Regulatory Guide 1.4: Difference between revisions

From kanterella
Jump to navigation Jump to search
(Created page by program invented by StriderTol)
(Created page by program invented by StriderTol)
Line 14: Line 14:
| page count = 6
| page count = 6
}}
}}
{{#Wiki_filter:Revision 1 U.S. ATOMIC ENERGY COMMISSION
{{#Wiki_filter:Revision 1 Revision 1 June 1973 U.S.     ATOMIC ENERGY COMMISSION
REGULATORY
                              REGULATORY
DIRECTORATE  
                                DIRECTORATE OF REGULATORY                               STANDARDS
OF REGULATORY  
                                                                                                                              GUIDE
STANDARDS Revision 1 June 1973 GUIDE REGULATORY  
                                                                REGULATORY GUIDE 1.4 ASSUMPTIONS USED FOR EVALUATING THE POTENTIAL RADIOLOGICAL CONSEQUENCES
GUIDE 1.4 ASSUMPTIONS  
            OF A LOSS OF COOLANT ACf',DENT FOR PRESSURIZED WATER REACTORS'
USED FOR EVALUATING  
THE POTENTIAL  
RADIOLOGICAL  
CONSEQUENCES
OF A LOSS OF COOLANT ACf',DENT  
FOR PRESSURIZED  
WATER REACTORS'


==A. INTRODUCTION==
==A. INTRODUCTION==
Sect ion 50.34 o1f 10 CFR Pairl 50 requires that each applicant fir a c(nstruiction permit or operating license provid,: an analysis and cvalua3ion of the design and of structures.


systems, and components of tile facility with [he objective of assessing fhe risk to public health and safety resulting froim operation of the facility.
==C. REGULATORY POSITION==
Sect ion 50.34 o1f 10 CFR Pairl 50 requires that each
                                                                                      1. The assuimptions related io the release of radioactive applicant fir a c(nstruiction permit or operating license material from the fuel and containment are as Ibllows:
  provid,: an analysis and cvalua3ion of the design and a. T we n t y -five percent of the equilibriut ierlo*rmance of structures. systems, and components of                             radioactive iodine inventory developed from imlaximu i tile facility with [he objective of assessing fhe risk to full power operation of the core should be assumtned to public health and safety resulting froim operation of the                           be immediately available for leakage from the prinmary facility. Tile design basis loss of" coolant accident                                reactor containment. Ninety-one percent of this 25 (LOCA) is one of the postulated accidents Used to                                    percent is to be assumed ito he ill Ithe forma ofelenllelllal evaluate the adequacy of these structures, systems. and iodine. 5 percent of this 25 percent ill the form of comiponents with respect to the public ltealth and safety.                          particulate iodine. and 4 percent of this 25 percent in This guide gives acceptable assumptions that may be                                  the form of organic iodides.


Tile design basis loss of" coolant accident (LOCA) is one of the postulated accidents Used to evaluate the adequacy of these structures, systems. and comiponents with respect to the public ltealth and safety.This guide gives acceptable assumptions that may be used in evaluating tIle radiologcal consequences of this accident for a pressurized water reactor. In some cases.unusual site characteristics, platit design features.
used in evaluating tIle radiologcal consequences of this                                   b. One hundred percent of the equilibrium accident for a pressurized water reactor. In some cases.                             radioactive noble gas inventory developed front unusual site characteristics, platit design features. or                            maximum full power operation od the core should be other factors may require different assumptions which                                assumed to be immediately available for leakage front will be considered on an individual case basis. The                                  the reactor containment.


or other factors may require different assumptions which will be considered on an individual case basis. The Advisory Committee on Reactor Safeguards has been consulted concerning this guide and has concurred in the regulatory position.
Advisory Committee on Reactor Safeguards has been                                           c. The effects of radiological decay during holdup consulted concerning this guide and has concurred in the                             in the containment or other buildings should be taken regulatory position.                                                                  into account.


==B. DISCUSSION==
==B. DISCUSSION==
After reviewing a number of applications for construction permits and operating licenses for pressurized wateli power reactors, the AEC Regulatory staff has developed a number of appropriately conservative assumptions, based on engineering judgment and on applicable experimental results from safety research programs conducted by the AEC and the nuclear industry, that are used to evaluate calculations of the radioloocal consequences of various postulated acciden ts.This guide lists acceptable assumptions that may be used to evaluate the design basis LOCA of a Pressurized Water Reactor (PWR). It should be shown that thc offsite dose consequences will be within thie guidelines of 10 CFR Part 100,'This guide is a revision of former Safety Guide 4.C. REGULATORY
d. The reduction in the amotunt of radioactive material available for leakage to tile environment by After reviewing a number of applications for                                   containment sprays, recirculating filter systems, or other construction permits and operating licenses for                                       engineered safety features may be taken into account.
POSITION 1. The assuimptions related io the release of radioactive material from the fuel and containment are as Ibllows: a. T we n t y -five percent of the equilibriut radioactive iodine inventory developed from imlaximu i full power operation of the core should be assumtned to be immediately available for leakage from the prinmary reactor containment.


