Friday, August 24, 2018

Unmet


https://relap53d.inl.gov/seminars/westyellowstone2003/Shared%20Documents/leyse.pdf


AN UNMET CHALLENGE: CONSIDERATION OF HEAVY FOULING IN THE ANALYSIS OF SEVERE ACCIDENTS



Robert H. Leyse, CEO

Inz, Inc., PO BOX 2850, Sun Valley, ID 83353

bobleyse@aol.com

aBSTRACT


The impact of heavy fouling of fuel elements has not been considered in the analysis of severe accidents such as Reactivity Insertion Accidents and Loss of Coolant Accidents.  Operation of nuclear power reactors with significant fouling deposits is commonplace.  Fouling deposits have substantial thermal resistance. This has led to fuel element failures in several instances as the zirconium alloy cladding has failed due to high temperature corrosion.  Although the details of current fouling have not been disclosed, in several instances the deposits have been unusually heavy with clumpy formations.  Such heavy clumpy fouling is complex with substantial thermal resistance. Relatively straightforward fouling at the Experimental Boiling Water Reactor (EBWR)  during the late 1950s was classified in terms of the thickness and the thermal conductivity.  Thickness of the scale was 0.013 cm, the thermal conductivity was 0.008 W/cm-C; thus the heat transfer coefficient was 0.6 W/(cm2)(C).  The peak heat flux in today’s large light water reactors is in the range of 150 W/cm2 and the temperature gradient for EBWR-type fouling would be 250 C.  However, the effective heat transfer coefficient of the heavy, clumpy fouling in today’s reactors is likely substantially less than the EBWR case. The real heat transfer is thus vastly degraded in contrast to the clean cores of current safety analyses. 





1.    INTRODUCTION



The renowned heat transfer expert, W. H. McAdams once observed (McAdams, 1942, p. 316), “The small amount of scale necessary to reduce a high (heat transfer) coefficient by a substantial amount is not generally realized.”  More recently, at the 50th anniversary meeting of the American Nuclear Society, the prominent nuclear safety expert, Theodore Rockwell asserted (Rockwell, 2004, p.40), “There is a good realistic story to tell based on facts, knowledge, and understanding.  Rockwell was followed by Eltawila of the United States Nuclear Regulatory Commission who added, “Realism comes from using the best information you have from science, engineering, and operating experience.”

  

        The heat transfer characteristics of the fouling in today's LWRs have not been reported.  However, operational experience reveals that with fouling and corrosion the fuel pin heat transfer characteristics are vastly degraded in contrast to clean pins.  In several instances, the severe fouling has led to corrosion thicknesses sufficient to penetrate the cladding of many fuel pins.  At more than 20 units fouling has trapped boron and this led to offsets in the power distribution. In one case, control rod binding was traced to guide tubes that deformed when fouled fuel pins lengthened beyond end space limits and bent. At Paks Units 1-3, reduced flow restricted the power level. Several units now employ ultrasonic means to remove fouling.  The impact of fouling has not been considered in the evaluation of  reactivity insertion accidents RIAs, loss of coolant accidents or normal operation of water cooled and moderated nuclear power reactors.  . 

       

        Fouling at the Experimental Boiling Water Reactor during the late 1950s severly limited the experimental program, however the impact on potential accidents has never been disclosed.  The impact of fouling on the severity of the reactivity insertion accident at the  SL-1 boiling water reactor on January 3, 1961 has not been evaluated.



An assessment of postulated reactivity insertion accidents for operating reactors in the U. S. A.  was issued by the United States Nuclear Regulatory Commission (NRC) on March 31, 2004.  The lengthy report considers the results of test programs worldwide, but includes no consideration of the impact of fouling on severity of RIAs.  There is no thermal analysis of the impact of oxidation or fouling.



