ML20054L904
| ML20054L904 | |
| Person / Time | |
|---|---|
| Site: | Clinch River |
| Issue date: | 07/02/1982 |
| From: | Longenecker J ENERGY, DEPT. OF, CLINCH RIVER BREEDER REACTOR PLANT |
| To: | Check P Office of Nuclear Reactor Regulation |
| References | |
| HQ:S:82:064, HQ:S:82:64, NUDOCS 8207090050 | |
| Download: ML20054L904 (118) | |
Text
_
11 Department of Energy Washington, D.C. 20545 Docket No. 50-537 HQ:S:82:064 JUL 0 21982 Mr. Paul S. Check, Director CRBR Program Office Office of Nuclear Reactor Regulation U.S. Nuclear Regulatory Commission Washington, D.C.
20555
Dear Mr. Check:
RESPONSES TO REQUEST FOR ADDITIONAL INFORMATION
Reference:
Letter, P. S. Check to J. R. Longenecker, "CRBRP Request for l
Additional Information," dated March 25 and April 30, 1982 This letter formally responds to your request for additional information contained in the reference letters.
Enclosed are responses to Questions CS 490.13, CS 760.10, 36, and 110 which will also be incorporated into the PSAR Amendment 69; scheduled for submittal later in July.
Sincerely,
(
Jo R. Longenec Acting Director, uffice of the Clinch River Breeder Reactor Plant Project Office of Nuclear Energy Enclosures cc: Service List Standard Distribution Licensing Distribution egg 7ggo ego o
A
3 page 1 W82-0337 (8,22) 22 Quest.lon_CS490213 Af ter reading the description of the FRST code in appendix A, it is apparent that the ductil ity limited strain model for evaluating f uel perf ormance is very dif f erent f rom the old " design procedure", or as it was al so called, the
" design reci pe" or "FCF213".
The information provided in the PSAR on this model is quite limited.
Please provide a detailed description of the model, including material properties used and the data to back those properties.
A l isting of the FRST code woul d be very helpf ul.
Please al so Indicate how the model has been cal ibrated and qual ified.
Responss A detailed description of the FRST code will be documented in a report to be submitted to NRC by January,1983.
This report will contain a description of the analytical models employed by the code, the material properties and the basis f or those properties.
The question addresses the dif ference between the FCF213 design procedure implemented f or FFTF and the FRST design code used as the design procedure for CRBRP fuel rods.
Both procedures calculate creep strains using the same creep equation f or solution annealed material.
Both procedures l imit the ductil ity limited strain:
Steady State 0.2% fuel FFTF and CRBRP (0.1% bl anket in CRBRP)
Normal, Anticipated 0.3% f uel
~3 FFTF used 0.7%
? CRBRP and Unlikely Events 0.2% blanket)
FFTF l imits were verif ied f or FFTF (e.g., see PSAR Sections 4.2.1.1.2.2, pages 4.2-6 th rough 4.2-8, and 4.2.1.3).
The CRBRP and the FFTF design procedure are based on the same type of assumpt i ons.
Tabl e 490.13-1 lists the assumptions for input parameters to the steady state cladding creep analysis including some of the implications of these conservation assumptions.
The most important implication is that the calculated strain overpredicts the actual str ai n.
CRBRP and FFTF employ slightly dif ferent procedures to calculate the input parameters.
These dif f erences are a resul t of the ef f ort to use consistent QCS4 90.13-1 Amend. 69 July 1982
page 2 W82-0357 (8,22) 22 properties and parameters consistent with the CRBRP nuclear, thennel hydraulic and mechanical analysis codes.
For exanple, 25 uncertainties are applied to plant expected conditions throughout the f uel perf ormance analysis for CRBRP whereas nominal temperatures are used in FCF213. Dif f erences between FCF213 and FRST steady-state property assumptions are summarized in Table QCS4 90.13-2.
The biggest dif f erence between both procedures is the smaller cl adding tol erance and contingency of the FRST procedure.
The FCF213 cladding loading due to 100% fission gas release might be thought to be more conserva-tive than the 2ar fission gas release.
However, FRST obtains fission gas pressures from the NICER and LIFE codes which are based on a defined set of coupled uncertainties which for high powered pins yield 100% release based on the +2o rel ease data. Theref ore, comparison between the two design procedures requires a case by case comparison.
In summary, the cladding loading and cladding temperatures used in FRST are more conservative than in FCF213.
The overpower transient evaluation of CRBRP rods with FRST is similar to the FCF213 approach, yet Individual properties input to each procedure are evaluated dif f erently.
Tabl e QCS4 90.13-3 summarizes similarities and dif f erences of both procedures.
The FRST temperatures are obtained f rom the FORE-ll code, which provides a consistent basis f or all saf ety analyses.
These cal cul ations use 3 a-uncertainties applied to thermal hydraulic design conditions.
Local conditions are considered in evaluating cladding damage.
Both f uel rod transient evaluation procedures are val idated based on the same fuel rod transient test data.
The results obtained with FRST are conservative in predicting f uel rod transient test f ailures.
The comparison of predicted and observed f ailure times for overpower transient tests will be included in the topical report of FRST.
The dif ferences and similarities between FCF213 and FRST, as discussed above and in the attached tables, can be sawnarized as follows:
o Steady state loading is omnparable only for fission gas loading (FRST considers steady state loading of the cladding due to FCMI).
o FRST calculates local axial loads due to transients which are higher than the column average loads f or the limiting location.
l o FRST uses consistently higher tanperatures than FCF213.
l QCS4 90.13-2 Amend. 69 July 1982
page 1 C82-0357 (8,22) 77 T/6LE QCS490.13-1 DESIGN PROCEDURE FOR OtBRP STEADY STATE CREEP ANALYSIS Calculated Parameters Paantred Assumotlons M
Strain rate Thermal creep rate for solution Overpredicts Irradiated 205 Cw annealed 316 stainless steel 316 SS creep rate Temperature Upper 2d local hot spot over 97.5% of time temperature is below design life this requirement Fission gas Total gradient totally relaxed by Primarily relaxed by non-damaging thermal creep Irradiation creep Fission gas Upper 2 F ilmit, linear by cycle Linear behavior more conservative i
than actual exponential increase Fuel loading Worst prediction considered worst combination of Irradiation Induced creep and swelling and f abricated variables Cl adding wastage Upper limit on tolerance, weer, Approximately 40% of original defects, sodlun corrosion and cladding thickness is assumed not fission product attack offective at end of design life Stress limit Below proportional limit No plastic strain allowed 1
1 a
t s
QCS490.13-3 Amend. 69 July 1982
- ni e,
-n
- ~
page 2 W82-0357 (8,32) 77 TABLE QCS490.13-2 III (X)WARISON OF FCF-213 AND FRST STEADY STATE HRFORMANT EVALUATION ASSUWil0N Pronertv FCF-21dII IRST h ts Cladding Loading Fission Gas Pressure
+2f Fission Gas + Un-Comparable at X/L = 1.0, (100% Nminal Release) certaintig)andFCMI FRST, More Conservative from L*FE Otherw ise Cladding Temperature N m inal Cladding ID Hot Spot Midwall with FRST More Conservative Uncertainties at +2r Level Cladding Tolerance 2.5 Mil s 1.5 Mils and Contingency Fuel Cladding Chenical 2.0 Mlls 9 BQ.
CDF/ LIFE Model FCF-213 Used for Gas Interaction Loading Only, No Etfeet Otherw ise Sodium Corrosion 2.1 Mit s Max. 9 EOL CDF/ LIFE Model NOTES:
(1) As described and verifled in addendum to HEDL-TE-75-48 (2) Corrected by wastage to give same stress QCS4 90.13-4 Amend. 69 July 1982
- an_nte,
page 3 C82-@W9 (GbZ$D W
~
\\
TABLE QCS490.13-3 IU COWARIS(N OF FCF-213 AND FRST OVERKWER 1RANSIENTS EVALUATION ASSUWTIONS III Pronerty FCF-213 ff.$1 Comments Fuel & Cladding Nminal by ARGUS Code 3F Hot Spot by FORE-Il FORE-ll Nminal Tempera-
]
Temperature Increase Code tures Similar to LIFE-IV (TREAT)
Cladding Thermal Same Conservative Relative to Expansion Failure Time Fuel Axlat Expansion Same Cladding Pressure 100$ Fission Gas Only
+2 Fission Gas and at Time Zero LIFE SS FCMI Translent increase of SS Loading Very Conservative Plenum Temperature Outlet Coolant Local Cladding During Transient Temperature Temperature I
Basis for Translent Fuel Column Axlal At Local (X/L)
Little Dif ference for l
Contact Pressure Average Conditions EBR-il/ TREAT, FRST Conservative for Limiting X/L Stress-Strain Curves aP = 0.2%
g P = Prior PL, Necessary for Multiple a' = 0.7%
g* = 0.3% for DLS Transients, Stress Same for Contact Pressure At ge is Same J
BQIE:
(1) Per HEDL-TE-75-40, R. E. Bears, September 1975 4
i
(
QCS490.13-5 Amend. 69 July 1982 no.m o
~ ~'
l rcgs z tez-UF/4) LB,22J 799 Ouestion CS760.10 The purpose of the analyses supplied in Chapter 15.2 for reactivity transients is to provide substantiation of the adequacy of the reactor shutdown system (RSS) design. As such, this means that the accidents are protected and that the physical Interation of the plant protection system (PPS) as well as the plant control system (PCS) with the neutronic and thermal /hydraulle responses must be coupled in the predictive tools to correctly follow the transients.
The CRBRP heterogeneous core dif fers f rom the previous homogeneous core in many ways. The heterogeneous core used 32.8% enriched f uel (Pu/(U + Pu)), as opposed to 17.4 and 25.1% enrichment in the homogeneous core. The fissile inventory is also significantly larger (10 to 25%). At the same time, the Project states that the control rod worth requirement is considerably lower for the heterogeneous core ($17.44 primry for B004 as opposed to $26.53 primary for the equilibrium cycle of the homogeneous core).
The CRBR Project has computed the Doppler Coef ficient to be -0.0084.
This val ue f or other LMFBRs (with homogeneous core) ranges f rom -0.0032 to -0.0060.
A caref ul assessment of this prompt negative coef ficient of reactivity is essential, as it also impacts on the (PPS) and the (PCS).
Please provide the distributton of Doppier as welI as sod!um vold and f uei expansion reactivity coef fIclents for BOL and EOL cores with and without sodium. The PSAR gives these numbers of regions only.
(Table 4.3-18 gives the axial distribution f or BOC-1 only.)
Resoonse The attached provides the reactivity worth distributions for flooded and volded Doppler, sodium void worth, and f uel pellet and steel material worths f or clean-core conditions at the beginning-of-cycle-one and f or f ul ly burned core conditions at the end-of-cycle-four (550 ef fective f ulI power days).
Figure QCS760.10-1 shows the assembly numbering scheme for fuel and inner blankets in a 1200 core sector.
Figure QCS760.10-2 shows the positions of the 20 axial nodes distributed along the active part of the core assemblies. The reactivity worths are provided in units of T dk/dT per channel for the Doppler and$1L for the sodium, pellet and steel worths at the 20 axial node locations for e$ch of the f uel and Inner blanket assemblies in the core. Tabl e QCS760.10-1 lists the masses of f uel and blanket constituent materials which can be used to convert the units in the data tables to reactivity worth (ak).*
This reactivity worth data is consistent with that provided previously to the NRC for the use in the CRBRP HCDA analyses.
- $ =4k/.0034.
QCS760.10-1 Amend. 69 July 1982 fMBENO
POge 3 (82-0374) [8,22] #99 Bealnnino-of-Cvele-One Reactivity Worths Table QCS760.10-2 contains BOC1 flooded Doppler constants (T dk/dT) by channel (Figure QCS760.10-1) and the corresponding 20-axial-node weighting f actors.
The 80C1 Doppler values in Table QC3760.10-2 represent the total Doppler constant for the total number of times each channel appears In the full core (for example, channel 1 appears three times and channel 2 appears six times in the f ull core). The Doppler constants were determined f rom 3D First Order Perturbation calculations with 21-group ENDF/B-Ill cross-section data by elevating the U238 and Pu239 temperatures 10000F above normal het-full-power core conditions.** Figure QCS760.10-3 gives the ratio of volded Doppler to flooded Doppler by assembly.
Table QCS760.10-3 presents the B001 sodium vold worth (ak per kg of sodium) by assembly-node in the f uel and inner blankets. These reactivity worths were determined by removing sodium and substituting f ully volded 21-groups ENDF/B-llI cross-sections for the equivalent flooded cross-sections in a 3D-FOP calculation at 8001.
Table QCS760.10-4 presents the reactivity worth of adding steel in each assembly-node in units of ak per kg of steel.
Table QCS760.10-5 presents the reactivity worth (ak per kg of pellet) of adding f uel or blanket pellet (heavy metal plus oxygen) in each assembly-node.
In the axial blankets, the pellet worth is that for adding material fran the nearest f uel region, simulating core f uel sweep-out through the axial blankets.
Table QCS760.10-6 summarizes the total regionwlse reactivity worths (ak) for f uel, inner blanket and axial blanket regions. This information serves as a check on the sum of the nodal values f rom Tables QCS760.10-2 through 5.
End-of-Cvele-Four Reactivity Worths l
Table QCS760.10-7 contains the E004 flooded Doppler constants (T dk/dT) by assembly (Figure QCS760.10-1) and the corresponding 20-axial-node weighting factors. The E004 Doppler values in Tables QCS760.10-7 represent the Doppler constant for a single assembly. Therefore, the assembly-Doppler values must be multiplied by the number of times a particular assembly appears In the core to obtain the total core feedback (for example, assembly 1 must be multipiled by three and assembly 2 by six). Tables QCS760.10-8 gives the equivalent volded E004 Doppler constant distributions.
1 i
- Hot-f ull-power pel let everage temperatures are fuel = 20700F, inner 11000F and (burned) = 18180F, upper axial blankets and blankets (fresh)
=
extensions above the Inner blanket central 36" region = 10270F, and lower axial blankets and extensions below the inner blanket central 36" region =
7560F.
QCS760.10-2 I
Amend. 69 July 1982
hage~k(82-0374)[8,22](99 Tables QCS760.10-9 presents the E004 sodium vold worth (ak per kg of sodium) by assembly-node in the f uel and Inner blankets.
Table QCS760.10-10 presents the reactivity worth of adding steel in each assembly-node at E004 in units of Ak per kg of steel.
Table QCS760.10-11 presents the reactivity worth (4k per kg of pellet) of adding f uel or blanket pellet (heavy metal plus fission products and oxygen)
In each assembly-node at E004.
In the axial blankets, the pellet worth is that for adding material from the nearest f uel zone.
Table QCS760.10-12 summarizes the total E004 regionwise reactivity worth Gak) for f uel, inner blanket and oxial blanket regions.
l l
QCS760.10-3 Amend. 69 July 1982
Page 7 (82-0374) [8,22] #99 TABLE QCS760.10-1 CRBRP MASS OF SODIUM, STAINLESS STEEL, AND FUEL PELLET PER ASSEMBLY (kg/cm of Assembly Height *)
Region Sodium Stainless Steel Fuel Pellet **
(kg/cm)
(kg/cm)
(kg/cm)
Fuel
.449-1
.236
.409 l
inner Blanket
.3 01-1
.171
.700 Lower Axial
.462-1
.237
.430 Blanket Upper Axial
.413-1
.259
.430 Blanket Lower Axial
.306-1
.171
.700 Extensions Upper Axial
.272-1
.171
.700 Extensions
- See Figure QCS760.10-2 for nodal heights.
- Mass of fresh fuel is given since mass changes <.5% with burnup, i
QCS760.10-4 Amend. 69 July 1982 casa sw
I l
l Table QCS760.10-2 LCCAL nopetro wrTGw'ING FACT 00 AND CH ANNEL OnoPLEP COE FFICIENTS AT P3C1 (T DK/DT)
CHAMMEL A)tAL NOME 1
2 3
h 5
i
.51kie-p?
.5k70E-n2
.6P67E-02
.3647E-02
.5 A7 mE-02 7
.21a2e-01
.21kme-01
. 2355 F- 01
.1227e-01
. 2 210E- 01 l
?
. 2661E- 01
.2511 E- 01
.2736C-01
.142kE-C1
. 2579E- 01 k
.?49hE-Ci
.3km9r-01
.3658E-Oi 153kr-*1
.3531E-01 f
5 4907F-ni 50 2pE-G i
.5198E-Oi
.5k97r-ri
. 5216 E- 01 1
6
.6717r P1
.6724E a i
.689hF-01
.7517E-01
. 6999 E- 01 7
. ATC4E-P i 8158F-01
.MCO2E-Oi
.9155E-01
. 8661E- 01 8
06 k 6e-31
. 9 646 r- 01
.9768E-01
.1074E+C0
. 996 0E- 01 l
I 4
.in19E*3"
.iO39E+00
.1949E+00
.1145 E+00
.1063 E* 0 0 I
19
.1046E+0"
. i O 47 r + 9 0
.ie55E+00
.1136E+00
.116(E+0e x3 S
11 49 ACE-01 4889F-Oi 9943r-01
.iOkEr+PO
.9876E-Oi l
M 12
.gyngr-ni
.M731F-01 8762E-01 8943E-Ci
. 8 5 66 E-Oi P
13 7149e-01 7178r-01 7175 E-O i
.69k7E-Oi 6893E-01 14
.5626E-pi 9445E-01
.5193F-01
.5030F-ti
.5122E-01
-d
?
15
. 377 2r-91 376?E-Di
.3622E-Ci 3327F-01
. 34 69 E- 01 16
.237'F-01
.??16E-01
.2013F-Oi
.1918r-01
.2c65E-01 17
.iS34E-01
.143ar-01
.9782E-02 4046E-92
.13 f 3 E- 01 la
.ti3"E-91
.iO5pr-01
.71608-02
.293RE-02
. 9 584 E- 02 19 7 2 4 6F- 0 2
.6770E-02 4539 F-02
.1930F P2
. 6134 F- 02 28
.?21CE-ri
.1050E-02
.in99E-02
.6469F-03
.177kE- 02 ewArgrt, nopptro e, er er T CTENT ?
I
. 4722r "4
.94 65 E- 04
. 5 297 E-0 4
.1259E-03
. i O66 E- 0 3 l
O C.
B
I Table QCS760.10-2 (continued)
LOCAL 600ptro wcIGH'TNG ractoo AND CHANMet COPPLER COE FFICIENTS AT MOCi (T DK/DT)
CHAN4EL avtAL WonF 6
7 8
9 10 i
6194E-0?
76 70E-0 2 472 5 E-0 2 4139F 82 7977 E- 02 2
.2'?hr-at
.2667r-Oi
.1339E-01
.3013F-01
. 2651E- 01 3
. ?? q aF-01
.?847E-01
. iS9 9 E-01
.3493r-Ci
. 3 0 7 6 E- 01 6
.3674E-t?
1'22 E- 01
.3695F-Oi 4392E-Ci
.3929E-01 5
92118-71
.53m39-Ci
.5608E-Oi 6191*-51
. 5 492 E- 01 6
6951e-r i 7129r-01
. 757 5 E-01
.A012F-01 7228E- 01 7
457 tr-p g
. 4 7 55 E-G i
.9365E-Oi
.9797F-01 8859E- 01 9 911E- 01
.100ir+00
.1072r+00
.tii3E+00
.1010E*00 9
.1052E+0n
.1068E*00
.1141E+t0
.ii72F+00
.ic76E*00 10
.1052r*99
.1365E+96
.1133 E+ 0 C
.1141E + O C.
.iC64E*05 f
11
.Qa44r-01 9420E-ni
.iO45E*00
.1011E+00
. ?811E-81 i
y i?
9506*-01
. 8 6 2ir- 01 8911E-01 7896E-Oi
. 3 37 9 E- 01 P
13 6971e- 01 69 34 r-01
.6976E-01 4493F-ci 6598E-01 ik
.E? Die-01 5112r-ni
.5026E-01
.293pe-C1 4797 E-01
?
tr
.3511e-ci 3351E-ni 3234E-01
.iB94E-P1
'. 3157E- 01 16
. 2 07 2r- 01
.1761E-01
.1698E-01
.1126E-01
.17 5 2E- 01 17
.12 2 iE-11 8181E-02
.2407E-02 7C92E-02
.8667E-02 iP
.99GOE-PP 9974E-02
.1761 E-0 2
.5199F-C2
. 6346E- 02 l
10
.56P7r-02
. 3765 E- 0 2
.1115E-C2
.33C6E-r2
. ht P EE-0 2 I
2r
.144 2e- 0 2 4041E-f3
.2651E-03
.6499E-03
. 8 8 F 2E- 0 3 I
1 cuaNgrL OPooLED C Er rricTEute l
l
.116>E-c=
.ti84r-03
.1624E-c3
.1370r-o3
.14 88 E- 03 i
i l
ST EI I
cr a" fu 1
l l
Table QCS760.10-2 (continued)
LCCAL 00** Leo WETnHTTNG raC709 AND CHA NNEL DOPPLER C0FFFICIE975 AT BO*1 (T OK/DT1 CHAMMFt AYTAL POOR 11 12 13 in 15 1
.*11mr-pp
.q36qE-62 0523e-82 92F4F-f2
.4508E-82 2
. 267 ?e-01
.30k%E-01
. 33 85 E-01 3233E-fi
. 325 2 E- 01 I
3 2099F-01 1927E-01 3939E-Oi
.3760E-01
.3879E-01 6
194 AE-01 4419 F- 01 6774 E-O i 4627E-01 4711 E- 01 5
55 0 'e- 01
.6123r-Oi
. 615 4 E-01
.611Ge-ri
.6214E-Oi 6
7730' e.1
.A025E-31
.7063E-01
.7965E-C1
. 8 072 E- 01 7
.*P65F-ni 9802F-Oi
.*714E-Oi
.97c1E-91
. 985 nE- 01 A
. i O 11e+ 0 e
.1112E+OO
.1102F+04
.11f2E*00
.1118E*00 fl o
.iO'4E+0*
.ti72F+00
.1160E+00
.116gr*00
.1177 E* 0 0 23 19
.tc6ke+ni
.tikCE*60
.1126E*OP
.112*E*r0
.1145T*05 8
11
.qaO9E-01
.iO10e*06
. 902 8 F-t i
.99A2F-ti
.1012E+00 12
.A376e-01 77 97 e-O i
.7571E-Oi
.7670E-Oi 7 786E-Oi
_.o it
.6so1E-ni
.448ME-ci
.k12OE-Ci
.h323E-Ci 438 0E- 01 i
N 14 479 me- 01
. 29 27 F- 01
.7646r-Oi
.2913E-01
. 284 a E- 01 15 11k te- 01
.1877F-Di
.1741F-Oi
.1944F-01
.1A65F-01 il 16
.17 ' p e-P 1
.1103E-ci
.1110 E-01
.1203r-ci
.1214 E. S i 17
.94*9e-02
.6A75E-02
. 87? 3 E-0 2
.8379E-t2
.4075E-02 l
18
. 610 7E- 0 2
.5035E-C2
.6LO4E-02 6150E-02
. 2992 E- 0 2 iq
. 3a 3 5g-q 2
.3195E-02
. Ar96E-02
.392Or-C2
.199 8 E- 0 2 1
2" 832iE a 3 7 8 7kr-r 3
.111gE-02
.itS8F-02
.5206E-83 rw ANNrt nnpotre c.errrTCTENTS
.14 9 0 F- 0 3
.13 A8 E-0 3
. 6159 E-04
.133kF-C3
.1328 E- 03 I
i i
1 d
8 j
hfk GTB" 1
i I
i
I l
l l
(continued)
LOC AL Mqoples wcf r.HTI4r. r&Cv00 AND PH ANNFL 00DPLE# COEFFICIENTS A7 00C1 (T 04/07)
CHANNEL AvTAL We9r 16 17 19 19 20 1
.iasar-pt 98g5E-02
.6757E-02 6210F-02
. '65 9 E- 0 2 2
. 3 3 A SE-91
.29n3r C1
. 282 0 E-01
.2609E-01
. 2 673 E-O i 3716E-01
.2936r.01
.3316r-01
.1t60E-Ci
. 310
- E-81 i
i 4
.461?r-pi
.3961r-01 4151E-fi 3962E-01
.3939E-01 5
. 58 7 2 r- 01
.5 323 F- 01
.5kO*E-01
.M31kr-C1
.5365E-01 A
.7394r-01 711?E-01 7c11F-01 70 3 5E- 01 7
.eki'e-P1 977kE-01 3771E-01 9662F-01
. 8631E- 01 9
. t a A* r* Pa
.1016E+00
.in64E+00 9930E-01
.986kE-01 9
.112te+0e
.1070E+00
.1066F+00
.1098E+0B
.1C S 2 E+ 0 0 1
fg 10
.10*iE+09
.1059F+P0
.1552E+00
.iP49E*CO
.iG47E*05 t
f0 11 061 nr- 01 47 21E- 01
.9501E-01
.9693F-01
.9735E-Oi i
n 12
.'32*E-P1 9 2 55 E- 01
.6046E-01 8221r-Di
.6431E-Oi 13
.la8kg.gt
.gspig.01
. 615 7 E-01
.6457E-01
. 6 775 E-O i l
l-]o ik
.255aE-01
.k7 06 E- 01 4422E-01 47?OE-01
. 5 016E-41 s.
