Containment Vessel The graph of Wg versus time is least square fitted to yield an estimated straight line. The rate of the containment vessel air mass losa (or the containment vessel leak rate) is the _
slope b of the least square fitted line W g, :
hg = beg +a The value of a'and b can be determined by taking the first partial derivation of the sum of square of deviation Q (Q = I (W - W )2 with respect to a and b and minimize them:
1
.. \ *
- g. 6' E (W - Wg)2_ W = bc +a
=0 oa da W g -h=W1 g - bt g -a 6 Z(W1 - W )2
= 2 I (W1 - bc - a) = 0 6a E (Wg - bt g - a) = 0 Na + bett= ZW g (1)
Psgo 3 6 I(W 1
-0) hg = bc +a db 6b Wg h=W g - bt -a a I(Wg - )
6b
= 2E-t g(W1 -beg - a) = 0 I-tfW - beg - a) = 0 (2) attg + bItg = It gg W (3) with (1) and (3), a and b can be solved by matrix:
Na + (It g) b = IW g (1)
(Itg ) a + (It ) b = It gg W (3)
N IW g Itg It gg W nit gg W --(IW ) (It g) 1 b= (4) 2 N It nit g -(It g)2 It g Itf2 IW It g Itgg W It g2 IW Itg 2 , gt gt y a= =
(5) 2 N It g nit g -
(It g)2 It It g2 L = -b 144000% per day OBSRVD
(
- unless otherwise specified, all summation will be from i = 1 to i = N It is important to emphasize here that the slope b or leak rate is formulated on the following assumptions:
- the deviation of Wg from the true value are distrubuted according to the gas distribution function
- only the Wg contains random error, not the c
P gs 4 The Confidence Limit of the Slope of the Least Square Line As indicated in the error analysis, the random error is a major contribution which deviates the test result from the true value. Due to the random characteristics of this error, only statistical treatment can possibly evaluate the error effect on the test result. In order to choose a proper statiscical treatment, it is important to identify the charac: eristics of the observed data. In the previous derivation, it is found that L OBSRVD s the outce of the calculation from the observed temperature and pressure in the Containment i Vessel using the ideal gas law and curve fitting method. It is now obvious that the observed data is a continuous measurement which is completely different frc2 the discrete measurement.
The latter requires discrete statistical treatment (X CH1 SQUARE), while the former requires continuous statistical treatment (The t test). ~
l The t test, provides information which indicate how much the I calculated leak rate deviated from the true value, and at what j
probability.
In other words:
, L = kBSRVD 1 " Deviation" (percent of probability)
For t test method " deviation" is defined as:
Deviation = c S b
- t is a tabulated value which corresponds to the number
, of Data sets taken and the required probability (in this case 95% is chosen on popular basis). The value of t is on enclosed Table 2.
b is the standard deviation of the variance of the containment
-S air weight.
Equation (4) indicates that b = f(k' ) and by definition of variance:
S b
" S w (5) where S, is the variance of W g:
i I
- - -e_- . , , . . + ,
l Pagn 5
~"~
2 , ("i *i) (6) w N-2 The (N-2) is chosen here instead of N because the least square line Wg is restricted by value of b and at The l freedom to evaluate the variance of W gis reduced by 2 even N data is recorded:
NIc gg W -
(IWi) (It )
6 t ob ,
3E i ~ (rEi) 6W 6W 1et c = nit g -
(In g) 6 nit g1 W -( g) (It)) t At .
6W g 6Wg 1 6 3E ii ~( i) ( *i) c 6W i
, ,1_ Ntg - It g 1
=
h -
Ntg - It g (7)
Substitute (7) co (5)
S
,2 , I (Net - It i) b c I (N e g - 2Ntg Itg + (It g) )
c (N It g - 2 nitg Itg + N(Itg ) )
c 2 2 2 '
S w (N It g - N(It t)') (8) 2 Substitutec= hit 2 , (7t{)2 to (8):
S =
Ns w b
= She x
, - . m-
Paga 6 nit - It l 1 I = It 2 , gt 2 1 N
2 "
SW 8
b 2 2 It g - It g N
The identity provides:
E(e g - E) = It g
- = It g - E It g S S S S = = =
(9)
It g -It 1
I(t y-E) Itg -E It N
A.4 Summarization:
The following are the essential equations used in developing ILRT computer program:
0.541 f(P-P )N + 0.297 f (P-p [ + .162 f(P-P )'l 1 i T Ju i T y)L L T II i
0.541 f(P-P ) + 0.297 ' (P-Py ) + .162 f(P-Py )I
( T y/u ( T /L \ T I T = IT V kk -
5 = btg+a nitg W - (IW 1) (It g) b= ')
2 nit g - (Itg)'
IW1 (It 12) -
(It ) (It W )
nit g - (Ic y)
= -b OBSRVD OBSRVD (95%) = L OBSRVD I b
Pcgs 7 t value is on enclosed cable corresponding to f = N-2 and and 0.975 .