        The challenge for the licensees of nuclear power reactors is to produce thorough evaluations of the impact of heavy fouling on severe accidents.  Leyse has submitted several petitions to the NRC calling for the consideration of fouling in the evaluation of  RIAs, LOCAs and normal plant operation.  The NRC has denied that fouling is a significant safety issue.  In general, the NRC believes that fouling is more accurately described as crud, a very thin loose deposit that has no impact on the hydraulics and thermal hydraulics of operating reactors.  Moreover, all of the past and current thermal hydraulic experimental programs worldwide have not considered any impact of fouling,





2.    RECENT EXPERIENCE WITH FOULING IN NUCLEAR POWER REACTORS



Thick, tenacious fouling is ubiquitous among the fleet of nuclear power reactors in the U.S. A. and it also occurrs in reactors elsewhere.  Following are several examples.



2.1    Fouling at the River Bend Boiling Water Reactor



 An analysis of fuel pin failure timing for severe accidents at the River Bend Station (RBS) would be revealing.  Entergy issued a Licensing Event Report that partially describes the severe fouling that occurred at RBS during 1998 (King, 2000).  Multiple fuel pin failures were attributed to "…an unusually heavy deposition of crud on the fuel bundles."  It was, "Determined that an insulating layer of crud caused accelerated fuel rod corrosion."  There is no quantitative disclosure of the effective thermal conductivity of the insulating layer of crud.  It is disclosed that "Measured zircaloy oxide thickness on high power unfailed HGE bundles was up to 6 mils at the 50" level where the perforations occurred."  However, there has been no public disclosure of the measured zircaloy oxide thickness on the  failed HGE bundles.



        Schneider, et al. (2004. p28) partially describe the River Bend event as follows.  An unusual water chemistry condition was encountered during 1988-99 at one plant (River Bend, Cycle 8) resulting in 7 fuel assembly failures.  Although the available water chemistry measurements indicated general conformance to the EPRI Water Chemistry Guidelines, the fule condition was observed to be highly unusual as characterized by an extremely thick, non-uunifirm layer of reactor system corrosion products (crud).  The observed failure mechanism at River Bend during cycle 8 was crud-induced accelerated oxidation of the cladding.  With the high thermal resistance provided by the the thick crud layer, elevated cladding temperatures were encountered which then resulted in oxidation to the point of  failure.  It is noted that another event, apparently similar to Cycle 8, occurred at the same plant in Cycle 11(2002-2003) and resulted in 8 fuel failures, this time in non-GNF first-cycle fuel.



        Entergy did not issue a Licensing Event Report describing the extensive fouling of Cycle 11.  However, Ruzauskas and Smith (2004) issued a somewhat detailed report of the fouling.  Following are excerpts from the abstract of this paper.  Examinations performed during the refueling outage indicated that Span 2 (the axial location between the second and third spacers form the assembly bottom) in both failed and unfailed one-cycle assemblies had an unusually thick and tenacious crud on peripheral rods.  The cause of failure was determined to be accelerated oxidation of the cladding in Span2 resulting from unusually heavy deposits of insulating tenacious crud. The most probable cause of the insulating tenacious crud was that copper and zinc were available in sufficient quantity to plug the normal wick boiling paths within the crud or clad oxide resulting in diminished heat transfer in local areas of the cladding surface. 



        The reference to wick boiling in the abstract is interesting; however, there is no reference to this in the body of the paper.  The paper includes ten figures that reveal several aspects of the severe fouling.  See Figure 1 for a typical photograph of the fouled rods and a discussion of the ten figures.




































































Figure 1:   This photograph and the captions are copied from the slide presentation by AREVA staff at the cited conference.  The heavy deposits were sufficient to bridge the gap between the two rods on the left side of the above illustration.   Other figures that are in the cited reference reveal (quoting from the captions) Heavy textured crud with nodules in Span 2 before brushing; Areas of spalling crud in Span 2 before brushing; Typical Appearance of Rods in Upper Spans of a Failed Assembly; On Some Assemblies Brushing Span 2 Removed all of the Tenacious Crud;  On Other Assemblies Brushing Removed Very Little of the Tenacious Crud in Lower Span 2; Examples of Tenacious Crud that Could not be Removed with Washing and Aggressive Brushing; Example of Rod Bowing in Span 2 on a Failed Assembly; Typical Crud Remaining After an Aggressive Cleaning Operation on Peripheral Rod in Span 2.     