15
.1692E-ri 3192r-fi
.3CO3E-01
.3222r-fi
. 3363E-81 16
.116 9 r- 0 1
.2046E-Ci
. 2019 E-Oi
.2115E-C1
.1948 E- 01 17
.17k 2E- 01
.1362r-Ci
.140kE-OL
.1456E-ci
. iC 27E-81 19
.1279r-01
.1002E-01
.1032F-01
.iD70E-Ci 7 513E- 02 14
.91kkE-07
.6k 20 F-D 2
.660tE-02
.6453r-12 4753E- 02 20
. ?i' Or-P 2
.1897 E-S 2
. iB97 E-0 2
.1995E-02
.iiC0F-32 PWAwMet nopatro CreertrTrqvs
.6ktsr-c4
.k152E-04
.1022 E-0 3
.ii28F-c3
.15 C 7E- 03 I
1 l
E $
i
)
l Table QCS760.10-2 (continued)
LCral 09D t ro ucTGH71HG cAC7qo aND CHANNEL DOPPLER C0FFFICIE47? AT 9001 (T DM/DT)
CHANNFL Avf 4L N00E 71 22 23 24 25 i
. Aa9 9F-P E 7692E-n2
.6262F-02
.6704F *2
.5 917E- 0 2 2
. ?" 9 a"- p i
.?676F-01
.2616E-01
.2829F-01
. 25C8 E- 01 3
.Sohit-01 311??-01
.3P67E-01
.3315F-ri
. 29 43E- 01 k
.3810E-01 194 3E-c i
. 304 9 E-01 6158E-01
. 38 67 E- 01 9
. ci ? 9E-n 3 536a E- 01
.*?10E-01
.ek15r-01
.5328E-01 6
67a'F ni 7n37E-01 7016E-G1 7115r fi
. 7 0 93 E- 01 7
4390E-pi
.m611F-01
.P665E-01
.877me-Di
. 877 8E- 01 I
8 9697e-01
.9 8 6s e.01
.*o32E-01
.100kF+t0
.1006E*0C 9
.103ke*OP
.10 52 E+ 0 0
'.ic58F+00
.1056E+00
.107CE*00 x3 10
.10'kF+00
.iO47r+GO
.1948E*03
.1052F+C0
.1159E*0r O
11 066Sr.c3
.o736r ni
.ggggr.01
.9597F-01
. 971 *E- 01 5
12
.*621r-01
.3610E-01
.8217F-01
.PC41F-01 8 25 C E- 01 f3 it 6P 2 8e- 01
. 6773 F-01
. 665 2F-01
.6151F-fi
.6457E-01 ik
.5121E-01 501kE-01
.k715E-01 4417F-ti 4'rJ1E-01 j3 it 3ek 1r.n t
.33sar.01
.3217F-01
. 2 99 8E-91
. 3187 E- 01 16
.23ngr ni
.1945 T- 01
. 2110 E-01
.201kE-fi
. 20 62 E- 01 i
17
.1?ki!-01
.10 2kE-01
.1451 E-01
.160Cr.D1
.13 58 E- 01 i
1A
.1137E-ni 7490 E-0 2
.1067E-01
.iO20E-01
.9996E-02 19 7226E-02 47370-02
.6P10E-02
.6582F-92
. 64: 4 E-6 2 2*
.20?aE-02
.te00E-n2
.1990E-02
.1895E-02
.18 88 E- 0 2 r.H augrt neoptro C nFreTCTrN'9
.121"e-03
.1510 E- 0 3
.1116 E-0 3
.1*31E-t3
. 418 9E-O k i
cT 8 i
l i
i 1
1
Table QCS760.10-2 (continued,)
treat nnootee wetr,H77pr, raCTOo AND CHAMMEL 00PPLER COErFICIENTS AT 9001 (T 04/0T1 CHAMMEL l
Aytal WO9E 26 27 28 29 30 i
417 4 r- 0 2
.5930E-P2 4991F-02
.k998r-C2
. 5C 42E- 0 2
{
7
.220cF n1
.2254F-01
.2212E-Oi
.2233F-fi
. 2 25 7 E-O i
?
.?690F-01
.2650r.01
. 2 62 4 E-01
.2625F-Ci
. 2 E5 3 E- 01 4
.3621E-ci
.3c8kE-01 3585F-01
. 3624 E- 01 5
.5144E ai 5081E-01
. 502 9 E- 01
.5029r-Di
. 5 6 8 4E- 01 6
.6sger-01
.64100-01
.6741E-Si
.67k2F-ri
. 6812 E- 01 7
.9k68e-Di 8?89E-01
.A390E-01
.8471E-Oi 1
9
.9859E-Ci 475pr-01 4'79E-01 467qr.ni
.9759E-01 o
.105 4F' P a
. ink 6E*c0
.1C39E+00
.10398+PO
.1046 E6 00 to
.1059E+09
.iO4FE6CC
.ir42E+0C
.ir42F+CD
.1;46E*O0 Q
11 4759E-?1 4765E-01 977 0 E-01
.9770E-01
. 9 764 E-81 f3 N
12 94k?E-01
.*505r-01
.855kE-01 8553r.01
.6732E-01
.6Pnee-01 6971E-01
.6970F-Ci
.6885E-01
(__.
14
.5049e-01
.5169e-01
.5262E-01
.5261F-ri
. 516 6E-O i
=
?
15 1478r-Di
.35m6e-fi
.3669E-Oi
.3667r-ti
.3563E-Oi 16
.2?S6e-01
.? 3 35 E-01
.2396F-01
.2395E-01
. 2332 E- 01 17
.199 4E-91
.tS69F-01
.1610 E-01
.1610r-91
. iS 66E- 01 18
.110 9e-01
.1155E-01
.1196E-01
.1185E-01
.1154E-Oi 10 7100r-D2 7417 F-D 2 7611E-02
.76*7F-r2 74 C 6E- 0 2 l
?"
.?iSTE-C2
.2263F-02
.2138E-02
.2306E-D2
. 225 6E- 02 CHatswrt enoptep c.ce rrT C T ENT C
.72itE-ch
.8002E-04
.8372E-Ok
.83P6r-04
.8040E-Sk t
cr 8" 3
1
Table QCS760.10-2 (continued) 1 LCCAL 00*ptr9 w"Tr,wetpc racreo AND CH A NNFL DOPPLER COErrICIENTS AT 80Ci t' DK/DT)
CHANNEL i
AVTat M0mE 31 32 31 34 35 1
. 513 7e-12
.3966F-02
.2a56E-02
.2977E-C2
. 30 23 E- 02 2
.??A9E-01
.1143F-01
.in75F-01
.1093r-01
.1127 E-81 3
. 27 51r- 01
.1324E-Oi
.1254F-Oi
.1274E-01
.1315E-81 4
16M"E-01
.3117E-01
. 3237 r.3256F-01
. 33 8 0E- 01 9
. 514
- E-91 4957E-01
. 5C 5 4 E-01
.50'Or-fi
. 5 233 F-01 6
. 6
- 0 0E-r i
.6990E-Gi
.6954E-01
.6966F-C1 715 8E- 01 7
..957?e-Di
.A689F-01
. 87 2 0 E-01
.972nr-01 8933 E- 01 9
9461E-01
.1009E+00
.iGiiE*00
.1011E*00
.iG30E*00 9
.10thE*00
.1090r+00
.1091E+00
.iO91F+00
.11C5E*00 10
.10c 1E+ 0 e
.1102E+00
.1102F+00
.11"2E+r5
. iiO 8 E6 00 11
.979,r-01
.1044E*00
.1043E+00
.iO43F+00
.1038E*00 n
12 9k 3 0e-D i 4253E-01
.9234E-01
.9237F-01 9 071E- 01 4
g3 1
d 13 677 9E- 01 7629E-01 7611F-01 7619E-01 7365 E-01
' ~ ~ ~
14
.5044E ai
.5779E-01
.5780E-01 5773F-01
. 5514 E- 01 15 1475E-91
.3945E-01
.3073F-Ci
.3959E-ti
.3747E-01 l
?
16
.. 2 2 C 3"- 01
.?3 23r-01
.2372F-01
.2347E-Ci
. 2222 E-81 a
17
.tC01F-01
.9148E-02
.8273E-02 8033F-02 7698 E-0 2 in
.tiP6F-01
.6711F-02 611kE-02 9931F-c2
. 56 81E- 02 10 7095F-07 4275F-02
.3955E-02
.3824E-r2
. 3 664 E-9 2 2r
.?i40E-02
.1136E-D2
.134 7 E-0 2
.1270E-02
.ii98E-82 n
l euaggFL DODOLEp CCrrrecTgg7e
.7262F-04
.2397F-04
.1045F-03
..1092F-C3
.1268 E- 0 3 l
l 4
47 8" l
e i
)
l Table QCS760.10-2 (continued)
LCCal nonet ro wc TGM TT Wr. r ac700 AND CHANNEL DOoPLEP COEFFICIEN75 AT BOC1 (7 04/07)
CHAMNEL t
~
i AVTAL N00F 36 37 38 34 40 l
1 10 Fir-0 7
. 3 RS 6E-0 2
.509hE-C2
.3977F-52
. 4 2 41E- 0 2 2
.1191r- 01
.128ke-Ci
.1563E-01
.1293E-31
. ilki E- 01 l
3
. ils ke-n g
.tkgqE-01
.ta05E-01
.ist:E-01
. iS 51E- 01 4-1h14e-01
.356SE-Gi 4128E-01 3673F-ti
. 363 5 E- 01 5
.5?iLF-Pi
.E346E-01
.6252E-01 56tgr-01
. 547 9 E- 01 6
7 0 0 0r- 0 1 7203r-ti
.P442E-01 7624E-01 7383 E- 01 i
?
.
- ar ir-n i
.Re26E-01
.1042F*00 9k52F-01
. 9130 E-G i
)
P
.1021E*0P
.10 2 6r+ 0 0
.119 8 F + 0 0
.1092E+00
.1046F600 o
.inq'F*0r
.1101F600
.1253E+00
.1150F+r0
.11169 00 l
f3 19
.110'e+30
.1196F600
.1219F+0c
.1136r+00'
.iii2E*00 23 11 1017e+00
.10?9E*00
.1077F400
.iO40E*f0
.1035E*00 g
12 011?E-01 9110 r-01
.8232E-01
.M729E-01
. 89 63 E- 01 i
17 7kk it- 01 7445E-01 4619F-01
.6679E-01
. 7195 E- 01 I
o ik 954Ar-31
.E56MF-01
.2951E-01
.k761E-ti
. 5 301E- 01 i
i 15
.1816P-D 1
.3704F-Di
.1853F-fi
.3110F-01
. 34 90E- 01 16
. ? ? 6 Ar- 01
.2n26E-01
.ir36F-01
.176?F-01
.18 9 B E- 01 i'
770 9r-0 2
.916AF-D2
.3378F-02
.5655E-r2 4879E- 0 2 18
. G 6 ? ir-P P 3792F-02
.2k89E-02 4159F-02
. 357 0 E- 0 2 1
to
.164 t r-n ?
.2 415 F- 0 2
.iS99E-02
.26620-c2
. 2 261E- 0 2 Fr
.111tr-92
.6417F-93
.k956F-03 7742F-03
. 5 361E- 0 3 I
PWAMMFL n0potrP CorreyrveNTC i
.?669r-07
. ? 9 23 E- 0 3
.iS67F-03
.31a6E-03
,.14 91 E- 0 3 l
l i
I.
ME.
5.
W*
10 0
Table Qts 760.10-2 (continued)
L0eAL 00pptED Nrinpy5ng cACT00 AND CH AN#FL DO PPLER COEFFICIENTS AT BOCi (T DK/DTl CHANNEL t
AYTAL Mn0r 41 42 43 44 45 6
1 439aF-PP 4231E-8 2
.5362E-02 3731F-02 30 92E- 02 i
2
.136 ke- 01
.i?45F-01
.iS99E-01
.1371F-C1
.1266E- 01 l
3
.ievar-Oi
.iS56 F-01
.1844E-01
.iM98E-Ci
. 1658 E- 01 e
b 1661r-F i
.?715 F-01 4172E-01
.3778E-91
. 355 3E- 01 l
5 5k9ar-Di 6667r-gi 6286E-01
.5606F-01
.5 333E- 01 6
739AE 91 7655F-Oi
.ek6GF-01 75b7F-01
. 7 231E- 01 I
7
.9116r-01 4464E-01
.ich2E+00
.93kkF-01
.90 tit-01 l
9
.ichar+nf
.3082F+00
.118 6 E+ 0 0
.ip7CE+tg
.103AE*03 i
9
.1116r+0C
.1149E+00
.1251E+00
.ti38r+g3
.1108E*00 it
.. it i ?E+ n 0
.1136F+00
.1217 E+ t c
.1125F*P0
. iir 6E* 00 11
.103kE+09
.1039F+00
.107 5 F+ 0 C
.iC31F+00
.iO29E*00 i
g 12 4961r-61
. 8 7 29E- 01
. P22 6 E-01
.A694E-01
.8926E-Oi j
l m
13 7192E-01
.6678F-01 4F43E-01
.67n9E-01 7182 E-01 4
in 9291r-01
.47 66 E- 01
.284*F-Oi 4819E-Pi
. 5336 E- 01 L
15
.3471E-pi
.306*E-01
.i?34E-01
.31RSE-fi
.3620E-01 d
16
..1967'-01
.1692F-01
.iOOiE-81
.iA65E-01
. 2182E- 01 I
17 4592'-02 5096r-02
. 3117 F-0 2
.6316E-C2 7 793 E= 82 18 1390F-02
.3735F-02
.2?89E-02 4639F-32
.5736E-02 19
.?ikgr-gp
.g37sE-n2
.1462F-02
.2963E-t2 3679E-02 2P 47k'e-0 3
.60 61E-8 3
.htSME-e3
.82 6F-03
. iiO 2E- 02 rMaNwel rnooteo cecerictrNTe I
.1522E- 0 3
.?iS8'-P3
.1603E-t3
.3774F-c3
. 3255E- 03 i
C ct 8 W
Table QCS760.10-2 (continued)
S AND CH ANNE L 00pPLE# COEFFICIENTS AT 90C1 (T OK/DTI Locat 0000 Leo wetGHTTwG raCTO CHA44EL RYTAL N06F 46 47 I
1 11pir-97
.3764F-02 2
.174'r-01
.1377E-0*
3
. tk 6 "r- 01
.160%F-01 h
.3787E-01 5
5337E-01 4 6 ISE-c i i
A 723 kE- 01 7554r-01 7
900 3E-01
.9349r-Di 8
.1036E+00
.1070r+00 9
.110Br+00
.113g r p 0 10
. tin'E*00
.1125E+00 j@
11
.1029'+00
.1031E+00
%)
12
.992ke-pi 9690E-Pi g
13 71*Sr-01 67 06 r-c i L
14 9331E- 01 4612E-Gi o
ir 5617E-01
. 317 m E-01 1
16
. ti7 9r- 01
.1858E-Ci 17
.7770?-D2
.627 2F-0 2 in
. 572 ce-0 2 4 6 06E-0 2 19
.1671r-02
. 29 40 F- 0 2 20
.iO9FE-02
.9096E-03 CH ANNFL 00**LFP CerrrTCTrNT9
.326ae-r3
.3sO2r-as I
WW ct 8 u) l
l 1'0CD011i1ii1iC0C0001 00000000000008000000
- + + + +**+* + +* + * * + *+* -
EEEE EEEEEFEEEEEE EEEE 598474792676669278387 43928212443774846276 03536084774815891348 12361112222114163211
)
i0gO1iii11ii1100e011 S
C0tC0c0C00cG000Cc000
- + + + *+++++++*+++++ - -
E?rEEFFEEFEEEEEEEFEE 0
427m58S3773?909405423 1
84139k39514526393417 00593329228134319461 Y
?1151233kk3121721192 G
K
. /
W tE 3
D 1O0010iii1ii0OC0O001
-0
(
0OC0000CO0t00O00O000 L
- + + + - + + ++ + + + * + + + ++ + -
1 1
E FEFEFErEEEErEEEFEEfE 0
C N
36735504777231F891985 6
. 0 N
7591809A698639370373 7
. 9 A
958 61 62?008419713190 S
H 1236261i221193284312 C
T C
Q A
e N
l b
O a
T T
T u
1008i0i1ii1i0g06000i q
0030O00000000300000C i
- + * +
- ++++++*++6
+++ -
. o EEEFEErEEErrEgEFEEEE T
230000473299g2s18052R S
4925983 2O3132g92666i I
24801027O0340O53345n O
1237761122119327321i H
T OW 1tP 01C11i1i1in0erC01 T
00R000060000n010r000 P
- + + + - + + ++ + + * * + + + +++ -
V EEFeFrFEEET?eFceeerE i1o10P3?P31 O k B 9 i711 q k M
9k6686?336k024S62692 U
1k7644h922O609?9234R 12 3 5 1 '. t.12 2. ?.1 11 ?. 6 1 21. i T
O F
E 0
0 N 1234567*90123k5679o0 L
11*
. i 1111t2 A
T Y
A a R g
,_a'
- Fa" $
]
rt Ec _
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.li!i!
jjlj4 j
il i
i,
i Table QCS760.10-3 (continued) contUw Vef n unoTu nTo79T AU'T ON ' A7 03Ci (DELK/KG X 10**5) i CHANNEL AWTAL NOne 6
7 8
9 10 1
.1274E-91
. 97 77 F-4 2
.2P03E-61
.4472F-ti
. 3719e- 01 2
.?8'kr*0"
.?i16E*00
.1310E*00
.E617r+00
.478kE600
?
..k356F+0r
.125cr+00
.188SE+00
.8495r+00
.7264E*OO j
4
.'041r+0n
.9469E+00
.6339E*Cn
.1599r+0i
.1402r*01 5
. 644 9E-C P
.1604E+00
.1417E*01
. 6 485 r,+c e
.,67 8, E 0 0 6
.9602F+ae 9741E*00
.2341E+Ci
.4P73r+ft
.5 382F* 0 r 7
..16k"E+01
.1736E*Di
.32ikF+0i
.1308E+0i
.1489E+01 8
.2246E+ni
.2318E+01
. 387 8 E* 01
.2155E+Ci
.221E!*01 o
.*S'6E+01
.2634E*01 4?25 E+ 0i
.2549e+0i
.2599E*01 in
.250'e+rt
.261*E+0i 4199e*01
.2516E+ci
.2583E*01 11
.'306r*01
,7337E+0i
.3A09E+01
.20k3F+0i
.2181E*01 1
12
.177ke+01
.1792E+0i
.3117E+0i
.1095E+t1
.1487E*01 f3 13
.in9?E*D1
.1108F+Ci
.2269E+0i
.2868E+CO
.6633E+0c ik 165mE+0F
.3997e+00
.1413E+01
.7992E+00
.13t 6E* 0 C i~~~ ~
15
.112gr+ct-
.2439E+0F
.6739F+0D
.1072E+Ci
.8C49F600 in
.97t?E+0F
.621kE+00
.iO12E*00
.1278E+01
.1400E*01 j) 17
.kO40E+00
.4356E+00
.3549E+00
.4904F+00
. 6 49h E+ 0 0 m
iP
.?o9?r*Of
.3181r+t0
.2614E+0D
.3589E+C0
.4761E*00 in
.imoSe+0e
.2006e+00
.1679F+0n
.2273E+C0
.2987E*0:
2n
.$197F-01
.2112E-Oi
. 2k97 E-01
.2637F-ci
. 3 08 4 E-Oi l
1 t
+
EF cr 8"
,l:'
l!ll!ii
!I
~
11i1i1i11116CiiiC0Ci 0000000000000000000O
- *+ +++++* + -
- + +* + - +++E EeFEEEEEEE EEEEEEEEE 57597 6629869334374i99 166993435856q76799k88 1531 1ii9338361468015 81221ki.1221g51116533 i01ii1iiiiig01i1000i
)
t0C000CCCtCe000Cr00f 5
- + ++ + - + + + + + e+++++++
r E r r Er E EEr Er r EE E Er EF 0
4k3i7 e2O9693186120514 1
141P7t5?363913S68 2k ? 7 0811i81933436ik668n5 7 712 i 3112 210 9 i i 16 k.1. 3 Y
G.
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00n00C0C000000000000
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- + + + +++ + + + * ++++++++-
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- C N
1O 18833732k3817001591 1M9297041980191653954
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1 7345e91k4175 3S78915 R
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7 7
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(
T 2751A90933909362' 9741 S
1 1979173* 0692 3 88906?1 t
894' 3342693179020637 4 5 9. i 6 k. 1 2 2 2 2 1 ?. 7 1 1 5 3 2 2 n
H Too W
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000P 000f0n00000000n0 O
- * *+ + * + * * + * ++***+*+ -
V reEEeErrrrerEEEEFrEC 10769t6o*6190* 9kk0?11 M
124n941n421O132*19t 16 U
' 72165g265 ?5820458n1
- 1. k. 7 1 k.5. i 2 ? ? ?.1 6 1 9 1 6 4 1 3 no S
r 0
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100130ii11110011006i 0000000000000080000O
- * * * **+ +*+*+++**+*+ -
EEEEEEEEEEEEEEEEEEEE o16203463113551229646 t03985498097463187034 0 9966542762S53t60971 55816412222i62i18534 i011iD01i11000ii000i
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5 C0000G00000000P00C0t
- + + + ++* +++ +++ + + + + +* -
FEEFEEEEEErEEEFEEEFF 0
992224679204O77270366 1
122*39769609k01271237 19O0i422663762043695 Y
56i2i261111A26116423 G
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860093191e2i953216934 0
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0 9
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H 6P12211P667911116433 7
T C.
S) 4 Cd Qe N
u O
en T
li 7
bt 0121i11i1iiii1i1000i a n U
To B
0r000r00C00CnCC0000O c
I
+ + + * ++* ++ + +++++*++* -
R FrFEFEFEEeFEFEEEFEEF
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T 76e02474459656362715i S
14088292902 57092 9 592S T
31069022320740P649Sm 571223.'.3333222.i.193.?.2 O
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1 jl:i' ii
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+ * +
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581116216371614362668 298915363469C3041C247 31079123320A41865058 57122333333222115422 i01i1iiOO00B1ii10e0i
)
5 C0Ot0O0eC000C0000c0O
- 4+ * + ++ ++* ++ *++++++ -
EEEFErTEEEEEEEEEEFEE 49227929S?SS1087699S0 0
1 2806187845PB7903081k3 132727210kk203S7580k X
681?2110667911i16k33 G
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0 1
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0 N
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=
A 190t 2512663633n43606 H
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c I
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2646159354k5k833S1352 S
2739420091085201A 0247 T
99966542772" 63061971
- h. *. 8 16 4 1. ?. 2 2 216 21 1 8 5 3 4 O
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1f?11ic1111i!ci1Crri 0O000C00000P 00000fSO
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5 OC00Cr0O00tt0CF00PCO
- +* + ++* *+ + +++*+++++ -
EEEFEEFEEFEeEEEEEEEE 96180634523696369O502 0
2k3c574i39P9k2660i129 1
- 06753i32168i23424k8 357111i98889i1115322 X
G M
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FFEEEEEEEFEEEEEEFEEF 1
1 0
0 N
62269524R796772573O67 6
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l u
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7 753647375O15c3646S686 2 075132082 q
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l Table QCS760.10-3 (continued) j l
ConTUS VnTr wosTu 015T0190'I04 A7 *001 (DELW/WG Y 13'*51 l
CHAMMEL AXTAL N0nF 31 32 33 34 35 1
.4 0 67 r- 01
.12k2E-01
.1039E-01
.10iSE-01
. i S3 k E- 01 2
.5761r+po
.o606r.gi
.igsgr.01
.1230E-ni 4072E- 01 1
.6771?+99
.1431E+00
.i'41E-01
.13*0F-Ci
. 5499E- 01 4
.2759e+Pi
.km94E+00
.157aE+00
.ikS2F+C0
.3414E+02 l
5
.?552E+nt 48R4E*30
.6209E*00
.6038E+C0
.ic20E+01 6
.2A03E+0i
.iS44F+0i
.1190E+01
.1169r+0i
.182SE*01 7
.100AT+91
.?iS1T+0i
.i?34E+0i
.1710E+0i
.258?E+0i 4
M
.3142E+0i
.?64'E*01
.2163F*01
.2136F+01
.3163E*01 j
9
. 314 5E + 0 i
.2910 F + 0 i
. 2413 E+ 0 i
.?386F*P1
.3484r+0i ia
.3147F*01
.29c4F*01
.2455e+0i
.24?8E+fi
.3502E*01 11
.2006E*01
.27728*01
.2299E+0i
.2264r+ci
.3224E*01 p?
12
.P79'T*01
.2396E+0i
.1943 E+ 0i
.io20F+11
.27C2E+01 Z]
13
.?443F+01
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.1469E+01
.1450E+C1
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14
.?i2iE+ai
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.9385F+co 4231E+r3
.1292E*01 P
19
. iR16e+ P i 7514E*D0
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1F
.1531T+n1 1287E+00
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i 0
17
.9073E*00 5963E-01
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. 29 0 2 E- 01 18
~.3711E+00 4 R 01 E-91
.1815E-Oi
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. 2 05 8 E- 01 ia
. 2 3 4 *E + 0 *
.?819E-01
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.i?14E-01 l
20
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.?is1E-ni
.147 5 E-0 2
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. 7 492E- 0 3 l
l EF cre m."
4
i I,*
1220i111i11111C~ 0C12
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00000000000000000000
- - - * +** *+ * *** * + ** + - -
EEE EFEEEEEEEEEEEEEEE 0 A 9 9113 5 0 2 8 A 6 7 6 4 9114 2 411468197326217432005 1530O0850959121C5188 1223i223333221511163 1
i1i0i11i11ii1i01i113 5
C0r0C00CCCCc0000c000
+
- - - + +++ +* + + + * ++ - - - - -
FEEEEFEFeEEEErEFEFEE 0
990432964k29k1i347925 1
3321R 6863867i2i177784 9549999?884A02136042 X
13421123333221925424 G
K
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1 L
- - - + ** + +* + + + * ++4 1
E EEEEFEEEEEEEEFEFFEEE 0
0 N
87827962837225159580k 6
0 N
339435962871648226924 7
S 9
A 953A9763663591726139 C
H 524i8123333211511171 Q) 7 C
... ~.................
d 4
e e l u N
b n O
ai T
Tt n T
o U
12300i11i1i1i1O10012 c
B 00000D 0CD00300P0000F
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T
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O ErEEEFFErEFEFrEEFEFE T
77k752737A7615?085289 9
3A11 92325984P60493285 1
2250192700A370525107 146281?2.'.3.?.211471177 0
H T
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FrrEEEcrErrrr'ErFrEc 67i1o*2?o224?* 5AF3?a i M
36' 6?41* R01 9"
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3A2S46382299A1062229
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FEEEEEEEEEEEEF EEEEEE 574181758491846671921 471107094558932830269 8428587599580i061551 4129712333322i322198 200ii1i11i11110B0Oi2
)
_ 5 tnCCC0f0t000G0000CC0
- ++ - + * + + + + *+++++ ++ - -
F EEEFEEFFEEEEEEEEFEE
_. 0 444420257967772478622
_ 1 425510608k23862615047 21820242772333" 30435 91121234444321k.22107
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FEEEEEEEEEEEEEEErEEE 1
C N
3200O744i361990213603 0
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H t67281233332115i2111 S
T C
C
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l n
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o r00900000000D09 cn00C c
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V rrrEFErrrerFrrEEEEFr 1 e 9 318 4 a a 2 9 6 9 k ? 0 *
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T o r r T r r EE r F r EEE EF r Er E F c
I
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O 70027y773742839916892 2
T 3 77818 46S59g52175609 S
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. O H
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o EEeereEeErrEFErErFee E?5kl n7q s? aP?3?kk490m V
1i a ? 1 a 6 7 ' aik?1k1712 M
k0342668450950Ot161563 U
61.?.071213112.?i32?.198 T
n e
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A T
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O i;;II i!i ll lli; 2
i
Table QCS760.10-4 l
.tTret Wno'M OTSTRI4UTION A7 9nCi (DELK/MG X13**5)
CHA4NEL Ayfal NOne 1
2 3
4 C
i
.1119E-91
.13 60 F- 01
.180kE-01
.1947E Ri eiS34E-01 2
..1195E*ne
.1163E+00
.1175E+DO
.85k6r-Oi
.1206E*00
?