Z(W1
- a - be g)2 S ,2 = N-2 S
S "
b" It i
-tit i 4
Page 8 TAar.a 2 Critical Values for Student's t-Distribution
- Pr{ Student's 7 6 tabled valuc} = 7 f 0.75 0.90 0. m. 0.975 0.99 0.995 1 1.0000 3.0777 6.3138 12.7062 31.4387 63.6574 2 0.8165 1.seS6 2.9308 4.3027 4.9644 9.9248 3 0.7649 1.6377 2.3534 3.1424 4.3407 S.8409 4 0.7407 1.3332 2.1318 2.77M 3.7469 4.4041 3 0.7267 1.4739 2.0130 2.3706 3.3649 4.0322 6 0.7176 1.4398 1.9432 2.4469 3.1427 3.7074 7 0.7111 1.4149 1.8944 2.3644 2.9900 3.4995 8 0.7064 1.3968 1.439S 2.3060 2.4MS 3.3334 9 0.7027 1.3830 1.1331 2. 3 22 2.8214 3.2498 to, 0.6998 1.3722 1.8125 2.2221 2.7638 3.M93
. If 0.6974 1.3634 1.7959 2.2010 2.7181 3.1058 12 0.6955 1.3562 1.7823 2.1788 2.M10 3.0345 13 0.6938 1.3302 1.7799 2.1406 2.6303 3.0123 14*. 0.6924 ~ 1.3430 1.7613 2.1448 2.6245 2.9768 15 0.6912 1.3406 1.7531 2.131S 2.602S 2.9467 1[ 0.6901 1.3364 1.7459 2.n99 2.3833 2.9208 17 0.6492 1.3334 J 7396 2.10M 2.3669 2J982 -
la 0.6884 - 1.3304 2.7341 '2.1009 2.3324 2.8734 19 0.M76, ,t 3277* .1.7291- 2.0938 2.339S 2.8609 m 0.6s7o,
- 1.32S3 1.7247 2.osee . 2.32se 2.84S3 21 0'.68$4' 2 1.3232 1.7387 2.C7M ' 2.3177 2.8314 22 0.68S4- '.1.3212 1.7172. 2.0739 2.3083 2. alas 23 0.6453' *13195 9 1.~7139- :2.0687 2.4999 2.3073 34* 0.6848 . 1.3178 1.7109 2.0639 2.4922 2.7969 25- 0.4844 1.3163 1.7081 2.0595 2.44n 2.7874 26 O.6840 1.3130 1.7056 2.0553 2.47a6 2.7787 27 0'.6837 1.3137 1.7033 2.0518 2.4727 2.7787
'.Ja. 0.6834 1.3125 1.7012 2.0684 2.4671 2.7633
- 29 0.6a30 1J114 1.6991 2.04S2 2.46 3 ~2.7344 Jef 0.6828 1.3184 1.6973 2.0623 2.4573 - 2.7300 31 0.6425~ 1.3095 1.6955 2.0395 2.4528 2.7440 32 0.6432 1.3006 1.4939 2.0369 2.4487 2.7385 33 0.6a K "10077 1 6936 2.0345 2.4444 2.7333 34 0.6418, 1.3070 1.6909 2.0322 2.44u 2.7234 33 0.6s14 ,
1.3062 1.68M . 2.0301 2.4377 2.7238
~ .
36' O.6411 1.3055, 1.6883 2.0281 2.434S 2.7195 37 0.6815 -Es3069. 1.6871 2.0262 2.4314 2.7154 38 0.6410 1.3042 1.6860 2.0244 2.4286 2.71M 39 0.6408 1.3036 1.6849 2.0227 2.4258 2.7079 40 0.6807 1.3031 1.6439 2.t211 1.4233 2.7045 41 0.6405 1.3025 1.6829 2.0195 2.438. 2.7012 42 0.6a04 1.30 m 1.68 3 2.0181 2.4145 2.6901 43 C.6a02 1.3016 1.68H 2.0147 2.4163 2.6931 44 0.6a01 1.30n 1.6802 2.0154 2.4141 2.6923 45 0.6800 1.3006 1.6794 2.0141 2.4121 2.6aN
- D. B. Owen, NAS efsteristimf TaWer. AMi.aa., Wesley PubEshans Co.,1962. (Courtesy Atomic Energy N=: *8er., W m-==_. D.C.)