        Although the severity of the fouling at River Bend has been most intense in limited regions, it is evident that fouling has been sufficient throughout the entire core to significantly impact reactivity insertion accidents, loss of coolant accidents, and the conduct of normal operations.  The investigators consistently refer to the high thermal resistance of the thick crud, but there is no thermal analysis.  And the vague inference that “good” crud, via wick boiling, may enhance heat transfer is unsubstantiated.

2.2     Fouling at the Columbia Generating Station Boiling Water Reactor









     

       

2.3    Fouling at other  Boiling Water Reactors



The experience at River Bend shows that even with severe fouling the amount of thermally induced fuel element failure has been modest.   According to Schneider, et al. (2004) fuel element failures have recently been very infrequent with GNF fuel at other at  BWRs.  Of course, this does not prove that fouling has not been sufficient to impact reactivity insertion accidents.  The authors refer to Increased Tenacious Crud Deposits on Fuel as a performance challenge.  However, this illustrates the lack of the thoroughness of the fuel reliability initiatives since no data are reported on the extent of the problem.  They report: Detailed post-irradiation examinations of fuel from the initial NobleChemTM application and a subsequent reapplication at the Duane Arnold plant were conducted at the GE Vallecitos hotcell facility.  These examination results largely show a thick Zn-rich tenacious crud layer with relatively little oxide growth.  The inspections confirmed that the observed spalling was due to the thick tenacious crud and was not oxide; corrosion in general was low.

     

2.4   Fouling at Paks Units 1-3       



An analysis of fuel pin failure timing for the Paks Units 1-3 would be revealing.  In a May 2003 report to the Chairman,  Hungarian AEC, the extensive fouling of the Paks units is candidly discussed. There is no description of the thermal resistance of the fouling or the amount of zircaloy corrosion.  However, the fouling (magentite)) has been extensive.  Quoting, "...magnetite deposits in the fuel assembles increased and the cooling water flow-rate decreased.  Consequently the power of Units 1-3 had to be decreased."  Chemical cleaning of fuel elements in batches of seven elements became routine.  In 2002, Framatome ANP expanded the cleaning process to 30 element batches.



        On 10 April 2003, while the assemblies were being cleaned for Unit 2, severe damage occurred to an entire batch.    The state of the fuel prior to the accident has not been disclosed. But as this data including the extent of fouling become available, it is likely that analysis will yield further insights on the impact of fouling on severe accidents.  The cleaning process for the 30 element batch was designed by Framatom ANP.  V. Asmolov, the Director of the Kurchatov Institute observed, "... it was a hand-made accident caused by those who, mildly speaking, clumsily thrust where they shouldn't. This is a precious experience." 



2.5  Axial Offset Anomaly (AOA)



More than 20 LWR's have had power distribution shifts caused by boron-loaded fouling.  EPRI reports, The root cause of AOA is corrosion product deposition in the upper spans of fuel assemblies as a result of sub-cooled nucleate boiling.  EPRI does not report the thermal conductivity of the deposits or the extent of zirconium oxidation.  Deposits were scraped from several fuel assemblies following a cycle that experienced AOA.  The thickness of the samples was in the range of 125 microns, however, that likely does not include zirconium oxides that are integral with the base cladding.  Again, it is clear that the deposits constitute a significant thermal resistance that should be incorporated in analyses of reactor accidents



        Frattini, P. L., et al., 2001, have apparently described a relationship between PWR primary chemistry and  axial offset anomaly.  However, the report is copyrighted and apparently has not been publicly disclosed to the regulatory authorities and is thus not detailed here.

      

        NRC Information Notice 97-85 clarifies AOA:  Axial offset (AO) is a measure of the difference between power in the upper and lower portions of the core.  This difference must remain within limits established in the technical specifications to ensure that both SDM and clad local peaking factors are not exceeded.  Exceeding these limits could result in the reactor fuel exceeding 10 CFR 50.46 limits on fuel clad temperature (1204C).  If the reactor approaches these limits, compensatory measures, including a power reduction, must be taken to maintain the reactor within its operational limits.