Ninety-one percent of this 25 percent is to be assumed ito he ill Ithe forma ofelenllelllal iodine. 5 percent of this 25 percent ill the form of particulate iodine. and 4 percent of this 25 percent in the form of organic iodides.b. One hundred percent of the equilibrium radioactive noble gas inventory developed front maximum full power operation od the core should be assumed to be immediately available for leakage front the reactor containment.
pressurized wateli power reactors, the AEC Regulatory                                  but the amount of reduction in concentration of staff has developed a number of appropriately                                          radioactive materials should be evaluated on an conservative assumptions, based on engineering                                        individual case basis.


c. The effects of radiological decay during holdup in the containment or other buildings should be taken into account.d. The reduction in the amotunt of radioactive material available for leakage to tile environment by containment sprays, recirculating filter systems, or other engineered safety features may be taken into account.but the amount of reduction in concentration of radioactive materials should be evaluated on an individual case basis.e. The primary reactor containment should be assumed to leak at the leak rate incorporated or to le incorporated as a technical specification requirement at peak accident pressure for the first 24 hours. and at 50 percent of this leak rate for the remaining duration of the accideint.
judgment and on applicable experimental results from                                        e. The primary reactor containment should be safety research programs conducted by the AEC and the                                  assumed to leak at the leak rate incorporated or to le nuclear industry, that are used to evaluate calculations                              incorporated as a technical specification requirement at of the radioloocal consequences of various postulated                                  peak accident pressure for the first 24 hours. and at 50
acciden ts.                                                                            percent of this leak rate for the remaining duration of the accideint. 2 Peak accident pressure is the maximum1 This guide lists acceptable assumptions that may be pressure defined in the technical specifications for used to evaluate the design basis LOCA of a Pressurized containment leak testing.


2 Peak accident pressure is the maximum1 pressure defined in the technical specifications for containment leak testing.2 Thte effect on coniainnmeni leakage tinder accident conditions of features provided to reduce the leakage ot" radioactive materials from the containment will be evaluated on an individual case basi
Water Reactor (PWR). It should be shown that thc
                                                                                            2 offsite dose consequences will be within thie guidelines                                      Thte effect on coniainnmeni leakage tinder accident of 10 CFR Part 100,                                                                  conditions of features provided to reduce the leakage ot"
                                                                                      radioactive materials from the containment will be evaluated on
      'This guide is a revision of former Safety Guide 4.                            an individual case basis.


====s. USAEC REGULATORY ====
USAEC REGULATORY GUIDES                                       Coples of published guldes may be obtained by request Indicating the divisions desired to the US. Atomic Energy Commission. Washington. 0.1, 20545, Regulatory Guides are issued to describe and make avaliable to the public          Attention: Director of Regulatory Standards. Comments and tuggrsilons for methods acceptable to the AEC Regulatory staff of Implementing specific parts of  impfrovements In these guides ere encouraged end should be sent to the Secretary the Commission's regulations, to delineate techniques used by the staff in        of the Commission, US. Atomic Energy Commission, Washington. O.C. 20545.
GUIDES Coples of published guldes may be obtained by request Indicating the divisions desired to the US. Atomic Energy Commission.


Washington.
evaluating specific problems or postulated accid3nts. or to provide guidance to    Attention: Chief, Public Proceedings Staff.


0.1, 20545, Regulatory Guides are issued to describe and make avaliable to the public Attention:  
applicants. Regulatory Guides are not substitutes for regulations and compliance with them is not required. Methods and solutlons different from those set out in    The guides are issued In the following ten broad divliions:
Director of Regulatory Standards.
the guides will be acceptable if they provide a basis for the findings requisite to                                              8. Products the issuance or continuance of a permit or license by the Comrrssio


Comments and tuggrsilons for methods acceptable to the AEC Regulatory staff of Implementing specific parts of impfrovements In these guides ere encouraged end should be sent to the Secretary the Commission's regulations, to delineate techniques used by the staff in of the Commission, US. Atomic Energy Commission, Washington.
====n.     ====


O.C. 20545.evaluating specific problems or postulated accid3nts.
===1. Power Reactors===
                                                                                    2. Researcha nd Tast Reactors             


or to provide guidance to Attention:  
===7. Transportation===
Chief, Public Proceedings Staff.applicants.
                                                                                    3.  Fuels and Materials Facilities          8. Occupational Health Published guides will be revised periodically, as appropriate, to accommodate      4.  Environmental end Siting                9. Antlitrust Review comments and to reflect new informatio" or experience.                              5.  Materials and Plant Protection        1
 