1 I
l i
l 1
l l
i Page 9 i
l 1
TAsta2 (Continwd)
Pr(Student's 7 $ tabled value} = 7 0.30 0.es 0.s7s 0.99 0.995 1 0.7s 44 0.6799 1.3002 . 1.67s? 2.0129 2.4102 2.6s70 47 0.H97 1.299C 1.6779 1.01U 2.4083 2.64M 48 0.67M 1.2994 1.6772 2.0106 2.40M 2.6422 49 0.H95 1.2991 1.6766 2.00M 2.4049 2.5800 SS 0.67M 1.2987 1.6739 1.0006 2.4033 2.6778 S1 c.6793 1.2904 1.6733 2.0076 2.40U 2.6757 52 ' O.H92 ,1.2900 1.6747 ' 2.00M 2.4002 2.6737 IfG W 2.3988. 2.6715 "33'.T.679f. .1.2977 2.0037 34 0.H91, ,L_2974 T.U36 2.0049 2.3974: -2.6700 SS 6.67M' .t.2971 1.6730 2.0060 2.3M1 2.6682 1.2M9 1.H2S 2.0012 2.3948 2.664S S6 Is.He9 2.3934 2.6M9 37 ;0.67s8 1.29M 1.6730 2.0023 "O.HST, 1.2H3 ,1.6716 2.0017 2.3934 1.6433 38 0.6787- 1.2M1 1.H11 2.0010 2.3912 2.6418 39 48 30.H86 1.M .- -hWOW 2.0003 2.3901 2.6403 61 t.6785 1.29M 1.6702 1.9996 2.3890 2.6589 62 3.6743 1.2954 1. Hee 1.9990 2.38e0 2.6575 0 0.H84 1.2951 1.HM ~ 1.9983 2.3870 2.6561 M s.6733 1.2M9 1.H90 1.9977 2.3860 2.6549 63 0.6733 1.2947 1.H86 1.9971 2.3851 2.6536
, 64 , 0.6782, 3.2MS 1.6683 1.9966 2.3442 2.6534 H 0.H82 1.2M3 - 1. M79 . 1.9960 2.3833 2.6312 es' O.6781 1.2M1 1.M76 1.9933 2.3834 2.6501 69 4.678L 1.2939 1.M72 1.9969 2.3816 / 2.6490 70* ~4:6788; 1.2938 1.6649 1.99M 2.3800 ~ 2.6479 71 *0.670s 1.2936 1.M66 1.9939 2.3800 2.6449 1.2934 1.H63 1.9935 2.3793 . 2.6439 72 ~0.6779 1.9930 2.3785 2.6449
- 73. ;0.H79 1.2913 1.H60 74 1.H78 1.2931 1.MS7 1.9925 2J778 2.6439 75 0.HFS 1.2929 1.MS4 1.9921 2.3771 2.6430 74 0.6777 1.2928 1.MS2 1.99U 2.3764 2.6421 77 0.6777 1.2936 1.6649 1.9913 2.3758 2.M12 78 0.6776 1.2925 1.M46 1.9908 2.3751 2.6403 79 0.6776 1.2924 1.6644 1.990$ 2.3745 2.09S 30 0.6776 1.2922 1.H41 1.9901 2.3739 2.6387 81 0.6775 1.2921 1.M39 1. N97 2.3733 2. 079 at 0.6773 1.2920 1.6636 1.N93 2.3727 2.6371 83 0.6775 1.2914 - 1.M34 1.N90 2.3721 2.63M 84 0.U74 1.29U 1.6432 1.9884 2.3716 2.6356 SS 0.H74 1.2916 1.6430 1.Ns3 2.3718 2.6349
. 86 0.6774 1.2915 ' 1.H28 1.M79 2.3705 2.6342 87 0.6773 1.2914 1.M26 1. N76 2.3700 2.6335 i
88 0.6773 1.2912 1.M24 1.M73 2.3695- 2.6329 89 0.e173 1.2911 1.M12 1.N70 2.3690 2.6322 1 90 0.6772 1.2910 1.6420 1.9867 2.3645 2.6316 ,
l
l l
Pzga 1 ,
1 APPDTDIX B RAW AND PROCESSED DATA
Page 2 TABLE OF CONTENTS Ssetion I - Leak Rate Determination: 0245 a.m., Sept. 26, to 1445 a.m., Sept. 27 A. Mass Plot Analysis - 95% Confidence interval B. Leak Rate Analysis - Deviation of observations from predictions C. Normalized Air Weights - Containment and individual compartments D. Weighted Compartment Averages - Individual compartments E. Leak Rate Initialization - Compartment volume fractions and calibration curve coefficients for individual instruments F. Raw Data from Instrument Readings G. Calibrated Data from Instrument Readings H. Calibrated Air Weights - Containment and individual compartments I. Plots of Data Ssction II - Verification of Measured Leak Rate by Imposed Leak of .276% per day:
1600 Sept. 27 to 0130 Sept 28 A. Mass Plot Analysis B. Leak Rate Analysis C. Normalized Air Weights D. Weighted Compartment Averages E. Instrument Histories F. Leak Rate Initialia;ation G. Calibrated Data from Instrument Readings '
H. Trend Test I. Calibrated Air Weights J. Plots of Data K. Raw Data
- +
Faga 3 SECIION I
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_15 82269: 635 -0.1344369 0.0891299 0.3126967 96 82267: 630 -0 t 0901933 0,1025129 0.2952191 17 82269: 645 -0.0955435 0.0758489 0.2458412 ~ ~ ~ ~ ~~~~
'--'~~'~~~~D th 82269: 700 -0.0664680 0.0834861 0.2334401 t 19 82269: 715 -0.01423Z2 0.1299901 0.2742174
' __ 20 82269: 730 -0.0003647 0.1280439 0.2564524
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} _25_ 922691_290 .D.DZRIZZ2 0.1733841 0.2679909 ___
! 26 _022621_215. 0.115M54 0.219Q231 0._3124113 _. .