.17'ne+fP
.1740E+00
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.1226E+C0
.180GE*00 k
.130ke+0*
.1934E*PO
. ii71 F* 0 0
. 2 ". 2 3 E
- 0 0
.12 22 F+ 0 0 5
.2k'1E+0D
.2122E*00
.2975F+00
.55kkF+C0
.3202E*00 6
.6971E*0"
.6007e*00
.6?13E+00
.45SiE+r0
. 7 P56 E* 0 0 7
.10'2F*01
.9566E+00
.itiBE+0i
.1326F+0i
.1210E*01
.11? 9 E* 01
.12 22E* 01
.1390E*01
.16PSE+fi
.1531E*01 I
9
..ik*3F*01
.1189F+0i
.1451E+01
.1751E+C1
.1706E*01 10
.1531r+gi
. 1410E*01
.ik78E+0i
.1719F+01
.1707E+01
'S 11
..it7&c+C1
.1245E+fi
.135 3 E+ 01
.1574E+Ci
.1538E*01 O
i?
.1131r+0i
.1065F+0i
.1116 E + 0 i
.12PSE+Ci
.1234E*01 13
..R0kar+ce
. 7557F600
.785kF+0p
.0315E*fD
.8511T+0L 14
.446*E+0*
.411?E*00 k ?S 3 F+ 0 0
.5789F+00
.4529E*00
?
15
.o78kE-n1
.7519e-01
.7361E-01
.27kkE*C0
.8932Ee01
's 15
.io61e*n0
.2141?*00
.2622E+09
.522SE-Ci
. 2 P 9 5E* 0 P I
17
.13'Se+03
.1399E*00
.185 8 E+ 00
.ir56F+0C
.1375E*03 l
19 9909e *1
.19 36E* r0
.1366F+Co
.an59E-Ci
. i O 2 0 E* 0 0 19
.Ak%3r-01
.671PE-Ci
.8719E-01
.5kS6F-01
. 66 47 E- 01 20
.118'E-91
.ii62F-01
.1225E-01
.1480r-ri
.122 0 Fe 01 i
E"E i
cr a" l
'l, I
10CCC011i1i190100001 00000000000000000000
- * * + ** * *+++*+* - * + +
- EEEEeEEEEEEEEEEEEEEE-e762717835C626M7k0374 i947508035k9798674186 1112444BC07355177027 3233281i221183842211 i G 0 3 0 0 1 1 i i 1 i 0 O O 0 0 0'0 i f0 crc 090[rrC0GG0r0ct
- + + + ++
- ++ +++++++++-
EEErFFgEEEEFFEEEEErE 9629k77379Si24464542k
)
S 651541680Ak1701937 15 7666r548107i67F0150S 32332911221i1 134211i 0
1 W
G M
/
M 11100iii1i1i00020011 L
000000c0000000000000 E
L
- - - + *++ + + + + + +++ - + + - -
4 D
E EEEEFFrEEEEEFEEEEEEE
(
N 8E55544g8R52S6909554O 0
N 502090n7?1432922714i 1
1 A
19649 0 368863686S735*
0 C
H 260251111111052i11n1 6
0 C
7 9
S
)
C d T
Q e A
u e n N
l i
b t O
100100ti11ii001e00i1 a n i
090000c009P c100p00r0 T o t
- + + -
+*e+++6
+ + + - + * + - -
c EEEFEErEEFFrEEErerrE u
(
n 75110 0P0q14730cFC84kS i
37940 ? 2s11467179 32nE o
6054?02c7752551794i2 111738111111947211.q1 7
e T
q M
'oP 1r0A0?ii1iiiP 6 tn00i1 W
0900nnP p0" 0nr0Oa09n0
- + + + ++*++*+++* - e*+
L EFrEEEEreEEeEErrrFEE s7 kn7 2" ig0 9c'59 Ai e912 e"
95?802? F2 kP
- 1 14o1702 T
63050*2577520 72g7223 11S13'.1111119.k.7.o 1 1 3 1 C
rnO N i2* 6 567P9e127k5s7m0r L
t111i1i1i12 A
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A 3O$* _ ?@
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10C?0011111i00000" 01 00000000000000000000
- ++ **+* * * * *+* * * * * *6 EEFEEEEEFEEE EEEEEE0E 5 4330C138P 39979734672 129085744059?95646303 0375265f328282537( 39 56951812221112462211 1000g0ii11i1S0000001 0000c0t0C0C00f000C00
- ++ ++++ + + ++*+ ++ + + ++ -
EEFrrEEEEEEEEEEEEEEE 489307878822883628648
)
5 10054162273627 h28P985 62752590228282527929 43k51912221112462111 O
- i
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.- G
- K
/
K 1000101ii1i110000001 4
L 00000000" 00000000000 0
E L
- ++ +
+*++++* - ++ * + * + -
D E
EFEEEEEEEFEEEFEEEEEE 1
(
N 37A331046700619379752 N
155740740309117593191 0
6 1
A 95272227a9903' 847329 C
H 63565611i11182462211 7S 0
C CQ 4
)
d T
e e l
u A
b n
N a i T
t O
1000001ii1ii00000001 n
0900000000000Q000n00 T
oc T
- +* * ++*++++++*+**+* -
(
U FEEErEEFEEEFEEEEEEEE 9
2369704194S11809607k2 I
154 09 33714 O 7 35954903 A
. R 746727491i7i7650 1605 23328112.?.1.i.11352111 T
1
. S T
D
- H
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. e 10np C01iiii191160cri w
00000000000000000pcp
- * ++ * -
- +++++++++ErErcE
- + * +
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.- t T r E E E E r E E '9 k 7 9 9 1 e t 4 S '
e 1'
a74S639 1 r
1 k ? 4 t R 0 ? 9 7 519 C 4 3 h 9 4 " A 1i1?46&9008376?R7037 t
32132811221193942.?11 S
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0 N i214M6789n123k467R40 L
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- 6 ** * * **+***+ * *6 EE FEEEEEEEEEFEEFEEEE 0'
11432M6377546114833 22E9949C7216273181366 757018592295719536S2 323428112211941532i2 i0001011i1i1000I0001 CC0000C0000C00C C0000
- ++ + - + + + +* +++ + ++ +++ -
EEEEFEEEFEEEEErFEEEE 943959i678i75i9195319 1
- 5 1238962O13k3726762964 493746i5775i37364719 324535i1111i72142111 O
i X
- G K
- /
- E 10000100000000000001 4
- L 00000000002000000000
-0 E
L
- +++ * - 4 * + * +* + +++ ++ + -
1
- D E
EFFEEEFEEEEEFEEEEFEE
(
M 82524799S838132660868 0
M 191275132852354538275 6
1 A
74147721676151664818 7
0 H
335e45367764113* 2111 S
C 0
C O) 9 d
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u A
l bni N
at Tn 0
i0O00000000000O000i1 o
t C0" 0000000000rC090D0 c
7
- +* + ** + + + 6 ++ + +++ ++ - -
U FrEtFErrFFEt{EEEFFEE
(
B 757 rot 1 P345M27435D1025 I
10361689273430675 0 5 60 R
2053R026198754561595 T
13498376655555552101 S
T n
4 Tro i* " 01n1iiii11P0F" 001 W
P08 0000P0n0?0P00e000
- + * * - *
- 6 + * +* - * * + *+
- t ErrEFEEcEErrEEEerFEr r
A*
4" ?1* '?E7 Mh9747cK ' t e
1611P1452C 10?0 0o5' i9n T
6869 11 27996028R57O?o 4 12 6 5 6 1 1 1 1 11 9 7. k. 6 2 ? i. t 9
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+*6 6*+
- +
- EEEEEEEEEE 599222294998633991248 2361168826221722926G1 2064913720 9855661 SOS 33498876665555552iii
... e 1O50t19500000B800S0i 0F00t0000r000D000G0O
+*++
+*+++*+++++++-
EEEEEfEEEEEEEFEFEEEE 410k9R959049890770164 35761133173217900k87
)
5 2 84158C217741Si675P18 3358 4636776 4ii3* 2111 0
1 Y
r, K
/
t 1000101iiiii00000001 4
t 00000030000000000000 E
L
- + *+ - ++ + + + + +* *+++*+ -
0 D
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Table QCS760.10-4 (continued)
_q 57trL Weo'H DTS7pIRUTION AT 9001 (DELK/WG YiO*'51 i
CHANMFL t
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11
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1 Table QCS760.10-4 (continued)
MTErl WO*'H 07STRI90 TION AT 90C1 ( DELM /MG X10 * *5)
CHA4NEL u
AYTAL N00F 66 47
~
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4
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=
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2 2 4 3 7 9 2 2 e 6 9 0 0 i 9 5 819 7 4 9
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+ +** + ++ +* + *+ + + + + +++
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t e e e e e e e e e e e e e e e e e e e e E
t eMMMMNNNNNNNMMMMoon.
u w s. ss o c O s o u u o w c c o u e o a
+ + + + +4 +
+++4
++ ++++++ +
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.-MMwMM-NNewW-MM oc L o c u G O O. C O O o C o c O C G O O O FO F
++++++
- * +*++*******
F w w w w w w w w w u w w w w w w u.
w w u
kW@N@@@@NW@MMoomM@@@@
H JDM@@MbmMMhNNPM@d@.c F
Mtm@MCMODOm46NhamMGN
.} >
- v. e. N. r. r. e. e. W. e M. e. c e. m.M N. a.n. a. e.
, v e
e e
M C
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ccMcWWWMNNWWMeeWMt cp i 3 ococcco...
econocoe.
4 44
+4+4 4 4 + 4 4 4 4 4 4 4 4 4 +
F u w w u w v u w w u w w u w u w u. u w w vs
@s JMF @a @CFrOMOherhF a a Y G O F M N t> M M a t J N t F Jk@mh J
@ h e @ N G O N O D > d M a t m D M V. E w
J M N. M r. 4. K W W W @ t h. r. F. N. W F m. M.
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l i.
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=
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QCS760.10-36 Amend. 69 July 1982
e o
l ssMMMmNNNNNNNNMMMacuc cosommeeSpopecommees
+e44 44 4 444 ee_+eeeeeee l
WWWWWWWW WWWWWWWWWWWW i
l mMModemmMdMNNC@dMMech Mec@dhd@@bmNoN9dNMdhe h @ w @ m d M m & @ us M U M 9 u e d u &
Ed@meWWWWMMMMNdM9hme I
e e e e e e e e e e e e e e e e e e e e i
i r
2 eMMMMNNNNNNNNMMMMemo s o p o e t* G o c o n o c o c o a c c o
++++++++++
+ + + + + + + + + + k' k b k a Bs W W W W k;W hs W k' ktW ki4 W 6 an.m JNo@eMkokk@No@dNOPMew MP>cJMA@N e4 V' F F P= b N so @ m M rs O' o M @ c o e M ui e
GMkedWMm@@mN eo
@NMmeWMweMWMMbdMMkre M
e e e e e e e e e e e e e e o e e e e e O
v i
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oMMMMNNNNNNNNMMMucco W
coaccoccupoooooooooo m
e
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+ + ++++4
+ ++++++++++++
o e -
W WWWWWWhkWWWWWWh.WWWWk i
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kt MU EMMWWWWWHkdN@NUW i
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D e+++++++++++++++++++
i E
W W b k W W W W W W b'b'W W W W k W kt W H
N@@tmedLed&NEkNekNNN4
' E MWPFNem@@dhe@@NF,mkme@
@edW@cNdmmdMM@dk@mcM m
CNYVhedMMM*MO@dNONm*
M e o e e e o e o e e o e o e e e e o e e C
I E
k O
C i 2 uMmeMwNNNNNAMWWWMoco ecconcoccuccccotcccc e
++++4+
+ ++ + ++++++++++
b b e ts b ' b
- W k b b.* be k' W b b k k. k b'k k. W c@= - - e e w k @ u. e e
, J MOuMadrF J
MwdrdhcwttmVE@UNkKNCO l
k JMMNJO NModYemNcNH@@d V F.C. *. @. M M. M @ @ >. V. Y 9. @. w. @.
l D
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QCS760.10 37 Amend. 69 July 1982
?
51111222222221i11100 00000000000O00000000
- 6
+6
+ * * *&6 *+ 6 66 6 +
- 66 EEEFFEEEEEEEEEEEEE EE6732O4i5k8376S77i12 oEti719436k333631B62c57 02237t2kSS42t9563O77 62357.i1iii11i7531i61 tiit1i222222i1i1i0B0 fC0e0P00tCCc"90Cc0t0
+ +++++* + + + + + * +++ + + + +
EErE0FEFEFEEEFFF*EEE 1
935mh8136011672263737 5
100791373211355k39721 3B5915i344311870i7P8 6i2.k79i111119643i861 O
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GM
/
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011iii2222221iii1000 5
E 0000C0f0C00D00000000 D
L 6 +*+++* +
- 6 + + * +++** + +
(
E EEEEFEEEEEEEEEEFEEEE 0
M s66041938068230645240 1
1 M
i79223995421393250559 0
C A
06k926134431* A580625 6
0 H
412679111111e64217* 1 4
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S )d Ce T
Ou A
n ei lt N
bn 0
ao 7
0iii1i22222i11110000 T (c 7
00DD0000P00000000900 U
+ +*++++6*
+ 6 + +
6 * * + + +
P EFEErErEEEEEErEEEFrE 7036712566k26677167e2 Y
R 143P 53k0k101499477033 1390010122i555732333 7
3 114. A. 9 1 11 1. i 9 7 5. ?. 2 8 6 4. i.
9 T
D H
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011112222?222ii11r9p 00000000Pnn9n0n06010
- +*+****a**++++**+
T.
r r e e ' 01 o P 6 h k 117 7e*'r'rEErEEEE'1 e
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Table QCS760.10-6 CRBRP 80C1 i
REGIONWISE REACTIVITY WORTHS SUP9%RY (Net ak/k)
Inner Lower Axial Upper Axial Lower Axial Upper Axial Parameter _
Fuel Blankets Blanket Blanket Extension Extension Doppler
-8.8212-4
-2.0069-3
-1.1273-4
-4.0571-5
-8.2071-5
-2.9981-5 Sodium Void
-1.5370-3
+4.6889-3
-8.5440-4
-5.9318-4
-3.8357-6
-4.7842-5 m
s g
Steel
-1.4996-2
-1.3500-2
+1.9594-3
+1.5392-3
+1.7516-4
+2.2005-4 Pellet
+5.0252-1
-9.9146-2.
+2.7117-2
+1.2035-2
-1.5729-3
-3.1805-4 i
bGB W
i
\\
l Table QCS760.10-7 1
l LOCAL 00*PLER WEIGHT 1NG F ACTOR AND ;HANNI. DO FPLER COEFFICI ENTS AT EOC4 FLOOOED tt OK/07)
CH ANNEL 4XIAL NODE t
2 3
4 5
1
.1792 E-01
.1849I-01
. 2 07 4E-01
.ST46E-32
.1969E- 01 2
.2 815 E-G 1
.28751-01
.3d94E-G1
.15 50E-Ji
. 3J 17E- 01 r
3 4 353 E-31
.4414E-01
. 4 62 4E-G i
.23376-31
. 455 ;E-E1 4
.3 39t E-01
.3440I-01
.3 6 G 7E-31
. 36 60E-51
.3458E-El 5
.4 7*3 E-31
. 47901-01
.4 9 8 4E-01
. 52 2 4 E-Ci
.483sE-01 6
.6 265 E-01
.63061-01
.6 5 0 2E-01
. 6918 E-Gi
. 636 6E- 01 7
.7 665 E-01
. 7724I-01
.7 313E-41
. E 5 : 5 E- 01
. 77 8 5E- 01 8
.t 615 E-01
.e644I-01 8817E-31
.9608E-91
. 8 714E-91
't ff 9
.3253E-G1
.32791-01
.9443E-Gi
.1132E+03
. 93 4 0E- 01
- l 10
.s36sE-31
. 93925-01
.9 54 EE-01
.1042E+0J
. 943 JE- 01
,o 11
.L 9 22 E-01
.e950E-01
.9 C9 tE-Li
. St 74E- 01
. 8 9 5 *E- 01 12
. 011 E-31
.d0391-01
.8163E-01
. 87 53E-Ci
.7995E-C1
?
13
.6 962 E-01 63911-01
.7 0 8 4E-01
.7397E-J1
.6878E- 01 14
.5 41* E-31
.5429E-01
. 5 4 5 EE-C 1
.55 29E-Ji
. 5 281E-C1 15
.J 8 54 E-01
.3837I-31
.3 746E-c i
.3825E-a1
. 3 68 5E-81 16
.2 515 E-31
.2449I-01
. 2147E-01
. 23 E0E-01
. 2318E- 01 17
.3 31T E-01
.3132I-01
.2212E-01
.1487E-31
. 3 0 3 9E-C1 18
.157'+ E-01
.14465-01
.9028E-02
.7048E-02
.14 0 6E-81 19
.7 3 68 E-0 2 63851-02
.3811E-02
. 316 0E-C 2
. 6163E-82 20 4193 E-0 2
.37531-02
. 2179E-0 2
.17 (1E-3 2
. 3484E-8 2 C4ANNEL 30PPLER ; 0iFF ICIE NT3
)
.210e E-0 4
.21071-34
.2 277E-C4
. 6135E-Cg
. 2ii9t- 0 4 l
C' BS
j Table QCS760.10-7 (continued)
LOCAL DOPPLER WEIGHFING F A CT O R AND 3 H AMME. 00FPLER COEFFICIENTS AT EOC4 F CH ANNEL l
I AX1AL NODE i
7 6
9 10 1
.2 065 E-01
.2288I-01
.1152 E-C i
. 22 6 5E- 01 2266E- 01 2
.31Gr E-01 33241-01 17 26E-G1
. 34 64E-Gi 3353E- 01 3
4 65F E-01
. 43501-0 1
. 2 512E-01
. 5143 C-;1 49 2 CE- 01 l
4 3 553 E-01
.3674I.-81
.3864L-01
. 39 25E oi
. 37 22E-61 2
5 4903E-01
.50711-91
.5419E-Ci 52 TOE-31
.SS88E-01 l
6
.6 4 23 E-01 65901-01
.7 535E-Gi
. E518E-01
.6595E-Ci 7
.7 8 25 E-61 79961-01
.8637E-Gi
.8259E-01 7993E-Ei Q
A
.o 715 E-01 6693i-01
.9 699E-C i
.9tC7E 61
.8864E-02 x3 9
.7 3 2f E-01
.95051-31
.1039E+00
.982iE-di
. 945 tE- 01 19
.? 415 E-01
.9586i-01
.1(47E+SD
.5874E-Ci
.952 tE-C1 y
11
.c 943 E-01
.91001-01
.9 9 2 EE-01 9323E-31
.9039E-(1
,o i
?
12
.4 013 E-01
. 6127E-01 8836E-Ci
.6235E 31
. 8 0 71E- 01 j
0 13 6935E-Oi
.6989E-31
.7 449E-C i
.E945E-Gi 6955E-81 14 5335E-41
.53171-01
.5524E-Ci
.4836E-Ji
. 5269E-Gi 15
.3 70L E-01
. 35 751-91
.3695E-01
. 23 T6E-01
. 35 3 3E- 01 i
16
.2271E-01
. 195 61-0 1
. 2 r,3 7E-G i
.13 39E-31
.199 4E-Ci 17
.2 79s E-31 19521-01
. 9 3 3 0E-3 2
.16 8 5E-C i
. 20 6 9E- 01 18
.1213 E-I l 75161-02
. 3 69 3E-0 2
. 7134E-o 2
. 7971E- 0 2 J
19
.510L E-0 2
.33001-02
.1482E-02
.29(2E-02
. 3166E- 0 2 2C
.2 765 E-S E 1550!-02
.710 5E-G 3
.15 35E-02
.165 3E- 02 C4 ANNEL 30PPLER 30iFF ICIE NT3
.2 203 E-0 4
.2287I-84
. 65 8 3E-C4
. 22 CEE-og
. 2 24 0E- 0 4 i
cra?
l
l l
Table QCS760.10-7 l
(continued) l l
l
\\
I LOCAL 00PPLEP WEI GHT ING ACT O S AND 3 H ANNE. CO FPLER COEFFICIENTS AT EOC4 FLOODEO ( T DK/DT)
CHANNEL 4XIAL NO3E il 12 13 14 15 i
.2 311E-01
.2349E-01
.2126E-Ci
. 2177E-21
.22G9E-01 i
2
.3 395 E-01
.3524I-01
.340dE-51
.3430E-G1
. 3459E- 01 l
3 4 965 E-01
.5204I-01
.5 22 4E-Gi
. 5L 18E 61
. 5229E- 01 i
4
.3 745 E-01
.39581-01
. 4 04 EE-01
. 39 65E-G 1
. 4 0 0 iE-91
)
5
.3135 E-01
.5306E-01
.5330E-G1
.5303E-Li
. 5317E-91 i
6
.6614 E-01
. 6337I-01
.6 8 5 2E-01
.6834E-01
. 66 4 3E- 01 l
7
.1034E-31
.3268I-01
. 8275E- 01 f3 i
p 2
.b86TE-31
.92061-01
. 9 23 4E-01
.9211E-J1
. 92 0 3E- 01 i
N 9
.e 45F E-01
.93131-51
.9847E-01
. 95 E 3E-bi
. 9814E-81 O
10
.9525E-3i
. 95 61I - C 1
. 9 b 99 E-s i
.SB76E-01
. 98 64E-81 11
. i O 3' E-G i
. 93 07E -01
. 9 34 3E-01
.S325E-Ci
. 9 313E- 01
?
12
.t 065 E-01
.E219I-31
. 8 246E-G 1
.8238E-01
. 8 22 2E- 01 i
13
.6 947 E-01
.6927I-91
.6325E-01
. 69 41E-Ji
. 692 6E- 01 14
.5 25F E-01
.4816E-01
. 4 75 3E-01 4T59E-Li
. 4 78 5E- 01 15
.3 513 E-01
.23735-G1
.2245E-01
. 2317E-U 1
.2308E-81 16
.1965 E-01
.13101-01
.1306E-01
.13 28E-J1
.1319E-(1 j
17
.2 016 E-01
.16271-01
.170(E-Ci
.1T21E-01 1705E-01 18
.7 635 E-3 2
.67691-02 7288E-02
. 74 29E-J2
. 733 6E- 0 2 19
.2975 E-0 2
.27775-02
.3 09 2E-L 2
.21(3E-32
. 3 0 5 0E- 0 2 i
21 1505 E-0 2
. 139 01-0 2
.17G3E-02
.16 91E-J 2
.164 6E- 02 j
C4 ANNEL 30PPLER 3 0EFFICIINT5
.l
'.19 27E-34
.19 3 0E- 0 4 l
.2 241E-0 4
.2210I-04
.176SE-C4 ET E ct 8 m."
N i
j l
j
Table QCS760.10-7 (continued)
LOCAL 002PLER WEIGHT ItG ' ACTOR AND ; HANNE. 00FPLEE COEFFICIENTS AT EOC4 FLOODEO LT DK/DT)
CHAhNEL AXIAL NODE 15 17 13 19 20 218 0E- 01 2153 E-01
.16571-01
.1774E-Ci
.17 79E-01 j
i 2
343? E-01
.2519I-31
. 29 9 2E- 01
. 29 59E-61 3 281E- 01 4869E-Ci 5 25J E-01
.45231-31
{
3 3722E- 01
.061E-01
.3532I-01
.3733E-01
. 3b 2 8E-61 4
50 5 3E- 01 j
5 5 342 E-9 i 89091-01
.4964E-01 43 00E-Ci 8
6 6 863 E-01
.64431-01
. 6 4 6 2E-01
.t4G1E-G1
. 6545E- 01 t
5 294 E-01 7377E-01
. 7 8 8 2E- 01 7813E-01
. 79 2 7E- 01 7
9 23) E-01
.o7851-01 87 8 )E-01
.6FC6E-G1
.878 DE- 01 8
8 9
9 83) E-01 9*0 21 -D i
.9389E-Gi
. 9315E-si
. 93 6 9E- 01 9865E-01
.9488I-Gi
.9 4 68E-01
.94iOE-Gi
. 944 7E- 01 10 3 323 E-01
. 9J 0 7I-01
. 8 9 7dt- 01 2927E-G1
. 8979E- 01 g) a 11
- 2E E-31
.c048E-01
. 8 0 C 4E-01
.79tGE-J1
.8J53E-01 12 691) E-31
.69351-01
. 6 8 59E-O i
.68t4E-J1
. 699 3E- 01 i
13 4 741E-01
.5277E-01
. 515 3E-01
. 52 47E-U1
.5367E-01 14 2235E-01
. 36371-0 1
.3481E-G1
. 36 31E- 01
. 367 7E-81
-l 15 16
.1303 E-01
. 2344E -01
. 22 6 CE-01
. 23 E4E-J1
. 213 7E- 01 1697 E-01
.2972i-01
.288EE-bi
.33E4E-61
. 2 2 3 3E- 01 17 18
.7 3 3F E-0 2
. 13541-01
.129 EE-G 1
.13 52E-J 1
. 8 655E- 0 2 1
19 3 0 64 E-0 2
.58881-02
. 5 5 3 2E-0 2
.5979E-J2
. 343 6E- 0 2 l
20
.1684 E-0 2
. 3422E-0 2
. 3135E-C 2
.33 78E-02
.18 0 7E- 02 1
Ci ANNEL 30PPLER 30E FF ICIE NT3
.1772E-0 4
. 107 31-04
.1356E- 04
.14E9E-J4
.2066E-04 l
j i
E'E 48a.