===0. General===
 
.1
2. Acceptable assumptions for atmospheric diffusion              From a semi-infinite cloud, the gamma dose rate in air and dose conversion are:                                        is:
      a. The 0-8 hour ground level release concentrations may be reduced by a factor ranging from                                  ,D    = 0,25E
one to a maximum of three (.see Figure I) for additional dispersion produced by the turbulent wake of the                Where reactor building in calculating potential exposures. The volumetric building wake correction, as defined in                            beta dose rate from an infinite cloud (rad/sec)
section 3.3.5.2 of Meteorology and Atomic Energy                              gamma dose rate from an infinite cloud
1968. should be used only in the 0-8 hour period: it is                        (rad/sec)
used with a shape factor of 112 and the minimum                        EO3= average beta energy per disintegration cross-sectional area of the reactor building only.                            (Mev/dis)
      b. No correction should be made for depletion of'              E = average gamma energy per disintegration the effluent plume of radioactive iodine due to                               (Mev/dis)
deposition on the ground, or for the radiological decay              X = concentration of beta or gamma emilling of iodine in transit.                                                          isotope in the cloud (curie/m3)
      c. For the first 8 hours, the breathing rate of persons offsite should be assumed to be 3.47 x 10'                    f. The following specific assumptions are cubic meters per second. From 8 to 24 hours following            acceptable with respect to the radioactive cloud dose the accident, the breathing rate should be assumed to be        calculations:
1.75 x 104 cubic meters per second. After that until the                  (1) The dose at any distance from the reactor end of the accident, the rate should be assumed to be            should be calculated based on the maximum
2.32 x 104 cubic meters per second. (These values were          concentration in the plume at that distance taking into developed from the average daily breathing rate [2 x 107        account specific meteorological, topographical, and cnv'/dayJ assumed in the report of ICRP, Committee              other characteristics which may affect the maximum
11-1959.)                                                        plume concentration. These site related characteristics d. The iodine dose conversion factors are given in        must be evaluated on an individual case basis. In the case ICRP Publication 2, Report of Committee 11,                      of beta radiation, the receptor is assumed to be exposed
"Permissible Dose for Internal Radiation," 1959.                to an infinite cloud at the maximum ground level e. External whole body doses should be calculated          concentration at that distance from the reactor. In the using "Infinite Cloud" assumptions, i.e., the dimensions        case of gamma radiation, the receptor is assumed to be of the cloud are assumed to be large compared to the            exposed to only one-half the cloud owing to the distance that the gamma rays and beta particles travel.         presence of the groun


Regulatory Guides are not substitutes for regulations and compliance with them is not required.
====d. The maximum cloud====
"Such a cloud would be considered an infinite cloud for         concentration always should be assumed to be at ground a receptor at the center because any additional [gamma          level.


Methods and solutlons different from those set out in The guides are issued In the following ten broad divliions:
and] beta emitting material beyond the cloud                              (2) The appropriate average beta and gamma dimensions would not alter the flux of [gamma rays              energies emitted per disintegration, as given in the Table and] beta particles to the receptor" (Meteorology and            of Isotopes, Sixth Edition, by C. M. Lederer, J. M.
the guides will be acceptable if they provide a basis for the findings requisite to the issuance or continuance of a permit or license by the Comrrssion.


1. Power Reactors 8. Products 2. Researcha nd Tast Reactors
Atomic Energy, Section 7.4. .1.-editorial additions            Hollander, I. Perlman; University of California, Berkeley, made so that gamma and beta emitting material could be          Lawrence Radiation Laboratory; should be used.


===7. Transportation===
considered). Under these conditions the rate of energy absorption per unit volume is equal to the rate of energy            g. The atmospheric diffusion model should be as released per unit volume. For an infinite uniform cloud        follows:
3. Fuels and Materials Facilities
containing X curies of beta radioactivity per cubic meter                (1) The basic equation for atmospheric the beta dose in air at the cloud center is:                    diffusion from a ground level point source is:
8. Occupational Health Published guides will be revised periodically, as appropriate, to accommodate
                        D! = 0.457 EOX
4. Environmental end Siting 9. Antlitrust Review comments and to reflect new informatio" or experience.
                                                                                      X/Q= ruaya The surface body dose rate from beta emitters in the infinite cloud can be approximated as being one-half this Where amount (i.e., 0DD' = 0.23 E'X).
                                                                      X  = the short term average centerline value of the ground level concentration (curie/meter3)
For gamma emitting material the dose rate in air at the Q = amount of material released (curie/see)
                                                                      u = windspeed (meter/see)
uloud center is:
                                                                        y = the horizontal standard deviation of the plume (meters) [See Figure V-I. Page 48.


5. Materials and Plant Protection
7 .D = 0.507 Ey(
1
                                                                                Nuclear Safety, June 1961, Volume 2.