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. 2L_ B2262 s_.239. _ __9.137Z940 A 23G1500 0.3222221 _ . _ . _ _ . . .
_ _21: 822h29 945 O_13(1922.,_ _ D.2316971 0.3ti?850 _ _ , _ __
_2?__p;269: 1000 0.159M26 0.2278309 0.3121193 1 Qu 82259 sin {5 0,17_88879 O_t255_3275 0.3318872 31 82269: 1030 0.1854289 0.2567843 0.3279998 32 82269s1045 0.j@Z9142 0 2536984 0.3203027
_ M _ 8226?: 1100 0,.j@92669 0.2587569 0.3142469 )
34 82269 1115 Osl976290 0.2565547 0.3154804 ____
__.M _82249_ 11?a___ _ O,_19?j380 Oz2546086 0.3I0o792 36 82269s1145 0,t935746 0.2466871 0.2997995 )
37 82269s1200 O.t928542 0.2431706 0.293487I
! _JG_ 8226981215 O n 2006820 0.2487212 0,2967603 - - - ~ ~ ~ - - ~ - - --*
- 39 82269 1230 O.1978031 0.2437004 0.2895926 --~ ~ ~'-- ' '--~~ 3 l 40 82269
- 1245 O.1912768 O.2350049 O.2803329
\ ~ 4) 02269s1300 0.1983381 0.2337119 0.2760858 42 82269:1315 0.1957352 0.2361463 0.2765573 )
43 02269: 1330 0.1947215 0.2333531 0.2719847 ~~
44 82269:3345 0.1893795 0.2269799 0.2645302
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, 46 8226981415 O.1931996 0.2276618 0.2621240 47 82269:1430 0.1877395 0.2215000 0.2552622 4 (q 4,8 82269 1445 0.1836727 0.2165290 0.2493853 - )
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,j 52 02269 1545 O.1860219 n.214A386 n.2433553
'J 3 . .[:2269: 1600 0.1850076 0.2126782 0.2403480 54 82269 1685 0,1866736 0.2133154 0.2399573 _ _ _ _ _ )
FE5811 TS OF 00tJTAllJr1ENT HASS FtOT ANAL _YSIS(7./ DAY)
___ _ . _ _ . _ _ . _ _ _ Jt3 p
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- 7. 8??6981634 o.18*.9694 0.2116987 0.2374279
/, R ,3:22&?!l645 4.1812620 0.2067344._ O,232206?
".7 82260sl76u O.170'.441 0.2041046 U.2788651 #
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122._ 822798 930 Oe9642240___ h 07H2693 O d212ti5 __ _ . . _ . . . _ _ _ _ _ _
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- 20127 82270 I045 O.0636358 O.0765406 O.0894454 ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~
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~i33 ~~fMCy 8_ l5~ 6".O 74354 0.07955".O 0.09137I6
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134 82270s1230 0.0673946 0.0793314 0.0912682 . _ _ _,_
Q,QZ@M48 9.' 125. 922?Qs.4 245.__ __Q.9464431 O.0900862 _ . _ _ _ _ _ _ _ _ _ _ _ _ _ _
__ 136___D2270 1290 0.06640D7 0.0780575 O.0897062 _,_..__..__ _.___
._13Z__B22Z0tt315 A DM7ZB1 Dd7625St 0 009_Z3ZZ 12@__@2270:1220 _9,9M0?79 0.0782890 0,0895221 NOTE --Readings-148-through-186-include--imposed Leak Test - -- _ _ _ _ _ _ . _ _ _ _
_slh39 822ZQs1345 0 0663660 _Qio776524 0.0008183
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I41__D22Z011445 0 QM5996. O dZZQ291 O d876706 . _ _ __ __ _ _ _
. l _ i _ EN Z98_l'AO 0,9M3637 O dZ69917 0 99Z222_6 '
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l _ 132___92279!15.45 Ot 0665Z10 0.OZh5279 Od8M239 ._ _ __ , _ . _ _ _ _ ,_.