I
@88 e
-n
,.,-w-
-w.
,,---r
--e--
w
Table QCS760.10-7 (continued)
LOCAL DOSPLEF WEIGHTING F ACTOR AND 3 HANNEL. 00 FPLEE COEFFICIENTS AT EOC4 FLOODED (T OK/DT)
CH A NNEL AXI AL NO3E 2L 22 23 24 25 1
.18 35 E-01
.2159I-01
.179 3E-Ci
.iT69E-31
.166 SE- 01 2
.2 9 TT E-01
.3289I-01
.2973E-01
.30C7E-01
. 28 3 2E- 01 3
4647E-3i 4378E-01 4 69 3E-01 47'1E-21
. 45 3 6E-91 4
.3 584 E-01
.3727I-01
.3 63 7E-J1 3T43E-Ci
. 36 0 JE- 01 5
.4 8 4S E-31
.5058E-01 4908E-31 49 73 E-01
. 4917E- 01 6
.6 331E-01
.65495-01
.6407E-01
.6470E-Gi
. 644 9E- 01 7
7 72+ E-01
. 793 0E-01
. 7617E-Li
.7866E-J1
. 7 8 8 2E- 01 8
.5 59F E-3 i
.2781I-Si
.8707E-G1 6T60E-01
.8787E-01 9
.9 20L E-01
.93681-01
.9 312E-01
. 95 e 6E- 01
.9403E-01 10
.3 2% E-31
.94461-01
. 9 3 96E-01
.9462E-01
. 948 3E- 01 R
M 11
.e852E-31
.89771-01
.8 9 2 3E-01
. 29 71E-G1
. 9 0 01E- 01 m
,o 12
.7 9 55 E-S i
.4348E-01
.7 973E-01
.79 95E-31
. 0 0 4 JE- 01 13
.6937E-31
.69901-31
.6o7EE-G1
. E6 5 3E-Li
.692TE-Si g
14 5384E-01
.5364I-01
.5 24 3E-01
. 5145E-J1
. 5 269E-41 15
.3 81 E-01
.36731-01
. 3 62 3E-01
.3 74E-01
. 3630E- 01 i
16
.2 49t E-01
.2132I-01
.2 35 7E-01
. 22 53E- 01
. 2338E- 01
. 3 05 E-01
.25 75E-;1
. 296 3E- 01 3
17
.3180 E-01
.2224I-01 14
.1416 E-31
.85961-02
.138 5E-01
.12 9 0E-G i
.1349E- 01 19
.5 98F E-0 2
. 340 2E -0 2
.5935E-G2
.54S7E-J2
. 5855E- 02
.3 32T E-0 2
.1778i-02
. 3 33 7E-0 2
.31C2E-J2
. 3 394E- 0 2 20 C1 ANNEL 30PPLER 30iFFICIENTS
.157) E-0 4
. 20661- 04
.1469E- 04
.13 58E-J4
.1974E- 0 4 EF GB"
Table QCS760.10-7 (continued)
LOCAL 00PPLE P WEIGHf1NG C ACTOR AND 3 HANNE. DOPPLER COEFFICIEPGS AT EOC4 FLOODED (T DK/07)
CH ANNEL AXIAL NO3E 26 27 28 29 30 1
.1543 E-01
.156SI-01
.1582E-Ci
.15t4E-01 1574E- 01 2
.2 655 E-01
. 267 3E-01
. 2 6 7 dE-C 1
.26E0E-01
.2677E-01 3
4 311 E-01
. 4307I-01 43 C EE-Gi 43C8E-41
. 4 314E- 01 4
.3 493 E-41
. 34611-01
.345 JE-41
.3452E-01
. 34 6 6E-31 5
4 815 E-01 478 2E -01 47 65E-J 1 4767E-01
. 47 8 6E- 01
(
l 6
.6 345 E-01
. 630 3E-01
. 6 2 6 0E-01
. 62 6 2 E-J i
. 6 30 FE- 01 7
777)E-01
.7729I-Ci
. 77 0 3E-G i
. 7T C1E-31
. 77 3 2E- 01 8
.t 695 E-31
. b64 4E-01
. 8 6 0 9E-01 86L9E-C1
.8 645E-81 9
.3 31s E-31
. 927 0E -O L
.9 23 4E-01
.92 34E-31
. 927 JE- 01 fg vs 10
.?423E-01
. 93 78E -01 9245E-01
. 93 45 E-Li
. 93 7 6E- 01 5
11
.19 63 E-01 39341-01
.8 9110-C i
. 6910E-L i 89 31E- 01 12
.c 044 E-31
.e3291-01
.f.t2GE-01
.6019E-Ci
.80251- 01 5
13 6 986 E-31
.69881-01
.7100E-01
.6999E-J1
. 698 4E- 01 14 5 403 E-91
.54361-Ci
.5465E-01
.5464E-01
. 5 43 2E- 01 15
.3 8 33 E-01
.38501-01
.3917E-Ci
. 3316 E-G1
. 3 8 7 6E- 01 16
.2 54t E-01
.2585E-01
.2 617E- 01
. 2615 E-01
. 2 581E-31 17
.3 261 E-01
. 33571-01
. 3 4G EE-01
.34C4E-G1
.3351E-01 1e
.1515 E-01
.15691-01
.15 9 2E-01
.15 90E-01
.15 66E- 01 19
.6715 E-0 2
.6965E-02 7 C5 5E-0 2
.7546E-02
.69 4 2E- 0 2 20 4 0 01 E-0 2 413 6E -0 2
.4174E-62 4165 E-C2
. 4112E- 0 2 C4 ANNEL 30PPEER 30EFFICliNT5
.9 30+ E-0 5
.1025I-04
.it71E-C4
.10 tie-44
.10 2 6E-8 4 E' E cre" W
Table QCS760.10-7
~
(continued)
[0FPLEF COEFFICIENTS AT EOC4 FL OODED (T De(/DTI L OC AL DOPPLER WEIGHIING F ACf 0 R AN3 3 HANNE.
CH ANNEL AXIAL N0GE 31 32 33 34 35 i
.155+ E-01
.9093I-C2
.8789E-32
.E974E-02
. 9335E- 0 2 2
.2 665 E-41
.1460i-01
.1427E-01
.1447E-01
.149 5E- 01 3
4 322 E-01
.21815-31
.2186E-01
. 22 0 6E- 01
. 2 26 9E- 01 4
.349FE-31
.3429I-01
.3504E-01
. 35 24E- 01
.3580E-01 5
.4 81) E-31
.4970I-01
. 5 0 55E-C i
.5072E-01
.513!E-Oi 6
.6 353 E-01
.6651I-01
. 6 7 39E-G i
. 6T 54E-01
. 68 21E- 01 7
.7762E-01
. 62715-01
. 8 329E-Si
. E3 41E-01
. 8 40 4E- 01 8
.t695E-01
.55211-01
.9 45 CE-01
. % 59E-01
.95 0 CE- 01 9
.9 31$ E-01
.1032E+00 16 2)E +0 0
-.1520E+GO
.10 2 2E+ 0 0 8
m 1C 3 41T E-01
.iC47I+00
.1C34E+s0
. 10 34E+00
.10 34Et 0 0 y
11 396LE-91
.99711-01
.9 8 5 JE-C i
.9555E-Ji
. 98 25E- 01 l
8 12
.c 0 33 E-9 i
.6866I-01 8 8 0 8E-01
.8812E-51
. 8 755E- 01 l
0, 13
.b981E-01
.74081-01
. 7513E-51
. 7515E-01
. 744 CE- 01 N
14
.5405E-01
.5689E-01
.5E12E-01
.5808E-Gi
. 571 tE-Gi 15
.382)E-31 4324I-01 4119E-01
.aiG5E-J1
. 4018E- 01 16
.2 537 E-31
. 2578E-01
. 2 6 35E-01
.25[6E-G1
. 25 5 0E- 01 17 3254E-01
. 17 315-01
.1712E-01
.16 E9C-31
.1649E-C1 18
.i S12 E-31
.6843I-02
.8 29 3E-32
.8071E-02
. 79 31E- 0 2 19 668) E-3 2 4121E - 0 2
. 3 814E-C 2
. 36 3 3E-G 2
. 3526E- 02 20
.3 9 7', E-0 2 e2511E-02
. 2 271E-0 2
. 2147 E- 02
. 20 0 2E- 02 C4 ANNEL 00PFLER COEFF ICIENTS
.9 313 E-0 5
.48895-04
.5584E-04
.5596E-04
.599 GE- 0 4 E'E GB"
l i
1 l
Table CES760.10-7 (continued)
LOCAL DOPPLER WEIGHIING F ACT OR AND 3 H ANNEL DO FPLEE COEFFICK ENTS AT EOC4 FLOODED (T OK/DT)
CHANNEL j
4XIAL NODE 35 37 35 39 40 1
.3 443 E-8 2
. 1073I-01
. 2116E-01
.1D29E-01
.1112E-91 2
.15 35 E-31
.16351-01
.3254E-Ci
.1619 E- 01
.168 3E- 01 3
.2293E-Oi
.24191-01
.4926E-51
.2427E-31
. 2 47 2E-G 1 l
4
.3 61+ E-81
.37755-01
.3940E-Oi
. 37 6 2E-21
. 379 8E- 01 5
. 5155 E-01
.53181-01
.5 3 2 0E-01
. 5317E-C i
.5345E-Gi 6
.5 8 31 E-01
.6978I-31
.6 e 97E-01
.7004E-01
.700 6E-Ei o
7
.5403E-01
.25261-01
. 8 37 2E-01
. 25 77E-31
. 8 55 GE-91 d
8
.? 465 E-31
. 95631-01
.9 295E-21
.9645E-ci
. 959 6E- 01 8
9
.101$E+00
.1326I+08
.1004E+CO
.1334E+3G
.iO28E600 10
.1033 E *O O 10371+00
.it03E+00
.10 43E+ C3
.10 3 7E
- 0 0 l
?
11
.4 793 E-91
. 98635-01
.9 52 6E-01
.5874E-Ji
. 98 42E- 01 j
g]
12
.% 7 51 E-01
.6613I-01
.6 3 9 9E-01
.6753E-01
. 8 761E-Oi 13 7 465 E-01
. 7534E-31
.74C9E-si
. 7 47 2E- 01 14 5 773 E-81
. 57701-01
.4869E-01
. 55 48 E-G i
. 5 686E-31 15 4 055 E-01
.3350E-01
.2 45 7E-31
. 3710 E-61
.22751-01
.13 6 5E-01
. 22 23E-61
. 22 4 3E-81 17
.1625 E-01
.1131E - 31
.1612E-41
.13 3 8 E- 01
.1149E-Oi 18
.7 615 E-9 2 45751-02
. 7 3 52E-0 2
. 6319E-3 2
. 4 64 3E- 0 2 19
.3 313 E-6 2
.187 71 - D 2
.3754E-G2
.25 93E-OZ
.188 2E-D 2 23
.1853E-02 10075-02
.8116E-C 2
.13 79E-02
. 978 CE- 0 3 CH ANNEL. DOPPLER COEFFICIENT 5
)
.6113 E-8 4
.6554I-84
. 2 351E- 04
. 6319E-0 4
. 65 0 tE- 0 4 E'N cra" 1
i b
~
t Table QCS760.10-7 (continued) i LOCAL DOSPLER WEI GHIING FACT OR AND 3 H4NNE. DO FPLEs COEFFICIENTS AT EOC4 FLOODEO (T OK/OTI I
CH A NNEL
)
AXIAL N0DE 41 42 43 44 45 1
.1147 E-01
.1106I-01
. 2 224E-O i
.il19E-ui
.9 0 4 0E-8 2 2
.1725 E-01
. 16 56E - 01
.3354E-Ci
.16 43E-01
.1513E- 01 3
.2 5 35 E-01
.2505!-01
. 5 C2 EE-L i
.24t6E-01
. 23 4 EE-Ci l
4
.3 8 32 E-01
.3S411-01
.3998E-Gi
. 28 6 4E-Ji
. 3667E- 01 5
.5 37'+ E-D i
.5388I-Oi
.5374E-G1
.5334E-01
.5193E-C3 6
.7 0 23 E-01
. 73 61I -O L
.6927E-01
.7tC9E-Ci
. 68 6 2E- 01 f3 7
.3 5 63 E-01
.8617I-01
. 8 36 3E-C i 2565E-31
. 8 417E-ti l
e
.9 604 E-01
.5667I-01
. 9 38 5E-C i
. 95 96E-;1
. 9454E- 01 cn 9
.10 2) E+0 0
.13 35I + 0 9 1002E+00
.1327E+03
.1014E*00 l
7" 19 1037E+3G
.1G43E+50
.1CG7E+DO
.1D36E+00
.1025E*OS I
11
.9842E-Oi
.9875I-01
.9 49 tE-01
.95 23E-ei
. 9 75 0E- 01 12
. 7bE E-O i 8752I-01
_. 8 3 7 0E- 01
. 87 33E-S i
. 8719E- 01 13 7 463 E-31
.74041-01
.6979E-01
.7442E-Ci
. 75 0 5E- 01 14 5 67e E-81
. 55231-01
.4853E-01
.55 t4E-Ci
.5783E-Ci i
15
.3 845 E-91
.3647E-01
.2407E-01
. 37 3 5E-31
.405]E-Gi l
16
.219F E-01
.2115I-01
.130 8E-G 1
. 22 50E-01
. 2 56 4E- 01 1
17
.13 94 E-01
.12065-01
.153 2E-u i
.13 67E-G 1
.163 4E-C1 1
18
.4 275 E-0 2
.5398I-02 6 28 7E-G2
. 59 53E-0 2
. 75 01E- 02 j
19
.1681E-0 2
.23771-02
.313 9E-92
.24 ETE-62
. 3194E- 0 2 20 340&E-93
.1018I-02
. 6 517E-G 2
.12 9 2E-02
.174 6E- 0 2 i
j C4 ANNEL 30PPLER C OE FF ICIE NTS
.b 521E-B 4
.6361E-04
. 2 3 6 8E-04
.54 61E-04
.4364E-04 i
[
Gr 8" n
j Table QCS760.10-7 (continued) 1 L OC AL GOSPL ER WEI GHf 1NS F ACI OR ANO 3 H LN NE. DOPPLEE COEFFICIENTS AT EOC4 FLOODED (T OK/DT)
CH A hMEL i
AXIAL NO3E 45 47 i
.3 082 E-0 2
.1032I-01 2
.151S E-01
. 165 61-0 1 3
.2 3 5L E-01
.2500I-01 I
4
.3 672 E-01
.36181-01 5
.5195 E-01 5348I-01 6
.6 66F E-01 7019E-01 l
7
.c 42) E-01
.oS72I-01 8
- 7. 4 55 E-31 95981-01 pp 9
.1014E+00
.1027I+00 vi M
11
.10 25 E +3 0
,1J36I+DG
,o 11
.9 745 E-91 9818I-01 12
.f 715 E-01 67261-01
?
13 7 535 E-01
.7434I-01 81 14
.5 775 E-01
.5575I-01 15 4 045 E-31
.3724I-01 16
.2 560 E-Q i 2238I-01 17
.1633 E-01
.1355I-01 18
.7 47+ E-0 2
.5913I-02 19
.3177 E-0 2
.2419I-02 23
.17 30 E-0 2
.1252I-02 CH ANNEL 30PPLEP 30EFFICIEN73
.4 3 65 E-0 4
.5463I-04 cra I
l Es I
l Table QCS760.10-8 t
L OCAL 00* P.ER WEI GHT IWs FACTOR ANO lHANDE. COPPLER COEFFICIENTS AT EOC4 VOIDED (T 0s/07)
CHANNEL AXIAL NODE 1
2 3
4 5
i i
.2 553 E-01 2618I-Oi
.2 8 2 2E-01
.13 47E-01
. 27 8 GE-O L 2
3 415 E-31
.3473I-01
.3664E-01
.1858E-Gi
.3647E-Ci 3
.'+ 98 3 E-3 1
.5036E-01
.5 20 EE-01 26 45E-01
. 5 20 7E- 01 4
.3 515 E-01 3567I-01
. 3 76 0E-01
.35E1E-Ci
.3583E-Oi 5
.4 773 E-01 4827I-01
.5:63E-ui
.61J3 E-01
.6185E-01
.6438E-01
. 6912E- 01
. 6 229E- 01 7
.T365E-01
.7438E-01
.769EE-Gi
.83 41E-Gi
. 7484E- 01 8
5 215 E-01
.d2631-01
.6 5 C9E-C i
.93 2 6 E-01
. 8 316E-Oi 9
.6 76S E-01
.6615I-Oi
.9 C56E-01
. 95 56E-Gi
. 88 6 3E-Gi 10
. 6 8 55 E-31
.630i!-01
.9131E-01
.10 L 3E+ 0J
. 89 2 5E- 01 11 A4*5E-Si 3493I-01
.8705E-01
.9518E-C i
. e 485E- 01 8
12
.7 623 E-01
.7664E-01
.7349E-01
.64E4E-61
. 760 SE-Ci L
13
.6 63r E-01
.6618I-Oi
.6929E-G1 72 3 OE- 01
. 6556E- 01
~
?
14
.5 233 E-O 1 5259I-OL
.5 22 2E-01
.55 5 2E-01
.5104E-Oi m
15
.3 815 E-O 1
. 3793E-01
.3707E-01
.3857E-il
. 3 63 dE- 01 16
.2 553 E-91
. 247 7E-01
.212 9E-G i
.24SOE-Ci
. 23 4 5E-91 17
.3 775 E-01
. 3 532E- 01
.2 38 0E-Gi 16 SSE-Oi
. 34 6 3E- 01 18
.18 63 E-31
.1635I-01 1CC6E-01
.8424E-02
.1669E- 01 19
.4795E-02
.7365E-02
.4474E-02
. 39 90E-02 7699E- 02 20
.563tE-32 4997I-02
. 279 0E-02
. 24 C 2E- 02
. 47 01E- 0 2 Ci ANNEL 30PPLER 30 EFFICIENT 3
.154e E-0 4
.1568I-04
.17 41E- 0 4
. W12E-04
.148 2E- 04 E*E Ga W
NW
l
~
l (cont.nueo)S760,10-8 TabJe N i
l LOCAL DOPFLE R WEI GHTING F ACT O S AND ;H4N PE. DO FPLER COEFFICIENTS AT LOC 4 VOIEED (T OR/DTI l
CH ANNEL l
LXIAL NODE 5
7 8
9 13 l
1
.2 873 E-01
.33961-01
.15 3 EE-C i
. 3145E-31
. 30 8 JE- 01 l
2
.3 735 E-01
. 39391-01
.2 C37E-31 4152E- 01
. 398 3E-81 3
.5 29) E-01
.546di-01
.2 319E-01
.5654E-G1
. 5555E- 01 4
.3 695 E-81
.3335I-01
.410 0E- 01 4128E- 01
. 3891E- 01 5
.4 953 E-01
.5153I-01
. 5 581E-01
.53 E8E-G1
. 5169E- 01 6
.6 311 E-01
.6530I-01
. 711 EE-01 6765E-G1
. 652 SE- 01 7
.7 555 E-81
.77851-01
.8522E-01
.8036E-01
.7760E-C1 8
..*355E-Ci
.85951-01 9 473E-31
.E678E-51
. 854 0E- 01 l
j@
9
.E 8 35 E-01
.c1291-01
.1J0SE+03
.9407E-Ci
.9054E-Ei e431E-01
.9098E-01 E]
10
.b 945 E-01
. 91841-01
.1;14E+00 e
g 11 6 513 E-81
.8727I-01 96 2 3E-01
.89C9E-Gi
. 8 63 tE-Gi i
12
.7 65! E-01
. 78231-01
.6577E-01
.7551E-01
. 77 4 3E- 01 13 4 635 E-81
. 67341-01
.7 303E-01
.6537E-si
. 667 4E- 01 o
O, 14
.5165 E-01
.5173I-Ci 5545E-01 4623E-Ji
. 511]E- 01 15 3 6% E-01
.35141-01
.3736E-G1
. 22 44E-31
. 3 473E- 01 l
16
.2 275 E-81
. 19101-01
. 2 09 3E-01
.12 15 E-C 1 1970E-01 17 3115 E-01 2054I-01
.1033E-01
.1848E-Ci
. 224 0E-81
)
18
.1413 E-01
.8154I-02
.416 2E-0 2
. 82 24E-L2
. 9015E- 0 2 19
.E 213 E-0 2
.34291-02
.17 5 6E-12
. 36 31E-C 2 3796E- 0 2 20
.3 651 E-0 2
. 19311-02 9143E-C3
.2029E-02
. 217 2E- 0 2 C4 ANNEL DOPPLER C OE FF ICIE NT3
.1553E-04
.16751-04
.5202E-04
.1446E-G4
.1521E- 04 EN Gr8"
Table QCS760.10-8 (continued)
LOCAL 00sPLER WEIGHTING ACT OR AND 3HANNI. DOPPLER COEFFICIENTS AT E004 VOICED (T OK/CT)
CHANNEL LXIAL NO3E il 12 13 14 15 i
3137E-01
.32271-01
.2965E-01
.3031E-Gi
. 307 2E- 01 2
4 0 32 E-01 4223I-31
.4110E-01 4136E- 01
. 417 2E-C1 3
.5 603 E-01
.53251-01
.5S67E-01
.5940E-01
. 59 7 6E- 01 4
.3 91S E-01 4165I-01
. 4 2 7 2E-01 42 CSE-G i
. 422 4E- 01 5
.519' E-31 5419E-01
.5 460 E-31
.5426E-J1
. 5 442E- 01 6
.654TE-01
.67891-01
.6806E-01
.67tSE-01
. 679 6E- 01 7
.7 7 7S E-01 635 2E -01
.6 C63E-01
.8C45E-01
. 8 05 0E-C1 6
.r551E-01
.6885i-01
. 8 8 8 6E-01
.eS72E-Ci
. 8871E-Ci f?