===0. General ===
1.4-2
.1 2. Acceptable assumptions for atmospheric diffusion and dose conversion are: a. The 0-8 hour ground level release concentrations may be reduced by a factor ranging from one to a maximum of three (.see Figure I) for additional dispersion produced by the turbulent wake of the reactor building in calculating potential exposures.


The volumetric building wake correction, as defined in section 3.3.5.2 of Meteorology and Atomic Energy 1968. should be used only in the 0-8 hour period: it is used with a shape factor of 112 and the minimum cross-sectional area of the reactor building only.b. No correction should be made for depletion of'the effluent plume of radioactive iodine due to deposition on the ground, or for the radiological decay of iodine in transit.c. For the first 8 hours, the breathing rate of persons offsite should be assumed to be 3.47 x 10'cubic meters per second. From 8 to 24 hours following the accident, the breathing rate should be assumed to be 1.75 x 104 cubic meters per second. After that until the end of the accident, the rate should be assumed to be 2.32 x 104 cubic meters per second. (These values were developed from the average daily breathing rate [2 x 107 cnv'/dayJ
Number 4, "Use of Routine Meteorolo-ical                    Time Observations for Estimating Atmospcheric                  Following Dispersion," F. A. Gifford. Jrj..                         Accident                Atmospheric Conditions o" = the vertical standard deviation cf the pluii.e (meters) ISee Figure V-2, Page 48, Nuclear              0.8 hours    Pasquill Type F. wiudspeed        I meter/sec.
assumed in the report of ICRP, Committee 11-1959.)d. The iodine dose conversion factors are given in ICRP Publication
2, Report of Committee
11,"Permissible Dose for Internal Radiation," 1959.e. External whole body doses should be calculated using "Infinite Cloud" assumptions, i.e., the dimensions of the cloud are assumed to be large compared to the distance that the gamma rays and beta particles travel."Such a cloud would be considered an infinite cloud for a receptor at the center because any additional
[gamma and] beta emitting material beyond the cloud dimensions would not alter the flux of [gamma rays and] beta particles to the receptor" (Meteorology and Atomic Energy, Section 7.4. .1.-editorial additions made so that gamma and beta emitting material could be considered).  
Under these conditions the rate of energy absorption per unit volume is equal to the rate of energy released per unit volume. For an infinite uniform cloud containing X curies of beta radioactivity per cubic meter the beta dose in air at the cloud center is: From a semi-infinite cloud, the gamma dose rate in air is: ,D = 0,25E Where beta dose rate from an infinite cloud (rad/sec)gamma dose rate from an infinite cloud (rad/sec)EO3 = average beta energy per disintegration (Mev/dis)E = average gamma energy per disintegration (Mev/dis)X = concentration of beta or gamma emilling isotope in the cloud (curie/m3)
f. The following specific assumptions are acceptable with respect to the radioactive cloud dose calculations:
(1) The dose at any distance from the reactor should be calculated based on the maximum concentration in the plume at that distance taking into account specific meteorological, topographical, and other characteristics which may affect the maximum plume concentration.


These site related characteristics must be evaluated on an individual case basis. In the case of beta radiation, the receptor is assumed to be exposed to an infinite cloud at the maximum ground level concentration at that distance from the reactor. In the case of gamma radiation, the receptor is assumed to be exposed to only one-half the cloud owing to the presence of the ground. The maximum cloud concentration always should be assumed to be at ground level.(2) The appropriate average beta and gamma energies emitted per disintegration, as given in the Table of Isotopes, Sixth Edition, by C. M. Lederer, J. M.Hollander, I. Perlman; University of California, Berkeley, Lawrence Radiation Laboratory;
Safqev', June 19(1. Volume 2. Number  
should be used.g. The atmospheric diffusion model should be as follows: (1) The basic equation for atmospheric diffusion from a ground level point source is: X/Q= ruaya Where X = the short term average centerline value of the ground level concentration (curie/meter3)
Q = amount of material released (curie/see)
u = windspeed (meter/see)
y = the horizontal standard deviation of the plume (meters) [See Figure V-I. Page 48.Nuclear Safety, June 1961, Volume 2.D! = 0.457 EOX The surface body dose rate from beta emitters in the infinite cloud can be approximated as being one-half this amount (i.e., 0DD' = 0.23 E'X).For gamma emitting material the dose rate in air at the uloud center is: 7.D = 0.507 Ey(1.4-2 Number 4, "Use of Routine Meteorolo-ical Observations for Estimating Atmospcheric Dispersion," F. A. Gifford. Jrj..o" = the vertical standard deviation cf the pluii.e (meters) ISee Figure V-2, Page 48, Nuclear Safqev', June 19(1. Volume 2. Number 4."Use of Routlinc Me leorological Oh,'ervations for Estimating Atmospheric Dispersion," F. A. G;ifford.