        However, the Notice does not include any discussion of the very substantial temperature increase of the limiting fuel pins that results from the same fouling that leads to the AOA.  This temperature increase likely exceeds 250C, however the consequent increase beyond the 1204C limit during loss of collant accidents is far greater than 250C because the fuel rods bend, distort and burst during the accident.  There is a simultaneous set of physical and chemical occurrences.  The fouling layers and the zirconium oxide layers become cracked, broken, shocked and loosened while zirconium-water reactions proceed at accelerating rates as additional zirconium is exposed to the water steam conditions at increasing temperatures.  .  



2.6  Ultrasonic Fuel Cleaning



Operators of several pressurized water reactors and one boiling water reactor have  deployed ultrasonic fuel cleaning (Varrin, 2002) for mitigation of axial offset anomaly via crud removal.  The patent owner, EPRI, promotes the process as follows:  Ultrasonic fuel cleaning is a patented EPRI technology that removes deposited corrosion products from nuclear fuel pin surfaces by emitting radially distributed ultrasonic waves through the fuel pin bundle, followed by the use of water to carry crud from the fuel to the filters. The industry has used the technology with great success at several pressurized water reactor (PWR) nuclear power plants for mitigation of axial offset anomaly as well as the ancillary benefit of radiation field reduction.





3.    EARLY EXPERIENCE WITH FOULING AT LOW POWER BWRs



During the late 1950s and early 1960s corrosion of aluminum structures led to severe fouling probems at two low powered boiling water reactors that were developed at the Argonne National laboratory.



3.1    Experimental Boiling Water Reactor  (EBWR)



The Experimental Boiling Water Reactor (EBWR) was designed and operated by Argonne National Laboratory during the late 1950s and early 1960s.  An unfortunate selection of aluminum alloy for core filler pieces led to deposits of hydrated alumina on the zirconium clad fuel elements.  Thickness of the fouling was 0.013 cm, the thermal conductivity was 0.008 W/cm-C; thus the heat transfer coefficient was 0.6 W/(cm2)(C).  The peak heat flux in today’s large light water reactors is in the range of 150 W/cm2 and the temperature gradient for EBWR-type fouling would be 250 C.  However, the heat transfer coefficient for the combined fouling and zircaloy oxide of today's units is likely substantially less than the EBWR case.



3.2    Argonne Low Power Reactor (SL-1)



The SL-1 was destroyed in a Reactivity Insertion Accident (RIA) on January 3, 1961.  Fouling of the aluminum clad fuel plates likely intensified the severity of the accident.  However, fouling was not considered by the analysts who investigated this RIA.  Here is a quote from GE Report, Additional Analysis of the SL-1 Excursion, Report IDO-19313, 1962: The thickness of the cladding has an important effect on the magnitude of the excursion.  Because of the extremely short period, this 0.89 mm cladding became an effective thermal insulator and impeded the flow of heat to the reactor water where it could initiate shutdown of the reactor.  Now, inasmuch as the thermal conductivity of aluminum is  about 200 times greater than the corrosion on the fuel plate, a corrosion layer only 0.00445 millimeters thick would have the same temperature gradient as 0.89 mm of aluminum cladding. Alternatively, the measured corrosion product thickness of 0.09 mm has 20 times the temperature gradient of the aluminum cladding.  Ignoring the corrosion thus yields a grossly incomplete analysis in determining turnaround characteristics.





4.0    FOULING AND RUNAWAY



There has never been a runaway zirconium water chemical reaction in a nuclear power reactor that was induced by fouling.  However, there have been cases of rapid zirconium (zirconium alloy) reactions with water.  One case was the rapid oxidation that occurred during the Chernobyl accident.  And, during the accident at Three Mile Island there were likely times during which the cladding reaction  was relatively rapid.  As is clear from the River Bend experience, severe fouling leads to extensive corrosion of the cladding.  At River Bend, there was no runaway zirconium water reaction.  However, with the very thick deposits, it is not clear that limited runaway was not imminent. Following are two experiences with runaway that occurred during documented test programs.



