Regulatory Guide 1.99: 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 1: Line 1:
{{Adams
{{Adams
| number = ML003740284
| number = ML12298A136
| issue date = 05/31/1988
| issue date = 04/30/1977
| title = (Task Me 305-4) Revision 2 Radiation Embrittlement of Reactor Vessel Materials
| title = Effects of Residual Elements on Predicted Radiation Damage to Reactor Vessel Materials
| author name =  
| author name =  
| author affiliation = NRC/RES
| author affiliation = NRC/RES
Line 10: Line 10:
| license number =  
| license number =  
| contact person =  
| contact person =  
| document report number = RG-1.99, Rev 2
| document report number = RG-1.099, Rev. 1
| document type = Regulatory Guide
| document type = Regulatory Guide
| page count = 10
| page count = 7
}}
}}
{{#Wiki_filter:Revlalon 2 May 1988 U.S. NUCLEAR REGULATORY  
{{#Wiki_filter:RE U.S. NUCLEAR REGULATORY  
COMMISSION
COMMISSION  
iREGULATORY
A)REGULATORY
GUIDE OFFICE OF NUCLEAR REGULATORY
GUIDE OFFICE OF STANDARDS
RESEARCH REGULATORY  
DEV9LOPMENT
GUIDE 1.99 (Task ME 3054) RADIATION  
REGULATORY  
EMBRITrLEMENT
GUIDE 1.99 EFFECTS OF RESIDUAL ELEMENTS ON PREDICTED
OF REACTOR VESSEL MATERIALS  
RADIATION  
DAMAGE TO REACTOR VESSEL MATERIALS ,vision 1 priI 1977


==A. INTRODUCTION==
==A. INTRODUCTION==
General Design Criterion  
General Design Criterion  
31, "Fracture Prevention of Reactor Coolant Pressure Boundary," of Appendix A, "'General Design Criteria for Nuclear Power Plants," to 10 CFR Part 50, "Domestic Licensing of Production and Utilization Facilities," requires, in part, that the reactor coolant pressure boundary be designed with sufficient margin to ensure that, when stressed under operating, maintenance, testing, and postulated accident conditions, (l) the boundary behaves in a nonbrittle manner and (2) the probability of rapidly propagating fracture is minimized.
31, "Fracture Prevention of Reactor Coolant Pressure Boundary," of Appen-dix A, "General Design Criteria for Nuclear Power Plants," to 10 CFR Part 50, "Licensing of Produc-tion and Utilization Facilities," requires, in part, that the reactor coolant pressure boundary be designed with sufficient margin to ensure that, when stressed under operating maintenance, testing, and postulated accident conditions, (1) the boundary behaves in a nonbrittle manner and (2) the probability of rapidly propagating fracture is minimized.


General Design Criterion
Appendix G, "Fracture Toughness Re-quirements," and Appendix H, "Reactor.
31 also requires that the design reflect the uncertainties in determining the effects of irradiation on material properties.


Appendix 0, "Fracture Toughness Requirements," and Appendix H, "Reactor Vessel Material Surveillance Program Requirements," which implement, in part, Criterion  
Vessel Material Surveillance Program Requirements," which were added to 10 CFR Part 50 effective August 16, 1973, to implement, in part, Criterion  
31, necessitate the calculation of changes in fracture toughness of reactor vessel materials caused by neutron radiation throughout the Service life. This guide describes general procedures acceptable to the NRC staff for calculating the effects of neutron radiation embrittlement of the low-alloy steels currently used for light-water-cooled reactor vessels.
31, neces-sitate the prediction of the amount of radiationdamage to the reactor vessel of water-cooled power* reactors throughout its service life.This guide describes general procedures acceptable to the NRC staff as an interim basis* for predicting the effects of the residual elements copper and phosphorus on neutron radiation damage to the low-alloy steels currently used for light-Water-cooled reac-** tor vessels. The Advisory Committee on Reactor Safeguards has been consulted concerning this guide and has concurred in the regulatory position.
 
The calculative procedures given in Regulatory Position 1. 1 of this guide are not the same as those given in the Pressurizod Thermal Shock rule (§ 50.61, "Fracture Toughness Requirements for Pro tection Against Pressurized Thermal Shock Events," of 10 CFR Part 50) for calculating RTPTS, the reference temperature that is to be compared to the screening criterion given in the rule. The information on which this Revision 2 is based may also affect the basis for the PTS rule. The staff is presently considering whether to propose a change to § 50.61.  The Advisory Committee on Reactor Safeguards has been con sulted concerning this guide and has concurred in the regulatory position.
 
Any information collection activities mentioned in this regulatory guide are contained as requirements in 10 CFR Part 50, which pro vides the regulatory basis for this guide. The information collec-tien requirements in 10 CFR Part 50 have been cleared under OMB Clearance No. 3150-0011.


==B. DISCUSSION==
==B. DISCUSSION==
Some NRC requirements that necessitate calculation of radia tion embrittlement are: 1. Paragraph V.A of Appendix 0 requires the effews of neutron radiation to be predicted from the results ofperdnent radiation effcts studies. This guide provides such results in the form of calculative procedures that are acceptable to the NRC. 2. Paragraph V.B of Appendix 0 describes the basis for setting the upper limit for pressure as a function of temperature during heatup and cooldown for a given service period in terms of the predicted value of the adjusted reference temperature at the end of the service period. 3. The definition of reactor vessel betline given in Paragraph
The principal examples of NRC requirements that necessitate prediction of radiation damage are:* Research and construction experience with low-residual-element compositions of these steels is accumulating rapidly and is ex-pected to provide a firm basis for acceptable procedures in the near future."*Lines indicate substantive changes from previous issue.1. Paragraph II.H of Appendix G defines the beltline in terms of a predicted adjustment of reference temperature at end of service life in excess of 50 0 F; paragraphs III.C and IV.B specify the ad-ditional test requirements for beltline materials that supplement the requirements for reactor vessel materials generally.
11.F of Appendix G requires identification of regions of the reactor vessel that are predicted to experience sufficient neutron radiation embrittlement to be considered in the selection of the most limiting material.


Paragraphs M.A and IV.A.1 specify the additional test requirements for beitlie materials tha supplement the requirements for reactor vessel materials generally.
2. Paragraph II.C.3 of Appendix H establishes the required number of surveillance capsules on the basis of the predicted adjusted reference temperature at the end of service life. In addition, withdrawal of the first capsule (when four or more are required)
 
is to occur when the predicted adjustment of reference temperature is approximately
4. Paragraph n.B of Appendix H incorporates ASTM E 185 by reference.
50°F or at one-fourth of the service life, whichever is earlier.3. Paragraph IV.C of Appendix G requires that vessels be designed to permit a thermal annealing treatment if the predicted value of adjusted reference temperature exceeds 200°F during their service life.4. Paragraph II.B of Appendix H incorporates ASTM E185-73 by reference.


Paragraph  
Paragraph  
5.1 of ASTM E 18542, "Standard Prac tice for Conducting Surveillance Tests for Light-Water Cooled Nuclear Power Reactor Vessels" (Ref. 1), requires that the materials to be placed in surveillance be those that may limit operation of the reactor during its lifetime, ie., those expected to have the highest adjusted reference temperature or the lowest Charpy upper-shelf energy at end of life. Both measures of radiation embrittlement must be considered.
4.1 of ASTM E185-73 requires that the materials, to be placed in surveillance be those that may limit opera-tion of the reactor during its lifetime, i.e., those ex-pected to have the highest adjusted reference temperature or the lowest Charpy upper-shelf energy at end of life. Both measures of radiation damage must be considered.
 