Jr.I (.2) For lime periods of greater than 8 hours the plume shouid hI assumed to meander and spread ovcr a 22.i" sector. The resultlant e'quaition is: 2.032 x/Q = lx\Vhicrc x distance from point of release to the receptor;.
===4. uniform direction===
other variables are as given in g( 1).(3) Tlhe at mospheric diffusion model" for ground level releases is based on the information in the following lable.-' 'This niIdo.l' %liould be useud until adequate site metcorologic'al d:ta are obtained.
                    "Use      of Routlinc Me leorological Oh,'ervations for Estimating Atmospheric                8-24 hours Pasquill Type F, windspced            I metcr/s.c.


In some ,-uses. available information.
Dispersion," F. A. G;ifford. Jr.I                                    variable direction within a 22.5" sector
            (.2) For lime periods of greater than 8 hours the plume shouid hI assumed to meander and spread                            1-4 days    (a) 4(Y,,%( Pasquill Type  D. windspeed      3 tini*ormly ovcr a 22.i" sector. The resultlant e'quaition is:                            rilel r/sec (b) 600,, Pasquill Type F. windspeed 2 leter/sec
                                        2.032 x/Q =        lx                                            (W' wind direction v: riabie within a 22._.


such u,;  
sector
topography and geovaphicut.
\Vhicrc
                                                                            4-30 days (a) 33.35, Pasquill Type C, windspeed            3 x        distance from point of release to the receptor;.                          meter/sec other variables are as given in g( 1).                                    (N) 33.3%'. Pasquill Type D. windspeed        3 ineter/sec
            (3) Tlhe at mospheric diffusion model" for                                  (c) 33.3%; Pasquill Type F, wirdspeed 2 ground level releases is based on the information in the                                  viieter/sec following lable.                                                                          (d) Wind direction 33.3,:, frequency in a
                                                                                          22.50 sector
    -''This    niIdo.l' %liould be useud until adequate site metcorologic'al      d:ta are obtained. In some ,-uses. available information. such u,;       tnic*orology. topography and geovaphicut.                 (4) Figures 2A and 213 give the groud level tocalion. may dictate Itic use of a more restrictive model to                release atmospheric diffusion factors based on the insurc a conscrvative eltimuie of potentla oflfsitc exposures.              parameters given in g( 3).
                                                                      1.4-3


tocalion.
bI                .1-GiAK
                                                                      buPRIP IOýAO
  2.5                                                                      FIGURE 1
                          2 O.SA-SO  meters
0                                P'mtr
                                                      2
                                                                                      4.


may dictate Itic use of a more restrictive model to insurc a conscrvative eltimuie of potentla oflfsitc exposures.
0 .5A-1000 -nws              O.SA-2500atr
                            2                      meti
      2  O.BA-1500 motors              0.5A-3000meru p.            O.5A-2000 metonus ý
w
0
                            ccI
                        zI
w1.5
4                                                                          I
                        uII
                                        I                                I      i      . . I *
                                                                              10w Distance from Structure (metars)


Time Following Accident Atmospheric Conditions
I
0.8 hours Pasquill Type F. wiudspeed I meter/sec.
                                                                        III _ . II
      3 L
                                                                    FIGL
                                S1i        ..         _.


uniform direction 8-24 hours Pasquill Type F, windspced I metcr/s.c.
10-A
                                                                                    I
          a- ...                    *-
                  - --      --                  ......
                        7----
      0
                        4--I
                                0\
  1  o          *      .               '1                  %
                                    Ditne      rmSrut-          (ees
            44sanc4m                    .tu.            St . ..    tes
                                                  1.4-5