4.1  Runaway During a Severe Fuel Damage Scoping Test



On Feb. 22, 1983, MacDonald of Idaho National Engineering Laboratory (INEL), in testimony to the Advisory Committee on  Reactor Safety (ACRS) discussed a destructive test in the Power Burst Facility (PBF).   A 32 rod array of PWR 17x17 fuel, 36 inches long, was heated to high temperature with fission heating and then exposed to a steam/water mix.  MacDonald stated, "We observed rapid oxidation of the lower portion of the bundle.  It wasn't expected.  It cannot be calculated with existing models. It is a flame-front phenomenon which is not addressed in the existing models.  It will probably be addressed in the coming months or years. ... Think of a sparkler.  That kind of phenomenon.  One of the problems with the existing models, all the axial loadings are extremely course.  They just do not deal with the spread of a zircaloy fire."  This was a case of substantial and unexpected runaway, and contrary to MacDonald’s forecast, the problem has not been addressed.



4.2    Runaway During FLECHT Run 9573



A series of experiments called Full Length Emergency Cooling Heat Tansfer (FLECHT) was initiated during the late 1960s and continues to this day under multiple programs at many laboratories.  The early tests were conducted with simulated fuel element assemblies.  A 7 by 7 array of  electrically powered stainless steel clad heaters, 12 feet long, was preheated to temperature in the range of 1000 to 1300 oC and then bottom-flooded with cooling water.  Temperatures along the test rods were monitored with thermocouples that were mounted internally.  A limited number of tests were run with zircaloy clad heaters.

       

        The extensive failure of the FLECHT assembly at 18 seconds after reflood was not anticipated.  (Limited runaway.) This may be fertile territory for SCDAP/RELAP5-3D.  Tasks would include analysis of Run 9573 as well as design and analysis of further tests. 



        In issuing its document, “Acceptance Criteria for Emergency Core Cooling Systems for Light-Water Cooled Nuclear Reactors-Opinion of the Commission,” Docket No. RM50-1, December 28, 1973, the Commission concluded, “It is apparent , however, that more experiments with zircaloy cladding are needed to overcome the impression left from run 9573.”  It is a fact that more experiments of the type called for have not been conducted.

4.3  Runaway Discussions at the Advisory Committee for Reactor Safeguards (ACRS)



The USNRC is currently working on revisions to rule 10 CFR 50.46 concerning emergency core cooling systems for reactors.  The process is called  risk-informing the regulation.  The ACRS discussions of Friday, May 31, 2002, are revealing in that several aspects of the revisions were discussed, however, the ubiquitous fouling of today’s LWRs was not considered.  This was a combined meeting of three of the most influential subcommittees of the ACRS: Materials and Metallurgy; Thermal Hydraulic Phenomena & Reliability and Probabilistic Risk Assessment

        Member Graham B. Wallis was especially enraged by the limited approaches to fuel integrity under LOCA conditions.  In response to detailed descriptions of fracture of corroded specimens of cladding from irradiated power reactor fuel he asserted:  It seems to be that both these coursing tests and hitting tests, impact tests and the squeezing tests are not really typical of the loads imposed on the real cladding.. I keep wondering what the relevance of all these tests are to the real truth.”  He also reacted to the discussions of  runaway,  “I think when you come back and talk about run-away to this committee you better have a criterion for run-away and not this sort of vagueness about heat transfer.”