148 8227_OsliQO Od_M3204
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- 151 82270:1645 0.0669665 0.0765128 0.0860591 152 02270s1700 0.0673168 0.0767406 0.0061644 153 82270s1715 0.0680704 0.0774015 0.0067326 154 82270:1730 0.0684053 0.0776182 0.0868380 155 82270:1745 0.0682073 0.0773079 0.0864085 156 82270 1000 0.06@4Q87 0.0773857 0.0863697
__I57 812Z2sjS15 0.06'1186 0.0780728 0.0869771
$58__.9227981830 0.0694339 0.0782269 0.0870199 IM 02270s1945 0.0693644 0.0700489 0.0867334 - "~~
160 R2270s_tCOO O.0696II4 O.0788886 O.0867658 ~ ' '
161 82270s1985 0.0703611 0.0788674 0.0873737 162 82270: 3930 0.0707552 0.0791631 0.0875750
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. __. RESs 4.T S__OF_f 0NT AINMENT__NASS_F1.OT ANAL _YSIS t %/ DAY )
8100 TIME HINIHtXI OBSERVED HAl(IlSJH IIO DAYsilR LEAK RATE I_EAK RATE LEAK RATE ' - " ~ ' ' " ~ ~ ~ ~ " ~ ' "
.__.lt.3 OZZZQs1945 020711449 0.0794562 0.0877676 164 8227082000 0.0717657 0.0799992 0.0882328 1 165 82270:2015 0.0725306 0.0807045 0.0888784
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_. Par 3 & _ _ 88.389 ..e7 330 87.50 86.960 **6.700 86.7t0 g6.600 29.710 34.409__ 29.370_.__._ _ _ _
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..DN#L1 .76 82O___04,360 84,180 84 1 220 832 910 85.440 86.400 82.850 86.MO 95.800
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10 READING AT 82269: 500 '
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BAr#: A 25.470 25'950 2M.070 259.070 257.070 257.070 259.070 257.070 257.060 25E O70 ~ ~ ~ ~ - - - ~ ~ - ~ - - - - -
-3.090
' ' h_id_ .T_T_ ~_. _ _' k.._9.V_J__~_ ~D.9___. '_3 4 ~ ' 2__i.l. 46 46 550 4 F.D-- O. OOF-- 6 069--- 6'. D56 6_.~O56. --~'- ""-~'- _"_. .-~_ ~ _ "_
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' brJi- 3 ~~ ~ 14.675- 93.MS-- 4F455- 65.535--~54:455- 54:945- 54:550 B6 115-- 557730 07:126 - ~ - - - - - - - '
D4t#: 3 85.540 87 545 86.460 84.440 86.500 r.5.370 05 450 80 T70 57:23G 07 370
.. EAT E'_j$8_ $_76 ~ 67.:5_h0 Z O__7.470 _66.B70 B&:570 B5:U5 B&.525- 77.G' O_ 32:655-]9._515 Z-]~_- Z-' _7 reta: 5 "'- 3t. 600 5K926- 34!B90 27 170 30 540 29.190 33 060- 2F 030 26 000 M 510 -- -- --- ~ ~ ~
F4ta; 6 25 455--'253M 259.030 257.08o 257.000 257 U%T 25E7iGU- 257 U75 257 075-~75G70 - - ' - ~ ~ - -
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~B4ti J_ Z _24.352-~ 2 O 56 -3.790 4F750 49.520 O.009
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_._36 READING AT_Q22698Ii45
_PAf*; I & 840 83J60 87 750 83 810 82 580__ 85.J70 85.960 82.620 e6.330 95.400 t%t#' 2 94.860 *2.940
~
93.420 85.530 84.470 84.930 84.060 85.990 55.690 87.120 DAte 3 85.070 83 O60 8 U 30 84.460 86.400 85.350 85.480 88.120 87.210 87.420
--- ~ ~ ~ - -
. L'Na' *.4 - __ . 88.140 ._ 87.150_._87. 350_B6. 72D _B6. 610_ _B5.2ML__ P6J10 '30.230___31.7Z0 27.299_ ___ _ _ _ __ _
.._ Data: > 34.260___28.010 30d90 26.790 2a.220 27.499____33.910 26 Q'O 26 030 25&D0 _ _ . . _ _ _