variable direction within a 22.5" sector 1-4 days (a) 4(Y,,%( Pasquill Type D.rilel r/sec (b) 600,, Pasquill Type F.leter/sec (W' wind direction v: riabie sector windspeed
d*
3 windspeed
10-     I
2 within a 22._.4-30 days (a) 33.35, Pasquill Type C, windspeed
                                                                                                                                                  I
3 meter/sec (N) 33.3%'. Pasquill Type D. windspeed
                                  I I   A ...; I .... 1       1
3 ineter/sec (c) 33.3%; Pasquill Type F, wirdspeed
          .",   . - - -I.-- I--,- - .-*"i ... v -   .1 - 1 %ý
2 viieter/sec (d) Wind direction
                                                                                                                            FIGURE 2(81             -
33.3,:, frequency in a 22.50 sector (4) Figures 2A and 213 give the groud level release atmospheric diffusion factors based on the parameters given in g( 3).1.4-3 bI .1-GiAK buPRIP IOýAO 2.5 FIGURE 1 O.SA-SO meters 2 0 P'mtr 2  4.0 .5A-1000 -nws O.SA-2500atr
                                _____0-8                                                                   hours7~
2 meti 2 O.BA-1500
.. ,D   L
motors 0.5A-3000meru p. O.5A-2000
IU
metonus ýw ccI 0 zI w1.5 4 I uII I I i ..I *10w Distance from Structure (metars)
    E
I 3 L FIGL S1i .. ._10-A 7----4--I a -... *---- -- ......0 0\44sanc 4m St .tu. ... tes 1 o .* '1 %Ditne rmSrut- (ees I II _ .II I 1.4-5
                            .1.N..                                           '          I                 I I*
10-I I I A ... ; I .... 1 1 I.", .---I.-- I--,- -.-*" i ... v -.1 -1 %ýFIGURE 2(81 -_____0-8 hours7~..,D L IU E 0.1.N.. I I ' I%, ...:.7 ::::: 'V t~rV~'I F-W 0 * ,p -I *.X1 ,-,I- --7I..~.i... I_... ... -10 163 1 1 .ý 10.5 b 7 1 Distance from Structure (maters)1.4-6}}
* I
                                                                                                            .      %, . . :.
    0
                                                                                                    7   :::::
t~rV~
F-W                                                             0 * -,pI  *       . 'I
                                                                                    X1
                                                                                                      'V
                                                                                          ,
                                                              -,I-                                 -
                                            -7I
10
      163
              ..~.i...                 I_... ...                                                       1. 1ý 10.                       5 b
                                                                                                                                            -
                                                                                                                                              7 1 Distance from Structure (maters)
                                                                                        1.4-6}}


{{RG-Nav}}
{{RG-Nav}}

Revision as of 11:24, 4 November 2019

Assumptions Used for Evaluating the Potential Radiological Consequences of a Loss of Coolant Accident for Pressurized Water Reactors
ML13350A195
Person / Time
Issue date: 06/30/1973
From:
US Atomic Energy Commission (AEC)
To:
References
RG-1.004, Rev. 1
Download: ML13350A195 (6)


Revision 1 Revision 1 June 1973 U.S. ATOMIC ENERGY COMMISSION

REGULATORY

DIRECTORATE OF REGULATORY STANDARDS

GUIDE

REGULATORY GUIDE 1.4 ASSUMPTIONS USED FOR EVALUATING THE POTENTIAL RADIOLOGICAL CONSEQUENCES

OF A LOSS OF COOLANT ACf',DENT FOR PRESSURIZED WATER REACTORS'

A. INTRODUCTION

C. REGULATORY POSITION

Sect ion 50.34 o1f 10 CFR Pairl 50 requires that each

1. The assuimptions related io the release of radioactive applicant fir a c(nstruiction permit or operating license material from the fuel and containment are as Ibllows:

provid,: an analysis and cvalua3ion of the design and a. T we n t y -five percent of the equilibriut ierlo*rmance of structures. systems, and components of radioactive iodine inventory developed from imlaximu i tile facility with [he objective of assessing fhe risk to full power operation of the core should be assumtned to public health and safety resulting froim operation of the be immediately available for leakage from the prinmary facility. Tile design basis loss of" coolant accident reactor containment. Ninety-one percent of this 25 (LOCA) is one of the postulated accidents Used to percent is to be assumed ito he ill Ithe forma ofelenllelllal evaluate the adequacy of these structures, systems. and iodine. 5 percent of this 25 percent ill the form of comiponents with respect to the public ltealth and safety. particulate iodine. and 4 percent of this 25 percent in This guide gives acceptable assumptions that may be the form of organic iodides.

used in evaluating tIle radiologcal consequences of this b. One hundred percent of the equilibrium accident for a pressurized water reactor. In some cases. radioactive noble gas inventory developed front unusual site characteristics, platit design features. or maximum full power operation od the core should be other factors may require different assumptions which assumed to be immediately available for leakage front will be considered on an individual case basis. The the reactor containment.

Advisory Committee on Reactor Safeguards has been c. The effects of radiological decay during holdup consulted concerning this guide and has concurred in the in the containment or other buildings should be taken regulatory position. into account.

B. DISCUSSION

d. The reduction in the amotunt of radioactive material available for leakage to tile environment by After reviewing a number of applications for containment sprays, recirculating filter systems, or other construction permits and operating licenses for engineered safety features may be taken into account.

pressurized wateli power reactors, the AEC Regulatory but the amount of reduction in concentration of staff has developed a number of appropriately radioactive materials should be evaluated on an conservative assumptions, based on engineering individual case basis.

judgment and on applicable experimental results from e. The primary reactor containment should be safety research programs conducted by the AEC and the assumed to leak at the leak rate incorporated or to le nuclear industry, that are used to evaluate calculations incorporated as a technical specification requirement at of the radioloocal consequences of various postulated peak accident pressure for the first 24 hours2.777778e-4 days <br />0.00667 hours <br />3.968254e-5 weeks <br />9.132e-6 months <br />. and at 50

acciden ts. percent of this leak rate for the remaining duration of the accideint. 2 Peak accident pressure is the maximum1 This guide lists acceptable assumptions that may be pressure defined in the technical specifications for used to evaluate the design basis LOCA of a Pressurized containment leak testing.