        S. Bajorek of the NRC staff described Non-Conservatisms in the present day  Appendix K (10 CFR 50.46): “Now the processes that we've identified over the last few months which are strong candidates that need to be corrected are downcomer boiling, reflood ECC bypass and fuel relocation. Bajorek discussed fuel relocation as follows: “The issue of relocation has been around for several years. We hope to get better information in some of the newer tests that are being devised right now.  They are going to be running some tests with better instrumentation on the nuclear rods to try to get at fuel relocation which has been observed in tests in Germany, France and the U.S.  When we get this ballooning that occurs in the rod, it's possible that these fragmented pellets due to the vibrations can migrate down into the burst and rupture zone. The typical assumption in Appendix K is that these pellets remain as a concentric stack. Now I was talking to Dr. Ford who said why is this cladding temperature going down after it swells. It's good because you've swollen the cladding away from its heat source. If you are at low temperatures and zirc-water doesn't make any difference, this is a fin.  It's not a fin if you consider fuel relocation. It becomes much worse if there is a rupture involved and you have zirc-water reaction because now you've relocated the pellets, your local power is increased, you have very good communication now between the pellet fragments and the cladding itself. I have lost that fin effect. You see varying estimates on this. But we are identifying this as something that needs to be accounted for in future models.”



        The direct quotes from Bajorek are revealing.  The impact of fuel relocation on cladding heat transfer, temperatures, and oxidation reactions is emphasized.  However, the very definite impact of fouling on the course of a LOCA is not considered.  This is the case even though fouling is known to significantly impact the properties of the fuel pins at the beginning of LOCA.  .  The current 10 CFR 50.46 limits the calculated cladding temperature to 1200 oC.  With severe fouling, the cladding temperature during steady state power operation could exceed the starting temperature values in present LOCA documents by several hundred oC.  





5.  THE  IMPACT OF FOULING ON SEVERITY OF REACTIVITY INITIATED ACCIDENTS (RIAs) HAS BEEN OVERLOOKED



The U. S. nuclear power industry and the U. S. NRC have focused on the severity of RIAs in studies that are directed to extending burnup limits for PWR and BWR fuel.  These studies have not considered the impact of fouling on the severity of RIAs even though fouling is ubiquitous among the worldwide fleet of PWRs and BWRs.  A few years ago the NRC listed seven activities on high-burnup fuel research.  The following quotation is from the NRC’s then available document called HIGH-BURNUP FUEL RESEARCH.

“ A list of current NRC research activities on high-burnup fuel is shown below.

1. ANL (NRC) Hot Cell LOCA Tests of Fuel Rods and Mechanical Properties of Cladding

2. PNNL (NRC) Steady-State and Transient Fuel Rod Codes and Analysis

3. BNL (NRC) Neutron Kinetic Codes and Analysis of Plant Transients

4. Halden (Norway) Reactor Tests of Fuel Rods in Steady State and Mild Transients

5. Cabri (France) Reactivity Accident Tests of Fuel Rods and Related Programs

6. NSRR (Japan) Reactivity Accident Tests of Fuel Rods and Related Programs

7. IGR (Russia) Reactivity Accident Tests of Fuel Rods and Related Programs”



        Then, on June 12, 2002, the U. S. nuclear industry lobby organization, the Nuclear Energy Institute, provided the NRC with EPRI Report 1002865, Topical Report on Reactivity Initiated Accidents: Bases for RIA Fuel Rod Failures and Core Coolability Criteria.  This report purports to provide, “Revised acceptance criteria (that) have been developed for the response of light water reactor (LWR) fuel under reactivity initiated accidents (RIA).  Development of these revisions is part of an industry effort to extend burnup levels beyond currently licensed limits.  The revised criteria are proposed for use in licensing burnup extensions or new fuel designs.”  Clearly, the thrust of EPRI Report 1002865 is to extend burnup levels.  There is no consideration of fouling as a significant factor in the severity of RIAs.



        Next, on March 31, 2004, the NRC (Thadani, 2004) issued Research Information Letter No. 0401, “An Assessment of Postulated Reactivity-Initiated Accidents for Operating Reactors in the U. S.”  In the final paragraph of its cover letter to RIL 0401, the NRC states:  “We hope the attached assessment will provide NRR with independent information that will help in the review of EPRI Report 1002865, ‘Topical Report on Reactivity Initiated Accidents: Bases for RIA Fuel Rod Failures and Core Cool ability Criteria.’  The RES staff are available to assist NRR with that review, and RES is prepared to subsequently revise Regulatory Guide 1.77 on RIA safety analysis as indicated in the updated program plan,” In another paragraph of this cover letter, the NRC, for the first time ever, asserts that, “It should be noted that cladding failure thresholds vary only weakly with burnup level.  Cladding corrosion (oxidation) which might differ widely for different cladding materials at the same burnup was found to be the most important variable.”