. PA!a' h_.____25. 5 8 9__24,990 m _22b. !30 241,.169_._252,_120 252,259 _25_9,999_ 25_9,099_ 252,999__25.2,970
_ pat #'l 29.350 2L323 29 1.338 -3 t 740 40.570 49_,jli?O O.009 0,008 0,008 0,008 37 READlHO AT 82269:[200 DA C 1 76.080___f3.799___93.220 _ 02.010 83.500 85.149-__95 269 _ f2.699___E6.329 95,769 _ _ _ _ _ . _ _
__Dow 2 a4,360 92.280 93 g2O 85.490 84.47o 84 339 84,3 .O p%290 85 ZIO E7.150 ___a___
_ PN#1 3_ __B5.939__93. 050 86.329 _ B3.330 86.369 05.360 95.310 DL 129 87.299___DZ 560 _ _ _ _ _ _ _ _ . _ _
. _ PANPL S 63.170.__BZ.109 8Z,390 8b Z10 84ta19 _ Qb 919__ Hb 5N L._29,290 31, N9_ a9,310
- DAff 5 34.740 29.p Q 75 420 26.830 33.590 28,51Q ")2dlO Zb210 26.060 25,580 DAf 81 e _2% 699__2fu999__239,979__243 229 _252 J80 25L949_252 939_259_,979_25L 930__252,929 _ _ . _
__DN#: 7 29,355___29,2?8 29.343 -3.660 49 590 49 m 680 OtOO9 0,009 0,_0_08 .9,908 _ . _ __._-
38 READING AT 82269:1215 ~ "
bat #: 1 76.880 83.770 83.900 83.770 83.540 85.120 85.890 82.500 86.290 95.280
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DAt#' 2 94.830 92.960 93.380 85.480 84.470 84.860 84.120 86.030 85.670 87.170 DAt#: 3 85.030 83.040 86.390 84.420 86.470 85.330 85.390 88.120 07.850 87.430 DN#' 4 88.180 87.260 87.300 86.790 86.600 85.960 86.500 31.350 34.330 30.490 lete' 5 38.590 29.580 38.860 27.i50 36.860 39.330 32.800 26.910 25.970 25.570 DAHl: 6 25.660 25.980 258.300 258.930 258.930 258.930 258.930 258.930 258.940 258.930 DAl#: 7 29.357 29.340 29.343 -3.030 46.666 49 7550 5 659 0.009 5.555 0 667 39 READING AT 8226988230 - " - - - - -
UN#' I 76.880 85.720 83.9iO 83.750 83.5'30 85.I10 85.880 82.570 86.280 95.250 DN#: 2 94.820 92.900 93.350 85.440 84.420 84.830 84.000 86.000 85.660 87.100 DN#: 3 84.090 83.000 86.300 84.360 86.4IO 85.320 R5.360 88.060 87.070 87.430 DAt#: 4 88,090 87.210 87.260 86.760 86.590 85.900 86.470 30.990 32.460 30.270
_1%t#' 5 351990 29.170 32,970 27.470 29.A30 28.440 32J60 26,910 26.000 2L.h t 0 DAt#: 6 25.720 25.990 258.890 258.890 258.890 258.890 258.890 258.890 ?58.890 258.890 Ter#" 7 29.351 29.333 29.339 -3.680 40.6*'O 49.500 O.OIO O.009 0.008 O.009 40 REAltit#3 AT 82269: 1245 DN#: I 76.880 83.770 83.870 83.760 83.540 85.090 8".930 J
_ _ _ _ _ _ , , _ _ _ _ _ _ m 82.570 86.270 95.210 __ __ g Imt#' 2 94.810 92.950 93.340 85.450 84.430 84.790 83.990 85.990 85.600 87.030 DAr#' 3 85.000 rp 82.990 86.200 84.350 86.430 85.310 85.350 88.070 87.180 87.400 DN# ' 4 A8.030 87.140 87.290 86.760 86.560 05.960 86.470 30.745'-~ 38.860 30.050
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. _8 Ate: 7 29.346 29.326 29.335 -3.140 41.770 50.100 0.014 0.0:3 0.013 0.013 _ _ _ _ _ _ _ _ . . . . . . _ . _
63 READING AT 82269s1830 DAt#' 1 76.800 83.520 83.660 83.530 83.320 84.820 85.480 82.410 86.300 95.500
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- 2 94.600 92.820 93.230 85.260 84.260 84.650 83.910 85.7t0 85.490 87.010 EtMe' 3 84. 8*iG 82.830 85.930 84.180 86.300 85.120 85.000 87.920 87.060 87.260 .