Water Reactor (PWR). It should be shown that thc

2 offsite dose consequences will be within thie guidelines Thte effect on coniainnmeni leakage tinder accident of 10 CFR Part 100, conditions of features provided to reduce the leakage ot"

radioactive materials from the containment will be evaluated on

'This guide is a revision of former Safety Guide 4. an individual case basis.

USAEC REGULATORY GUIDES Coples of published guldes may be obtained by request Indicating the divisions desired to the US. Atomic Energy Commission. Washington. 0.1, 20545, Regulatory Guides are issued to describe and make avaliable to the public Attention: Director of Regulatory Standards. Comments and tuggrsilons for methods acceptable to the AEC Regulatory staff of Implementing specific parts of impfrovements In these guides ere encouraged end should be sent to the Secretary the Commission's regulations, to delineate techniques used by the staff in of the Commission, US. Atomic Energy Commission, Washington. O.C. 20545.

evaluating specific problems or postulated accid3nts. or to provide guidance to Attention: Chief, Public Proceedings Staff.

applicants. Regulatory Guides are not substitutes for regulations and compliance with them is not required. Methods and solutlons different from those set out in The guides are issued In the following ten broad divliions:

the guides will be acceptable if they provide a basis for the findings requisite to 8. Products the issuance or continuance of a permit or license by the Comrrssio

n.

1. Power Reactors

2. Researcha nd Tast Reactors

7. Transportation

3. Fuels and Materials Facilities 8. Occupational Health Published guides will be revised periodically, as appropriate, to accommodate 4. Environmental end Siting 9. Antlitrust Review comments and to reflect new informatio" or experience. 5. Materials and Plant Protection 1

0. General

.1

2. Acceptable assumptions for atmospheric diffusion From a semi-infinite cloud, the gamma dose rate in air and dose conversion are: is:

a. The 0-8 hour ground level release concentrations may be reduced by a factor ranging from ,D = 0,25E

one to a maximum of three (.see Figure I) for additional dispersion produced by the turbulent wake of the Where reactor building in calculating potential exposures. The volumetric building wake correction, as defined in beta dose rate from an infinite cloud (rad/sec)

section 3.3.5.2 of Meteorology and Atomic Energy gamma dose rate from an infinite cloud

1968. should be used only in the 0-8 hour period: it is (rad/sec)

used with a shape factor of 112 and the minimum EO3= average beta energy per disintegration cross-sectional area of the reactor building only. (Mev/dis)

b. No correction should be made for depletion of' E = average gamma energy per disintegration the effluent plume of radioactive iodine due to (Mev/dis)

deposition on the ground, or for the radiological decay X = concentration of beta or gamma emilling of iodine in transit. isotope in the cloud (curie/m3)

c. For the first 8 hours9.259259e-5 days <br />0.00222 hours <br />1.322751e-5 weeks <br />3.044e-6 months <br />, the breathing rate of persons offsite should be assumed to be 3.47 x 10' f. The following specific assumptions are cubic meters per second. From 8 to 24 hours2.777778e-4 days <br />0.00667 hours <br />3.968254e-5 weeks <br />9.132e-6 months <br /> following acceptable with respect to the radioactive cloud dose the accident, the breathing rate should be assumed to be calculations:

1.75 x 104 cubic meters per second. After that until the (1) The dose at any distance from the reactor end of the accident, the rate should be assumed to be should be calculated based on the maximum

2.32 x 104 cubic meters per second. (These values were concentration in the plume at that distance taking into developed from the average daily breathing rate [2 x 107 account specific meteorological, topographical, and cnv'/dayJ assumed in the report of ICRP, Committee other characteristics which may affect the maximum

11-1959.) plume concentration. These site related characteristics d. The iodine dose conversion factors are given in must be evaluated on an individual case basis. In the case ICRP Publication 2, Report of Committee 11, of beta radiation, the receptor is assumed to be exposed

"Permissible Dose for Internal Radiation," 1959. to an infinite cloud at the maximum ground level e. External whole body doses should be calculated concentration at that distance from the reactor. In the using "Infinite Cloud" assumptions, i.e., the dimensions case of gamma radiation, the receptor is assumed to be of the cloud are assumed to be large compared to the exposed to only one-half the cloud owing to the distance that the gamma rays and beta particles travel. presence of the groun

d. The maximum cloud

"Such a cloud would be considered an infinite cloud for concentration always should be assumed to be at ground a receptor at the center because any additional [gamma level.

and] beta emitting material beyond the cloud (2) The appropriate average beta and gamma dimensions would not alter the flux of [gamma rays energies emitted per disintegration, as given in the Table and] beta particles to the receptor" (Meteorology and of Isotopes, Sixth Edition, by C. M. Lederer, J. M.