In Paragraph
7.6 of ASIM E 185-32, the require ments for the number of capsules and the withdrawal schedule are based on the calculated amount of radikton embrittlement at end of lif
 
====e. USNRC REGULATORY ====
GUIDES The guides are Issued In the following ten broad divisions:
Regulatory Guides are issued to describe and make available to the public methods acceptable to the NRC staff of impieenting
1. Power Reactors 6. Products specific parts of the Commission's regulations, to delineate tech. 2. Research and Test Reactors 7. Transportation niques used by the staff In evaluating specific problems or postu- 3. Fuels and Materials Facilities
8. Occupational Health lated accidents or to provide guidance to applicants.
 
Regulatory
4. Environmental and Siting 9. Antitrust and Financial Review Guides are not substitutes for regulations, and compliance with 5. Materlals and Plant Protection
10. General them is not required.
 
Methods and solutions different from those set out In the guides will be acceptable if they provide a basis for the findings requisite to the issuance or continuance of a permit or be purchased from the Government licenseInting Office at the current GPO price. information on current GPO prices may be obtained by contacting the Superintendent-of This guide was issued after consideration of comments received from Documents, U.S. Government Printing Office, Post Office Box the public. Comments and suggestions for improvements in these 37082, Washington, DC 20013-7082, telephone
(202)275-2060
or guides are encouraged at all times, and guides will be revised, as (202)275-2171.


arpropriate, to accommodate comments and to reflect new informa tion or experience.
5. Paragraph V.B of Appendix G describes the basis for setting the upper limit for pressure as a func-tion of temperature during heatup and cooldown for a given service period in terms of thepredicted value of the adjusted reference temperature at the end of the service period.The two measures of radiation damage used in this guide are obtained from the results of the Charpy V-USNRC REGULATORY
GUIDES Comments should be sent to the Secretary of the Commission, US. Nuclear Regu-latory Commission, Washington, D.C. 20555, Attention:
Docketing and Service Regulatory Guides are issued to describe and make available to the public methods Branch.acceptable to the NRC staff of implementing specific parts of the Commission's regulations, to delineate techniques used by the staff in evaluating specific problems The guides are issued in the following ten broad divisions:
or postulated accidents, or to provide guidance to applicants.


issued guides may also be purchased from the National Technical Written comments may be submitted to the Rules and Procedures Information Service on a standing order basis. Details on this Branch, ORR ADM, U.S. Nuclear Regulatory Commission, service may be obtained by writing NTIS, 5285 Port Royal Road.  Washington, DC 20555. Springfield, VA 22161.
Regulatory Guides are not substitutes for regulations, and compliance with them is not required.


The two measures of radiation embrittlement used in this guide are obtained from the results of the Charpy V-notch impact test. Appendix U to 10 CFR Part 50 requires that a full curve of absorbed energy versus temperature be obtained through the ductile-to-brittle transition temperature region. The adjustment of the reference temperature, &RTNDT, is defined in Appendix 0 as the tempera ture shift in the Charpy curve for the irradiated material relative to that for the unirradiated material measured at the 30-foot-pound energy level, and the data that formed the basis for this guide were 30-foot-pound shift values. The second measure of radiation embrittlement is the decrease in the Charpy upper-shelf energy level, which is defined in ASTM B 185-82. This Revision 2 updates the calculative procedures for the adjustment of reference temperature;
1. Power Reactors 6. Products Methods and solutions different from those set out in the guides will be accept- 2. Research and Test Reactors 7. Transportation able if they provide a basis for the findings requisite to the issuance or continuance
however, calculative procedures for the decrease in upper-shelf energy are unchanged because the preparatory work had not been completed in time to include them in this revision.
3. Fuelsand Materials Facilities
8. Occupational Health 4. Environmental and Siting 9. Antitrust Review of a permit or license by the Commission.


The basis for Equation 2 for ARTNDT (in Regulatory Position 1.1 of this guide) is contained in publications by 0. L. Guthrie (Ref.  2) and G. R. Odette et al. (Ref. 3). Both of these papers used surveillance data from commercial power reactors.
5. Materials and Plant Protection
10. General Comments and suggestions for improvements in these guides are encouraged at all Requests for single copies of issued guides (which may be reproduced)  
or for place-times, and guides will be revised, as appropriate, to accommodate comments and ment on an automatic distribution list for single copies of future guides in specific to reflect new information or experience.


The bases for their regression correlations were different in that Odette made greater use of physical models of radiation embrittlement.
This guide was revised as a result of divisions should be made in writing to the US. Nuclear Regulatory Commission, substantive comments received from the public and additional staff review. Washington, D.C. 20555, Attention:
Director.


Yet, the two papers contain similar recommendations:
Division of Document Control.
(1) separate correla tion functions should be used for weld and base metal, (2) the func tion should be the product of a chemistry factor and a fluence factor, (3) the parameters in the chemistry factor should be the elements copper and nickel, and (4) the fluence factor should provide a trend curve slope of about 0.25 to 0.30 on log-log paper at 10"9 n/cm 2 (E > 1 MeV), steeper at low fluences and flatter at high fluences.


Regulatory Position 1.1 is a blend of the correlation functions presented by these authors. Some test reactor data were used as a guide in establishing a cutoff for the chemistry factor for low copper materials.
notch impact test. Appendix G to 10 CFR 'Part 50 re-quires that a full curve of absorbed energy versus temperature be obtained through the ductile-to- brittle transition temperature region. The latter is located by the reference temperature, RTNDT, which is defined in paragraph II.F of Appendix G. The"shift" of the adjusted reference temperature is defined in Appendix G as the temperature shift in the Charpy V-notch curve for the irradiated material relative to that for the unirradiated material, measured at the 50-foot-pound energy level or measured at the 35-mil lateral expansion level, whichever temperature shift is greater. In using published data that report only the temperature shift measured at the 30-foot-pound energy level, it has been assumed herein that the adjustment of the reference temperature is equal to the 30-foot-pound shift.The second measure of radiation damage is the decrease in the Charpy upper-shelf energy level. In the absence of a standard definition, the upper-shelf energy is defined herein as the average energy value for all specimens whose test temperature is above the upper end of the transition temperature region. Nor-mally, at least three specimens should be included;more specimens should be included when the shelf ,level appears to be marginal.


