ML19340A137
| ML19340A137 | |
| Person / Time | |
|---|---|
| Site: | Oconee |
| Issue date: | 07/06/1967 |
| From: | US ATOMIC ENERGY COMMISSION (AEC) |
| To: | |
| References | |
| NUDOCS 8001100602 | |
| Download: ML19340A137 (12) | |
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@;)BCQAL E33 @N C 11 3 35I U. S. ATOMIC ENERGY COMMISSION DIVISION OF REACTCR LICENSING REPORT TO ADVISORY COMMITTEE ON REACTOR SAFEGUARDS IN THE MATTER OF DUKE POWER COMPANY CONSTRUCTION PERMIT APPLICATION FOR OCONEE UNITS 1, 2 AND 3 ADDENDUM TO REPORT NO. 2 h
' Note by the Director, Division of Reactor Licensing The attached report has been prepared by the Division of Reactor Licensing for consideration by the ACRS at its ' July,1967 meeting.
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@AJBCBAL 4133 @FJ 1.0 -Introduction During the June, 1967 ACRS meeting, the applicant, Duke Power Company, was requested to submit in writing answers to questions on various aspects
- M the plant design.
In our Report No. 2 to the Committee dated June 16,
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1967,.ce stated that we would comment on.these answers in a supplemental re-port and this addendum is su M '
2 to this end.
2.0 Amendment No. 5 Amendment No. 5 to the Duke Power Company's application for three units at itu Oconee Nuclear Station includes 11 answers to questions asked by the Committee and additional information to confirm commitments made orally to the staff. Our comments on the information submitted in Amendment No. 5 follow:
2.1 Cold Water Injection The results of an analysis of the thermal transient seen by the reactor vessel during safety injection after a blowdown were presented. Ductile yield-ing, brittle fracture and fatigue failure were considered.
The results of the analysis indicate no loss of vessel integrity due to the thermal transient during core injection. The details of the calculational procedure were not presented, however, and we cannot conclude that the problem pproach
.is finally resolved. We are engaged in reviewing the Westing s
to'the analysis of this problem and expect to meet with B&W in tue future for a similar detailed review.
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2.2 Solutions ~ to the " Steam Bubble" Problem The applicant has acknowledged the possibility of core floeding being prevented by formation of a vapor lock or " steam bubble" between the core and a wa ar leg in the steam generator after a cold leg pipe' break. Two methods
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of relieving hot l leg pressure to the cold leg have been proposed as solutions to this problem:
(1) check valves located on the Core Support Shield which would be held closed by higher pressure in the outer annulus during pump oper-ation or tatural circulation, or (2) a rupture disk which would be designed to blow cut under internal steam pressure but' which would withstand the ex-ternal operating pressure differential. We understand that the appl cant prefers the check valves at present but that alternate means will continue to be studied as the design progresses. The check valves would be designed and supplied by-'a valve manufacturer with. experience in the use of check valves requiring similar specifications. The present conceptual design would use several' check valves with a maximum flow area of 10 ft These would open on a pressure-difference of less than 1 psi.
At 3.5 psi (at which point the core would be 1/2 covered) about 1500 lbs of opening force would be applied to a.24-inch valve.
We believe that the check valves proposed would provide an acceptable solution' to the steam bubble problem. Other potential problems arise, however, l
because of the use -of these valves which must be considered in the design.
j (1) The Core Support Shield must be locally strengthened to compensate for
_the_ removal of material.
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.@ u PQC0 A L U $ 2 @ Nts f (2) The forceful opening of the valves against the reactor vessei during blowdown must be considered.
(3)
The consequences of loss of a valve must be evaluated or the design must provide assurance against such loss.
(4) The effect on normal operation must be considered, particularly any, possibility of bypassing or short-circuiting the core during pu=p operation or nar.ur al circulation.
(5)
The valves must be capable of test and inspection.
We believe that the above problems are all capable of solution and that the present proposal could resolve the steam bubble problem.
2.3 Blowdown Forces on Reactor Internals The applicant has proposed that the stress levels to be met in the anal-ysis of. blowdown forces on reactor internals correspond to the minimum speci-fication yield strength value specified in Section III of the ASME Code.
For stainless steel the basic allowable code stress intensity (Sm) is 90% of yield stress at temperature (for carbon steel Sm would be 2/3 yield strength at temperature).
The applicant has stated that the design stress levels are conservative but it should be pointed out that the conservatism lies in the stress-limits set by the code rather than in the applicant's use of them. While some defor-mation is expected at the stress level _ corresponding to the yield stress, gross deformation would not be expected since the deformation at the yield stress corresponds to a strain of only 0.002.
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Based on our analysis of the applicant's proposal, we conclude that the proposed stress limits are acceptable since (1) they are being used for the will not have continuous high stress levels b
design of vessel internals whie rather than on the pressure barrier itself, (2) conservative margins are inherent in the stress levels specified by the code, and (3) the loadings are not expected to be applied more than once, in the service life of the vessel.
2.4 Maior Pine Break Within Primary Cavitv_
The applicant has stated that the primary shield pit could withstand the transient pressure resulting from an 8 ft break in the primary piping and has indicated that physical limitations, including pipe stops, would prevent a pipe break with area greater than about 4 f t We believe that with design. attention to physical restrictions within the primary cavity a pi e break larger than 8 ft can be ruled out.
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-2.5 Design of Submerged Weir in Intake Canal In Supple::ient 5 the applicant submitted the dimensions of the under-water weir to be placed in the intake. canal as well as the results of a stability analysis. Subsequently, at the request of the subcommittee we have asked Dr. Newmark to review the dam design from the standpoint of foun-dations, materials and earthquake resistance. We have obtained further infotmation from the applicant informally for this purpose.
