ML19347D562

From kanterella
Jump to navigation Jump to search
Responds to NRC 810209 Request for Addl Info Re Fsar.Info Will Be Incorporated Into Next Revision
ML19347D562
Person / Time
Site: Wolf Creek, Callaway  Wolf Creek Nuclear Operating Corporation icon.png
Issue date: 03/20/1981
From: Petrick N
STANDARDIZED NUCLEAR UNIT POWER PLANT SYSTEM
To: Harold Denton
Office of Nuclear Reactor Regulation
References
SLNRC-81-017, SLNRC-81-17, NUDOCS 8103260613
Download: ML19347D562 (13)


Text

g ..

SNUPPS Storiderdiaod Nucieer Unit Power Plant System 5 Choke Cherry Road Nicholas A.Petrick vil land 20050 Executive Director March 20, 1981 SLNRC 81- 017 FILE: 0541 SUBJ: SNUPPS FSAR - NRC Request for Additional Information Mr. Harold R. Denton, Director Office of Nuclear Reactor Regulation U. S. Nuclear Regulatory Commission Washington, D. C. 20555 Docket Nos.: STN 50-482, STN 50-483, STN 50-486

Reference:

NRC (Tedesco) letter to J. K. Bryan and G. L. Koester, dated February 9,1981, Same subject

Dear Mr. Denton:

The referenced letter requested additional infonnation regarding the SNUPPS FSAR. The enclosure to this letter provides the requested infonnation and will be incorporated into the next revision to the FSAR.

Very truly yours, Eks C C Nicholas A. Petric (k RLS/srz Enclosure cc: J. K. Bryan UE G. L. Koester KGE D. T. McPhee KCPL T. Vandel NRC/ Wolf Creek Site W. Hansen NRC/Callaway Site \

- . 1 t

81032600/3 A

SNUPPS 331.0 Radiological Assessment Branch 331.1 Section 12.1.2.5.b addresses a neutron shield (12.1.2.5b) design at the RPV in containment. Please specify the neutron and gamma dose equivalent rates that will exist at specific locations within the various levels of containment prior to shield installation and after the shield is installed. A figure or table showing respective dose rates would be a suitable format. Describe your plan for neutron personnel dosimetry when-ever an entry is made while the reactor is at power, the frequencies at which entries are made, and the number of people making these entries.

RESPONSE

The neutron shield design for the reactor vessel cavity consists of a water bag shield located in the reactor vessel flange area above the hot and cold leg nozzles, as shown in FSAR Figure 3.8-61a. Based on this design, an average neutron dose rate at the top of the refueling pool has been calculated to be 1.8 rem / hour, using the Morse Monte Carlo code (Ref. 1).

Dose rates in other areas of the containment were estimated using Cain's Hypothesis (Ref. 2) along with actual dose rate measurements (Ref. 3) taken at the Farley Nuclear Plant by Lawrence Livermore Laboratories (LLL). The dose rate values obtained using this technique are given below.

Location Neutron Dose Rate (mrem /hr)

Equipment hatch 8-31 Personnel hatch 56 D. E. Hankins and R. V. Griffith (Ref. 3) of LLL found that l

the neutron-gamma dose rate ratio in the Farley containment l was 7:1. Based on this ratio, the SNUPPS gamma dose rates

! are expected to be as follows.

l Location Gamma Dose Rate (mrem /hr)

Top of refueling pool 260 Equipment hatch 1-4 Personnel hatch 8 331.1-1 m f

. . SNUPPS The neutron dosemetry method will comply with Revision 1 of Regulatory Guide 8.14. Exposures will be determined by film and/or time-dose calculations, using rem meters. There are no specific requirements for personnel entry into the contain-ment during normal operating conditions. The frequency of entries will be based on operational needs and indications of abnormal conditions within the containment.

Entries into the containment when the reactor is at power will be made by at least two persons, one of whom will provide health physics surveillance.

REFERENCES

1. Straker E. A., Stevens P. N., Irving D. C., and Cain V. R.,

"The MORSE Code -- A Multigroup Neutron and Gamma-Ray Monte Carlo Transport Code," ORNL-4585, September, 1975.

2. Hopkins W. C., " Calculations of the Neutron Environment Inside PWR Containments," ORNL/RSIC-43, Page 127, February, 1979.
3. Hankins D. E. and Griffith R. V., "A Survey of Neutrons Inside the Containment of a Pressurized Water Reactor,"

ORNL/RSIC-43, Page 114, February, 1979.