The data base for Regulatory Position 1.2 is that given by Spencer H. Bush (Ref. 4).  The measure of fluence used in this guide is the number of neutron per square centimet having energies greater than I million electron volts (E > I MeM). The differences in energy spectra at the surveillance capsule and the vessel inner surface locations do not appear to be great enough to warrant the use of a damage func tion such as displacements per atom (dpa) (Ref. 5) in the analysis of the surveillance data base (Ref. 6).  Howeve, te neutron energ spectrum does change significantly with location in the vessel wall; hence for calculating the attenua tion of radiation embrittlement through the vessel wall, it is necessary to use a damage function to determine ARTNDT versus radial distance into the wall. Te most widely accepted damage flnc tion at this time is dpa, and the attenuation formula (Equation
However, if specimens are tested in sets of three at each test temperature, the set having the highest average may be regarded as defining the upper-shelf energy.The measure of fluence used herein is the number of neutrons per square centimeter (E>I MeV). An as-sumed fission-spectrum energy distribution was used in calculating the fluence for most of the data base.*However, for application to a reactor vessel, the calculated spectrum is used to predict fluence at a given location in the wall. This procedure is not in-tended to preclude future use of data that are given in terms of neutron damage fluence.As used herein, references to "% Cu" and "% P" mean the weight percent of copper and phosphorus as measured in the surveillance program per ASTM E185-73. However, if such results are not available, the results of a product analysis may be used.Use of the procedures for prediction of radiation damage given in the regulatory position should be limited to irradiation at 550 +/-251F, because temperature is important to damage recovery proces-ses. As a guideline, irradiation at 4501F has been shown to cause twice the adjustment of reference temperature and irradiation at 650°F, about half the ladjustment produced by irradiation at 550OF for the fluence levels and the steels cited in the regulatory
3) given in Regulatory Position 1. 1 is based on the attenuation of dpa through the vessel wall.  Sensitivity to neutron radiation embrittlemetnt may be affected by elements other than copper and nickel. The original version and Revision I of this guide had a phosphorus term in the chemistry factor, but the studies on which this revision was based ftond other elements such as phosphorus to be of secondary importance, i.e., including them in the analysis did not produce a significantly bet ter fit of the data.  Scatter in'the data base used for this guide is relatively signifi cant, as evidenced by the fact that the standard deviations for Guthrie's derived formulas (Ref. 2) are 287OF for welds and 17OF for base metal despite extensive efforts to find a model that reduced the fitting error. Thus the use of surveillance data from a given reactor (in place of the calculative procedures given in this guide) requires considerable engineering judgment to evaluate the credibil ity of the data and assign suitable margins. When surveillance data from the reactor in question become available, the weight given to them relative to the information in this guide will depend on the credibility of the surveillance data as judged by the following criteria:
*The data base for this guide is that given by Spencer H. Bush,"Structural Materials for Nuclear Power Plants." 1974 ASTM Gil-lett Memorial Lecture, published in ASTM Journal of Testing and Evaluation, Nov. 1974, and its addendum, "Radiation Damage in Pressure Vessel Steels for Commercial Light-Water Reactors." position when the copper content is about 0.15%. The effects of irradiation temperature on decrease in shelf energy should be considered qualitatively similar to those cited for the adjustment of referencej temperature.
1. Materials in the capsules should be those judged most likely to be controlling with regard to radiation embrittlement according to the recommendations of this guide. 2. Scatter in the plots of Charpy energy versus temperature for the irradiated and unirradiated conditions should be small enough to permit the determination of the 30-foot-pound temperature and the upper-shelf energy unambiguously.


3. When there are two or more sets of surveillance data from one reactor, the scatter of ARTNDT values about a best-fit line drawn as described in Regulatory Position 2.1 normally should be less than 287F for welds and 17oF for base metal. Evenifthe fluence range is large (two or more orders of magnitude), the scatter should not exceed twice those values. Even if the data fail this criterion for use in shift calculations, they may be credible for determining decrease in upper-shelf energy if the upper shelf can be clearly deter mined, following the definition given in ASTM E 185-82 (Ref, I).  4. The irradiation temperature of the Charpy specimens in the capsule should match vessel wall temperature at the cladding/base metal interface within +/-25OF.  5. The surveillance data for the correlation monitor material in the capsule should fall within the scatter band of the data base for that material.
Sensitivity to neutron embrittlement may be af-fected by other residual elements such as vanadium and by deoxidation practice, as indicated by the findings of current research.


To use the surveillance data from a specific plant instead of Regulatory Position 1, one must develop a relationship of ARTNDT to fluence for that plant. Because such data are limited in number and subject to scatter, Regulatory Position 2 describes a procedure in which the form of Equation 2 is to be used and the fluence fac tor therein is retained, but the chemistry factor is determined by the plant surveillance data. Of several possible ways to fit such data, the method that minimizes the sums of the squares of the error was chosen somewhat arbitrarily.
In predicting radiation damage for materials that differ in chemical content or deoxidation practice from those that make up the data base, such findings should be considered.


Its use is justified in part by the fact that "least squares" is a common method for curve fitting.
Other residual elements, notably sulfur, impair the initial Charpy shelf energy of these materials, and their con-tent should be kept low. Clearly, it is the remaining toughness at end of life or at some other critical period that is important.


Also, when there are only two data points, the least squares method gives greater weight to the point with the higher ARTNDT; this seems reasonable for fitting surveillance data, because generally the higher data point will be the more recent and therefore will rePre sent more moderm proced- e.  C. REGULATORY
Such toughness may be given in terms of the margin between the operating temperature (nominally
POSITION
550°F) and the limiting temperature based on toughness.


===1. SURVEILLANCE ===
A margin of 200 degrees is desirable to permit safe management of system transients.
DATA NOT AVAILABLE
When credible surveillance data from the reactor in question are not available, calculation of neutron radiation embrittlement of the beldine of reactor vessels of light-water reactors should be based on the procedures in Regulatory Positions
1.1 and 1.2 within the limitations in Regulatory Position 1.3.1.99-2
1.1 AdJusted Reference Temperature The adjusted reference temperature (ART) for each material in the beitline is given by the following expression:
ART W Initial RTNDT + ARTNDT + Margin (1) Initial RTNDT Is the reference temperature for the unirradiated material as defined in Paragraph NB-2331 of Section M of the ASME Boile and Pressure Vessel Code Of. 7). If measured values of initial RTNDT for the material in question are not available, generic mean values for that class* of material may be used if there are sufficient test results to establish a mean and standard devia tion for the class.  ARTNDT is the mean value of the adjustment In reference temperature caused by irradiation and should be calculated as follows: ARTNDT -(CF) f(O.2 8 -0.10 log f) (2) CF (OF) is the chemistry factor, a function of copper and nickel content. CF is given in Table I for welds and in Table 2 for base metal (plates and forgings).
Linear interpolation is permitted.


In Tables 1 and 2 "weight-percent copper" and "weight-percent nickel" are the best-estimate values for the material, which will normally be the mean of the measured values for a plate or forging or for weld samples made with the weld wire heat number that matches the critical vessel weld. If such values are not available, the upper limiting values given in the material specifications to which the vessel was built may be used. If not available, conservative estimates (mean plus one standard deviation)
At full power, the limiting temperature based on toughness is generally
based on generic data may be used ifjustifi on is provided.
150-200 degrees above RTNDT; hence, the latter should not exceed 150-2001F
at end of life. This limit also avoids the problems of providing for annealing, per paragraph IV.C of Appendix G. The levels of residual elements such as copper, phosphorus, sulfur, and vanadium that are required to achieve the limit of 200'F adjusted reference temperature at end of life in a given reactor vessel will depend on the initial values of RTNDT of the beltline materials and on tle" predicted fluence at the particular locations in the vessel where the materials are used.When surveillance data from the reactor in ques-tion become available, the weight given to it relative to the information in this guide should depend on the credibility of the surveillance data as judged by the following criteria: 1. Materials in the capsule should be those judged most likely to be controlling with regard to radiation damage according to the provisions of this guide.2. Scatter in the Charpy data should be small enough to avoid large uncertainty in curve fitting.3. The change in yield strength should be consis-tent with the shift in the Charpy curve.4. The relationship to previous isurveillance data from the same reactor should be consistent with the normal trends of such data. I 5. The surveillance data for the correlation monitor material in the capsule should fall within the scatter band of the data base for that material.1.99-2 C. REGULATORY
POSITION 1. When credible surveillance data from the reac-tor in question are not available, prediction of neutron radiation damage to the beltline of reactor vessels of light water reactors should be based on the following procedures.