9
.9 06L E-01
.94071-01
.9 4 0 7E- 01
. 93 5 4E-01
.9388E-Ei U
13 4131 E-01
.9425I-01 9427E-ui
.9416E-Ji
. 94 0 5E- 01 8
11
.e 633 E-01 65991-01
.8901E-01
.8594E-01
.8880E-Gi L
12
.7 7 33 E-01
.7878I-31
.7879E-Gi
.78 78 E-01
. 78 6 2E-61 c) 13
.666FE-01
.6619I-01
. 660 (E-C i 6521E-G1
. 6 60 4E- 01 1
0, 14
.5 0 94 E-01 4597E-01
. 4 53 5E-01
.4575E-61
. 455 (E-01 l
15 3 445 E-01
. 22131-01
.299sE-Ci
.21t0E-31
. 214 8E- 01 16
.1933 E-31
.12341-01
.125 3E-01
.12 66E- 01
.1253E- 01 l
17
.2162 E-01 17631-01
.16 d EE-01
.15 91E-Ci
.186 6E- 01 i
18
.L 5 2) E-0 2
. 76811-02
.8600E-02
. 85 74E- 02
. 8 423E- 02 l
19
.3 515 E-0 2
.3323E-02
. 3 83 CE-0 2
. 3B G OE-32
. 3711E- 0 2 20 1945 E-3 2
.17981-02
.2 3 5 2E-0 2
. 22 t 6E-0 2
. 220 6E- 02 CH ANNEL DOPPLER "0EFF ICIE NT5 1
.15 22 E-0 4
.1447I-04
.1108E-04
.12 20 E-0 4
.1220E-04 hfk crao
Table QCS760.10-8 (continued)
LOCAL DO*PLER NEIGHIING 2 ACT OR AND 3HANNEL DOPPLER COEFFICIENTS AT EOC4 VOIDED (T ON/07)
CHANNEL 4XIAL NO3E 15 L7 18 19 20 1
2 993 E-01
.23931-01
. 2 5/ 0E-G L
. 25 64E-J i
. 2983E- 01 2
.4143 E-91
. 344 61-01
. 3 67 7E-31
.3641E-di
. 3912E-Ei 3
.5 993 E-01
. 51931-01
.5509E-01
.'406E-J1
. 5516E- 01 4
4 28B E-01 3727I-01
.390GE-J1
.3791E-01
. 39 01E- 01 5
.5 473 E-01 49501-31
. 5 3 21E-41 43 48 E-01
. 5141E- 01 6
.5 61* E-01
.6310E-01
. 6474E- 01 Q
7
.E 0 65 E-O 1 7562E -01
. 7 5 61E-Gi
.74e6E-ui
. 769 CE-Ji 8
8 885 E-81
.c3571-01
.8343E-01
. 82 71E-J 1
. 845 0E- 01 y
cn 9
.939)E-O1
. 38831-01
. 8 2 6 5E-01 8r69E-01
. 8957E- 01 10
.9 415 E-01
.39401-01 5 914E-31
. 68 45 E-J 1 9006E-01 o"
11
.8 88T E-O 1 24991-01
. 8 461E-01
.84C8E-31
. 45 6 dE-41 12 7 86! E-81
.76331-01
. 7 5 7 8.E- 01
. 75 47 E-Ji
. 7711E-81 13
. 6 563 E-81
.66081-G1
. 65 0 4E-01
.tS22E-01
. 67 0 5E- 01 14
.4 5 23 E-01
.5115I-01
.495fE-Gi
. 53 46E-Ci
. 52 3 ?E-81 j
15
.2 093 E-31
.3624I-01
. 3 4 36E-01
. 3 5.' 2 E-01
. 36 2 2E-41 16
.12 43 E-01
.2415I-01
.2308L-01
.2413E-31
. 2114E-Ci j
17
.18 72 E-31 34421-01
.3 32EE-01
. 35 28E-ji
. 241EE-31 18
.551TE-02
.1650I-01
.157 2E-01
. ib 84E-31
. 97 81E- 0 2
]
19
.3 78t E-3 2
.7634E-02
.714SE-02
.7662E-32
. 4115E-8 2 2C
.2 395 E-9 2
. 4916E - O 2
.4486E-02
.47 3E- 02
. 23 6 3E-8 2 CH ANNEL DOPPLER 00EFF ICIENT3
.1193 E-0 4
.6824I-05
. 817 8E-05
.91CZE-35
.1371E- 0 4 i
E' 3"
- ' e i
~
1 e
to 4
4 I
Table QCS760.10-8 (continued)
LOCAL DO*PLER WEI GNIING ACT OR AND 3 HANNEL CO FPLEE COEFFICIENTS AT EOC4 VOIDED (T OK/073 f
CH A NNEL AXIAL NODE 21 22 23 24 25 1
.2645E-Oi
. 293 6E -01
. 2410E-81 3656E-si
. 3 46 2E-91 2
.3 651 E-01
.3923I-Ci
. 3 6 5 9E-01
. 55 30E-si
. 5 210E-41 3
.5 363 E-O i
.55271-01
.5 427E-Gi 4
.3 74? E-O i
.3337I-01
. 3 S S 1E-31 3911E-01
. 3 73 7E- 01 5031E 'ai
. 4 95 eE- 01 5
4 8 9'+ E-0 1
.51461-01
.4957E-Ci 6
.6195E-81
. 64781-01
.6270E-Ci 63 41E-J i
. 6317E- 01 j
75 67E-G1
. 756 7E-91 j
7
.7405E-Oi
.7694I-01
.7492E-Gi o
8
.6173 E-O i
. 64 52E-01
. 4359E- 01
~
. 8 8 8 2E-Oi E
9
.0695E-01
.o9581-OL
. 8 7 9 3E-01 8909E-01
. 8 93 6E-O i 10
.t 76? E-81
. 9C OTI-01
.8842E-01 84 54E vi
. 8 49 3E- 01 11
.e35!E-Oi
.c5671-01
.8 4 0 3E-01 75 65 E-Oi
. 7626E-Si 5'
12
.7 5 37 E-41
. 77091-0 1
.7541E-G1 64S4E oi
. 65 99E-81 g
13
.6 582 E-01
. 67021-01
. 6 514E-C 1 4948E-Ci
. 510 6E- 01 l
14 5185 E-O i
.5202I-OL 5 C37E-01 15
.3 76) E-81
. 36161-01
.3 5 7 2E-O i 3427E-Ci
. 3616E- 01 2299E-01
. 24 0 7E- 01 16
.2 524 E-81
.2107I-01
. 2 4 0 3E-01 3310E-bi
. 3 42 8E-Ci 17
.3 613 E-O i
. 24015-01
.1641E- 01 i
18
.1685 E-D i
.96861-02
.1671E-D i 73 ESE-J2
. 7 581E-8 2 19
.7 5 61 E-0 2
.40591-02
.76C4E-CZ 44ZiE-02
. 4861E- 02 20 4 615 E-0 2
.23321-02
.4703E-02 i
C4 ANNEL 30PPLE' 3 0EFF ICIE NT5
\\
8380E-05
. 682 6E- 05
.9923E-05
.1371E-04
.910 0E-0 5 i
i Gra I
i
y.,ye
-1
-., ~, -
l I
Table QCS760.10-8 (continued)
L OC AL 00P P.ER WEI GHi LNG F ACT OR AND ;H ANNE. [0PPLER COEFFICIENTS AT LOC 4 VOIDED (T O K/DT) t l
CH A NNEL AXIAL NODE 25 27 28 29 33 1
. 2 2 43 E-91
. 2289I.220?E-01
. 2310 E.2298E-01 2
.3 2 4r E-01
.3277I-01
. 3 285E-01 32 t8E- 01
. 328 5E-81 3
.w 943 E-01 49571-01
. 4 9 5 6E-31 4959E-21
. 496 7E- 01 4
3 61+ E-01
.3593I-01
. 3 582E-01
.35 t4E-31
. 3 599E- 01 i
5
.4 S 4r E-01 46151-01
. 4 7 98E-01 45COE-Gi
.48 2 0E-Qi 6
.5 233 E-81
. 61621-01
. 614 CE-01
.E141E-01
. 616 (E- 01 7
.7 461 E-91
.74031-01
.7376E-01
. 73 78E-Ji
. 740 7E-C1 8
.5 253 E-01
.52041-01
. 817 3E-01 8174E-01 8 20 6E- 01 i
9
.: 79? E-01
.c738I-01
.8703E-Ci
.BrC8E-01
. 873 9E- 01 10
.5 8 65 E-01
.e8161-01 8719E-01
. 87 89E-01
. 851 EE- 01 11
.L 451 E-31
.34121-01
.8293E-01
.8393E-31
. 841 JE- 01 12 r7 62r E-31
. 76011-01
.7595E-C1 7594E-Ji 759tE-Ei x3 i
O 13
.6 66i E-31
.66511-01 6661E-01
. 6660E-Gi
. 6647E- 01
- l 14
.5 25f E-31
. 5268I-01
.5293E-31
.5291E-01
. 5 26 3E- 01 i
l
.o 15
.3 8J5 E-01
. 38661-01
.3597E-01
.35 SE-Ji
.3861E-01 1
g 16
.2 6 2! E-91
.26621-01
.2688E-Ci
.2546E-Ci
. 2 65 7E- 01 i
17
.3 773 E-31
. 3367I-01
.3932E-01
.3928E-bi
. 3 8 78E- 01 S
it
.18 45 E-01
.19091-01
.1928E-01
.19 26E-51
.19 0 2E- 01
)
19
.5 691E-9 2
.89981-02
.9 C 6 8E-0 2
. 5 52E-G2
. 895 7E- 02 2C
.5 735 E-0 2
. 59005-02
. 5 c15E-0 2
.5817E-02
. 58 55E- 0 2 C4 ANNEL 30PPLER C OEFF ICIE NTS I
.604rE-05
.6645I-05
. 6 9 7 3E-0 5
. 69 73E-C 5
. 664 5E- 05 i
'E' ET cre"
( c.,,M.lf,. 0.,CS760.10-8 L OC AL DOS PLER WEI GHf ING - ACT OR AND 3 H&NNE. 00 FPt.E F COEFFICIENTS AT EOC4 voIEED IT Dx/DT)
CHANNEL 4 XIAL NODE 3L 32 33 34 35 1
2 263 E-01
.1278I-01
.122 7E-G 1
.12 48E-Gi
.129 4E '
2
.3 2 51 E-01
.1764I-01
.1711E-01
.17 33E-01
.179 JE- 01 3
4 955 E-01
. 2481E -01
.2471E-Gi
.2453E-01
. 2 563E- 01 4
3 6 2t E-01
. 36385-01
. 3 715E-01
. 37 3 6E-01
. 3 795E- 01 5
. 4 8 5e E-01
.5098E-01
.5192E-G1
. 5210E- 01
. 5 2 69E-91 6
.6 215 E-01
.6646E-01
.6 7 3 5L-G1 6755E-Ci
. 6812E-61 7
7 463 E-01
.6113I-01
.817 8.E-01
.8169E-ui
. 8 23 7E- 01 8
.$26?E-Q1
.9229I-01
. 917 5E-31 9188E-Gi
. 9 217E- 01 O
9
.979?E-01
. 993 7E -G1
. 3 3 3 fE-G 1
. 9 4 7E-01
.98 5 6E- 01 o
l g
10 8 863 E-01
.1006I+00
.9947E-G1
. 9 57E-Gi
. 9945E- 01 o
11
.,3 447 E-01
.e5941-01
.9 49 8.E-D i
.9303E-01
. 94 69E- 01 12
.7 6 22 E-91
. 85511-01
. 6 5 3 7E-G 1
.8544E-01
. 8 48 6E- 01 4
i 13
.6 653 E-01 7248E-01
. 7 3 47E-G 1
. 75 51E-01
. 72 7 2E- 01 0
14
.5 253 E-01
.5651I-01
. 5 7 7 5E-O i
.5775E-11
. 5 68 5E- 01 15
.3 8 25 E-01
. 4 G 9 dE- 01 16
.2 615 E-01
.2716I-OL
.2772E-G1
.2736E-Gi
. 269 ]E- 01 17 3 76+ E-01
.1964I-01
.19 3 0E-01
.1878E-01
.1873E-01 18 1837E-Oi
. 10461-01
. 9 8 62E-0 2
.%68E-02
. 941JE- 02 19 8 64+ E-0 2
.5114E-02 4 7 CSE-C 2
.4476E-02
.440 ZE- 02 l
20
.5 683 E-0 2
.33261-02
.3 (0 2E-C 2
.2537E-02
. 2 68 7E- 02 C1ANNEL 30PPLE3 30EF FICIE NTi i
.6 0 8J E-0 5
.4235E-04
. 8. 7 37E-0 4
.4F55E-C4
. 479 7E- 04 i
i ca" i
=
l j
t i
Table QCS760.10-8 (continued)
LOCAL DOPPLER WEIGHIING ACT OR AND 3 HANNEL DO FPLEE COEFFICK ENTS AT EOC4 VOIDED (T ON/DT) i CH ANNEL A XIAL N0DE 35 37 38 39 40 l
1
.1352 E-01
.1431E - Ci
.29d4E-Ci
.14G8E-01
.148 7E- 01 l
2
.179fE-01
. 19231-01
.3988E-Ci
.13 33E-01
.199 3E-31 3
.2 582 E-01
. 2705I-01
. 5 71 tE-01
. 27 41E-G1
. 27 71E- 01 4
.3 8 3? E-01 4G011-01 41SiE-Li
.3953E-01 40 25E- 01 5
.5 295 E-01 54731-01
.5497E-Ci
.54E7E-01
. 5496E- 01 6
.6 823 E -01
.7001I-01
. 69 2 7E-01
.7110E-01
. 7 G 2 2E- 01 i
7
.? 241E-01
. 64031-01
.8 231E-01
.e426E-01
. 841e E- 01 8
.3194 E-01
.9333I-01 9167E-01
. 93 78E-J1
. 9 3 5 4E- 01 i
g 9
.9825E-01
.9951I-31
.9727E-01
.9990E-01
.996 ;E- 01
,3 1
N in
.9 915 E-01
.10 0 3E + 0 0
.9756E-01
.10CSE+00
.10 0 EE
- 00 i
11
.9 44) E-01
.95561-01
.9 215E-G 1
. 55 3 2E-01
. 95 25E-G1 12
.5 485 E-01 8552I-01
. 815 4E-01
.84c2E-31
. 85 2 0E- 01 i
?
13
.7 315 E-01 73881-01
. 6 613 E-01
. 72 40 E-31
. 731 EE- 01 14
.5 733 E-01
.5738I-01 476EE-01
. 55 C 2E-G 1
.5647E-Oi 15 4123 E-01 4006E-01
.2360E-Ci
. 37 66E- 01
. 3 92 8E- 01 1
16
.2 693 E-01
.2358!-01
.125 EE-01
. 23 31E-ui
. 2 33 2E-61 17
.18 3L E-01
.1240E-01
.1914E-Ci
.1514 E- 01 128GE-Ei 18
.t953E-02
.52255-02
.8355E-02
. 7L 46E-L2
. 5417E- 0 2 i
19 4105E-0 2
. 225 61-02
.4868E-02
.32 56E-G2
. 231 EE- 02
^
23
. 2 475 E-0 2
.1313I-02
. 214 4E-Oi
.15 75E-02
.130 dE- 0 2 i
CH ANNEL 30PPLER 30iFFICliNT5
.4953 E-0 4
.5420E-04
.15 41E-G 4
. 47 43E-C4
. 50 38E- 04 c; >
x-i l
I
Table QCS760.10-8 (continued)
LOCAL 00PFLER WEIGHTING ACTOR AND CHLMNEL DO FPLES COEFFICIENTS AT EOC4 WOIDED (T DK/DT)
CH A NNEL AXIAL.NO3E 41 42 43 44 45 i
.152T E-81
.1498I-01
. 310 5E-01
.1412E-J 1
.12 75E- 01 2
.2 031E-01
.2018!-01
.4C86E-01
.19 2 0 E-G1
.18 3 5E- 01 3
.28G3E-01
. 28 25E-01
.5
- 3 7E-01
. 28 27E-Ci
. 2 676E- 01 4
4 06L E-01 41801-01 4 2350-C 1 4GEGE-Ci
. 3916E-81 5
.5 5 2T E-01
.5547E-01
.5537E-01
.5502E-01
. 5 35 2E-91 6
.7 0 43 E-01
.71811-01
.695CE-Ci
.7823E-01
. 68 6 3E- 01 7
.3 443 E-01
.e485!-01
.2255L-01
.6415E-G1
. 8248E-81 8
.9 37) E-01
.5421E-01 9153E-31
.9329E-01 916 fE- 01
?
9
.9972 E-01
.1302I+30
.9696E-01
.99 23E-01
. 9 766E-61 10
.19 35 E+0 0
.1J07E+08
. 9 717E-01
. 53 78 E-01
.9343E-Ci pg 11
.3 5 3! E-01
. 9551E -01
.9173E-C i
.9472E-01
. 937 6E- 01 v) 12
.r 523 E-01
. 650 4E-01
.8111E-51
. c4 5 8 E-J1
. 8 42 7E-41 5
13
.T 31b E-01
.72391-31
. 6 7 66E-t i
. 72 47E-01
. 7 311E- 01 l
14 5 63t E-01
. 54 E9I-01 4709E-01
. 5515 E- 01
. 572 3E- 01 15
.3891E-01
. 36811-0i
. 2 291E-01
.37 73E-Qi 4118E-81 16
.2 272 E-01
.2189I-01 1253L-01
.2348E-G1
. 270 2E- 01 a
a 17
.1203 E-31
. 1337I-01
.1696E-01
.15 41E-01
.18 59E-81 18 4937 E-0 2
. 59021-02
.7456E-52
. 710 3E-3 2
.8978E-02 19
.2045E-02
.25351-02
.3951E-02
. 310 0E- 0 2
. 4 0 5 4E- 02 20
.1113 E-0 2
.1345E-02
.1679E-01
.17 75E-02
. 242 5E- 02 C4 ANNEL DOPPLER 3 0E FF ICIE NT3
.5 063 E-0 4
.4802E-04
.15 6 *E-0 4
. 38 71E-b4
. 30 8 6E-24 E' E ra NW
Table QCS760.10-8 (continued)
LOC AL DOSPLER WEIGHIING T ACID E AND 3 H4NNEL 00 FPLER COEFFICIENT 3 AT EOC4 VOIDED (T DK/DT)
CHANNEL AXIAL NO3E 45 47 1
.1283 E-91
. 14281-01 2
.1843 E-91
.19 9 4E - 01 3
.2 66! E-O i
.28421-01 4'
.3 9 22 E-91 4J 77E-O L 5
.5 355 E-01
.55181-51 6
.5 865 E-O i
. 7 0 3 6E - 01 7
.2 255 E-01
.c4245-01 8
.516TE-gi 9335I-01 9
. 5 76T E-01
.9925I-Oi is in
.9 8 42 E-01
.9978E-31 g) 11
.9 37e E-01
. 94 E9I-01 os 12
.c.42+E-Oi
. t4 52E-01 13
.7 3 JT E-O i
. 72 381-01 2$
14
.5 715 E-O i 5503I-01 E
15 411! E-01
. 37 581 - O L 16
.2 693 E-01
.2331E-01 17
.1853 E-01
.15221-01 le
.t935E-92
.6975I-02 19 4 9 25 E-D 2 33 22I-D 2 20
.239FE-02
.1706E-02 Ci ANNEL 30PPLER 30EFFICIE NT3
.3087E-04
.3869I-04 E'N
. cr e -
Table 760.10-9 l
I SODIUM WOID WORTH GISTilBU TION AT EOC4 ( CEL E/(G X 10'*5)
\\
CH A NNEL
~
i A XI AL NOD E L
2 3
4 5
1
.4 5 25 E-91
.44801-01
. 50 3 EE-81 2
.2 372 E+0 0
.2316I+00
.2335E+09
.13 57 E-0 2
.2353E+ 80 l
3 636SE+00
.62761+08
.5644E+00
. 76 52E-Si
.5880E+04 i
4
.6 254 E+0 0
.636Ji+30
.567CE+00
.53t2E+00
.5243E*00 5
.4323E+00 3524I+08 412 5E+ 0 8
.1369E+31
. 60 8 2E+ 00 6
.1555 E+0 i
.1464E+0i
.1454E+01
.2T66E+0i
.1797E+81 I
7
.2 6J3 E+31
. 247 9I + 81
.2 4 3 8E+ 01
.3552E+01
.2915E+01 i
8
.3 4 63 E +0 i 33091+0i 3 245E+ 31
.4T44E+C1
.3818E+0i j@
9
.3945E+31
.J778I+01
.3697E+Ci
. 52 61E+ C1
.432 6E+ 01 if
.4 035 E +61
.3367I+0i
.3773E+01
. 53 3 8 E+ C1
.4406E+01 11
.3 713 E+01
.3565I+0i
.3477E+Ci 4369E+:1
. 4 J 4 6E* 01 y
f" 12
.3 0 5+ E + 31
.2923E+01
.2546E+C1 412 8E+ 0 i
. 3 301E+ G1 os 13
.2 063 E+01 19675 + 31
.190%E+01
.3L65E+G1
.223 5E+ D1 j
14
.597+E+0C 9285I+D8
.8 916E + 0 0 2t44E+01
.1089E+E1 0'
15
.2 463 E-G i
.66751-01
.1 C17E+ 0 0
. 95 3 4E+ C0
.135 3E-81 16
.5795E+00
.9992i+0g
.102 2E + 0i
.12 32E+ 0 9
. 855 6E+ 0 0 17
.749tE+00
.7733E+00
.99 3 2E+ 0 0
.ii75E+0J
. 7 331E* 00 l
1 18
.3 003 E+0 0
.3072i+00
.3 5 57E+00
.Ee49E-ci
.2974E*00 1
19
.1263 E+0 C
.1272i+08
.1406E*DO
. 38 9 9E-Ci
.127eE+38 20
.3 635 E-91
. 345 11-01
. 3 3 3 GE-01
.15 48 E-C i
. 3 651E- 01 6
I 4
i a
1 5
- c. p CY {
ga B$
l 1
i
i l
l Table 760.10-9 (continued)
SODIUM VOI L WORTH OI STR I BU TI ON AT EOC4 (D EL K/C G X 10 *
- 5)
CH ANNEL 4XIAL NODE.
5 7
8 9
10 1
.4 9 01 E-01
.5044I-01
.1262E-G1
. 73 59E-01
. 6 62 4E- 01 2
.235LE+30
. 2 3 8 6E + C 0
.3 561E 61
. 33 ' 6E+ 13
.2773E*00 3
.6223E+00
. 539 3E +0 0
.1292E+GO.
.8608E+03
.6735E*00 4
.6 011E+0 G
.4534I*00 3695E+00
.9567E+d3
. 68 3 2E+ 0 0 5
.4 9 75 E+J G 5791E+00
.15 4 9E
- 31
.1067E+30
. 3651E+ 0 0 6
.165)E+0i
.16 8 3I + 0 i
. 2 6 5 3E + 01
.12 E6E + Ci
. iS0 JE+ G 1 j
7
.2 7 42 E +3 1
.2718E+0i
. 3 69]E +t i
.2354E+31
. 2 572E+ 0i 8
.3624E+0i
.3562I+0i
.4486E+01
. 32 28E + C1
.3445E*01 9
. 113 E +31
.4334E+01
.496 tE+Ci
. 37 C1E+ Ji
.3919E*01 a
10
.'+ 191 E +01
.41065+01
.5 03 6E+C1
.37 7GE+ 01
.3989E+01 11
.3 841 E +31
.3768I+31
.4686E+C1
.3426E+;1
. 364 6E+ Li gg 12
.313r E +01
.3J70E+01
. 3 3 51E + b i
. 2715E+ ;1
.293 8E* 01 v,
M 13
.2 09+ E +01
.2359E+01
. 2 9 9 8E + 0i
.15 73E+01
.18 7 8E* 01 P
14
.3712E+00
. 96 54E + 0 3 1906E+Ci
. 20 0 5 E + 0 3
.7462E*00 15
.5775E-31
.75151-01
.8 49 3E+C0
.1125 E+ G 1
. 28 71E* 0 0 a
i
?
16
.? 9 4+ E +0 0
.11181+0i
.2788E-01
.15 6 2E+ 0i
.1172E+01 El 17
. 6 515 E+ 0 0
. 956 2I + 00
. 313 3E + J O
. 95 34E+ J G
.1040E* 01 18
.3373E+00
.3794E+30
.13 2 2E+ 0 3
.33 57E+ 30
. 38 6 3E+ 0 0 1
19
.1341 E +0 0
.1346I+00
.4 8 61E- 01
.1212E+ 0 0
.1340E*00 20
.3 44* E-01
.3379I-01
.143 2E-01
. 33 79E-31
. 30 65E- 01 EF3' 4
TBa 4
i
l Table QCS760.10-9 (continued)
SODIUM WOI O W0tTH LISTRI3UT131 A T EOC4 (DELK/(G X 10 " 5)
CH A NNEL 4XIAL NO3E il 12 13 14 15 1
.b 422 E-01
.7160E-01
.9 024E-Ci
.8404E-J1
. 8 43 2E- 01 2
.2 715 E +0 0
.3331E+00
.428CE+03
. 33 28E+ GG
.3924E+00 3
.6 6*i E+0 0
.b503E+00
.10 7 CE+ 61
.c776E+LO
. 9765E* 0 0 4
i 4
.674?E+0G
.9468E+00
.132 CE+ si
.1138E + G L
.113 EE* 01 5
.3 733 E+0 0
.1197i+30
.55.1E+C0
.21L2E+00
. 20 4 7E+ 0 0 6
.1503 E +01
.12761+01
.2945E+00
.8338E+GO
.8103E+00 7
.2 5 72 E+01
.23581+01
.1Gd8E+01
.17 52E+ 61
.175dE*01 8
.3 441 E +31
.32281+01
.17 2 3E + 01 2506E+01
. 251]E* 01 9
.3 912 E +J 1
.36965+G1
.205dE+01
.2309E+:1
.2912E*01 10
.398LE+01
.3762i+01
.211 &E + 0 i
.29 73E+ Ji
.2974E+01 ff
~4 11
.3 635 E+31
.3417I+01
.1833E+;1
. 26 53E+si
.2692E*01 ES 12 2 9 31 E+01
.2705E+01
.1415E+01
.21G8E+01
.210EE+(1 13
.1873 E +01
.iS63E+01
. 6 0 4 EE+ 0 0
. it 35E+ di
.1131E* 01 a
1 i) 14
.7363E+00
.iS61E+30
.4322E+00
.62526-01
. 6771E- 01 l
83 15
.2 993 E+0 0
.1141E+01
.126 7E + C 1
.1172 E+ G1
.117 7E+ 01 16
.1133E+0i
.1576I + 31
.iS05E+01
.132iE+01
.iS25E+ C1 -
17
.1051E+01
.9938E+00
.9330E+0S
.96 22E+00
. 965 6E* 00 3
18
.3923E+00
.33985+00
. 3 224E+J G
.34C3E+0J
.3420E*00
.1107E+LO
.12 33E+ 00
.121;E*00 19
.13 43 E +0 0
.120 75 + 0 0
.2 5 67E-01
.2558E-31
. 287 9E- 01 20
.3 J3* E-01
.3320i-01 l
l
'i C
GT 2."
N LO l
i G
$ 9
Table QCS760.10-9 (continueo; SODIUM VOIO WOITH DISTRIBUT101 AT EOC4 (DELK/(G X 10"51 CH ANNEL 4XIAL MODE 15 17 16 19 20 l
.9 05f E-01
.5725I-01
. 64 7 dE- 01
.5969E-;i
. 758 7E- 01 2
.4 2B6 E+0 0
.3178I+00
.35:5E+00
.3219E+ JG
. 3166E+ CO i
3
.107L E+01
.d966I+G8
.100 2E + 01
.8598E+0J
.7595E+00 4
.13 20 E +01
.1496I+01
.146 DE+ 01
.18 74E+0 i
. 8188E+ 00 5
.5 475 E+0 0
.1456E+0i
.1034E+G1
.3r20E+44
.1391E* 00 6
.296?E+00
.135 6E + 01
.5433E+00
. 39 t3E+ 00
.117 tE+ G1 7
.1092 E +G i
.1215E + 01-
. 6 47 5t-ui
.1117 E + 01
.215tE+C1
.1725E+01
.3308E+0i
.3 6 57E + 3 0 '
1691E+Ci
. 295 3E
- 01 1
9
.2 053 E +01
.9200i+00
.57 62E+0 0
.19 95 E+ C i
. 337 4E+ 01 8
10
.2114 E+G 1
.6962i+00
.617 9E+ 0 0 20 51E+ 31
. 3446E* 01 l
pg
.1883E+0i
.93185+00
. 4 9 21E+0 0
.1853E+J1
. 3151E* 01 5
12
.1417 E +01
.1025E+01
. 215 5E + 0 0 14J4E+41
.253 7E* 01 11 vs P
13
.6 015 E+0 0
.2258I+0i
.2 9 54E + 0 0 7660E+33
.158 EE* 01 14
.4 G5$ E*0 0
.1338I+01
.7540E+00
.4L49E-C1
.5719E+ (0 15
.1270 E+01
.130 2i + 01
.107EE+0i
.f422E+00
. 379 2E+ CG 2
16
.1503 E+01
. 1229E+01
.1295E+01
.1C93E+Ji
.122 EE* 01 17
.9 347 E+0 0
. 7164E + 0 0
.8 417E+ 4 3
.80 33E+00
.1070E*01 18
.3235E+00
.2547E+00
.2995E+C3
. 3 35E+30
. 4315E* 0 0 i
19
.1112 E +0 0 30119I-81
.1055E+00
.113 0 E+ 00
.1371E+ 0 0 1
.307 E-G1 20
. 2 585 E-01
. 2196I-01
. 2 552E-01
. 3 35E-G1 l
i
&N-cr a 1
f' s
1 1
i
QCS760.10-9 (continued) i '
SOCIUM WOID WOITH OIS TRIBU TI3N A T Eock- (DELK/(G X 10**5)
CHANMEL.