O O

e 331.1-2

. . SNUFPS 331.2 Radiation levels in excess of 100 R/hr can (12.2.1.3) occur in the vicinity of spent fuel transfer tubes; therefore, all accescible portions of the transfer tubes must be shielded during fuel transfer. Please address the manner in which shielding, access control and radiation monitoring will be incorporated into the radiation protection program to prevent either occupants or transient workers from receiving very high exposures during transfer of spent fuel from the reactor to the spent fuel pool through the fuel transfer tubes.

Use of removeable shielding for this purpose is acceptable. Provide appropriate figures (e.g. plan and elevation) that show the shielding arrays for all direct gamma radia-tion and streaming pathways from the spent fuel during the transfer. On the same figure show the location of any administrative controls by barriers, signs, audible and visual alarms, locked doors, etc. All acces-sible portions of the transfer tubes that cannot be adequately shielded shall be clearly marked with a sign stating that potentially lethal fields are possible during fuel transfer.

RESPONSE

The fuel' transfer tube is completely shielded with permanent shielding to within radiation zone limits. No special access control, radiation monitoring, or posting is required.

The expansion bellows for the fuel transfer tube are under water in the fuel transfer car,al in the fuel building (see revised Figure 3.8-48). There is no bellows inspection room or opening. The fuel transfer tube is completely surrounded by concrete or water, with the exception of the seismic gaps, so that no personnel access is possible.

The fuel transfer tube in the seismic gap between the contain-ment wall and the internal containment structure and in the seismic gap between the containment wall and the fuel building is shielded, using permanently installed lead loaded silicone foam rubber, to meet the radiation zone limits (Figure 12.3-2). Therefore, there is no unshielded portion of the fuel transfer tube.

I l 331.2-1 i

CNUPPS FIGURE 3.8 48

(

1 REACTOR BUILDING FUEL TRANSFER PENETRATION se t*

'e*. ... l

. .e ; e /

4.<..

LEAD IMPREGNATED ' *?

SLICONE FCAM i -

, m .e_a TO_ t

! /. 8 , OF REACTOR i*

e J ,. ,',

.. I r;

.* a/

'Q

.. i r

't' 9.r, '

f,7 .._..

Q VALVE .-

i i

.J j

( '

2* CCedPRESSIBLE MATL *j

' # 1, Je.'UNER & 4 o e .< :r u 4 E m .,, .

1* 2 . .. ....,-

O . ^

  • li
  • i.i;.

}$ UNER k. *. *

  • a.4 e'(?f 3

,<.

  • e .T. e v. *: , et

'an FC3 .

  • e-

),

e ..

.v g -

.._ _/_ . e.f.,xe

. - . . . . .f as J 6 .. ~-

3.m. nw

. .- J ....s ,>

p u f p l 9 ,J..l . , .

3 =_

,p, ,. a, ' ~

. -L ,

l_', ; g s 7 "q -

' u*

P .* 1.5.SLEEVC 9 ;. . . .y,! .

M. ,,I. .B.. .R. ./.,

,; o . ,j;..,,. &,. 3 3. .

p.

4. .o. .

r . . . _a r Y.? " J 55 SLEEVE -.

Q SPL1CE

  • ,' LEAD IMPREGNATED .

/- ' .<.. .,

'~- -SlWCONE FOAM -

..y }

4-qSPUCE

' . ' 4'.o* WIN) . '.[. - ~ .i

, ..h >

-I "A -

i

> ( Au saDEs)'. . ... . " : .'

el l. *. -

A.T *,.,W'. ?.. m. . :.c3..y .... .

a ,

r  ; p.

. .e #

,, .1

,... y - ".. RECESS COMPRE5518LE .. J.

,',.4.',.. 4 ; T. 5.

s MATL..3',(ne) .. <,. - f,' . . r.r -fg.. 4 .,4-M

  • T . - .., -
  • Aj-L;.p 7.. .' .., .

\ ,

. :.* .a Q _

u . .. , j. . .. ... . . : - ; ..

a e m g g *-:ff.m.-?p[ z.p _ W. ,.- ;..'

LEAD MPREGNATED i .

e Wuap

" SOLIO SLICONE ELASTOMER

- ' ~ -

, ;. ( i,

..w]..uf.y. M. . m. 3..(.,i. e,a.- , 7-+ ' -

. .,- 9.,80EZLE . . ..,

r. . ,. .-..._...e- .

. ~. a. .. - s. . .. c . .. .

.. . . . -y: .

4
.=.--. s=. -.l:-1.*Q.c .. s .W. ., -2&"' .
J.W.
.~ &'

4.o, 4 *:.