If there is no information available, 0.35% copper and 1.0% nickel should be assumed.
a. Reference temperature should be adjusted as a function of fluence and residual element content in accordance with the following expression, within the limits below and in paragraph l.c.A = [40 + 1000(% Cu -0.08)+ 5000 (% P -0.008) ] [f/ 1019]where A = predicted adjustment of reference temperature, OF.f = fluence, n/cm 2 (E>l MeV).% Cu = weight percent of copper.If % CuK 0.08, use 0.08.% P = weight percent of phosphorus.


The neutron fluence at any depth in dMe vessel wall, f(1019 n/cm, E > 1 MeV), is determined as follows: f -fsurf (e -0.24x)(3)where fsurf (10"9 n/cm 2 , E > 1 MeV) is the calculated value of the neutron fluence at the inner wetted surface of the vessel at the location of the postulated defect, and x (in inches) is the depth into die vessel wall measured from the vessel inner (weted) surface.
If % P5K0.008, use 0.008.If the value of A obtained by the above expression exceeds that given by the curve labeled "Upper Limit" in Figure 1, the "Upper Limit" curve should be used. If % Cu is unknown, the "Upper Limit" curve should be used.As illustrated in Figure 1 for selected copper and phosphorus contents, the above expression should be considered valid only for A >50°F and for f( 6 x 10'9 n/cm 2 (E > 1 MeV).b. Charpy upper-shelf energy should be as-sumed to decrease as a function of fluence and copper content as indicated in Figure 2, within the limits listed in paragraph l.c. Interpolation is permitted.


Alternatively, if dpa calculations are made as part of the fluence analysis, the ratio of dpa at the depth in question to dpa at the inner surface may be substituted for the exponential attenuation factor in Equation 3. The fluence factor, fO.28 -0.10 log f, is determined by calcula tion or from Figure 1. "Margin" is the quantity, OF, that is to be added to obtain con servative, upper-bound values of adjusted reference temperature for the calculations required by Appendix G to 10 CFR Part 50.
c. Application of the foregoing procedures should be subject to the following limitations:.
(1) The procedures apply to those grades of SA-302,. 336, 533, and 508 steels having minimum specified yield strengths of 50,000 psi and under and to their welds and heat-affected zones.(2) The procedures are valid for a nominal ir-radiation temperature of 550°F. Irradiation below 5251F should be considered to produce greater damage, and irradiation above 5751F may be con-sidered to produce less damage. The correction factor used should be justified.


2 A Sandr (4) *Th das f" eawtimang Iniia FLT,~ iB genealy deemIlned, fibr the welds withwhihdI
(3) The expression for A is given in terms of fluence as measured by units of n/cm 2 (E > 1 MeV);however, the expression may be used in terms of fluence as measured by units of neutron damage fluence, provided the constant 1019 n/cm 2 (E> 1 MeV) is changed to the corresponding value of neutron damage fluence.(4) Application of these procedures to materials having chemical content beyond that represented by the current data base should be justified by submittal of data.2. When credible surveillance data from the reac-tor in question become available, they may be used to represent the adjusted reference temperature and the Charpy upper-shelf energy of the beltline materials at the fluence received by the surveillance specimens.
d xz a g oncered by d~ii of eli flux (Unde 90 or other); kr uaemtl h SMStnadSeiiain Here, oI is the standard deviation for the initial RTNDT. H a meured value of initial RTNDT for the material in question is available, ol is to be estimated from the precision of the test method. If not, and generic mean values for that class of material are used, oI is the standard deviation obtained from the set of data used to establish the mean.  The standard deviation for hRTNDT, vA, is 28 *F for welds and 17OF for base metal, except that oA need not exceed 0.50 times the mean value of ARTNDT.  1.2 Charpy Upper-Shelf Energy Charpy upper-shelf energy should be assumed to decrease as a function of fluence and copper content as indicated in Figure 2.  Linear interpolation is permitted.


1.3 lnmtations Application of the foregoing procedures should be subject to the following limitations:
a. The adjusted reference temperature of the beltline materials at other fluences may be predicted by: (1) extrapolation to higher or lower fluences from credible surveillance data following the slope of the family of lines in Figure 1 or (2) a straight-line interpolation between credi-ble data on a logarithmic plot.b. To predict the decrease in upper-shelf energy of the beltline materials at fluences other than those received by the surveillance specimens, procedures similar to those given in paragraph  
1. The procedures apply to those grades of SA-302, 336, 533, and 508 steels having minimum specified yield stngh of 50,000 psi and under and to their welds and heat-affected zones.  2. The procedures are valid for a nominal irradiation tmpertr of 550OF. Irradiation below 525 OF should be considered to pro duce greater embrittlement, and irradiation above 590"F may be considered to produce lass embrittlement.
2.a may~be fol-lowed using Figure 2.3. For new plants, the reactor vessel beltline materials should have the content of residual ele-ments such as copper, phosphorus, sulfur, and vanadium controlled to low levels. The levels should be such that the predicted adjusted reference temperature at the 1/4T position in the vessel wall at end of life is less than 200 0 F.
 
The correction factor used should be justified by reference to actual data.  3. Application of these procedures to fluence levels or to cop per or nick content beyond the ranges given in Figure I and Tables 1 and 2 or to materials having chemical compositions beyond the range found in the data bases used for this guide should be justified by submittal of data.
 
===2. SURVEILLANCE ===
DATA AVAILABLE
When two or more credible surveillance data sets (as defined in the Discussion)  
become available from the reactor in question, they may be used to determine the adjusted reference temperature and the Charpy upper-shelf energy of the beltline materials as described in Rrgdatory Positions
2.1 and 2.2, respectively.
 
2.1 Adjusted Reference Temperature The adjusted referce temperature should be obtained as follows. First, if there is dear evidence that the copper or nickel content of the surveillance weld differs from that of the vessel weld, i.e., differs from the average for the weld wire heat number associated with the vessel weld and the surveilance weld, the measured values of ARTNDT should be adjusted by multiplying them by the ratio of the chemistry factor for the vessel weld to that for the surveillance weld. Second, the surveillance data should be fitted using Equation 2 to obtain the relationship of ARTNDT to fluence. To do so, calculate the chemistry factor, CF, for the best fit by multiplying each adjusted ARTNDT by its corresponding fluence factor, summing the products, and dividing by the sum of the squares of the fluence fa&Ltrs. The resulting value of CF when entered in Equation 2 will give the relationship of ARTýT to 1.99-3 TABLE I CHEMISTRY
FACTOR FOR WELDS, OF fluence that fits the plant surveillance data in such a way as to minimize the sum of the squares of the errors. To calculate the margin in this case, use Equation 4; the values given there for OA may be cut in half.  If this procedure gives a higher value of adjusted reference temperature than that given by using the procedures of Regulatory Position 1.1, the surveillance data should be used. If this procedur gives a lower value, either may be used.  For plants having surveillance data that are credible in all respects except that the material does not represen the critical material in the vessel, the calculative procedures in this guide should be used to obtain mean values of sA, ARTNDT. In calculatng the margin, the value of OA may be reduced from the values given in the last paragraph of Regulatory Position 1.1 by an amount to be decided on a case-by-case basis, depending on where the measured values fall relative to the mean calculated for the surveillance materials.
 