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DANK 4 87.900 87.130 87.210 86.720 86.490 86.410 86.370 31.250 32.630 30.480
_PAte' 5 37.120 29.590 33.850 27.540 29.730 28.490 32.900 27.200 26.3fo 25.910 DAt#' 6 2 % 830 26.140 226.850 233.510 239.020 243.140 248.990 247.700 252.230 253.880 f9.330 -3.IOO 41.590 50 440
" Eid 7 257 4f~~~f3.~322 0.0f4 0.003 0.013 0.013 - - _ _ - . . - . _ . -
64 HEAD 1NG AT 82269st845 -~~
76 040
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. _ BMK_2 89.B30 02.630 85.910 84.190 86.210 OLg?9 95,200 87,960 87.gZQ__gZm320 _ _ _ _ _ _ _ _
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,,_.two' 7 29.339 29.324 29.329 -2.990 41 530 50.360 0.014 0.014 0.013 0.013 _____ _ _ _ _ . .
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_ _PPl#' 2 94.600 92.830 93.210 85.260 84.190 84.660 83.890 8% 710 85.470 86.920
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_ peta: 5 3Z,990 28.330 37 960 27.260 32.140 28.320 32.490 27 220 26 310 25.950 ___.2
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l 66 READING AT 82269s1915
{ DANK 1 76.840 83.490 83.61O B3.5t0 83.290 84.850 85.380 82.300 86.070 95.330 3
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- 2 94 t S80 92.790 93.200 85.230 84.t90 84.720 832 930 85.660 85.450 86.910 I D M #' 3 84.830 82.800 85.860 84,200 86.250 85.070 85.090 87.930 87.030 07.200 i
. _ pme: 4 88 970 87d20 87 120 86.650 86.456 86.400 86.360 31.260 36.160 30.630
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BNa< 5 30.400 27.990 39.500 27.620 35.660 28.990 33.250 27.230 26.360 25.970 DANK 6 25.700 26.210 253.320 258.340 258.340 250.340 2".8.330 258.330 2*>8. 330 258.330
._,IWe' 7 29.345 29.325 29.332 -2.920 41.890 50.470 0.013 0.012 0.012 0.012 _ . _ _ . _ _ '
67 READINO AT 82269:1930 liAt#' 1 76.840 83.480 83.600 83.500 83.270 84.850 85.280 82.300 86.050 95.$io
__EOt4' 2 ?i,5ZO 92.750 93.170 1 85.210 84t220 84.640 83.010 85.670 85.460 86.860
,_ Data' 3 84.820 82.790 85.960 84.150 86.270 85.020 85.040 87.900 86.980 87.260 DN#: 4 87.960 87.020 87.150 86.640 86.430 86.370 86.340 31.390 32.730 30.410 i Ata' 5 36.340 28.290 34.230 27.360 30.250 28.240 33.450
_ _ . . _ - _ _ _ m 27.230 26.390 25.980 m Data'. 6 25.690 26.220 248.350 250.420 258.420 258.420 253.420 258.4iO 258.4iO 258.41o
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___for e' _ ) 76 320 h2.319 E 500 222.90o OL190 g3,28o 85.I?9 92.210 85 990 94dOO ._ ~~T'.
rmtr_2 93.c90 92.710 93.040 85,140 84.0e0 84.450 83.770 85.580 85.380 86 820 Dart: 2 OhD20 SLZOO 85.770 84,100 86t271 R41920 re.970 87,900 86.980 87.100 DNF 4 87,940 @2_aQ2O _ g?_,130 86.590 86 t 300 86.290 Ot s_270 31,OJ O '32.080_ E 390 _ _ . _ _ _ _ _
DANK 5 35.340 2'hg2O ]Q.730 27.010 28.180 27.550 32.780 27.350 26t420 ?6.020 DNF 6 25.p40 26 770 254.990 258.480 258.480 252 400 258.48n 258.480 253.480 258.480 DAPN' 7 29.332 29.313 29.320 -2.440 42.110 48.340 0.012 0.0ti O.011 0.011 _ _ _ _ _ _ _ _ ._
77 READING AT 82269:2200 DAte' I 76.820 83.360 83.480 83.370 83.170 84.780 85.420 82.300 85.900 94.870
___DAPN' 2 94.460 92.670 93.010 85.090 84.100 84.520 8?.750 85.540 85.410 86.770 DAra: 3 84.830 82.710 85.800 84.130 86.200 84.960 85.070 87.8"O 86.980 87.860 DAt#: 4 87.860 87.020 87.360 86.580 86.340 86.280 86.260 31.070 32.630 30.580 DN#' S 36.090 28.400 36.130 27.100 31.090 28.200 32.360 27.350 26.440 26.020
_ DArd ' 6 25.810 26.340 223.160 233.430 234.210 248.860 244.900 248.030 249.170 254.010 DNet 7 29.335 29.318 29.522 -2.390 4T 79o 78.270 8 0.012 0.012 0.611 0.011 - - - _ - . . - - - - - .