        In a clarifying letter to Leyse (Paperiello, 2004, APPENDIX A) the NRC asserts that there is no need to account for crud deposits in the analysis of RIAs.  In paragraph 4, the NRC explains, “Going one level deeper in technical detail, we can draw a further distinction between the effects of oxide and crud.  Specifically, the oxidation process releases hydrogen, some of which is absorbed by the zirconium-based cladding alloy, where it embrittles the cladding and could lead to cladding failure during an RIA power transient.  By contrast, crud sits on top of the oxide and does not produce any embrittling products that migrate into the cladding metal.  Therefore, crud has only a secondary effect, as it provides some insulation and leads to slightly higher cladding temperatures that accelerate oxidation.  Nonetheless, the correlation of RIL-0401 explicitly accounts for total oxidation, so crud has no additional effect and there was no need to account for crud deposits in that analysis.”   It is noteworthy that Paperiello refers to hydrogen absorption as a cause of embrittlement of the cladding alloy, however, he makes no mention of  dissolved oxygen in the zirconium alloy as described by Leyse, 1964, Hobson and Rittenhouse, 1972, and very likely, others.  Hobson and Rittenhouse present correlations that relate the degree of embrittlement of  Zircaloy tubing to the amount of oxide on the surface and the additional dissolved oxygen gradient into the wall.  



        The NRC does not address the heat transfer characteristics of the oxide or the crud or the combination of the oxide and the crud.  The NRC regards the amount of oxide as a measure of the embrittlement of the cladding.  That embrittlement could then lead to cladding failure during an RIA power transient.  The NRC asserts that crud provides some insulation and leads to slightly higher cladding temperatures that accelerate oxidation, and that since RIL-0401 explicitly accounts for total oxidation, there is no need to account for crud deposits.  As the NRC’s incomplete analyses reveal, the impact of fouling on the severity of  RIAs has been overlooked.



6. THE IMPACT OF FOULING AND OXIDATION ON FUEL CLADDING                   OPERATING TEMPERATURES



Fouling leads to substantially higher cladding temperatures during normal operation of the nuclear power plant.  Fouling also leads to higher power levels during RIAs.  The heat transfer characterists of the fouling in the worldwide fleet of today’s LWRs have not been openly reported.  However, the thermal resistance of fuel element scale deposits at the Experimental Boiling Water Reactor (EBWR) has been documented.  The impact of the EBWR deposits on its fuel element dimensional changes has also been recorded.  More recently, there have been allusions to boiling chimneys within the fouling of today’s LWRs. 



6.1   Thermal Resistance and Impact of EBWR Scale



The Experimental Boiling Water Reactor (EBWR) was built and operated at the Argonne National Laboratory (ANL) near Chicago during the late 1950’s and early 1960’s. The initial power level was 20 megawatts.  The operating pressure was 40 atmospheres and the expected surface temperature of the zirconium-clad flat plate nuclear fuel elements was in the range of 255 degrees centigrade over a wide range of heat fluxes.  However, plans to operate the EBWR at substantially higher power levels were significantly impacted when significant scale deposits were discovered on the nuclear fuel elements. Scale deposits were most pronounced in the central regions of the reactor core where the maximum heat flux was in the range of 50 W/cm2.  These deposits were mainly aluminum oxide that was exfoliated from allegedly corrosion resistant aluminum alloy structures that were incorporated in peripheral locations of the reactor core.  The scale was extremely adherent to the zirconium heat transfer surfaces until the thickness reached the range of 0.013 centimeters, at which point some of the scale flaked off and entered the flow of boiling water.