2.2 Charpy Upper-Shelf Energy The decrease in upper-shelf energy may be obtained by plot ting the reduced plant surveillance data on Figure 2 of this guide and fitting the data with a line drawn parallel to the existing lines as the upper bound of all the data. This line should be used in preference to the existing graph.1.99-4 0 Nickel, Wt-% r,0 0.20 0.40 0.60 0.80 1.00 1.20 0 20 20 20 20 20 20 20 0.01 20 20 20 20 20 20 20 0.02 21 26 27 27 27 27 27 0.03 22 35 41 41 41 41 41 0.04 24 43 54 54 54 54 54 0.05 26 49 67 68 68 68 68 0.06 29 52 77 82 82 82 82 0.07 32 55 85 95 95 95 95 0.08 36 58 90 106 108 108 108 0.09 40 61 94 115 122 122 122 0.10 44 65 97 122 133 135 135 0.11 49 68 101 130 144 148 148 0.12 52 72 103 135 153 161 161 0.13 58 76 106 139 162 172 176 0.14 61 79 109 142 168 182 188 0.15 66 84 112 146 175 191 200 0.16 70 88 115 149 178 199 211 0.17 75 92 119 151 184 207 221 0.18 79 95 122 154 187 214 230 0.19 83 100 126 157 191 220 238 0.20 88 104 129 160 194- 7ý 223 245 0.21 92 108 133 164 197 229 252 0.22 97 112 137 167 200 232 257 0.23 101 117 140 169 203 236 263 0.24 105 121 144 173 206 239 268 0.25 110 126 148 176 209 243 272 0.26 113 130 151 180 212 246 276 0.27 119 134 155 184 216 249 280 0.28 122 138 160 187 218 251 284 0.29 128 142 164 191 222 254 287 0.30 131 146 167 194 225 257 290 0.31 136 151 172 198 228 260 293 0.32 140 155 175 202 231 263 296 0.33 144 160 180 205 234 266 299 0.34 149 164 184 209 238 269 302 0.35 153 168. 187 212 241 272 305 0.36 158 172 191 216 245 275 308 0.37 162 177 196 220 248 278 311 0.38 166 182 200 223 250 281 314 0.39 171 185 203 227 254 285 317 0.40 175 189 207 231 257 288 320
TABLE2
* CHEMSTRY FACTOR FOR .ASE.METAL, -F Coper, Nickel, Wt-% f 0 0.20 -0.40 0.(Dr 0- o.o ... i.06 .D1.2 u 0.01 0.02 0.03 0.04 0.05 0.06 0.07 0.08 0.09 0.10 0.11 0.12 0.13 0.14 0.15 0.16 0.17 0.18 0.19 20 20 20 20 22 25 28 31 34 37 41 45 49 53 57 61 65 69 73 78 0.20 82 0.21 86 0.22 91 0.23 95 0.24 100 0.25 104 0.26 109 0.27 114 0.28 119 0.29 124 0.30 129 0.31 134 0.32 139 0.33 144 0.34 149 0.35 153 0.36 158 0.37 162 0.38" 166 0.39 171 0.40 175 20 20 20 20 26 31 37 43 48 53 58 62 67 71 75 80 84 88 92 97 102 107 112 117 121 126 130 134 138 142 146 151 155 160 164 168 173 .177 182 185 189 20 20 20 20 26 31 37 44 51 58 65 72 79 85 91 99 104 110 115 120 125 129 134 138 143 148 151 155 160 164 167 172 175 180 184 187 191 196 200 203 207 207 20 20 20 20 26 31 37 44 51 58 65 74 83 91 100 110 118 127 134 142 149 155 161 167 172 176 180 184 187 191 194 198 202 205 209 212 216 220 223 227 231 231 257 20 20 20 20 26 31 37 44 51 58 67 77 86 96 105 115 123 132 141 150 159 167 176 184 191 199 205 211 216 221 225 228 231 234 238 241 245 248 250 254 257.20 20 20 20 26 31 37 44 51 58.  67 77 86 96 106 117 125 135 144 154 164 172 181 190 199 208 216 225 233 241 249 257 255 26 26D 274 264 282 268 290 272 298 275 303 278 308 281 313 285 317 288 320 20 20 20 20 26 31 37 44 51 58 67 77 86 96 106 117 125 135 144 154 165 174 184 194 204 214 "221 230 239 248
 
===3. REQUIREMENT ===
FOR NEW PLANTS For beItline materials in the reactor vessel for a new plant, the content of residual elements such as copper, phosphorus, sulfur, and vanadium should be controlled to low levels.* Tle copper con tent should be such that the calculated adjusted reference temperamure at the 1/4T position in the vessel wall at end of life is less than 200OF. In selecting the optimum amount of nickel to be used, its deleterious effect on radiation embrittlement should be balanced against its beneficial metallurgical effects and its tendency to lower the initial RTNDT.  For mxe jfomtiua, we &e eAppead to ASTM SundaWd Specifcai A 533 (Rde. ).