4XIAL NODE 21 22 23 24 25 64t6E-Ji
. 573 e E- 01 i
.615+ E-01
. 75575-01'
.5987E-01 35 91E+ JJ
. 318 tE* 0 0 2
.311? E+0 0
.3160:*03
.3 2 21E+ 30 2 C4E+01
. 8 987E+ 0 C 3
.1255E+00
.75sii+00
.86 BEE +C3 14t2E+01
.150aE+01 4
.10 25 E +01
~
.o1681+00
.1375E+ 01 1C 25 E+ J 1
.14 59E + 01 5
.2 895 E*0 0
.1418E+00
.3716E+JJ 54 32E+ 00
.135 3E
- 01 i
6
.5113 E +0 0
.115'Ol+Gi
. 39 9 7E+ 0 3 5410E wi
.1217E+01 7
.126?E+01
.2158E+0i
.111SE + 0 i 36 66E+ 30
.16091+01 8
.1875 E+31
.2955E+01
.1692E+Ji 5770E+00
.9 21JE+ 00 9
.219) E +01
.3380i+31
.1997E+G1 6164E+3G
. 89 71E + 0 J l
.225TE+01
.34471+01
.2051E+01 pg 10 4920E+00
.9327E*00 l
v) 11
.2 0 53 E +31
. 315 2i + 0 i
.18 53E + 01 2151E+ JJ
.1026E+ G1 12
.1615 E *01
.25371+01
.1433E*Ci 2363E+00
.12 53E+ 01 f'
13 9113 E+0 0
.1587I+0i
.7647E+00 g
14
.15 43 E +0 0
.5705E+00
. 3 9 63t-J 1
.75 52E+ ba
.1339E + 01 18 77E+ 0i
.130 2E* 01 i
.5595 E+0 0
.3812i+00
.6 J35E +0S 12 56E+ 01
.122bE* 01 l
c) 16
.1135 E +01
.1230E*01
.1094E+01 84 21E+ 0J
. 716 3E+ 00 l
17
.! 525 E+0 0
.1072i+01
.8 (41E+0 0 29 56E+00
.254 tE* 00 18
.3235E+00
.4023I+00
.304(E+00 1957E+G0
. 912 3E- 01 I
19
.1201 E+0 0
.137 5E + 0 0
.1132E+00 23 62E-;1
. 22G 1E- 01 20
.2 985 E-01
. 308 11-01
.2848E-01 l
i I
s I
jr 27 CT 8
_. E' l
/
s.
k L
('
k' T
J 1
i i
.L 1C01OE010011000e0011 0000E00000000 E0d0060 j
++*+t+
- * + - - ++*++* - -
EEEEEEEEEEEEEEEEEEEE O
97755135tt 1949!2S4G17 215133630i147b8207141 448014702 50061261372
, 42618521117936896282 v~
ICD 1O0O0O001309GJ011
?
GC43G0L0G 0000GCJ000
- + + ++++++++ - + + + + + + - -
i EEEEEEEEEEEEEEEEEEEE 0
971233950877%492Z7i23 1
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17411232425896292
)
t G
t/
s K
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D 10312i 0S00010C00031i t
9 0300)000000G300039GO
(
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- + + ++++ ++ ++
++++++'-
h E
EEEEEEEEEEEEEEEEEELE 1
t f7J13k1S65(771d] 1( 121 w
276128726243.6te7C4649 0
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,4 i
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B 00Ct000030C00060C000 I
- + + + ++ + - + t-
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1EIEi1EE1iII1I1I 73574261684426319V:15 f
.s R
93 T
20' 30
. s 10032532118468 S
2 4
901478259C61252 s72 1
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4261 6521117t36e56 42 I
4 I
+
t 0
W x
t D
105ii1111G11i1i10011 O
0 G 0 0 0 3 0 0 3 0 0 0 c 0 0 C 0 0 0'Q I
- ++ + + + ++ + +++i+ + * + + - -
V EE,EEEEEEEEEEEEEEEEEE
)33L33 225 +
T5LF 2
% 8 J 7 3 5 0 5 0 5 '0 & '9 1 5 45) 326 M
292 U
56523220080022114350 4 2. T.1 1 1 1 1 1. i.1 1 1 1 1 1 E. 2 5 2 s
I D
x' O
S E
3 O
N 12345675931234567890 L
11111111112 A
I X
+
4 5
6 SZ g _ oM" d.3 S
)
e cMh$
a 3
4
- 4
3
.39 E6E+00
. 5 531E+ 00 S
.1305 E +01
.1528I+31
.124 4E +01
.12 42E+ 01
.1578E*01 6
.1275 E+01
.2434E+01
.2214E+01
. 2211E+ 0i
. 27 39E+ 01 7
.120!E+31 3393I+01
.3125 E+ 01
. 3L 21E+ 31
. 3812E* 01 j
8
.1053 E+01
.4081E+C1
. 3 6 5 3E+ 31
.3847E+01
. 464 2E6 01 l
ff y
9
.1005E+01 453 4E + 01 4307E+31 43 CiE+0i
. 515 2E
- 01 i
o it
.9 853 E+0 G 462 4I + 01
. 439 7E +31
.4591E+0i
. 523 7E* 01 11
- 4 005 E+31
.4343E+01
.4117E+G1 4112E+Gi
.4891E* 01 I
?
12
.1055E+01
.37271+01
.3503E+01
.3456E+0i
.415!E+01 a
S$
13
.12 35 E +51
.2960E+01
. 2 631E +0 i
.25 77E+G1
. 319 3E+ 01 14
.123f E+01
.23581+01
.1763E+J1
.iT59E+01
. 20 98E+ 81 l
15
.119fE+0i
.1154I+01
.8 6 2 3E+ 0 0 85 92E+ GO
.10 2 EE* 01 16
.111FE+0i
.42431+08
.1466E+00
.1433E+G0
.18 0 4E* 0 0 17
.6 45+ E+0 0 69221-01
.7 946E-01
.6360E-Gi
.10 26E* 0 0 I
in
.2 330 E+0 0
.70331-02
. 5 58 3E-01
. 57 27E-Gi
. 678 3E-Oi j
j 19
.3 5 2T E-01
.24031-01
.3 448E-c i
. 3b 12E-01
. 387 3E- 01 20
.2085E-91
.9516E-OZ
.13;1E-01
.1954E-01
.1259E- 01 l
i l
l l
Ef 3' GTB l
_. P e
i i
I
Table QCS760.10-9 I
(continued) 1 j
SODIUM V010 W0tT t DISTRIBUTION A T EOC4 ((ELK /CG X 10"5)
Di ANNEL EXIAL NO3E 35 37 32 39 40 i
.5 5 63 E-0 2 4965E-02
. 6 737E-01
.5G40E-02
. 317 0E- 0 2 2
.5 772E-0 2 4754!-02
. 3150E+0 0
. 813E-u2
. 90 22E- 0 2 3
.2 903 E-31
.5719E-01
.8 4 2 EE+ 0 0
.19 61E-G1
.9715E-Gi 4
.4375E+0u 450 8I + 0 0
. 97 8 3E+ 0 0 44t8E+00
.5516E*00 5
.138!E+01
.1334E+01
.1259E+00
.15 09E+61
. iS4 6E* 01 6
.2 451 E+01
.2337I+01
.1305E+0i
.27C8E+U1
. 2 67 5E + 0 i 7
.3441E+01
.3273E+01
.2 46 dE+C 1
.3516E+61
. 3 72 6E+ 0i 4
8 4212E+01 40061+01 3 29JE+ 01
.4674E+0i
. 4541E* 01 l
9 4 6S1 E +01
.4451E+01
.3777E+01
.51E7E+01
. 5 0 31E+ 01
)
ff N
10
.4 765 E+0 i
.45261+01
.364cE+01
. 52 60 E+J1
.5103E* 01 11 4451E +31
.4228I+01 3491E+01 48 8E+ 31
.4752E* 01 12 3 785 E+31
.3591E*01
.2 763E+01
.4106E+ci 4314E+ 01
?
13 2 892 E +0 i
.2735I*01
.16 26E+ d i
.3075E+Ci
. 306 E* 01 Ej 14
.187sE+01
.1764E+01
.2 63 3E+ 0 0
.1312E + 01
.1973E+(1 15 8 783 E+0 0
.dO60E+00
.10 2 7E + 01
. E47E+JJ
.9087E*00 16 5 43L E-01
.2431E-01
.1474E+C1
. 3164E-0 2
. 860 6E- 0 2 -
17
.1673E+00
.35291+00
.9 CS 4E+ C 0
.19 09E+ G J
.2968E*04 18
- o 9*T E-01
.1619I+00
.2 62 CE+0 0
. 83 49E-G 1
.1435E+00 19
.4 326 E-01
. 5965I-01
.4462t-02
. 34 4 3E-31
. 5551E- 01 1
20
.124F E-31
.13201-01
.2378E+01
.1459E-01
.1315E- 01 l
i i
oy 1
l g
i R3 $
i
...---. r
'i's
~
l
~-
l 1'
TABLE QCS 760.10-9
( conti nued)
SOEIUM VOID WORTH DISTRI3UTION AT E 004 (DELK/(G X 11+'5)
I CHANNEL LXI AL NODE-4L 42 43 44 45 i
7 03S E-0 2
.1175I-01
.6149E-Gi
.69c0E-02
.125 dE- 01 2
.1993 E-01
.14425-0L
.2963E+00
.6t99E-Ji
. 84 0 7E- 01 3
.1124 E+0 6
.53011-01
.812dE+00
.12 SOE+ 03
.1667E+00 4
.5 652 E +0 L 4823I+00
.9 4 85E + 0 0
.1353E+C0
. 8 0 4 EE- 01 5
.1553 E+0 i
.15 28I +0 L
.1471E+; 0
. it 24E+ J1
.6033E+0G 6
.2 675 E+0 i
.2704E+01'
.130 9E + 0 i
.2L87E+di
.163 7E* 01 7
.3 713 E +01
.3789E+0i
.2 3 33E+0i 3L 71E+ C1
.240 dE* 01 l
8 4 523 E+0 i
.4629E+0i
. 3 259E+G1
. 33 35E+ 01
.299EE+01 9
.5 013 E +0 i
.5129I+C1
.3 73 5E+C1 4310E+ C1
.3344E*01 10
.5 0al E+01
.5198I+01
.3d31E+0i
.4449E+31
. 340 5E+ G1 O
11 4735E+01 4830i+0i
.34470+01
.4140E+Ji
. 317 7E
- 01 i
x3 y
12
.3 995 E *01
.4056I+01
. 27 21E +01
.3476E+61
.2L84E*01 P
13
.3 Gv E+01
.3135E+0i
.1591E +G 1
. 25 64E+ 0 i
. 20 2 3E+ 0 i 14 1961E+0i 1$761+01
.2 279E+00
. iS 33E+Ji
.12 3 9E
- 01 '
i 15 5 9e E+0 0
. 7o5 71 + 0C
.1C6EE+01
.56 ISE+ 33
.4692E*00 g;
5 16
.101] E-01
.43771-01
.1512E + G1
.15 34E+ C0
.122eE+0G i
17
.3135 E+0 0
.2351E+00
.9 3 3oE+ S O
. 26 28E+ 03
. 2443E+ 0 0 18
.1453 E+0 0
.10 0 3E +00
.26o4E+03
.119 4E + 30
.109;E+00 19
.5 323 E-01
.3813I-G1
.3321E-02
. 43 45E-Ji
. 4 20 8E- 01 20
.1173 E-01
. 13881-01
.2116E + 31
.1960E-si
.10 41E- 01 4
c? 3"
~
9 S
,_N l
TABLE QCS 760.10-9 i
( continued) l l
l
.s00tud v010 WotTH DISTtIBUTION A T EOC4 ( [ ELK /( G X 10'*5)
CHANNEL
~
AXIAL NO)E 45 47
~1
.12 42 E-01
.6315I-02 2
.* 3 71E-01
.6020I-01 3
.1660E+00
.122ii+00 4
6185 E-01
.1993E+00 5-
.hG54E+00
.1129E+0i 6
.1643 E+31
. 219 4E + D i
)
7
.2 411E +31 3177E+01 l
8 2991E+01
.39391+01 9
.3*345 E +01
.4353E+0i 10
.34JTE+01
.4450E+0i
%)
11
.3173 E+01
. 4140E + 01 8;
12 2 66b E+01
.34765+01 L,
13
. 2 0 22 E +01
.2562E+01 c) 14
.1235 E+01
.1530E+0i l
E4 15
.4 682 E+0 0
.5646I+00 16
.1233E+00
.1574E+00 17
.2 451 E+0 0
. 28 63I+ 0 0 18
.id95E+00
.1216E+00 19
.4 234 E-01
. 449 0E-01 i
20
.10 5e E-01
. 1998I-01 i
S O
G B.
a
@ (D RS*
i' TABLE QCS 760.10-10 (continued)
STEEL W 0tTH OIS TRIBJTIoh ET EOC4 (DELK/KG E 10 D CH A NNEL i
AXIAL N00E.
L 2
3 4
5 1
.2 5 31E-01
.2518E-01
.2959E-01
. 88 9 3E-0 2
. 276 EE- 01 l
2 109)E+0C
.10 7 2i + 0 4
.10 6 6E+ 0 3
.23 76E-01
.19 9 6E* 0 0 j
3
.238)E+00
.2333E+00
.2 084E+ GO
.1545E-01
.222EE+06
~
4 7 612 E-01
.7837E-01 3 39 2E- 01
. 2b E9E+ CD e 42 4 EE- 01 5
.4915E+00
. 47 241 + 3 0
. 5 3 3 6E +0 0
.8012E+ C4
.5473E+30 l
6
.1083E+01
.10465+01
.10 6 3E + 01
.13 E6E+ C1
.1163E+C1 4
7
.1627E+01
.1574E + 01
.1532E+C1
.18 6 5E+ J1
.1727E+01 8
.2 346E+0 i
.198 4E + 0 i
.1982E+di
.22 %E+ ui
. 216 3t+ 0 i 9
.229LE+01
.2223E+0i
.2214E+;1
. 25 3 7E+ vi
. 2415E+ 01 c
10
.2 336 E+31
.22681+01
.2 255E+G1
.2373E+0i
.2455E+U2 0
11
.217+E+01
.2111E+01
.2 C98E+G1
. 23 S9E+ 0i
.227JE+01 cn 12
.1835 E +01
.178 4E + 01
.17 7 2E + 01
.2028E+0i
.19 01E* 01 9
13
.13 55 E +01
.1315E+0i
.1335E+01
.15 34E+ oi
.138 4E + 01 Es 14
.7 9 45 E +0 0
.7663E+00
.7 5 5 3E+0 0
. 93 39E + 03
.7947E+ 00 l
15
.2453E+06
.2253E+00
.2062E+00
.4755E+60
. 229 7E+ 0 C l
16
.2 315 E+0 0
. 2491E + 0 3 3 2 2 tE+ 00
. 72 35E-01
.2445E+00 i
17
.2 765 E+0 0
. 2921E + 0 0 4115E+ 0 0 7953E-Ci
.2827E+ 00 18
.1221E+0C
.1324I+00 17 6dE+ G O
. 52 72E-G1
.1298E+00 19
. 5 845 E-01 56355-01
. 6 2 0 EE-G 1
. 27 55E- 01
. 5884E- 01 2C 1730 E-31 16595-01
.1695E-C 1
.1127 E-01
.17 4 0E- 01 GB
~
'm i'
TABLE QCS 760.10-10
( continued)
STEEL W ORTH DIS TRIBJTIO N ST ECC4 (DELN/KG X105)
CH A NNEL i
9 to o
4XIAL NODE 5
7 1
.2 73e E-31
.2801I-01' 6555E-02
. 39 2 0 E-Gi
. 3 53 4E-G 1 2
1085E+00 5519E-OL
.6690E-02
.14 63E+ 03
. 12 3 7E* 0 0 3
.2273 E+0 0
.17 95E + 0 0
.5159E-C1
.3E32E+00
.24d:E*00 i
4
.5 2 21 E-31
.6265I-02
.3 214E+0 0
.15 3 0E + 00
. 7123E- 01 5
.5 36T E+0 0
.5604E+00
.810tE+00
. 44 7 4E+ 04
.5 028E+ 00 6
.1146 E + 01
.11385+0i
.1247E + 01
.10 t 4E+ 01
.1103E+ 01 7
.1705E+0i
.1673E+0i
.1441E+C1
.16 E8E+ 01
.1666E+ 01 2
.2136 E + 01
.20861+0i
. 2 22s E+01
. 2110 E + Ji
. 2 39 2E+ 01 9
.23eZE+01
.2323i+01
.2 457t+ C 1
. 23 56E+Di
. 2 331E+ Ji 10
.2 421E+31
.23591+0i
.249 CE+01
.23t9E+ui
.2365E+Ci o
p,
.2 2 44 E +01
. 2185E+01
.2322E+t1
. 22 L 3E+ C i
.2186t+01 y
.18 8 5 E +01
.1o 33E + 0 i
.19 6 7E + 01
.15 24E+.li
.182tE+01 11 13
.1374 E +01
.1331E + 0 i
.149]E+vi
.12 40 E + 01
.1305E+0i o
12
?
14
.7 64+ E+0 0
.7536i+00
.9560E+0S
.46 7 0 E+ 00
.6982E+ 00 D
15
.2 061 E+0 0
.1863E+00
.4317E+00
. 35 00E+ c0
.119 4E+ GO 16
. 2 953 E +0 0
. 3441E +C 0
.15 4 4E-t i 62 01E+ cd
. 3 544E+ 00 17
.3 31G E+0 0 4170E+00
.1952E+vo
.4LC3E+JO
.4273E*00 18 1473E+00
.175 2i + 0 0
.957%E-01 15 70E+ co
.177 6E* 0G 19
.b 215 E-01
.6516I-01
. 3 d 3 0E-01
.ELCCE-ui 6544E-di 20
.167! E-01
. 15621-01
.1 C d 7E-61
. LPG 7E ui
.1579E- 01 I
G8" D
N 9
i
i TABLE QCS 760.10-10 (conti.nued) l l
i STEEL WORTH DIS TRIBJT10 N % T EOC4 (DELX/KG ( 10*' il
)
CHANNEL
~AXIAE NO3E IL 12 13 14 15 1
.3 453 E-01
.3354E-01
. 4704E-Gi
. 44 28E-C i
. 4 442E- 01 2
.1213 E +0 0
.1457E*D0 187s.E+00
.17 25E+ C0
.1725E*0E 3
2357E+0G
. 298 2E + 00
. 3 9 21E + 0 0
. 35 36E+ d J
.3529E+00 l
4
.6623 E-01
.14 61E + 0 0
.3163E+do 23 68E+1d
. 2341E* 0 0 l
5
.5074E+00
.4547E+00
.14.79E+ 0 0
.30 L7E+ 30
. 3 G4 OE+ 0 0 I
6
.1111 E +01
.109 0! +0 i
.6442E+C0
. 87 20E+ Ju
. 8 75 6E* 0 0 7
.166T E+01
.1671E + 01
.1(9EE+0i
.1352E+ J1
.1395E+01 6
- 2 093 E+u 1
.2110i+0i
.1431E+ b i
.1719E+J1
.1781E* 01 9
.2 323 E+01
.2354E+31
.1613E+ 0i
.19 5 2E+ J1
.1993E+01 10
.2 3 61 E +D i
. 238 5I + 0i
.164 2E+ 01
. 20 23 E+ Ji
.2022E+C1 11
.2184E+01
.2199I+01
.1510E+Gi
.16 E 7 E + 61
.18 66E+ 01 c
w 12
.18 22 E+01
.18191+01
.1241E+01
.15 47 E+ 51
.1545E+ C1 g
13
.13 G L E + 01
.123 4E + O 1
. B C 69E+ d C
.13 43E+ C1
.104 ut+ C1 L
14
.6 93'. E+0 3
.4598E+00
.2C3cE+00
. 35 27E+.J
. 35 0'JE+ GC
?
15
.1123 E+0 0
.3581E+00 3 97tE+ 0G
.36C92+JO
.3634E+00 16 4 0 31 E +0 0
.62761+00
.5siiE+C0
.Si26E+J3
. 594 6E+ 0 3 17
.4 324 E+0 0
.41475+00
. 3 7 39E + 0 0
. 3311E+ JJ
. 39 2 2E + G d 12
.1790 E +0 0
.1583E+00
.1436E+0G
.15 36E+t 3
.1541E*0G 19
.6 535 E-01 6342I-31
.5352E-G1
.5848E-C1
.58 6 2E- 01 20 1555 E-91
.16691-G1
.1224E-01
.14 E7E-G1
.14 7 0E- 01 G "
N 9
i TABLE QCS 760.10-10 (continued)
S TEIL W ORTH DIS TRIBui10 N 47 EOC4 (DELK/KG (10 *' 5)
CH A NNEL 1XIAL NODE 15 17 18 19 20 1
.4 7 31 E-01
. 23601-01
.3415E-Ci
.3L93E-Ji'
. 3 968E- 01 2
.1875 E+0 0 14281+00
.160 2E+ 0 0
.1453E+uu
.1415E+00 3
.3 9 2! E +0 0
.35571+00
.3841E+3d
.32 73E+ 0J
.277SE+CO 4
.3173 E +0 0
.5J4Ji+05
.4 37dE+ 0 0
.27 54E+vo
.1363E+00 3,
5
.iSCIE+0 0 4J11E +0 0
.14 5 7E + 0 0
.13 5 0 E+ 'J G
.335 2E+ 00 j
6
.6 4 63 E +0 0
. 275 3E +0 0
.17 21E+ 0 3
.5706E+00
. 955 FE+ 0 0 j
7
.139)E+01
.1462i+30
-.4660L+03
. 96 57E+;0
.147 JE + 01 8
.143? E +01
. 19691-01
.6977E+00
.12 57E+oi
.18 6 0E* 01 o
0 9
.1614 E +31
. 42 40E-01
. 819 0E+ C 0
.141dE+01
.2b7 5E* 0 $
l M
10
.1642 E +01
. 56 261-01
. 8 412E + 0 0
.14 46E+ 31
.21G 8E6 Ci j
.c) 11
.1513 E +01
.2187E-01
.762cE+GG
.13 37E+ ui
.1955E+ G 1 g
12
.12 4) E+01
. 5510i-01
.595EE+00
.1110E+ J1
.1639E+ 01 13
.b353E+30
.196 5E + 0 0
. 319 7E+ 0 0
.77 G5E+ 03
.1174E+01 i
2!
14
.2 013 E+0 0
. 3114E + 0 0
.1694E-01
. 35 53E+ 00
.6269E*00 15
.3994E+00
.38291+00
.2383E+00
. 2517E-J1
. 90 7 5E- 01
)
16
.5 8 22 E+0 0
.430Ji+00
. 4321L+03
.34L1E+u3 4649E+0C 4325E+ 00,
17
.3 74* E+0 J
.2652E+00 3 9 8 7E+ 0 3
. 23 51E + 10
. 1809E+00 18
.143) E +0 0
.10 41E + 0 0
.123 0 E+t o
.12 59 E+ 00 i
19 5 36* E-01
. 41231-01
.4 73 5E-01
. 50 596 'Ji 6643E-J1 20
.132TE-01
. 10325-01
.12 2 6E-01
e a g.
!S 9
M S
s ss, TABLE QCS 760.10-10 (continued)
STEIL W0tTH DIS TRIBufIGH ti EOC4 (DELx/KG (10**5)
CH ANNEL AXIAL NO3E 2L 22 23 24 25 1
.3 252 C-31
.39581-01
.3197E-;i
.3424E-01
.2973E-Oi I
2
.1403 E+0 3
.1412i+00
.1455E+ 0 0
.16LSE+J0
.1431E* 00 3
.3145E+06
.2769I+33
.3 276E+00
.3347E+d0
.3565E+OO 4
.2575E+00
.13531+00
.2754L+00 43 t2E+ oJ 565 2Et 60 5
.1633 E+0 0
.3964E+00
.1J57t+QO
.1454E+00
.4019E*06 6
.6 095 E+0 0
.SS69E+Ou
. 5 71aE + 00
.17 28 6+ S3
.275tE+0E 7
.1015 E *31
.1471E + 0 i
.9669E+GO
. 46 69E+ b0
.1465E*00 i
8
.13 2i E +01
. 35 60i+ 0i
.125 6E+ U 1
.69 c5E+ 49
. 20 0 7E-C1 4
9
.1463E+01
. 23 75E +01
.1415E +0i
.8196E+63
. 4 22 (E- 01 10
.1513 E+31.
.2108I+31
.1446E+G1
.8415E+00
. 56 0 6E-G1 11
.14 63 E+01
.3954E+01
.13 3 7E+ 0 i
.16 2 0E+0 0
.2156E-G1 I
0; 12
.117f E+0 i
.1636E*01
.1110E+61
.59 5 2E+ 00
. 5547E- 01 a
M 13
.626TE+0C
.1173E + 01
.7698E+00
. 3191E + 90
.1988E*00 j
P 14
.4 092E+0 0
.6260E+00
.3584E+G3
.1525E-51 3117E
- 00 l
g 15
.2832 E-0 2
.69601-01
. 2 911E-01
. 23 89E+ ud
. 38 31E* 0 0 16
.3535E+0C 40 62E + 0 0 3405E+C0 43 25E+ G3
. 4 3 01E + E O i
17 3171E+0 C
.4333I+DO
.2955L+c0
.3068E+uG
. 2651E* 00 18 1365 E+0 C
.1812i + 0 0
.1263E+00
.12 31E+ bJ
.10 41E* 00 19
. 5 496 E-01
.6649I-01
. 510 6E-61
. 47 38E-ui
.4022E-01 20 1453 E-01
.1583I-01
.1365E-C1.
