ML20028C414

From kanterella
Revision as of 18:59, 20 December 2024 by StriderTol (talk | contribs) (StriderTol Bot insert)
(diff) ← Older revision | Latest revision (diff) | Newer revision → (diff)
Jump to navigation Jump to search
Discusses Evaluation of Radiological Consequences of Postulated Recombiner Failure at Facilities,Per Effluent Treatment Sys Branch 730724 Request.Tables Listing Consequences of Shine & Immersion Doses & Sources Used Encl
ML20028C414
Person / Time
Site: 05000000, Limerick
Issue date: 08/09/1973
From: Grimes B
US ATOMIC ENERGY COMMISSION (AEC)
To: Tedesco R
US ATOMIC ENERGY COMMISSION (AEC)
Shared Package
ML20027A594 List: ... further results
References
FOIA-82-545 NUDOCS 8301100088
Download: ML20028C414 (4)


Text

.

~,.........

=.

.e.n

.. '<(*hM%

9 UNIThO STATES

~ M \\

ATOMIC ENERGY COMMISSION'~

bM WD

'j '.4

  • wasMiNovos. o.c. :ss4s Q. ' '
  • 'h,y,
  • AUG $

1973 -

6' R. Tedesco, Assistant Director for Contain=ent Safety, L Harold R. Danton, Assistant Director for Site Safety,Y.h,b

~

Thru:

KADIOLOGICAL,CONSLQUENCES OF POSTULATED RECOMSINER FAILURE AT LIMERICK

[

As orally requested by tha.. Effluent Trestment Systc=s Branch on July 24, 197 the consequences of a reco=biner failure a: L1=erick were avalus:ed.-. This is a part of the Staf f's analysis, in the enviren= ental state =ent. of the applicant's proposed changes to their effluent treattent syste=.

Both a shine dose and an (=mersion dose ucro calculated for the assu=ed ten secsnd release.

(The time foc~ automatic closure of.the shut-off valve is :en seconds.) The core release rates of nobla gases were based on the NEM-1072

.~ Isotopic distribution assu=ing a total noble gas release rate of 100,C Z uCi after 30 =inutes decay;.the activation gas activities ucre also taken fro:

MEDO-10734.

A 15 second delay fro the core to the failed line was assu=sd.

Table I lists the consequences of the shine and it..r.e:sion doses, and Table $

lists the isotopes considered and the total activity released.

As shown in Table I, the shine dose is not a significant contributor to the total dose for large noble gas release rates.

The i==ersion dose f c= nobic gases is directly proportional to the noble gas release rate (assu=ing no

~

change in the isotopic distribution).

Therefore, for a significantly,1 cue:

. release rate, e.g.,10,000 uCi/sec af ter 30 =inutes, the shine ' dose beco=cs a significant contributor to the site boundary, dose since the shine dose is independent of the noble gas release rate.

The it=nersion dose for the environ = ental stata=ent was calculated assuming a wind speed of four tacters per second and -decay enroute to the site beundas As discussed in a =eeting with I. Van der Hoven of NOAA (see June 5, 1973 m.emo fro: R. Loose to D. R. Muller " Department of Co==arce (MOAA) Meetin; Report"), the =eteorological assu=ptions used for dete==ining compliance with Appendix I guidelines for this uncontrolled but anticipa:ed release were those stated in the proposed Annen to Appendix D of 10 C.:R Part 50, i.e.,

one-tenth the Safety Guida 3 ground level release value at the 2500 foot site boundary.

4s reco==end that this meteorology also be used fe s :(

releases during load rej ections at PWR's.

Of course the consequences cust be weighted by the saticipated yearly frequency of the respective events.

lin shine dose for the en tiron = ental statc=cnt was calculatcd by assuming o linc source frw thu tucbine building vent with a four =ctc per second

(

wind speed, an averagu activity and an avarage gar =a enc gy.

, Sac June 20,,

1973 =a=o fro: H. Denten to R. Engelken, " Dose Calculations Relating to the Guad-Cities 2 Rupture Dish Failure," for a discussion of the =ethod used to calculate the sbinn d Me).

Calculations were perforned at the site bounde.)

~

l and a distance of.1000 feu (Table I) for 1 and 10 meter pc: second wind l

l 5peeds which establi.simd Ihat the shine dose is not a particularly signific<

L j

co.tsideration in clu:s couputations.

Future dose esticates using the 10 8301100088 821207 PDR FOIA

[.

HIATTB2-545 PDR

55i'.

C]%

R. Tedcaco-...gg.g 3 g7y percentile mateorology can therefore be obtained from the Radiological Assess =cnt Branch, as conventional i=cersion dose calculation techniques are adequate.

The following uords were infor= ally transmitted to A. Lyle of Environ = ental Projects for inclusion in Section 3.4 of the L1=erick Draft Environ =cntal Statement:

"In the evaluation of the performance of this systc=,

the sta f f assu=ed that in the event of a recombiner f ailure ten seconds would be required for the auto =stic closing of isol.ation valves, allouing the release uichout treat-cent of radioactive noble and activation gases.

Assu=ing the meteorological dispersion which would be expected to occur 50% of the time and prior operation at an equivalent offp.as cate of 100,000 uCi/see at thirty minutes, the staf f esti=nted a whole body dose of less than 1 cre= at 2500 feet from the turbine building."

This work was perfor=ud by E. Adensam and R. Zavadoski of.the Accident Analysis Branch.

{

l

%J1u %

ss' Brian Crices, Chief Accident Analysis 3 ranch Directorate of Licensing

Enclosure:

Table I, Table II cc:

w/ enc 1.

J. Hendrie V. Benaroya J. Kastner A. Lyle J. Collin, D. Muilur EP B/C'.s I

R. Zavadu. ski l

E. Ade: sam /

1 e

{

  • T..

TABLE I ESTIMATED DOSE CONSEOUENCES FOR A l'OSTU' ATED RECOMSINER FAILURE AT LIMERIC'd Site Boundar~y (2500 feet) Doses, mean 3

Wind Spaed, m/sec X/Q, sec/m Ic= ersion Shine e

~4 1.0 5.95 X 10 3.3 0.01 4.0 5.'95 X 10-5

.0.85 0.04 1.9 X 10-5 0.45 0.10 10.0

, Doses at 1000 feet, mren Wind Speed, m/sce X/Q, sec/c I=cersion Shine 1.0 1.6 X 10-3 17.

0.02 4.0

  • 1.6 X 10-4 3.9 0.08 10.0 6.4 X 10-5 2.8 0.2 9

e a

O h

6


a' a~.L..__..

-~---n---

_3 C wa

Sk.

. i' i

E!;

mjy

^ ;=.

Table II.

Source Used toEstiente Dose Conscouences From a Pot:tulated P.ccombiner Failura st Limerick t.uclide Total Activity Released, curies

~

Kr83m

0. 3.4' b<

Kr85m 0.61 KrSS 0.002

~

~ ~

KrS7 2.0 Kr88

'2.0 Kr89 12.3 i

Kr90 17.

Kr91 9.8 0.0015 Xe131m Xel33m O.029 Xe133 0.82

'.6 2

xe135m Xel35 2.2 Xe137 14.

Xel38 8.7 Xe139 19.2 Xel40 14.

ti-13 0.15 tt-16 66.

1

'o-19 14.9 4

e 4

e

/

s y

r-