==D. IMPLEMENTATION==
==D. IMPLEMENTATION==
The purpose of this section is to provide information to applicants and licensees regarding the NRC staff's plans for using this regulatory guide. Except in those cases in which an applicant pro poses an acceptable alternative method for complying with specified portions of the Commission's regulations, the methods described in this guide will be used as follows: 1. The methods described in Regulatory Positions
The purpose of this section is to provide informa-tion to applicants and licensees regarding the NRC staff's plans for utilizing this regulatory guide.This guide reflects current regulatory practice.Therefore, except in those cases in which the appli-cant proposes an acceptable alternative method for complying with specified portions of the Commis-sion's regulations, the positions described in this guide will be used by the NRC staff as follows: 1. The method described in regulatory positions C. 1 and C.2 of this guide will be used in evaluating all predictions of radiation damage called for in Appen-dices G and H to 10 CFR Part 50 submitted on or 1.99-3 after June 1, 1977; however, if an applicant wishes to use the recommendations of regulatory positions C. 1 and C.2 in developing submittals before June 1, 1977, the pertinent portions of the submittal will be evaluated on the basis of this guide.2. The recommendations of regulatory position C.3 will be used in evaluating construction permit ap-plications docketed on or after June 1, 1977;however, if an applicant whose application for con-struction permit is docketed before June 1, 1977, j wishes to use the recommendations of regulatory'
1 and 2 of this guide will be used by the NRC staff in evaluating all predic tions of radiation embrittlement needed to implement Appendices G and H to 10 CFR Par 50.1.99-5
position C.3 of this regulatory guide in developing submittals for the application, the pertinent portions of the application will be evaluated on the basis of this guide.4 1.99-4
2. Holders of licenses and permits should use the methods described in this guide to predict the effect of neutron radiation on reactor vessel materials as required by Paragraph V.A of Appen dix.O to 10 CFR Pat 50, unless they can justify the use of dif ferent methods. The use of the Revision 2 methodology may result in a modification of the pressweýrCpratMr limits contained in Technical Specifications in order to continue to satisfy the requirements of Section V of Appendix 0, 10 CFR Part 50. 3. The recommendations of Regulatory Position 3 are essen tially unchanged from those used to evaluate construction permit applications docketed on or after June 1, 1977.1.99-6 REFERENCES
7w A = [40 + 1000 (% Cu -0.08) + 5000 (% P -0.008)][f/10191 1)400)-ýPl ,, 300 0 C.E 0 200 4-0 100 E 5-50 C., a, IL%I-.I I I I I III~..~~IIIIIIIIIIIIiIIIjTIIII[III
1. American Society for Testing and Materials, "Standard Prac tice for Conducting Surveillance Tests for Light-Water Cooled Nuclear Power Reactor Vessels," ASTM E 185482, July 1982. 2. G. L. Outrie, "'Tupy Tend Curves Based on 177 PWR Data Points," in "LWR Pressure Vessel Surveillance Dosimetry Xm provement Program," NURECICR-3391, Vol.2, prepared by Hanford Engineering Development Laboratory, HEDL-TME 83-22, April 1984.** 3. 0. R. Odette et al., "Physically Based Regression Correlations of Embrittlement Data from Reactor Pressure Vessel Surveillance Programs," Electric Power Research Institute, NP-3319, January 1984.t 4. S. H. Bush, "Structural Materials for Nuclear Power Plants," in Journal of Testing and Eblumlo, American Society for Testing and Materials, November 1974.*S. American Society for Testing and Materials, "Standard Prac tice for Characterizing Neutron Exposures in Ferritic Steels in Terms of Displacements per Atom (DPA)," ASTM E 693-79, August 1979.* 6. W. N. McElroy, "LWR Pressure Vessel Surveillance DosihnetY
i i i L l i i i ~ m- i i 1 11 11am 1 1 1 i i i i i i i i i i i i H HHHHH i i i i i i ! i H HHHHHHi ....II!I I i I I I i I IBI ,JI 0.25;M020
Improvement Program: LWR Power Reactor Surveillance Physics-Dosimetry Data Base Compendium," NUREo/ CR-3319, prepared by Hanford Engineering Development LaborWty, HEDL-TME 85-3, August 1985.** 7. American Society of Mechanical Engineers, Section m, "Nuclear Power Plant Components," 9f ASAE Boier and Pressure Vessel Code, New York (updated frequently).tt
/, rz z0.15% Cu-0.1(Ia I/ f I =I 1.LOWER LIMIT% Cu = 0.08% P = 0.008 2X10 1 7 4 6 8. 10 1 8 2 4 6 8 1019 2 4 6 FLUENCE, n/cm 2 (E > 1MeV)Figure 1 Predicted Adjustment of Reference Temperature, "A", as a Function of Fluence and Copper Content.For Copper and Phosphorus Contents Other Than Those Plotted, Use the Expression for "A" Given on the Figure.
8. American Society for Testing and Materials, "Standard Specifcatio for Pressure Vessel Plates, Alloy Steel, Quenched and Tempered, Manganese-Molybdenum and Manganese Molybdenum-Nickel," ASTM A 533/A 533M-82, Septemlier
1982.**Copies may be obtained foum the American Society for Testing and Mbater'ls, 1916 Race Steet, Pafladdphi, PA 19103.  *Copies may be obtaindum e Superinted of Docm= ,. U.S. Governme Printing Office, Post Office Box 37092, Wasington, DC 200D13-7062.