- : v. :.- :n.h.42:: .: u.L.J, ;.:w. r.g n A..y.-k .

e.. . . .. .. 2. V.,- .- . s.. u. .

l 4r . . . .. .

J .Y. .,. t;:e,  : - &:;.i.g:::. 7.v,.2$.* ~ = ;

$:41 , -

. .;. % .. n . . , . .

j .-. : .. ;. . ., . , T4 ..e . . . ;, . .

../4 "--

's . h

  • l.

e 3 *f >' -4 4.* .. . a .at'

. ' , 4

. ,4.*.. 64. . ; - ., i ~.2 2.

..KC.
- .J.Ct,i h* . . . ":. .A*

W.

ng

-,lAm.sy-C.'ie=
.. .* an
.y ..:.n% ..

, ;%w*(*'.P.* 4 .,a.r

. . -.* ., g. sK# g S . *4f .

4.. .

,, . + ., .m. m. . e s W1;pa.Q*M.7,4rggs.; p's ~.:5,Q4 e. p.s.t*:', -

.....,.'..f....,;.~~e Q3 u h,%e .g_ j .

.w. .w u_.e ..,. s'. w'

. ,..s.... .. . . .

.._...~.r.  :

M. ,..r...' rPLAN ..

q.:+.re s

". F U E L ' TR AN SFER TU BE' m gp,:,-K p;; E

.i. o:w.< :.-.i.. 32..r p . . . .j._ d.. .. ,-  ;

,, . . ., ,. .,,3 g.,,. .1 fc

, ,kM i ,

= 4 ?.W '"" p *.w

. y'*.g s -# '

. f, .

. .. . 4.. 4  : g*, ~,g

D.) &t*b .-

.p it . . , .4 I

?5 I.C : k .i ..&:4:i-..,.,....f

'. Yf?

h[* ~%. 4 $

W. . >I .;. *.*/ a*. I'V- J + - # sV/ M %'. Ime.f D a. *@

?

  • L'.$ M  ?".m5WWf'.;*
  • =' .

k..r*.9 ' .;#;.

5 .. ,

- 4rire..

%p.f..W['.':?

  • -h **1-
5. .

3 .

& *:  ?

SNUPPS 331.3 Describe the procedure for extracting a (12.2.1.2.3) sample from the Nuclear Sampling System of RCS, RHR and CVCS with as low as is reasonably achievable exposures to personnel withdrawing the sample. In your response include use of shielding, area monitoring, portable survey meters, hand contact with sample containers, dose rate levels in sampling area, dose rate level of sample container, etc. Consider samples taken during normal operations, anticipated operational occurrences and accidents. The response to this question should satisfy the requirements of NUREG-0578 item 2.1.8.a, Post Accident Sampling, with regard to Radiation Protection.

RESPONSE

The sampling systems for (a) reactor coolant, (b) contain-ment sump water, and (c) containment atmosphere are being modified to meet the guidelines of NUREG-0737, Item II.B.3.

A subset of these modifications pertains to the piping systems shown in Figures 9.3-2 and 6.2.5-1. These changes will enhance the capability to collect samples in a post-accident situation.

In addition, a new post-accident sample analysis system is being procured. The sample panel for this system is to be located in the auxiliary building at El. 2000, in the room where the boronmeter is located. However, the post-accident sampling system is to be functionally independent of the l boronmeter. The post-accident dose rate in this location has been calculated to be less than 10 r/hr.

The new system will be operable from a remote location, either in the control building or computer room, and will have the capability of in-line radionuclide spectral and chemical analysis of each of the three types of samples.

The chemical analyses will include those specified in NUREG-0737, Item II.B.3. The capability of collecting shielded grab samples from the sample panel will also be provided. A purchase specification hrs been written for this system, and bids are currently being evaluated.

An FSAR change containing more. detailed information about the revised sample systems will be prepared after selection of the supplier for the in-line sample analysis system.

The existing sampling systems, which provide the capability ,

to make required analyses under normal conditions, will be retained. Tables 9.3-3, 9.3-4, 9.3-5, and 9.3-6 list the l various systems which are sampled. Figures 9.3-2, 9.3-3, i l and 9.3-4 show the piping and instrumentation diagrams for j l

331.3-1 l

I l

L

stdures the sampling systems. Process radioactivity monitors for the sampling systems are indicated in the tables and figures mentioned above. The area and airborne radioactivity moni-tors for worker protection are given in Section 12.3.4 and are shown in Figure 12.3-2.