.12284-01
. iC 3 3E- 01 l
l l
i i
l
$? $
cT e" 1
~
4
- f e
j
m _'s w,
i TABLE QCS 760.1'0-10 (continued)
STEIL d ORTH' 01S TRIBUTIO N U EOC4 (D ELK /KG E 10++ 51 CHANhEL-P AXIAL NODE 25 27 26 29 3e i
.2 365 E-01
. 23 01E -01
. 2 3 3 5E-G i
.2339E-31
. 2 30 4E- 01 2
.1183E+00 1113E+00
.111 o E+i J
.1118 6+ 00
.1115E*00 3
.3013E+00 42696i+00
.2695E+o0
.1695E+0J
.269 3E+ JL 4
.4 41? E+0 0
.3277I+00
. 3 2 G Ei+ G J
. 32 L6E+ 0J
.32d 1E+ 0D 5
.3 76T E+U L
.1607I+00
.126 3E + C 0
.13 f 1E+ 3J
.16 0 9E
- 0 0 6
.2951E+06
.2299I-01
.613 7E- 01
.6L56E o1
.2295E-01' 7
.2071E+0G
.2977I+00
.2 5G EE+00
. 25 0 8 E+ u 0
.1977EtCO 8
.1147E+00
.J42iE+08
.4 067E* G 0
.49 69E+ 00
. 3 42 EE* S S 9
.69926-01
.4200i+00
.4910E+ 0 0
.4312E+L0
.420dE+00 10
.5893E-01
. 436 3E +0 0
.5 0 8 EE + 03
.5G67E+03
.4363E+0G 11
.e 17$ E-01
. 3899I +US
.456 2E+0 0
.45 t2E+ lJ
.3898E*00 0
12
.1335 E+0 0
.2935i+00
.3 499E+00
.3458E+JJ
. 290 *E+ 0 6 c
M 13 2 335E+0 0
.J329E+00
.17 8 2E + 0 0
.17 61E+ 0h
.132 7E* 00
.o 14 309FE+00
.37511-01
.8573E-U2
.65E7E-b2
. 377 3E- 01 g;
15 3 61l E+0 0
.1947I+00
.1834E+00
.153SE+dJ
.194dE* 00 i
16 39 33 E+0 0
. 3216E + 0 0
.3253E+C0
. 32 59E+s u
. 3217E+ 00 3
17
.2393 E+0 0
.22S*I+00
. 2 35 2E+0 0
.23 52E+ 00
.2284E+00 18
.9 521 E-01
. 954 di-O L
.9679E-Li
. 98 6 0 E-01
. 9548E- 01 19
.374FE-01
.38951-01
.4C46E-G1
.4047E-01
. 389 5E- 01 20
.9 7 23 E-0 2
. 10411-01
.i'o6E-01
.1986E-01
.10 41E- 01 cr e W
~
L
~
'N TABLE QCS 760.10-10 j (continued) l l
l STEEL WORTH DIS TRIBJT!0ti LT E004 (GELK/KG (10" 51
' CHANNEL 4XIAL NO3E 3L 32 33
'34 35 1
.2 3 72 E-I l
.41111-02
. 6 43 7E-02 66 37E-52 7867E-6 2 t
2
.1185 E *0 0
.1757I-02
.1956E-01
.19 29 E-31
. 2181E- 01 3
.3 015 E+0 C
.64801-01
.880GE-02
. % 61E-0 2
.19 0 0E- 01 4
.4423E+00_
.'2/38I + 0 0
. 2194E + 0 0
. 219 6 E+ C u
. 2 79 5E
- 00 5
.3 774 E+ 0 0
.6355I+00
.6 315E+ 0 E
.0517E+00
.769(E+00 6
.2 953 E+0 0
.1945E+01
.1091E+41
.1390E+31
.131CE* 01 7
.2 0 7', E+3 0
.14 3 2E + 01
.1519E+d1
.1518 E+ Ji
.16 0 6E
- 01 8
.1143 E+0 0
.17571+01
.18 7 CE + 01
.18 E9E+ C1
. 2 201E+ 01 9
.T003E-01
.196 2i + 01
. 2 C85E + C1
. 23 6 4E + 1
.2430E+C1 a
)
g 13
.5 915 E-01
. 230 2i +01
. 2127c + 01
. 2126 E + 01
.247cE+01
)
y 11
.6193 E-01
.18 781 + 01
.19 9 5E + 31
.19 9 4E + 01
.2317E*01 o
12
.1337 E+0 G
.1600E+01
.1734E+G1
.17 03E+ C1
.1974E+01 13
.2333 E+0 0
.1232i+01
.13C7E+G1
.13 06E+ si
.1514E* 01
?
14
.3 0 9t E+0 0
.8450I+00
.8736E+G0
. 67 24E+ JJ
.1006L*01 O
15
.3 615 E+0 0
. 465 0i +0 0
.4453E+00
.4434E+t,0
.5054E*00 16
.3935 E+I O
.15661+00
.9293E-Ci
.90tSE-01
.9829E-ui 17 2 3d3 E+0 0
.2605E-02
.5 5 3 7E-01
. 59 0 4E-01 6954E-01 18
.9 515 E-21
.2463I-01
.4587E-Gi
. 4713E-J 1 5409E-01 19
.3 745 E-01
.2J85I-01 2 6e J E-C i
.2660E-C1
. 30 2 7E- 01 2G 3 723 E-3 2 7824!-02
.9 031E-02
.2810E-02 iO 2 dE- 01 l
C2
~
90 4
x i
l
\\
TABLE QCS 760.10-10 (continued) l
$TEIL W 0tTH DIS T'RIBJTION LT EOC4 (DELK/KG (10*' 53 CHANNEL 4XIAL NO3E
~35 37 38 39 43 i
7730E-02
.88951-02
. 37 2SE-G i
. 725E-C2
.10 01E- 01 2
.2 44. E-01
.1789I-01 14G9E+00
. 2714 E-t i
.166 fE- 01 3
.5 453 E-0 2
. 25801-01
.3c3GL+C0
. 4510 E- 0 2
. 39 5 2E-41 4
.265LE*OC
.2863I+0B
. i S 1"5E+ C 0
.2816E+00
.3133E+ 00 5
.7613E+00
.76265+00
.4 713E + 0 0
.6L E9E+ 00
. 80 8 (E+ 00 6
.13 G5 E + 01
.1c84I+01
.112 2E + 01
.3402E+C1
.1354E+U1 7
.1804E+01
.17 E5i + 01
.1713E + 01
.1936E+0i
.1655E+01 8
.2197 E+01 -
.2142E+0i
.2176E+01
. 23 52E+ 01
. 22 4 7E* 01 9
.2 4 3! E+31
. 2367E +01
.2 43 3E+ 01
.2597E+Ui
. 2472E* 01 10
.2475E+01
.2405E+01
.2463E+01
. 26 31E+ 61
.2511E+01 8
11
.2 316E+01
.2253I+01
.2273L+0i
.2452E+.11
.2344d*01 12
.19bl E+0 i
.1328E+0i
.13764+01
.2074E+ei
.1991E+ 61 8
13
.1525 E +01
.1486I+01
.12 6 2E+ 01
.15 63E+ ui
.1520E* 01 L.
14
.1012 E +01
.9799I+00
.5ce1E+C0
.99 07E+ 00
.9947E+ 00
?
15
.5 0 J2 E+0 0
.46791+00
.2985E+C0
.44E4E+00
.47 2 tie + 0 3
'. 7 6 31 E-0 1
.51071-02
.5763E+00
.2855E-01
.143 2E- 01 m
16 17
.9 3 50 E-01
. 2052E +0 0
. 3 8 31E+ u 6
.1155 E+ G O
.iS05E+00 18
.6 37L E-01
.1085E+00
.130EE+00
. E519E-01
.10 0 3E* 0 0 19
.3 26F E-01
.4371I-01
.1626L-ui
. 30 28 E-J1
. 416 2E- 01 20
.10 27 E-01
. 1110I-01
.9 293E+0 0 1110E-Ji
.1091E-C1 i
e GB" 88-N
Table QCS760,10-10 4
I (continued)
STEIL W ORTH DIS TRIBJTION % T COC4 (DELK/KG X 10 !)
CHANNEL I
AXIAL NO3E 4L 42 43 44 45 i
.3 472 E-0 2
.14 79E-Ji
.145 3E- 01 2
.11e5 E-31
.17941-01
.1326E+ 0 0
.49 53E-61
. 5 57 2E- 01 1
3
.4691E-01
. 20731-01
.2 e 5 2E+ 0 0
. 5156 E-ci
. 726aE-G1 1
4
.3 206E+0 0
. 30 0 2i + 0 0
.1338E + b d
.17 74 E+ 0 u
.105aE+ 00 5
- 414)E+00
.8305E+00
.4851E+LO
.Ib20E+00
.484aE+ 00 6
.1355 E + 01
.14 07I +01
.1129E+01
.119 5 E+ di
. 90 32E+ OC 7
.18 5+ E*01
.19 3 2E + 31
.1717E+ 0 i
.16 78E + Ji
.1282E+01
'.1564E* 01 8
.2 243 E +01
.2340i+01
.216 6E+ b i
. 26 46E+ 0i 9
.2 472 E+0 i
.2579I+0i
. 2 41 tE+01
. 22 58E+01
.1731E* 01 10
.2 503 E +31
.2612i+01
.2 4 5 5t + 0i
. 22 9 0 E+ 61
.176 sE* 01 x3 Q
11
.2 335 E+B 1
. 2434E+01
.2256t+0i
.2140d+Li
.1649E+0i M
12
.1985 E+01
.20595+01
.186EE+Gi
.1519E+G1
.1411E+ 01
~
P 13
.1515 E +01
.1551E +01
.1269E+01
.13 71E+ 01
.10d EE+ 01 14
.9893E+00
. 9771I t 00
.4924t+Go
.6519E+ 03
.6979E*00 i
i
?
15
.*645E+00
.4271E+00
. 317 dt+ b 0
. 35 26E + 00
.3075E+00 16
- J015E-02
.16065-02
.5969E+03
.3022E-01
. 8299E- 02 17
.1873 E+0 0 13 76E + 60
.3947E+00
.14 39E+ 0d
.1159t+ 0 0 if
.1011 E+0 0
. 73545-01
.132EE+08
.77 t3E-ui
. 666 LE- 01 19
.4 021 E-31
. 317 11 -01
.1603E-ci
.33 43E- 01
. 299 3E- 01 1
20
.1035E-01
.1050!-G1
.oi73E+00 9267E-C2
. 8 5 21E- 0 2 I
l
]
EN 4" a" 1
i l
Table QCS760.10-10 1
(continued) l STEIL WotTH DISTRIBUTION LT EOC4 (DELK/KG (10'* 5)
I CHANNEL l
4XIAL NO3E 45 47 1
.1453 E-91
. 14651-01 2
.5 565 E-01 49391-01 3
124? E-01 5J415-01 4
.1065E+0u
.179 31 + 0 0 5
.w 65S E +0 0
.66471+00 6
.3 045 E+0 0
.11981+01 ja 7
.1285E+0i
.3680i+01 l
v>
8
.1565 E +01
.23481+01 5
9
.17 3? E +31
. 22 59E + 01 it
.17 63 E+01 '
.2291E+Di 11
.1643 E+01
.2140i+01 do 12
.1410 E+01
.181Si+01 u'
13
.1Gd6E+0i
.1370i+01 14
.6 9 74 E+0 0
. t S0 3E + 0 0 15
.3 0 63 E +0 0
.3505E+90 i
16
. 6 8 25 E-0 2 32271-01 17
.116?E+00
.1455E+00 l
18
. 6 675 E-01
. 785 8E -01 i
19
.2 995 E-D 1
.3377E-31 20
.6 553 E-0 2
.9375I-92 i
1 l
cr a m
i 1
l I
a Table QCS760.10-11 PEL.ET W3RT4 DISTRIBUTI ON A T EOC* (GELK/KG XiO'*S)
CHAhkEL AXIAL NOJE 1
2 3
4 5
i
.4 015 E+0 0
.4117I+00 46 21t+G J
. 2217E-61
.428 3E+ 0 G 2
.1251E+01
.12631+01 1361E+01
. 86 C1E-vi
.133 5E+ G1 3
.2 373 E+01
. 237 91 + 01
. 2 4 95E + 01
. $ 566+;3
.2523E+01 4
.3 795 E +01
.37661+01
.38C9E+01
.1191E+Cd
. 3999E
- 01 5
5265E+01
. 5221E + 01
.5 24 EE+0i
.5366E+u3
.553 5E+ C1 6
6 875 E+0 i
. 63 0 6i + 0 i
.6839t+01
. 93 5 9E+ 40
. 721JE+ G1 l
j@
7
.S 36f E+31
.6275I+31
.625*E+0i
.1311E+ L1
.8754E*01
%)
8
.d 8 37 E+31
. d74 0E + 01
.d692E+0i
.12 31E+ 01
. 9216E+ 01 g;
9
.9 461 E +31
.9374E+0i
.9 313E+ 31
.13 77E +;i
.9869E+01 10
.9595E+G1
. 949 0i + 0i
.9423t+01
.13 9 8 d + ;1
.9969Et di 11
.9177 E+0 i
.9376E+01
.9 011E+ 01
.12 54E+ Li
.9506E+G1 c3 os 12
.h 272 E+01
.o155I+D1
.a123E+Li
.13 7 0E+;1
. 853 aE + 01 13
.7 873 E +31
'. 775 7I + 0 i
.7745E+31
.13 56E+ 91
. 8G 8 EE* 01 14
.622fE+01
. 6167E + 0 i
.6141E+ 0 i
.8941E+60
.6349E+ 01 15 4 5 71 E+01
.4530i+01
.4523E+01
. 4514E+ s 3
.461dEt01 16
.313s E +01 31061+0i
. 313 5E+01
. D 45E+.3
. 3132E
- 01 17
.177F E+01
.1728E + 01
.1634E+31
. 73 35 E-U L 1747E+ 01 18
.9 2 46 E+0 0
.o6471+00
.7661E+00
.2038E 1
.8S75Et 00 19 4 373 E+S O 4131E +0 0
.341EE+00
. 2513t-t 2
. 410 3E+ O C 20
.1441E +0 0
.13451+00
.1L77E+00
.33 62E-93
.1292E*00 j
E g.
c.
m 5.
G; -
1 83 $
4
-,.,e---
Table QCS760,10-11 (continued)
PEL.ET W3RT4 DI STR130TIo1 A T EOC4 (DEL K/EG X 10*
- 5)
7 8
9 10 1
453LE+00
. 49 57I + 0 0
.3C *E-01
.4bt3E+60
. 4641E* 00 2
.1373 E +01
.1449I+01
.7036E-61
.13 9 8 E+ ci
.138 7E* 01 3
.2 55s E+01
.2645E+0i
.200SE+30
. 2519E+ Ji
.2565E+01 4
4 023 E+01 4C131+01
.2 C5GE+3J 42 39E + G1
. 40 7 (E* 01 i
5
.5541E+01
.55061+0i
. 5 5 61E+ G O
. 58 39E+ J1
.56deE+0i 6
.7183E+01
.7124E+0i
.9431E+30
.75 41E+ 31
. 724 7E+ 01 i
7
.$70FE+01
.o613I+01
.129 5E+ G1
. 9B E SE+ 0i
.8741E* 01 8
.9143 E+31
. 99 39E + 01
.1197E+C1
. 9b 32E+ ui
.9119E+L1 9
.9 7 63 E+31
.5664E+01
.1J3SE+01
.1327E+02
.9733E+01 10 3485E+01 9757I+01
.1354E+C1
.1925E+G2
. 951iE+ G1 11
.9435E+01
.93075+01
.1253E + 01
.971E+J1
. 93 6 7E+ 0 i
.133 SE + 0 i 376E+01
.842 5E+ 01 a
S 12
.e48FE+Il
.63681+01 13 0063E+01 7949I+0i
.1336E+01
.8673E+.1
. 6G 51E + C1 P
14
.b36?E+31
.6260i+0i
.8766E+00
.(645E+61
. 6 34 2E + C 1 g
15
.465LE+01 4570i+0i
. 4 22 3E+ 0 0
. 43 0 2E+ ui
.4614E+01 16
.3172 E+01
.3132i+01
.3222E-G1
. 3115E+ 01
.3149E+01 17
.1701E+01
.15581+01
.3427E-vi
.1428E+01
.15 b JE+ C1 g
18
.3 4J6 E+0 0
.71571+00
. 29 5 3E-C 1
.E942E+03
. 727 7E* 0 0 w
19 3773 E+0 0
.3055E+00
.142 EE-b i
. 3156E + 0 0
. 3159E + 0 0 20
.1155 E+0 0 8882i-01
. 29 91E-G 2
.92 C4E wi
.9294E-01 E'E GB W
Table QCS760.10-11 (continuea; PEL.ET W3RT4 DISTRI3UTIO4 LT EO C 4 (DEL K/KG X10' *5)
CH ANNEL 4XIAL NO3E 1L 12 13 14 15 1
4725E+00
.4810E+00
. 379 2E+C 3
'. 4141 E+ 3 3
. 42d 2E& G 0 2
14JZ E +01
. 14211+01
.114 8 E+ 01
.12 56E+01
.1267E+01 3
.2 582 E+01
.26165+0i 213 3E+ ti
.2335E+Li
. 2 34 9E
- 01 4
4063E+01
.*261E+01
.3651E+Li
. 35 71E+ 01
. 36 6 *E+ 01 5
.5 613 E +01
.58591+01
.5 06 2c+01
. 53 49E+ ui
. 5362E+ 01 6
.7 2 54 E+01
. 755 7I + 01
. 65 5 2E+ C i
. 6914E+ di
.6926E+01 l
43 7
4 743 E +0 i
.93951+01
.7890E+ti
.83 26E+ 01
. 8 33*E+ 01 O
8 5115 E +01
.9634E+0i
.3 3 a 4E + 01
.2629E+bi
. 88 33E
- J 1 l
M 9
.9 72i E *01
.1327I+02
. d 9 3 4E+ 01
.9410E+G1
.9410E+t1 10
.3 8 u) E +01
.10 3 5E + 0 2 9C3dE+01
.94t8E+Ci
. 948 5E* 01 g
11 635sE+01 93E1E+01
.8597E+01
.93 53E+ ai.
. 93 4dE+ 01 j,
12
.E 413 E+0 i
.8566E+0i
.7748E+01
. 815 5E+ 01
. 814dE* 01 oo 13
.5 045 E+01
. o663E + 01
. 7 544E + 91
.7975E+31
.796sE+01 14
.6 3I+ E+01 683 5E + C 1
.5961E+G1
.63C5t+Ci
.629dE+01 15
.4 60r E+01
. 439 2i + C1
. 419 5E+ d i 4463E+C1
. 447 7E+ 01 16
.31*L E +01
. 310 3E
- 01
.2 63 3E+b i
. 26 3 3E + Ji
.28 2 70+ 01 j
l iT 154L E+W 1
.1405E+01
.113JE+01
.12 49E+ 01
.1242E+01 i
18
.F 114 E +0 0
.6749E+00
.5 47 5E+ 6 0
.6350E+0C
.599dE*00 19
.3043E+00
. 33 24E +0 8
.2476E+C0
.2F22E+00
.266dE+ 00 20
.2 762 E-01
.e625E-01
. 76 8 2E-G 1
.4318E-C1
. 8141E-31 i
I C
GT a"
'l j
i Table QCS760.10-11 (continued)
PEL.ET W3RT4 DISTRI3UTI ON A T Eock (DEEK/ KG X10* *5)
CH A NNEL AX1AL NODE 15 17 13 19 23 1
.364 E+00
.2162E+D0
.2 7 5 3E+ 0 0
. 2914E+ CQ 4129E* 0 0 l
2
.115F E+01
.65261+C0
.o7 27E+5 0 93 44E+ Sa 1244E+01 3
.2145 E+01
.1315E + 01
.1663E+01
.17 59E+ di
. 2 312E* 01 l
4 3 663 E+01
. 260 61 + 01
.3 097t+C 1
.3L50E+61 3 771E
- 01 j
I 5
.5 07t E+01
.372RI+0L
.4 3 5 6E+ 61 44L1E+st
.519sE+di 6
.6565E+0i 45'J 5E + 01
.5685E+Ci
.!T29E+G1
.6705E*01 7
79 03 E +31
.5344I+Di
.6673E+C1
. 63 28 E+ 01 808uE+01 8
.t395E+0i
.6327E+01
.7 24 EE+ G 1
. 7212 E+ 01 8 42 2Et Ji 9
.E 9 *! E+01
. 675 3E +Di
.77 2 SE+Li
.7774E+J1
.5987E+Si 57 10
.i G 14 E+01 6315I + 01
. 77 93E+ J 1
. 75 4 8E+ J1
. 9G 7 2E 6 G 1 11 6603E+01
.6506I+01
.7 44 7t+61
.7456E+st
.866tE+01 as 12 7 7%) E+0 i
.58631+G1
.6 71 EE+ G1
. 67 59E+ di
.7822E+01 13 7 543 E+31
.54581+01
. 63 3 34+ s i
.6412E+01
. 7 512E* 01 2$
14 5 953 E +J i
.42591+01
.49 67E + J 1
.5G49E+bt
.5963E*01 5
15 419?E+0i
.30165+0L
.3533E+01
.3646E+G1
. 43 8 7E+ 01 16
.2 62P E+01
.195 2E + 0 L
.23cvE+Li
.2433E+di
. 30 3 3E+ G 1 17 1125E+J1
.6968E+00
.1 C7 5E + C 1
.1212E+ C1
.1495it01 18
.544) E+0 0
.4537i+G0
.5393E+33
.1120E+ C 0
. 70 3 3E
- 00 5
3J7 E*06 19
.2453E+0C
.21191+00 25 C 4E+ 0 3
. 28 41E + C U 20
.7 564 E-01
. 68581-01
. 9181E- 01 l
I er r cr a i
_. P-b$
n Table QCS760.10-11 (continued)
P EL.ET W3RT1 DISTRIBUTION AT EOC4 (DELK/KG X1G+*5)
CH ANNEL 4XIAL NOSE 21 22 23 24 25 1
.3 0 TT E+0 0
. 414 4E + 00
.2 9 38E+ G O
.2779E+C0
.218CE+00 2
.9 763 E +0 0
. 12 461*01
.9 3 92E + 0 D
. tT 77E+ 00
.698 3E* 00 3
A 865 E+01
.2314I+C1
.1161E + 01
.16 76E + G1
.134JE*01 4
.3193 E +01
. 377 3E +G 1
. 315 9E + G 1
. 31 C 6E+ G1
.2614EtG1 1
5
.4443E+0i
. 5191E + 0 i
.4411E+01 43 69 E+ 01
. 3 732E* 01 6
6 773 E+01
.6705I+01
. 57 39E+G 1
.5657E+01
. 49 0 5E* 01 I
ja 7
.6 982 E+31
.o3781+01
.6937E+01
. 66 2 4E+ 01
.5954E+01 I
v) 8
.7 325 E+01
. 84161 + 01
.7 289E+G1
. 72 56E+ 01
.6335E+01 5
9 J 8 2* E+01
. 895 0! + 01
.77 8 tE+G1
.77 36E+ G1
. 675 5E* 01 f'
10
.7 903 E+01
.9365E+0i
. 7 852E+0i
.7e(4E+G1
. 68 2]E+ 01 11
.7 5 61 E +01
.6660E+31 7499E+01
.745JE+01
. 65 0 iE+ C 1 d3 12
.6 835 E+31
. 7614E + 0 L
.6765L+01
.6717E+01
.5863E+c1 c) 13
.6 52S E +01
. 75 0 61 + 0 i
. 6412E +b i
. 63 3 3E+ 01
. 5458E+ 01 14
.5193 E +01
.59581+G1
.5 "4aE+01
.43 65E+ 31
.425 tE+ G 1 15
.3 815 E +01
.4383I+01
.3644E+01
. 35 31E+ 31
. 3J 14E* 01 16
.2 60Z E+01
.3029I+01
. 2 431E+01
.2346E+=1
.19 5 3E+ 01 17
.13 33 E+81
.14911 +01
.1 113E + d i
.1G73E+J1
.8954E*00 18
.6 705 E+0 0 7001E*00
.6 31 CE+ 0 0
.53 76E+ dJ
.452EE*00 19
.3 093 E+0 0
.3354I+00
. 2 8 23E+ 0 0
.24 52E+0J
. 2111E+ 0C 23
.9 711 E-01 90701-01
.6943E-G1 79 31E-31
. 6 81J E- 01 i
I Er F ci a" h3 i
I l
Table QCS760.10-11 l
s (continued) l i
P EL.ET W3RT4 DI STRI3 U 1[ 0g A T EOC4 (DEL K/MG X i&* *S) t CH A NNE L l
4XIAL NO3E 25 27 26 29 3J 1
.1765 E +0 0
.19 29E t G 0
. 2 :30 tE+C 0
. 20 0 9E+ 33
.153 6E+ 00 2
.5 791E +0 G
. 62 94i + 0 3
.6 5 2 2E+ 0 3
.E524E+ba 542dE*0G 3
.112L E +0 i
.1222E+01
.1263E+Li
.12 64E+ G1
.10 50E+ 01 4
.2195 E +01
.2255E+01
.23J3E+C1
. 23 L 96+ si
. 2259E+ C1 5
315,E+31
.3204E+01
.3 271L+01 32 73E+ Ji
.32JdE+Si 6
.416+ E+01
.4214E+01
.4 2 s 7E +01
.4299E+J1
. 4219Et G 1 i
IS 7
.5 07L E+01
.5127I+01
.5 227E+ui
. 52 28E+ J1
.5132E+Ji i
O 8
.5 413 E +01
.5456E+0L
.55 61E+ 01
. 55 62E+ Ji
.5460E+ J1 8
9
.5 7 93 E+3 f.