tclsmay be obtained how the ecrcPower Research Insftitut
~~~U.,3UU
3412 Killview Avenue, Palo Alto, CA 9430. t1o1smay be obtained fromn Se American Society of Mechanical Engineers, 345 E. 471h Sawee, New York, KY 10017.1.99-7
.-20 0.25-- -------- 0.20 -0.15-0.15 0.10-- W wL IT C,"___ O. 10---.05 ---I Z 2 11 4 6 8 08 6 8 1092 4 6 FLUENCE, n/cm 2 (E > 1MeV)Figure 2 Predicted Decrease in Shelf Energy as a Function of Copper Content and Fluence.Aftk --
2 3 4 6 6 7 8 10,, Fluence, n/cm 2 (E > I MOV)2 3 .4 6 6 7-8.91 w10 FIGURE I Flummo Factor for Use ia Equation 2, the Expression for ARTNDT 0 am " U" 9 0 -UJ S " 0I1 S..lost 2' 3 4 6 6 7 8u 1 1014;L u ............. ....  .........  1.G it ........ ..... ...a l. ....  .8 ............ .. 11HP .. ....7 .76....  .....". ...I 1 1 , i l5 H IM.1 -flfl .6. ......  .......1 1 1 1 1 -z ....  -.4 ...... ..  7 -T iI oio
UNITED STATES NUCLEAR REGULATORY
60 50 40 30 20 10 0.10 -0.05 jHHHHHHill P.PfPIIPPI
COMMISSION
I pl`j-Vý 'A:i huh-10F i iii i i 1 1 1 1 1 1 11 1 Illlll 1 m1;1 1 K!1 1 !t!2 X 10 1 7 4 6 8 1018 2 4 6 8 1019 FLUENCE, n/cm 2 (E > 1MeV) FIGURE 2 Predicted Decrease in Shelf Energy as a Function of Copper Content and Fluence p -!11I I I I Ih I mII I I I IT Ilf ~~l7 I % COPPER BASE METAL WELDS 0.35 0.30 0.30 0.25 0,25 0.20 0.20 0,15 0.15 -0.10--C u'p 0) C 2 4 6-1 .... -.... 11.1 ........
WASHINGTON, D.C. 20555 OFFICIAL BUSINESS PENALTY FOR PRIVATE USE, $300 POSTAGE AND FEES PAID U.S. NUCLEAR REGULATORY
REGULATORY
COMMISSION
ANALYSIS A copy of the regulatory analysis prepared for this Regulatory Guide 1.99, Revision 2, is available for inspection and copying for a fee at the Comnmission's Public Document Room at 1717 H Stree NW., Washington, DC, under Regulatory Guide 1.99, Revision 2.1.99-10}}
UCi' 7-L NN r? C ULFLL F U EF l",%:PEFLC
110N t, [F R C E U 3 1 AUFAVENI K TN rc 0 F P R US i A PA 1'J4Lu/}}


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

Revision as of 12:00, 15 July 2019

Effects of Residual Elements on Predicted Radiation Damage to Reactor Vessel Materials
ML12298A136
Person / Time
Issue date: 04/30/1977
From:
Office of Nuclear Regulatory Research
To:
References
RG-1.099, Rev. 1
Download: ML12298A136 (7)


RE U.S. NUCLEAR REGULATORY

COMMISSION

A)REGULATORY

GUIDE OFFICE OF STANDARDS

DEV9LOPMENT

REGULATORY

GUIDE 1.99 EFFECTS OF RESIDUAL ELEMENTS ON PREDICTED

RADIATION

DAMAGE TO REACTOR VESSEL MATERIALS ,vision 1 priI 1977

A. INTRODUCTION

General Design Criterion 31, "Fracture Prevention of Reactor Coolant Pressure Boundary," of Appen-dix A, "General Design Criteria for Nuclear Power Plants," to 10 CFR Part 50, "Licensing of Produc-tion and Utilization Facilities," requires, in part, that the reactor coolant pressure boundary be designed with sufficient margin to ensure that, when stressed under operating maintenance, testing, and postulated accident conditions, (1) the boundary behaves in a nonbrittle manner and (2) the probability of rapidly propagating fracture is minimized.

Appendix G, "Fracture Toughness Re-quirements," and Appendix H, "Reactor.

Vessel Material Surveillance Program Requirements," which were added to 10 CFR Part 50 effective August 16, 1973, to implement, in part, Criterion

31, neces-sitate the prediction of the amount of radiationdamage to the reactor vessel of water-cooled power* reactors throughout its service life.This guide describes general procedures acceptable to the NRC staff as an interim basis* for predicting the effects of the residual elements copper and phosphorus on neutron radiation damage to the low-alloy steels currently used for light-Water-cooled reac-** tor vessels. The Advisory Committee on Reactor Safeguards has been consulted concerning this guide and has concurred in the regulatory position.

B. DISCUSSION

The principal examples of NRC requirements that necessitate prediction of radiation damage are:* Research and construction experience with low-residual-element compositions of these steels is accumulating rapidly and is ex-pected to provide a firm basis for acceptable procedures in the near future."*Lines indicate substantive changes from previous issue.1. Paragraph II.H of Appendix G defines the beltline in terms of a predicted adjustment of reference temperature at end of service life in excess of 50 0 F; paragraphs III.C and IV.B specify the ad-ditional test requirements for beltline materials that supplement the requirements for reactor vessel materials generally.

2. Paragraph II.C.3 of Appendix H establishes the required number of surveillance capsules on the basis of the predicted adjusted reference temperature at the end of service life. In addition, withdrawal of the first capsule (when four or more are required)

is to occur when the predicted adjustment of reference temperature is approximately

50°F or at one-fourth of the service life, whichever is earlier.3. Paragraph IV.C of Appendix G requires that vessels be designed to permit a thermal annealing treatment if the predicted value of adjusted reference temperature exceeds 200°F during their service life.4. Paragraph II.B of Appendix H incorporates ASTM E185-73 by reference.

Paragraph

4.1 of ASTM E185-73 requires that the materials, to be placed in surveillance be those that may limit opera-tion of the reactor during its lifetime, i.e., those ex-pected to have the highest adjusted reference temperature or the lowest Charpy upper-shelf energy at end of life. Both measures of radiation damage must be considered.

5. Paragraph V.B of Appendix G describes the basis for setting the upper limit for pressure as a func-tion of temperature during heatup and cooldown for a given service period in terms of thepredicted value of the adjusted reference temperature at the end of the service period.The two measures of radiation damage used in this guide are obtained from the results of the Charpy V-USNRC REGULATORY

GUIDES Comments should be sent to the Secretary of the Commission, US. Nuclear Regu-latory Commission, Washington, D.C. 20555, Attention:

Docketing and Service Regulatory Guides are issued to describe and make available to the public methods Branch.acceptable to the NRC staff of implementing specific parts of the Commission's regulations, to delineate techniques used by the staff in evaluating specific problems The guides are issued in the following ten broad divisions:

or postulated accidents, or to provide guidance to applicants.

Regulatory Guides are not substitutes for regulations, and compliance with them is not required.

1. Power Reactors 6. Products Methods and solutions different from those set out in the guides will be accept- 2. Research and Test Reactors 7. Transportation able if they provide a basis for the findings requisite to the issuance or continuance

3. Fuelsand Materials Facilities

8. Occupational Health 4. Environmental and Siting 9. Antitrust Review of a permit or license by the Commission.

5. Materials and Plant Protection

10. General Comments and suggestions for improvements in these guides are encouraged at all Requests for single copies of issued guides (which may be reproduced)

or for place-times, and guides will be revised, as appropriate, to accommodate comments and ment on an automatic distribution list for single copies of future guides in specific to reflect new information or experience.

This guide was revised as a result of divisions should be made in writing to the US. Nuclear Regulatory Commission, substantive comments received from the public and additional staff review. Washington, D.C. 20555, Attention:

Director.

Division of Document Control.

notch impact test. Appendix G to 10 CFR 'Part 50 re-quires that a full curve of absorbed energy versus temperature be obtained through the ductile-to- brittle transition temperature region. The latter is located by the reference temperature, RTNDT, which is defined in paragraph II.F of Appendix G. The"shift" of the adjusted reference temperature is defined in Appendix G as the temperature shift in the Charpy V-notch curve for the irradiated material relative to that for the unirradiated material, measured at the 50-foot-pound energy level or measured at the 35-mil lateral expansion level, whichever temperature shift is greater. In using published data that report only the temperature shift measured at the 30-foot-pound energy level, it has been assumed herein that the adjustment of the reference temperature is equal to the 30-foot-pound shift.The second measure of radiation damage is the decrease in the Charpy upper-shelf energy level. In the absence of a standard definition, the upper-shelf energy is defined herein as the average energy value for all specimens whose test temperature is above the upper end of the transition temperature region. Nor-mally, at least three specimens should be included;more specimens should be included when the shelf ,level appears to be marginal.

However, if specimens are tested in sets of three at each test temperature, the set having the highest average may be regarded as defining the upper-shelf energy.The measure of fluence used herein is the number of neutrons per square centimeter (E>I MeV). An as-sumed fission-spectrum energy distribution was used in calculating the fluence for most of the data base.*However, for application to a reactor vessel, the calculated spectrum is used to predict fluence at a given location in the wall. This procedure is not in-tended to preclude future use of data that are given in terms of neutron damage fluence.As used herein, references to "% Cu" and "% P" mean the weight percent of copper and phosphorus as measured in the surveillance program per ASTM E185-73. However, if such results are not available, the results of a product analysis may be used.Use of the procedures for prediction of radiation damage given in the regulatory position should be limited to irradiation at 550 +/-251F, because temperature is important to damage recovery proces-ses. As a guideline, irradiation at 4501F has been shown to cause twice the adjustment of reference temperature and irradiation at 650°F, about half the ladjustment produced by irradiation at 550OF for the fluence levels and the steels cited in the regulatory