O e

6 6

331.3-2

SNUPPS 331.4 Table 12.2-7 indicates the radionuclide con-(TABLE 12.2-7) centration in the spent fuel pool (SFP) water. Relevant reactor operating experience shows that the 60Co. activity, from crud transferred to the SFP from the interchange of the primary coolant water during refueling, is several orders of magnitude greater than that shown in the table even after purifica-tion by the SFP clean-up system. Please justify the values given in the table for 60 Co, Co, 134Cs, and 137 Cs and show that these values will be retained after several years of reacter operation. Provide an estimate of the dose rate above the SFP during a refueling operation and for the period thereafter. Include in the estimate the effect on the dose rate of any radioactive equipment that might be stored therein.

RESPONSE

The radionuclide concentrations given in Table 12.2-7 were calculated based on the primary coolant activities given in Table 11.4-7 without consideration of the crud which could be released to the refueling pool and the spent fuel pool

~

during refueling operations. Typical spent fuel pool con-l centrations at operating plants with similar cleanup systems are listed in revised Table 12.2-7.

As stated in Section 9.1.2, the plant is designed so that dose rates above the spent fuel pool will not exceed 10 l mrem /hr during refueling and 2.5 mrem /hr for the storage period.

The above dose rates consider the contribution from spent fuel and the spent fuel pool water. No other radioactive equipment that would significantly contribute to the dose rate is stored in the pool.

e l

t 331.4-1 l

l

SNUPPS 12.2.1.2 Auxiliary Building 12.2.1.2.1 Residual Heat Removal System The pumps, heat exchangers, and associo ed piping of the residual heat removal (RHR) system contain radioactive materials. For plant shutdown, the RHR pumps and heat ex-changer sources result from the radioactive isotopes carried in the reactor coolant, discussed in Section 12.2.1.1.2, considering 4 hours4.62963e-5 days <br />0.00111 hours <br />6.613757e-6 weeks <br />1.522e-6 months <br /> of decay following shutdown. The radia-tion source terms for the RER system are listed in Table 12.2-5.

12.2.1.2.2 Chemical and Volume control System The CVCS source activity is.the reactor coolant inventory which is provided in Table 11.1-4. More than 1 minute of N-16 coolant activity decay is provided before the letdown line exits the containment, and, therefore, is not signif-icant in determining shielding requirements for the CVCS equipment outside the containment.

Major equipment items include the letdown and excess letdown heat exchangers, mixed bed and cation bed demineralizers, reactor coolant filter, volume control tank, and charging pumps. The seal water subsystem for the reactor coolant pumps includes the injection and return filters and the seal water heat exchanger. The design activities of the CVCS components are listed in Table 12.2-6. Heat exchanger and piping activities are derived from primary coolant activities, Radiation sources in the various pumps are assumed to be identical to the liquid sources in the tank from which the pury takes suction.

12.2.1.2.3 Nuclear Sampling System The major radiation sources in the nuclear sampling system originate from the RCS, RHR, and CVCS systems. The greatest radiation exposure would be to personnel taking the samples.

To minimize this exposure, an integral shield has been incorporated int 7 the sampling station design.

12.2.1.3 Fuel Building 12.2.. 3.1 Spent Fuel Storage and Transfer The predominant radioactivity sources in tne spent fuel storage and transfer areas in the fuel building are the spent fuel assemblies. Spent fuel assembly sources are .

l discussed in Section 12.2.1.1.5. For shielding design, the spent fuel pool assumptions are given in Section 9.1.2. The major radionuclide concentrations in the water are provided in Table 12.2-7.

12.2-3 v

. M. m go SNUPPS l TABLE 12.2-7 SPENT FUEL POOL WATER ACTIVITIES Isotope

  • Activities (pC1/cc)

Co-58 1.3E-04 Co-60 4.0E-04 Cs-134 2.0E-05 Cs-137 2.0E-04

  • 0ther isotopes will be present in much lower concentrations.

o

SNUPPS 331.5 Please clarify how iodine radioactivity (12.3.4.2.2.2.2) levels can be " inferred from the particu-late and noble gas radioactivity levels" when monitoring the exhaust from the radwaste and auxiliary buildings as addressed in section 12.3.4.2.2.2.2 and 12.3.4.2.2.2.4.

RESPONSE

The referenced FSAR sections have been revised to indicate that particulate iodine radioactivity levels in the HVAC duct flow paths (prior to filtration and discharge to the

.radwaste building ar.d auxiliary building vents) will be

' determined by periodic laboratory isotopic analyses of the particulcte cartridge filters associated with monitors 0-GH-RE-22 and 0-GL-RE-60. Also, if required, grab samples will be taken at various room locations to locate the source of the release. Analyses of these grab samples will be made for particulate, gaseous iodine, and noble gas activity.