.5837E+01
. 5 9 50E+G 1
.5951E+J1
.5541E+ G1 10
.5 8 53 E +31
.5902i+01
.6 G13E+ C1
. E; 2 0E+ 11
.5905E* 01 j) 11
.5 595 E+01
. 564 4E + D i
.576;E+31
. 57 6 0E + ci
.5646E+01
]
g 12
.5 0 45 E +31
.5395E+01
.520tE+01
. 52 C6E+ 21
.5096E+01 13 4693E+01
.4773E+01
. 4 3 5 4E+C 1 45S4E+J1 4773E*G1 l
i 14
.3 685 E +01
. 3768E + 01
.3 8 76E + U 1 36 78E+ 01
. 3767E+ 01 15
.2 643 E +01
.2737E+01
.2332E+21
.2831E+J1
.2736E+C1 1
16
.17 45 E +31
.1633E+01
.19CsE*01
.13 67E+ C1
.18 3 2E + 01 l
17
.: 235 E+0 0
.9226I+00
.970tL+G0
. 97 0 0E+ 00
.9217E+ CD 18
.* 26? E +0 0
.4790E*00
.504SE+00
. 50 46E+03 478 2E+ 0 L 1
19
.2 0 2f E+0 0 22791+00
.24J3E+03
.E4 tid +G'J
.2274E+00 2C 5 716 E-01 753 CE-01
.7 3 2 4L-01
.7b57E-;1
. 7494E- 01 4
GT B" i
l i
e QCS760.10-ll (continued)
. P EL. ET ORT 4 DISTRIBUTION AT EOC4 (DELK/KG X10* *5)
CHANNEL 4XIAL NO3E 3L 32 33 34 35 i
.179e E +0 0
.2073I-01
. 2 C74E-61
. 2L 18E-C i
. 214 5E- 01 2
.5 815 E+0 0
.61071-01
.51. 6E-01
.53tSE-ui
. 4967E-C1 3
.1125E+01
.169 3E + 0 0
.15 5 3E + 0 3
.15 74E+ 00
.162 7E+ 0 G 4
.2 205 E+31
.2260i+00
.1697E+C0
.1301E+ad
. 219 5E+ 0 C 5
.3163 E +01
.5231I+00
.5174E + 0 0
. 5L 74E+ GJ
.596 E+ 00 6
4171 E +01
.c570i+DE
.68a9E+JG
.86CSE+00
.1015Et 31 R
7
.5075E+01
.1173I*01
.122 2E+ G 1
.12 2 2E+ 51
.139dE* *J1 8
.5 425 E+01
.10 9 2i + 01
.1136E+0i
.1138 E+31
.12 7 4E* 01 i
g 9
.5 797 E+01
.12 3 Ji + 01
.1276E+01
.12 t GE+ J i
.1.424E+ C1 10
.585FE+41
.1258I+G1
.133tE+G1
.13 C 8E+ J1
.1445E+01 o
11 e5593E+01
.1175E+01
.1215E+ 31
.12 22L+J1
.1348E + 01 d3 12
.5 045 E+01
.'987Gi+00
.102?E+G1
.1L 29 E+ 31
.1131E t G 1 13 4 690 E+01
.1117I+01
.116 4E + C 1
.itE3E+hi
.13 3 2E+ 01 N
14
.3 66+ E+01
.7745E+00
.7917E+0J
.79 L 2E+ 00
.877 3E+ 00 15
.2 64T E+u t
.4401E+00
.4256L+ 0
. 42 33E+ 00
. 459 5E+ 0 0 16
.17*!E+01
.1655i+00
.12 24E + C 3
.1108E+G3
.1163E+0C 17
.3224E+00
.1222i+00
.8 5 5 3E-01
.8351E-J1
. 9 764E- 01 18
.4 253 E+0 3
.3683i-01
.2440E-01
. 2167E- 01
. 279 JE- 01 19 202tE+00
.6345I-02
.2 3 G CE-0 2
.19 53E-u2
.405 3E- 02 20
.666)E-01
.3364I-02
. 2 4 41E-0 2
. 22 485-d2
. 22 4 5E- 0 2 4
qg
s Table QCS760.10-11
~
(continted)
PEL.ET W3RTH DI STRIB UTIO1 AT EOC4 (DELK/KG x1G'*S)
Q1 ANNEL 4XIAL NODE Ji 37 38 39 43 2 213 E-01'
. 26 971-01
. 5 747E +c 0
.2432E-91
. 2 716E- 01 1
4 862 E-01
.6430E-01
.17 4 3E + 01
. 49 ( 6E-s i
. 6 212E- 01 2
1534 E+0 0
.18561+00
.3234E+C1
.15 35E+ CJ
.186 9E + 0 C 3
2145E+JD
.2425E+00
. 49 3 0E + G 1
.1316 E+ 60
. ib5 'E+ 00 4
5 987 E +0 C
.6137I+00
.6651E+01
. 52 C9E+ JJ
. 5 231E* 0 0 5
1015 E+01
.13181+01
.b 912E + c i
. 92 55 E+ C0
.9155E+00 l
6 1403 E+01
.2392i+0i
.1079E+G2
.12 98E+ J1
.1268E+ 01 l
7 1265 E+31
.12675+01
.1166E+ C 2
.12 0 3E+ 21
.1164E+01 8
1435E+01
.1411E + 0 i
.124 5E + C 2
.13 46E+.1
.1299E+01 g7 9
1464 E +31
.143 5E + 0 i 1256E+02
.13 66E+ ;1
.1313E+ G1 1C g
13 64 E +01
.1337I+01
.1195E+32
.12 61E+ 01
.122 dE* 01 m
11 1151 E+01
.1130i+G1
.10 71E + 0 2
.1237E+J1
.1013E+01
?
12 1315 E+31
.1300E+01
.1107E+02
.13 3 6E+ ;i
.1334E+ 01 13 886!E+00
.8726I+0G
.7855E+ei
. tS t 1E+ C3
.8886E+ CD j3 14 459FE+00
.4401E+00
.5516E+C1
.4049E+GG
. 445*E+ 0G i
15 10 37 E+0 0
.46431-01
. 3 454E+ L i
.5663E-61
.5358E-Di 16 7 84F E-01 22141-01
.1713E+ J 1
. 37 67E-C i
.1147E- 01 17 1953E-G1
.2883!-01
.8 6 3GE+G G
.55 24E 62
. 2613E-Ei 18 1423 E-0 2
.1400E-01
. 4 611E+ 0 0
. 23 56E-J2
.1410E-C1 19 1825 E-0 2
.14505-02
.2 o 2 0E-C 1
.75 c3E.3
. i T6 6E- 0 2 20 h
ra"
Table QCS760.10-ll (continued)
PEL.ET W3RTO DI STRI3UTICS AT E0C4 (DELK/KG XiC**S)
CHANNEL 4XIAL NO3E 41 42 43 44 45 1
.2 935 E-01
. 2844I-01
. 6 3 4SE+C J
.15t1E-;1
. 865 8E- 02 2
.6 7 2) E-01
.59511-01
.17 9 FE+ u i
. Eb 28E-C1
. 4%C 3E-C2 3
.1965 E+0 C
.17 0 8i +0 0
.326iE+C1
. 94 2 8 E-Li
. 44 66E-01 4
.id9sE+00
.1633E+00
. 4 9 71E+ C1
. 75 59E-Li
. 5816E- 01 i
5
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.5276I+00
.6886E+01
.4007E+03
.323cE+00 6
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.9242i+30
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.76C6E+uo
.620 JE+ 80 7
.1265E+01
.12881+0i
.1040E+02
.13 91E+ J i
.8919E*00 l
f3 8
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.118 7I + 0 i
.116 EE + 0 2
.1C G6E+Di
.8423E*06
%3 9
.1296 E +01
. 1326I+01
.124 4E + 3 2
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.9451E*00 13
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.12 5 4E+ 0 2
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.9636E+00 11
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. 895 2E+ 0 E 1
5) 12
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.106 5E +0 2
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13
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.6293E+00 15
.4 381 E+0 0
.3866I+03
.5531E+0i
. 3125E + 03
.3323E*00 16
.4 35F E-01
. 328 0E-01
.3431E+GL
. 25 GT E-u2
. 3 73 7E- 01 17
.2 06f E-01
.13671-01
.165CE+Ci
. % 20E-02
. 2 0 3 4E-J i l
it
.2 963 E-01
.66391-02
.8 C8 CE+u 0
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. io 2 4E- 03 i
19
.14 56 E-01
.65$8I-02 4132E+ 0 J
.56786-L2
.327(E-02 20
.1813 E-0 2
.1767I-92
.2664E-01
.3550E-03
. 2 32 5E- 0 3 l
1 1
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Table QCS760.10-ll (continued) i PEL.ET W3RT1 u1 STRI3uTION A T EOC4 (DELK/KG X1C' *5)
CHANNEL 4XIAL NO3E 45 47 1
.6 9 65 E-0 2
. 1723I-01 2
.459TE-92
.27145-01 3
.4 5 03 E-01
.9588E-01 4
.5 6 *i E-01
.77311-01 5
.3245E+00
.43161+0S 6
.5205 E+0 3
.7613E+00 I
7
.292!E+00
.1J91E+01 6
- 4 403 E+0 G
.10J5E+01 x3 Sl 9
.3425E+0e
.112 7I + 01 y
10
.3601E+06
.11451+01 P
11 0925E+04
.10581+01 12
.7 45) E+0 0
. 670 6E + 00 a
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13
.3 5 75 E+0 C
.2144E+01 14
.6285E+00
.7172i+00 15
.3 015 E +0 6
.3103E+00 16
.3675E-01
.30445-03 i
17
.1995E-01
. 76401-02 18
.4193 E-0 3
.71605-02 l
19
. 3 394 E-0 2
. 615 2E -0 2 l
20
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. 56091-03 l
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Table QCS760,10-12 CRBRP E0C4 REGIONWISE REACTIVITY WORTHS SUP91ARY (Netak/k)
Lower Axia11 Upper Axiall Lower Axia12 Upper Axia12 Parameter Fuel Inner Blankets Blankets Blankets Extensions Extensions 1
Flooded Doppler
-7.9482-4
-1.4936-3
-l.6588-4
-6.0106-5
-1.3400-4
-5.3886-5 Volded Doppler
-5.1221-4
-1.1314-3
-1.341 3-4
-4.5993-5
-1.2324-4
-4.8144-5 i
Sodita Void
+4.7522-3
+5.5325-3
-7.0104-4
-7.0716-4
-2.7978-6
-5.9951-5 Steel
-2.4829-2
-1.5961-2
+1.4943-3
+1.8212-3
+6.3656-5
+2.4625-4 l
B l
10 Pellet
+3.7824-1
-4.1285-2
+2.1507-2
-1.1794-2
-9.6522-4
-5.5480-5 I
8g' e*
(1) Above and below core (2) Above and below inner blankets l
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FIGURE QCS760.10-1 :
CRBRP ASSEMBLY (CHANNEL)
NUMBERS 120' SYMMETRIC CORE SECTOR 31 25 31
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15 46 28 j
46 15 21 47 47 21 27 22 12 12 22 45
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6W FIGURE QCS760.10-2 AXIAL N0DE '
7.069 cm > Upper, Blankets: 35.74 cm.
3':0 POSITIONS (H0T-FULL-POWER
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' DIMENSIONS)
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QCS760.10-98
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g QCS760,10-99 Amend. 69 July 1982
Pego 1 (2 2-0417) #112 Ouestion CS760.36 Concerning the potential sodium / water reaction, the steam generator design considers only a design basis leak consisting of a single tube, double-ended gulilotine rupture of a steam tube followed by two additional single double-ended tube guillotine ruptures, spaced at 1.0 second intervals, a.
From the very closely packed CRBR steam generator tube arrangement, with one tube surrounded by six adjacent-tubes, if one steam tube was a double-ended rupture, the six adjacent tubes can be involved.
Please discuss this case and include your analysis.
b.
In the three tube ruoture model, the f ailures of second and third tube follow at 1.0 second intervals. The effects of this assumption are essentially the same as for a single tube rupture model.
Furth er substantiation as to why adjacent tubes can't rupture at the same time is needed.
c.
What is the response to three simultaneous tube ruptures instead of three staggered ruptures?
d.
The TRANSWRAP results in the PSAR show the initial pressure pulse f alls to burst the rupture discs. The peak pressure in the IHX is 331 psia and the design pressure for the lHX tubes is 325 psig.
If more than one tube ruptures at the beginning, can the initial pressure pulse burst the rupture discs? What will be the pressure history in the IHX?
e.
The steam generator tube bundle is welded to the tube-sheets.
During the Na/H2O reacti ressure pulse shSeb*riIku8e ihe mosf af fected.pe of the tube bunhlethe tube sheet im a t h de stick sha t
Ifthe1owertubesbeetfalIs,can't the water pour into the shell-side and provide f urther sodium / water reaction offects?
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QCS760.36-1 Amend. 69 July 1982 n&4vms
Page 2 (t:2-0417) #112 Resoonse a.
Double-Ended Guillotine (DEG)
DEG f ailure of a steam generator tube is not a credible event.
It is raiher a convenient and conservative definition on which to base a calculation.
Because conditions are not uniform around the initial tube f ailure, the adjacent 6 tubes will not all be equally af fected. Typically, the initial f ailure will be the consequence of a local ef fect in the tube wall which results in a directional f ailure that restricts the reaction zone f or potential overheating of adjacent tubes to those tubes that f ace the initial failure.
Stati sti cal ly, tubes are observed to f all to less than one DEG and to f all asymetrically so that f ewer than six adjacent tubes would be subsequently involved.
The Design Basis Leak (DBL) is derived from analysis of bench scale and large leak test data.
Bench-scale tests have led to the understanding of how typical small leak progression occurs in the steam generator tube wall. Figure 15.3.3.3-1 in the PSAR Illustrates a typical development of a leak within a steam generator tube. These tests have shown; (1) that a smaljIbm Hinitial leak progresses, resulting in a leak rate o 10-0/sec within two hours, and (2) that a leak of 10-pIbm H 0/sec magnitude can produce wastage rates of 2
9 0.001 to 0.005 Inches /second on target material.
Large Leak Test Reg (LLTR) Series ll Test A3 was a leak progression test initiated by exposing a pre-drilled 0.0013 in2 hole simulating the self-wastage leak Indicated in Step 5 in Figure 15.3.3.3-1.
This initiator produced a wastage f ailure in a tube.wo rows away af ter sixty seconds. The f ailure area was less than 0.017 in2 as compared to the CRBRP SG tube cross-sectional flow area of 0.13 in2 Conservative aspects of this result are:
(1) the initiator was aimed and spaced to produce the maximum wastage rate on the target tube *, (2) the sodi um was initially static, and (3) the target tube contained initially static water. The l eak f rom the 0.017 in2 f ailure produced a wastage / overheating f ailure in the thin-wal l (0.025" compared to 0.109" prototypic)
Injection tube within 25 to 37 seconds. The flalure area in the injection tube was measured post-test as 0.125 in2,
- The target distance (two rows away) was previously determined by bench scale experiments to yield the maximum wastage rate on the target tube.
QCS760.36-2 Amend. 69 July 1982
Page 3 (W82-0417) #112 Within 18 to 23 seconds af ter the injection tube f ailure, three tubes failed due to a combination of wastage / overheat!ng, undercooling, and overpressure.
The latter two ef fects were conservative in that the initially static, subcooled water in the tubes was vaporized and expelled into the water supply system and the pressure in the tubes rose to 2400-2600 PSI prior to failure These three failures were determined to be 0.1, 0.20 and 0.17 in Japanese large leak tests results have shown that (1) Intermediate sizeleaksproducedsecondarywastagefailureswithintensofseconds:
failure areas were 0.005 to 0.05 in, and (2) DEG leaks did not produce secondary failure.
Based upon LLTR and foreign data, a plausible leak progression can be developed for the CRBRP steam generator. Taking the representative leak progression sequence illustrated in Figure 15.3.3.3-1 and assuming (1) a leak magnitude equal to or greater than that Indicated in Step 1 of the progression depicted, (2) that this leak does not plug, and (3) that this leak and resultant leaks escape operator action, a plausible sequence is as follows:
1.
Within two hours the leak has enlarged as shown in Step 5 of the progression depicted.
2.
The enlarged leak produces a wastage failure in another tube af ter more than one minute. The area of this first secondary failure is 2
0.005-0.05 In 3.
The total water injection rate of about one Ibm /sec results in burst of the expansion tank rupture disks (150 PSID) within a few minutes.
The event is then terminated by isolation and blowdown of the three steam generators in the affected loop.
4.
It is conceivable that additional wastage failures could occur during the few minutes in which system pressure is increasing to the rating of the expansion tank disk.
Given (1) that a water leak produces a turbulent diffusion flame which is itself situated in a turbulent flow field of high-conductivity, high-heat capacity liquid sodium, and (2) observed wastage failure areas, the size of these potential additional failures would very likely be comparable to the first secondary failure. These potential secondary failures would simply shorten the time to burst of the expansion tank disk. The sequence described above is considered to represent a conservative, plausible leak progression scenario.
In order to defino a clearly conservative DBL (which is not Intended to represent either a plausible or mechanistic sequence),
it is necessary to include burst of the SWRPRS rupture disks (325 PSID).
A rapid Equivalent Double-Ended Guillotine (EDEG) failure serves analytically to burst the SWRPRS disk and also to cor.servatively bound the failure magnitude. The DDL is defined as follows:
QCS760.36-3 Amend. 69 July 1982
Pag 3 4 (W82-0417) #112 2
An Equivalent Double-Ended Gulllotine (EDEG) failure (0.26 in ) of a steam generator tube followed by two additional EDEG tube failures. The two additional EDEG failures occur as follows:
One additional EDEG failure occurs at one second after the initial EDEG failure.
A second initial EDEG failure occurs at two secon'ds after the initial EDEG failure.
This sequence of three EDEG failures occurs after an Intermediate-size leak (less than a DEG) from a steam generator tube has increased local pressures in the IHTS to the threshold of SWRPRS rupture disk burst.
The CRBRP DBL is conservative in both the magnitude of and the timing of secondary failures, compared to the conservative plausible leak progression scenario presented above.
b.
A tube failure mechanism already introduced into this discussion is a precursor tube leak, leading to an adjacent tube material wastage /
overheating, subsequently leading to pressure rupture of a tube.
Figure 760.36-1 shows an array of tubes in cross-section where tube "p" (precursor) is postulated to have an undetected material or manufacturing defect which eventually produces a leak which escapes operetor action and causes wastage / overheating on one or more adjacent tubes. The shaded area l
depicts a potential leak Jet, the other surface of which reacts with sodium and thereby develops a high temperature (theoretically as high as 2700 F, measured as high as 2200 F in LLTR tests). The source temperature for the overheating is greatest at the reacting Interface between the water and the sodium, and less away from the reacting Interface.
As the surface of the jet Impinges upon the tubes the tube material heats up locally.
Fluctuations in the geometry of the jet and the reacting interface during this dynamic event will mitigate the wastage of the adjacent tube but may be insuffIclent to prevent the metal temperature of an affected tube from rising locally to the point at which the tube wall is too weak to withstand the internal pressure and, therefore, ruptures.
Any one of the affected tubes could reach this condition first.
When the pressure rupture occurs, a new, larger water / steam Jet is created, with a different profile of tube impingement and localized material wastage / overheating. While the preceding smaller jet and localized material overheating profile may have raised spot temperatures on more than one tube, the pattern of localized overheating is immediately superseded by a new pattern caused by the new, larger water jet. The probability of an additional tube completing its localized wastage / heat-up to a failure temperature before the new overheating profile takes over is considered negligible.
(Such an eventuality would be conservatively imposed upon an event which is already extremely uniIkely).
In any case, two tube failures, both with plausible rupture areas of 20% of an EDEG l
l QCS760.36-4 Amend. 69 July 1982
Paga 5 (W82-0417) #112 tube failure, would.still be umbrellaed by the one EDEG tube failure recommended for the design basis event definition.
For added conservatism, it may be assumed the larger water jet and resultirg material overheating pattern, may, like the precursor jet and associated overheating pattern, be sufficiently stable long enough for rupture temperature to be reached on a nearby tube thereby resulting in an additional tube rupture. On the one hand, the larger jet Impinges on more tubes than did the precursor jet, thereby increasing the' probability of a failure.
On the other hand, the much larger jet is more turbulent and diffuse and less likely to permit the reacting surface of the jet to stay on any particular tube area long enough to ovc-heat it to failure. Of more significance than either of these points la recognitilon that the new, large jet and resulting sodium / water reaction create a rapidly expanding bubble of hydrogen which drives the sodium rapidly away from the tube rupture location.
This rapid movement of the sodium Interface substantially reduces the potential for a stable reaction zone on the stationary tube surfaces, c.
As discussed previously the CRBRP DBL is clearly conservative in both magnitude and timing of secondary failures. As such, the Project considers it inappropriate to evaluate the simultaneous tube ruptures.
d.
Referring to the footnote on Table 5.5-11 of the PSAR, the water injection history input to the TRANSWRAP calculation of the SWR DBL in the evaporator correspond to the following leak sequence:
Time (Sec)
Event 0.0 - 0.3 Water flow rate constant et 2.5 lb/sec (this represents the undetected moderate sized leak which has pressurized the system to just below the disk burst pressure - PSAR page 5.5-24b).
0.3 First Equivalent Double-Ended Guillotine (EDEG) break.
1.3 Second EDEG.
2.3 Third EDEG.
Referring to Figure 5.5-4A and page 5.5-28 of the PSAR, the sharp Increase in lHX pressure at 480 milliseconds corresponds to evaporator rupture disk j
buckling in response to the fIrst ED1IG at 300 ms.
Predicted peak pressure l
in the IHX is 331 PSIA as compared to an allowable
- range under emergency conditions of 400 to 760 PSIA.
(
l
- Based on ASE Code Case 1331-8 primary membrane stress eriterIa.
QCS760.36-5 Amend. 69 July 1982
Prge 6 (W82-0417) #112 As discussed previously the CRBRP DBL is clearly conservative in both magnitude and timing of secondary failures.
As such, the Project considers it inappropriate to evaluate more than one tube rupture at the l
beginning.
e.
The results of the analysis of the Na/H 0 reaction predict that the 9
maximum pressure, 365 PSIA, occurs on the upper tube sheet. The pressure time history at this location is shown in Figure 5.5-4b.
The peak pressure at the lower tube sheet during this event is 348 PSIA.
The design pressures on the tubesheets are 325 psig on the sodium side and 1900 to 2400 psig on the water / steam side depending upon the tube sheet location and whether the unit is an evaporator or superheater.
Since l
these Na/H 0 reaction peak pressures would be enveloped by the design 9
pressure dif ferentials across the tubesheet, these loadings can be accomodated with the same degree of structural reliability as normal operation.
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QCS760.36-6 Amend. 69 July 1982
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PnECURSOR LEAK "P" PRODUCES JET WHICH HEATS ADJACENT TUBES Figure 760.36-1 Amend. 69 QCS 760.36-7
TABLE 5.5-11 CALCULATED RESULTS FOR LARGE SWR DESIGN BASIS LEAK
- IHX FAILED PUMP PEAK PEAK PRESSURE IN ADJACENT TIME TO FAILURE PEAK UNIT PEAK PRESSURE STEAM GENERATORS, PSIA CLEAR FIRST RELIEF LOCATION PRESSURE PRESSURE PSIA 9 SEC.
9 SEC.
LINE, SECONDS PSIA 9 SEC.
PSIA 9 SEC.
EVAPORATOR SUPERHEATER Evaporator 331 395 373 320 337 4.24 0 0.412 0 0.420 9 0.436 0 0.391 0 0.364 Superheater 304 333 311 254 3.65 9 0.311 9 0.548 90.619 0 0.438 Y'
E
- Water injection rate = 2.6 lb/sec (evaporator) or 2.2 lb/sec. (superheater) for 0 < t < = 0.3 sec (Precursor Leak).At t = 0.3 sec, one EDEG occurs. At t = 1.3 sec., one additional EDEG occurs.
At t = 2.3 sec., one more EDEG occurs.(total 3 EDEG) l h
C48 W
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P;ge 5 (82-0358) [8,22] #93 Ouestion CS760.110 The pump head provided by the various main feedwater and auxiliary feedwater pumps will vary with mass flow rate and pump speed.
What are the relation-ships? Are hariologeous pump curves avellable?
Resoonse The main (steam generator) feedwater pumps are designed to operate at constant speed. The design speed is 3579 RPM for each of the three 50% capacity motor-driven pumps. The predicted constant speed characteristic curve at the design speed for these pumps is shown in Figure CS760.110-1. These pumps are not saf ety-related, see Section 10.4.7.1 of the PSAR.
As such, the applicant will not specifically update this information if changes are made to this technical Information unless requested by the NRC.
The AFW pumps are designed to operate at a constant speed. The design speed is 3560 rpm for the two motor-driven pumps and 4000 rpm for the turbine-driven pump.
The predicted constant speed characteristic curves at the design speed for the motor-driven and turbine-driven pumps respectively, are provided in PSAR Figures 5.6-10 and 5.6-11.
l l
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QCS760.110-1 Amend. 69 July 1982
Figure CS760.110-1 STEAM GENERATOR FEED PUMP iiEAD - CAPACITY CURVE 0000
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O 1000 2000 3000 4000 5000 6000 7000 8000 9000 10000 I!OOO TOTAL FEEDWATER FLOW IN GPM EE CURVE A ONE PUMP OPERATION G{
CURVei B: TWO PUMP OPERATION G'
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ptge - 2 (8,22) M6 5.6.1.2.3.2 Auxillarv Feedwater Pumos (AFWP)
The AFWP will be a multi-stage, centrifugal pump selected from a commercial vendor's equipment line.
No special requirements should be necessary since these pumps have been proven to be rollable in commercial applications. The
. turbine driven pump will be sized to deliver a 1432 GPM flow rate at 3927 feet l
developed head, and the two motor driven pumps will be sized to deliver one-half of this flow rate each at the same head. The predicted constant speed head / flow curves for the turbine driven and motor driven AFW pumps are shown on Figures 5.6-10 and 5.6-11 respectively.
These motor drives will tw synchronous speed squirrel cage Induction motors of 980 horsepower.
These mo.~
wilI be selected from a vendor's standard Iine and no special requirements are anticipated.
AFWP Turbine Drive This component will be obtained f rom an experienced vendor and will be sized to produce 1960 horsepower. The turbine will be constructed with sufficient quality assurance coverage to assure its reliability during service.
The auxiliary feedpump turbine is not kept hot for quick start operation. The drive tu'rbine concept selected for the Auxiliary Feed Pump is based on the capability of this turbine to withstand severe service conditions.
This is I
accomplished by constructing the turbine wheel from a single forging with buckets milled into the forging.
The start-up procedure is similar to that for the RCIC turbine in a BWR in that it will occur without pre-warming.
Pumo Integrity The auxiliary feed pumps will be designed to the requirements of ASE B&PV Code, Section lil, Class 3.
In addition, the pumps and their supports will be designed to Seismic Category I requirements.
Allowable stress limits are specified in Table 3.9-3 and pressure limits are specified in Table 3.9-4.
5.6.1.2.3.3 Protected Water Storage Tank (PWST)
The PWST hotds the protected water to be supplled to the steam drums in the event of loss of normal feedwater or normal heat sink. The size is determined by detailed analysis of the heat removal conditions during the first several hours after shutdown and by anticipated component leakage rates. The tank will be constructed to the requirements for an ASE Section Ill/ Class 2 vessel i
and it will operate at low temperature (<200 F) and low pressure (<15 psig).
5.6-6a Amend. 69 July 1982
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