  • The data base for this guide is that given by Spencer H. Bush,"Structural Materials for Nuclear Power Plants." 1974 ASTM Gil-lett Memorial Lecture, published in ASTM Journal of Testing and Evaluation, Nov. 1974, and its addendum, "Radiation Damage in Pressure Vessel Steels for Commercial Light-Water Reactors." position when the copper content is about 0.15%. The effects of irradiation temperature on decrease in shelf energy should be considered qualitatively similar to those cited for the adjustment of referencej temperature.

Sensitivity to neutron embrittlement may be af-fected by other residual elements such as vanadium and by deoxidation practice, as indicated by the findings of current research.

In predicting radiation damage for materials that differ in chemical content or deoxidation practice from those that make up the data base, such findings should be considered.

Other residual elements, notably sulfur, impair the initial Charpy shelf energy of these materials, and their con-tent should be kept low. Clearly, it is the remaining toughness at end of life or at some other critical period that is important.

Such toughness may be given in terms of the margin between the operating temperature (nominally

550°F) and the limiting temperature based on toughness.

A margin of 200 degrees is desirable to permit safe management of system transients.

At full power, the limiting temperature based on toughness is generally

150-200 degrees above RTNDT; hence, the latter should not exceed 150-2001F

at end of life. This limit also avoids the problems of providing for annealing, per paragraph IV.C of Appendix G. The levels of residual elements such as copper, phosphorus, sulfur, and vanadium that are required to achieve the limit of 200'F adjusted reference temperature at end of life in a given reactor vessel will depend on the initial values of RTNDT of the beltline materials and on tle" predicted fluence at the particular locations in the vessel where the materials are used.When surveillance data from the reactor in ques-tion become available, the weight given to it relative to the information in this guide should depend on the credibility of the surveillance data as judged by the following criteria: 1. Materials in the capsule should be those judged most likely to be controlling with regard to radiation damage according to the provisions of this guide.2. Scatter in the Charpy data should be small enough to avoid large uncertainty in curve fitting.3. The change in yield strength should be consis-tent with the shift in the Charpy curve.4. The relationship to previous isurveillance data from the same reactor should be consistent with the normal trends of such data. I 5. The surveillance data for the correlation monitor material in the capsule should fall within the scatter band of the data base for that material.1.99-2 C. REGULATORY

POSITION 1. When credible surveillance data from the reac-tor in question are not available, prediction of neutron radiation damage to the beltline of reactor vessels of light water reactors should be based on the following procedures.

a. Reference temperature should be adjusted as a function of fluence and residual element content in accordance with the following expression, within the limits below and in paragraph l.c.A = [40 + 1000(% Cu -0.08)+ 5000 (% P -0.008) ] [f/ 1019]where A = predicted adjustment of reference temperature, OF.f = fluence, n/cm 2 (E>l MeV).% Cu = weight percent of copper.If % CuK 0.08, use 0.08.% P = weight percent of phosphorus.

If % P5K0.008, use 0.008.If the value of A obtained by the above expression exceeds that given by the curve labeled "Upper Limit" in Figure 1, the "Upper Limit" curve should be used. If % Cu is unknown, the "Upper Limit" curve should be used.As illustrated in Figure 1 for selected copper and phosphorus contents, the above expression should be considered valid only for A >50°F and for f( 6 x 10'9 n/cm 2 (E > 1 MeV).b. Charpy upper-shelf energy should be as-sumed to decrease as a function of fluence and copper content as indicated in Figure 2, within the limits listed in paragraph l.c. Interpolation is permitted.

c. Application of the foregoing procedures should be subject to the following limitations:.

(1) The procedures apply to those grades of SA-302,. 336, 533, and 508 steels having minimum specified yield strengths of 50,000 psi and under and to their welds and heat-affected zones.(2) The procedures are valid for a nominal ir-radiation temperature of 550°F. Irradiation below 5251F should be considered to produce greater damage, and irradiation above 5751F may be con-sidered to produce less damage. The correction factor used should be justified.

(3) The expression for A is given in terms of fluence as measured by units of n/cm 2 (E > 1 MeV);however, the expression may be used in terms of fluence as measured by units of neutron damage fluence, provided the constant 1019 n/cm 2 (E> 1 MeV) is changed to the corresponding value of neutron damage fluence.(4) Application of these procedures to materials having chemical content beyond that represented by the current data base should be justified by submittal of data.2. When credible surveillance data from the reac-tor in question become available, they may be used to represent the adjusted reference temperature and the Charpy upper-shelf energy of the beltline materials at the fluence received by the surveillance specimens.

a. The adjusted reference temperature of the beltline materials at other fluences may be predicted by: (1) extrapolation to higher or lower fluences from credible surveillance data following the slope of the family of lines in Figure 1 or (2) a straight-line interpolation between credi-ble data on a logarithmic plot.b. To predict the decrease in upper-shelf energy of the beltline materials at fluences other than those received by the surveillance specimens, procedures similar to those given in paragraph

2.a may~be fol-lowed using Figure 2.3. For new plants, the reactor vessel beltline materials should have the content of residual ele-ments such as copper, phosphorus, sulfur, and vanadium controlled to low levels. The levels should be such that the predicted adjusted reference temperature at the 1/4T position in the vessel wall at end of life is less than 200 0 F.

D. IMPLEMENTATION

The purpose of this section is to provide informa-tion to applicants and licensees regarding the NRC staff's plans for utilizing this regulatory guide.This guide reflects current regulatory practice.Therefore, except in those cases in which the appli-cant proposes an acceptable alternative method for complying with specified portions of the Commis-sion's regulations, the positions described in this guide will be used by the NRC staff as follows: 1. The method described in regulatory positions C. 1 and C.2 of this guide will be used in evaluating all predictions of radiation damage called for in Appen-dices G and H to 10 CFR Part 50 submitted on or 1.99-3 after June 1, 1977; however, if an applicant wishes to use the recommendations of regulatory positions C. 1 and C.2 in developing submittals before June 1, 1977, the pertinent portions of the submittal will be evaluated on the basis of this guide.2. The recommendations of regulatory position C.3 will be used in evaluating construction permit ap-plications docketed on or after June 1, 1977;however, if an applicant whose application for con-struction permit is docketed before June 1, 1977, j wishes to use the recommendations of regulatory'

position C.3 of this regulatory guide in developing submittals for the application, the pertinent portions of the application will be evaluated on the basis of this guide.4 1.99-4

7w A = [40 + 1000 (% Cu -0.08) + 5000 (% P -0.008)][f/10191 1)400)-ýPl ,, 300 0 C.E 0 200 4-0 100 E 5-50 C., a, IL%I-.I I I I I III~..~~IIIIIIIIIIIIiIIIjTIIII[III

i i i L l i i i ~ m- i i 1 11 11am 1 1 1 i i i i i i i i i i i i H HHHHH i i i i i i ! i H HHHHHHi ....II!I I i I I I i I IBI ,JI 0.25;M020

/, rz z0.15% Cu-0.1(Ia I/ f I =I 1.LOWER LIMIT% Cu = 0.08% P = 0.008 2X10 1 7 4 6 8. 10 1 8 2 4 6 8 1019 2 4 6 FLUENCE, n/cm 2 (E > 1MeV)Figure 1 Predicted Adjustment of Reference Temperature, "A", as a Function of Fluence and Copper Content.For Copper and Phosphorus Contents Other Than Those Plotted, Use the Expression for "A" Given on the Figure.

~~~U.,3UU

.-20 0.25-- -------- 0.20 -0.15-0.15 0.10-- W wL IT C,"___ O. 10---.05 ---I Z 2 11 4 6 8 08 6 8 1092 4 6 FLUENCE, n/cm 2 (E > 1MeV)Figure 2 Predicted Decrease in Shelf Energy as a Function of Copper Content and Fluence.Aftk --

UNITED STATES NUCLEAR REGULATORY

COMMISSION

WASHINGTON, D.C. 20555 OFFICIAL BUSINESS PENALTY FOR PRIVATE USE, $300 POSTAGE AND FEES PAID U.S. NUCLEAR REGULATORY

COMMISSION

UCi' 7-L NN r? C ULFLL F U EF l",%:PEFLC

110N t, [F R C E U 3 1 AUFAVENI K TN rc 0 F P R US i A PA 1'J4Lu/