The rate of iodine radioactivity discharged from the radwaste building vent and the unit vent is continuously monitored by 0-GH-RE-10A and 0-GT-RE-21A. These instruments monitor particulates and gaseous iodine. Parallel monitc.s 0-GH-RE-10B and 0-GT-RE-21B monitor noble gases.

An alarm from either the particulate monitor upstream of the HVAC filters or the noble gas monitor downstream of the filters will indicate that an increase in airborne activity is occurring. Laboratory analyses of the cartridge filters from the continuous monitors and the grab samples would then be used to determine the level of gaseous iodine.

331.5-1

SNUPPS duct through an isokinetic no::le, in accordance with ANSI Standard N13.1-1969, to ensure that a representative sample is obtained. After passing through the fixed filter detector assembly and the pumping system, the sample is discharged back to the duct. The cartridge filter will be removed periodically for laboratory isotopic analyses. Monitoring upstream of the filter adsorber provides the most rapid response to airborne radioactivity in the system.

The high and high-high alarms function to alert the operator to airborne particulate radioactivity in the radwaste building.

Indication for this monitor is provided on the AiRMS CRT in the control room.

If required, the portable monitor described in Section 12.3.4.2.2.2.9 and/or grab samples will be utilized to determine airborne radioactivity levels and iodine con-centrations in specific areas to aid in the determination of the source of the release.

12.3.4.2.2.2.3 Waste Gas Decay Tank Area Ventilation Exhaust Radioactivity Monitor The waste gas decay tank area ventilation radioactivity

. monitor, 0-GH-RE-23, continuously monitors for gaseous radioactivity in the discharge duct from the waste gas decay tank area upstream of the radwaste building exhaust filter adsorber. The sample point provides rapid detection of a leak in the waste gas processing system and, in conjunction with the radwaste building exhaust radioactivity monitor and the radwaste building effluent monitor, helps localize the affected area in the event of an alarm on either monitor.

The sample is extracted from the exhaust duct and passed through the fixed volume noble gas detector assembly and the pumping system. Then the sample is discharged back to the duct. The high alarm provides indication of a leak in the decay tanks, compressors, piping, or valves. The high-high alarm indicates that concentrations in the decay tank room are at or near 10 MPC for the most restrictive. isotope expected to be present (Kr-85 or Xe-133).

Back up for this monitor is provided by the radwaste building exhaust and effluent monitors.

Indication of this Et;nitor is provided on the AiRMS CRT in the control room.

e 12.3-33

SNUPPS 12.3.4.2.2.2.4 Auxiliary Building Ventilation Exhaust P.adio-activity Monitor The auxiliary building ventilation exhaust radioactivity monitor, 0-GL-RE-60, continuously monitors for particulate radioactivity in the auxiliary building ventilation system upstream of the filter-adsorber units. The sample point is located to monitor between the last point of possible radioac-tivity entry to the ventilation system from the areas served and the filter adsorber unit. The sample is extracted through an isokinetic nozzle, in accordance with ANSI Stan-dard N13.1-1969, to ensure that a representative sample is provided to the fixed filter particulate detector assembly.

Then the sample is discharged through the pumping system back to the duct.

The cartridge filter will be removed periodically for labora-tory isotopic analyses.

The high alarm alerts the operator to high airborne particu-late radioactivity levels in the auxiliary building. Indica-tion of this monitor is provided on the AiRMS CRT in the control room.

If required, the portable monitor described in Section 12.3.4.2.2.2.9 and/or grab samples will be utilized to determine airborne radioactivity levels and iodine con-centrations in specific areas to aid in the determination of the source of the release.

12.3.4.2.2.2.5 Containment Atmosphere Radioactivity Monitors The containment atmosphere radioactivity monitors, 0-GT-RE-31 and 0-GT-RE-32, continuously monitor the containment atmo-sphere for particulate, iodine, and gaseous radioactivity which could result in personnel exposure during periods of containment access. Other functions of these monitors are covered in Sections 5.2.5, 7.3, 9.4, and 11.5.

Samples are extracted from the operating deck level (El.

i 2047'-6") of the containment thrcagh the monitoring system sample lines.

The monitors are located as close as possible to the con-tainment penetrations to minimize the lengthThe of the sample sample tubing and the effects of sample plateout.

points are located in areas which ensure that representative Each sample passes through the penetra-samples are obtained.

tion and then through the fixed filter (particulate), charcoal .

filter (iodine), and fixed volume (gaseous) detector assemblies.

I the sample is After passing through the pumping system, discharged back to the containment through a separate penetra-tion.

12.3-34 i .

I