Dr. A. J. Hendron of Dr. Newmark's staff will submit a report on the design of the underwater veir for the July-ACRS meeting on this application.
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@i10C0AL U$$ @NL/ -3. 0 Core Cooling Analvsis for the Spectrum of Breaks At the - request.of the subcommittee, we have held further discussions with the applicant on the ability of the emergency core cooling systems to cope with the full spectrum of primary coolant system pipe break sizes. The applicant had previously submitted, in the PSAR, a full analysis of the double ended rupture of the largest coolant pipe (14.1 ft break) and had also presented information on a spectrum of hot leg ruptures with respect-to system pressure and mass release during the blowdown.
In our previous reports to the Committee we have stated that the anal-ysis was not complete but that there was enough information available to provide assurance that the spectrum of breaks would be covered and that a construction permit could be issued. The applicant's continuing efforts in this area have resulted in more detailed information, particularly in the area of cold leg breaks and peak clad temperature.
In addition to the new data, as presented in this report, we have.
compared various calculations made by Westinghouse with those of B&W.
Table I-summarizes the more detailed information now available on the Oconee design for the spectrum of hot and cold leg coolant line breaks.
Information on the time and extent' of core uncovery and the pressure decay for the spectrum of hot leg breaks was presented in Figures 14-41 and 14-42 of the PSAR. A mass release of 310,000 lbs on Figure 14-41 indicates uncovery of the top of the core and the bottom of the core is uncovered at a mass re-lease.of about 400,000 lbs.
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@FFOC0AL U$2 bu:LY The information in Table I assumes that two accumulators ne initiated at 600 psi and that one high pressure pump functions.
The flow rate is varied as'a function of the pressure driving force. The pressure transient in the vessel is calculated without the effects of the accumulators and the injection water flow superimposed on this calculation. The applicant states that this is conservative since injection flow would condense steam in the annulus and lead to faster pressure decay and more residual water inventory.
The " mini-mum quiet level" indicated in the' table is an equivalent static core water level.
Although the applicant has not' completed the analysis and we have not completed our review, the information in Table I provides further assurance that the proposed design is practicable.
We have also compared the Babcock and Wilcox _ calculations for Oconee to calculations made by Westinghouse for the Indian Point II and Carolina Power and Light Reactors. These comparisons are presented in Figures 1 through 3 of this report.
Figure 1 shows the pressure decay for the three systems for a large cold leg break. The Indian Point II reactor is of similar size but of slightly lower average coolant enthalpy (575 Btu /lb vs 588 for Oconee).
The Carolinas reactor is smaller in coolant volume (9800 f t vs 11,800 for Oconee). The results of a comparison of the 3 ft break size was similar to that presented in Figure 1 for the 8.5 ft break.
The time to uncover the top of the core is presented in Figure 2 for the three reactors for break sizes ranging from 14 f t to 3 ft The core uncovery time is shorter for the Oconee case than for the Westinghouse reactors for the cold leg break.
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@M LY Figure 3 illustrates the major difference between the B&W and Westinghouse calculations. For the small break (about 0 5 f t ) the pressure in the Oconee reactor is calculated to " hand up" at a higher pressure and to retain a larget fraction of-the water inventory. Although both manufacturers use the FLASH code to calculate the blowdown transient, the Westinghouse calculation employs a constant steam-separation factor.while B&W varies the amount of steam sepa-ration with pressure. This assumption results, in the B&W calculation, in retention of a larger fraction of the water within the vessel and a higher vessel pressure.
The greater mass calculated to remain after blowdown is qualitatively substantiated by the results of LOFT semi-scale blowdown tests which resulted in substantially greater quantities of water remaining in the vessel than were predicted on the basis of the FLASH code with a constant steam separa-tion factor. We understand from B&W and from Phillips monthly report that a modification is being made to incorporate a variable steam separation factor in the Phillips calculational model.
Although our review of-the spectrum of breaks is not yet complate we believe that the results to date indicate a diligent effort by B&W and the applicant and that there is assurance that the analysis will be satisfactorily completed.
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4.0 conclusion The further information provided in Amendment 5 which verified oral-coc:mitments and amplified the previous submittals and the information obtained
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@FF0C0AL QI$E @NLY orally'on the spectrum of breaks analysia do not change our conclusions as set forth-in Report No. 2 to the ACRS dated June 16, 1967.
In. summary, we believe that the Oconee units can be built and operated without undue risk to the health and safety of the public.
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TA3tE I SPECTRUM OF COOLANT LINE BREAKS Mini =t=1-Positive Quiet Hot Hot Peak Moderator 1
eNak Level
- Spot Spot Temp.
(Full-
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Coolant (ft..above
. Uncovered Re-Covered Hot Spot Power -
(ft')
Locn Core Botton)
(Seconds)
(Seconds)
(*F)
Seconds) 14 hot-8
'4.0 17.5 1950 2.1 S.5 hot
-5.4 6.2 20.6 1700 3.5 cold
-7.5 5.0 22.3 1740 U
3 hot
.-2.3 17.6
'33.5 965 1.6 cold
-5.6 13.4 32 1320 U
. J hot
+4.7 790 1.42 cold
+4.0~
790 U
0.4 he
+12.1-1.4 cold
+6.9 730 0.05 cold
+12.3 1/ Hot spot at about +3'ft.
. 1/ Scram assumed.
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