Atomic Energy, Section 7.4. .1.-editorial additions Hollander, I. Perlman; University of California, Berkeley, made so that gamma and beta emitting material could be Lawrence Radiation Laboratory; should be used.

considered). Under these conditions the rate of energy absorption per unit volume is equal to the rate of energy g. The atmospheric diffusion model should be as released per unit volume. For an infinite uniform cloud follows:

containing X curies of beta radioactivity per cubic meter (1) The basic equation for atmospheric the beta dose in air at the cloud center is: diffusion from a ground level point source is:

D! = 0.457 EOX

X/Q= ruaya The surface body dose rate from beta emitters in the infinite cloud can be approximated as being one-half this Where amount (i.e., 0DD' = 0.23 E'X).

X = the short term average centerline value of the ground level concentration (curie/meter3)

For gamma emitting material the dose rate in air at the Q = amount of material released (curie/see)

u = windspeed (meter/see)

uloud center is:

y = the horizontal standard deviation of the plume (meters) [See Figure V-I. Page 48.

7 .D = 0.507 Ey(

Nuclear Safety, June 1961, Volume 2.

1.4-2

Number 4, "Use of Routine Meteorolo-ical Time Observations for Estimating Atmospcheric Following Dispersion," F. A. Gifford. Jrj.. Accident Atmospheric Conditions o" = the vertical standard deviation cf the pluii.e (meters) ISee Figure V-2, Page 48, Nuclear 0.8 hours9.259259e-5 days <br />0.00222 hours <br />1.322751e-5 weeks <br />3.044e-6 months <br /> Pasquill Type F. wiudspeed I meter/sec.

Safqev', June 19(1. Volume 2. Number

4. uniform direction

"Use of Routlinc Me leorological Oh,'ervations for Estimating Atmospheric 8-24 hours Pasquill Type F, windspced I metcr/s.c.

Dispersion," F. A. G;ifford. Jr.I variable direction within a 22.5" sector

(.2) For lime periods of greater than 8 hours9.259259e-5 days <br />0.00222 hours <br />1.322751e-5 weeks <br />3.044e-6 months <br /> the plume shouid hI assumed to meander and spread 1-4 days (a) 4(Y,,%( Pasquill Type D. windspeed 3 tini*ormly ovcr a 22.i" sector. The resultlant e'quaition is: rilel r/sec (b) 600,, Pasquill Type F. windspeed 2 leter/sec

2.032 x/Q = lx (W' wind direction v: riabie within a 22._.

sector

\Vhicrc

4-30 days (a) 33.35, Pasquill Type C, windspeed 3 x distance from point of release to the receptor;. meter/sec other variables are as given in g( 1). (N) 33.3%'. Pasquill Type D. windspeed 3 ineter/sec

(3) Tlhe at mospheric diffusion model" for (c) 33.3%; Pasquill Type F, wirdspeed 2 ground level releases is based on the information in the viieter/sec following lable. (d) Wind direction 33.3,:, frequency in a

22.50 sector

-This niIdo.l' %liould be useud until adequate site metcorologic'al d:ta are obtained. In some ,-uses. available information. such u,; tnic*orology. topography and geovaphicut. (4) Figures 2A and 213 give the groud level tocalion. may dictate Itic use of a more restrictive model to release atmospheric diffusion factors based on the insurc a conscrvative eltimuie of potentla oflfsitc exposures. parameters given in g( 3).

1.4-3

bI .1-GiAK

buPRIP IOýAO

2.5 FIGURE 1

2 O.SA-SO meters

0 P'mtr

2

4.

0 .5A-1000 -nws O.SA-2500atr

2 meti

2 O.BA-1500 motors 0.5A-3000meru p. O.5A-2000 metonus ý

w

0

ccI

zI

w1.5

4 I

uII

I I i . . I *

10w Distance from Structure (metars)

I

III _ . II

3 L

FIGL

S1i .. _.

10-A

I

a- ... *-

- -- -- ......

7----

0

4--I

0\

1 o * . '1  %

Ditne rmSrut- (ees

44sanc4m .tu. St . .. tes

1.4-5

d*

10- I

I

I I A ...; I .... 1 1

.", . - - -I.-- I--,- - .-*"i ... v - .1 - 1 %ý

FIGURE 2(81 -

_____0-8 hours7~

.. ,D L

IU

E

.1.N.. ' I I I*

  • I

.  %, . . :.

0

7  :::::

t~rV~

F-W 0 * -,pI * . 'I

X1

'V

,

-,I- -

-7I

10

163

..~.i... I_... ... 1. 1ý 10. 5 b

-

7 1 Distance from Structure (maters)

1.4-6