78 READING AT 82269:2215
__JN # wl Z61 920 8)t3tQ 83.470 83.350 83.160 94 Z10 85.410 82 2 230 8WO 94 @ O ~_ [1 _~~
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Data' 2 94._970 92.720 93.000 85.110 84.050 84.510 83.640 85.530 85.300 ab.800 Data' 3 84.880 87.680 85.750 84.080 86.180 84.930 85.040 87.830 86.970 87.140 DAtW 4 87.890 86.900 87.090 86.630 86.370 86.290 86.260 30.860 35.530 30.520 DMe' 5 37.840 27.900 38.900 27.540 34.430 29.0"O 33.060 27.340 26.470 26.020 DAt#Li 27 730 26.329 2221020 236t 290 239.800 244._450 249si?O___22138[O 254,_920 256.860 DAIF 7 29.336 29.32l 29.324 -2.410 42.130 48.270 0.013 0.012 0.012 O t_
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79 READING AT 82269:2230 '
ImHK_1 76 s 050 83 290 83.440 83t250 83,170 84 290 85.470 8],280 85.970 94,299_ _____ _ [ ~5 DMA: 2 04._i40 92 720 92.970 85.090 84.060 84 2LO 83.660 85.520 85.360 86.830
._ttANV 3 84.830 82.t00 85.770 84.070 86.200 84.920 85.020 87.840 86.910 87 120
_ DNC 4 87.960_,__86.960 87.040 86.6iO 86.330 86.260 86.230 3h440 37_.420 30.290 DAt#: 5 36.240 28.330 34.240 27.230 29.860 28.030 33.420 27.350 26.490 26.060 DAP4; 6 DAt#' 7 25.770 29.330 26.360 226.990 237.110 245.990 248.640 253.710 256.480 ?58.220 258.220 29.347 29.320 -2.350 41.970 48.310 0.013 0.083 0.012 0.012 _ _ _ - _ _ _ _ . _
80 READING AT 82269:2245 ~
. . _ imp #' 1 76 8_!O Bh 260 OL450 83.330 83.130 84.760 85.450 82.290 85.960 94.730
__LiA__t#' 2 94.420 222670 9_2 960 85.080 84.010 84.450 83.650 85.540 85.370 86.740
_DN!L3 89:829 82,109 __95,480 84.060 86.190 84.930 84.990 87.840 86.910 87.130 DANK 4 87.990 86.960 87.050 86.570 86.320 86.240 86.220 31.270 31.670 30.180 DN#'5 35.190 202 000 31.180 26.870 28.460 27.610 32.670 27.370 26.480 26.040 ImtM: 6 25.750
_ DAtM 7 29.330 26.3YO 215.350 228.060 29,3j5 -2,500 232.710 42 020 237.430 48.370 239.870 241.460 247 190 251.520 29_23_2O
_ t 0,013 02 013 0.012 6 }[2 81 READING AT 82269:2300 76.840 DAtat t DANI' 2 94.420 83.350 92 600 83.440 92.950 83.370 85.054 83.130 84.030 84.760 84.480 85.390 83.720 82.200 85.510 85.950 85.360 94.710 86.670
_ C' _ __EZ DANB: 3 84.810 82.710 85.730 84.120 86.160 84.800 84.990 87.840 86.940 87.050 DN N' 4 88.600 86.980 87.050 R6.560 86.330 86.260 86.230 30.620 34.520 30.150
't!
__ImtW 5 35,920 28.000 36.540 27.200 31.900 27.930 31.960
~~~~ ~~
DAP4' 6 25.800 26.390 257.280 253.200 27.3?O 26.490 258.200 258.t90 258.190 258.190 253.t90 258.I90 26.030 $
(D BAlW 7 24.335 29.317 29.'321 -2.600 42.030 48.320 0.013 0.612 0.013 0.D32 _ _ _ _ _ _ _ _ . y C2 READINO AT 82269:2315 Tild F i~ ~~~75. Nih
. Bi'.33 5 ~ 53.1iO' 63.330 83.t30 84.750 ~5.300 8 82.270 55.-955- 94.680 Dma' ? 04.420 92.650 92.930 85.060 84.06(s 84.500 83.660 85.510 85.350 86 2 730 DAtr. 3 84.840 82.690 85.740 84.060 06.120 84.870 84.97ts 87.810 86.850 87.050 Data; .4 . . 07.860 86.n70 87. M t .86.600__06 720 DNa e, 8.6.240_ c6.22n. so. 2rxe . 37, ton _29.970 m.2nn 2r:. 02n w.4no 27. n e.n v.. or.o n n'>o ,- = ., u<. v m ~ a-a
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