      

Breden and Leyse, 1960, reported a range of activities.  An overall fuel inspection was performed during April,1959.  Fuel element ET-51 which operated in a relatively high flux location since startup was examined in the Argonne  hot cell.  A substantial amount of scale flaked off during the handling.  (See Figure 2.) Thickness was about 0.013 cm.  Density was 2.5 gm/cm3 based on weight and volume. The scale was attracted by a magnet.  Composition based on wet chemical, spectrographic and X-ray diffraction measurements yielded the following: boehmite, 80.6 %; nickel oxide, 12.6 %; iron oxide, 5.1%; silicon dioxide 1.6%.  Thermal conductivity of the flat (planar) scale was 0.008 W/(cm2)(oC). 























 


 


 



Figure 2.  Assembly of the EBWR plate-type fuel element and a hot cell photograph of one section of plate fuel. The scale is peeling away from the zirconium cladding.  The scale was very adherent to the cladding until it reached a thickness in the range of 125 microns when peeling began.  The zirconium clad enriched uranium metal plate type fuel elements were extremely robust, however, the thick scale led to fuel plate temperatures beyond design.  Therefore, the fuel plates expanded longitudinally beyond design limits when the EBWR was operated at elevated power levels for brief times (a few hours).  With no fouling of the fuel plates, the operating temperature of the fuel plates in the boiling water system would increase relatively little as heat flux (reactor power) was increased.  However, with the extra longitudinal growth of the fouled fuel plates, the side plates were stretched.  During inspections of the core, the perforated side plates were then found to be bowed between the assembly spot welds.  Clearly, the fouling had no “boiling chimneys” that enhanced heat transfer.



6.2   Boiling Chimneys



At times, there are inferences that crud deposits enhance heat transfer.  Mr. Deshon of EPRI referred to “boiling chimneys”  during his presentation to the U. S. NRC’s ACRS Reactor Fuels Subcommittee, September 30, 2003.  On page 132 of the transcript of this meeting,  Deshon asserts that these boiling chimneys enhance heat transfer from the cladding to the coolant when the thickness of the fouling is up to a thickness of 20 microns.  Next, on page 133, he refers to a flake with a thickness of 125 microns with “… very large voids in the crud, representing these boiling chimneys.”   Now, it is unlikely that a chimnied layer having a thickness of 20 microns will enhance the heat transfer from the cladding to the cooling water, and it  is very unlikely that a porous layer of 125 microns will be anything other than a significant barrier to heat transfer.  Deshon presented no experimental data to prove the enhancement of heat transfer.



        Now, wick boiling has been discussed by many investigators as a means of improving the performance of heat pipes.  In those applications, the fluid is highly pure and the wick geometry is fixed by controlled means (wire mesh structures, specific chemical vapor deposition and perhaps others).  However, the crud formations on nuclear power plants will not have the prescribed boiling channels.  Even if an optimum boiling chimney array is built into the surface of the cladding, the lifetime of any enhancement would be nil as magnetite and other deposits ruin the system.

7.0  INCOMPLETE TESTING, INCOMPLETE CODES, DEFICIENT REGULATION      

Although billions of dollars have been expended on testing and code production, the products are grossly deficient in terms of producing the realistic bases for current regulation of water cooled nuclear power plants.  Moreover, there is a dearth of undirected exploratory research that could bear on the technology.

7.1    Incomplete Testing and Analysis of Test Data

During the last five decades there have been hordes of test programs.  Many have been significant and useful, but the preponderance of the work has been incomplete.  The Borax experiments of the 1950’s were an impressive exploration into the inherent safety light water reactors, but the work was incomplete when the approaches were abandoned.  Further Borax-type experiments in the 1960’s followed the destructive reactivity insertion accident at SL-1, but again, the work, Special Power Excursion Reactor Tests (SPERT) was abandoned before it was complete.  The common thread of inadequacy of these programs was the total disregard of the significant impact of fouling on the results and conclusions.  The work in the Power Burst Facility (PBF) was abandoned with no regard for the impact of fouling. 

        Fouling has been ignored in the design, conduct, and interpretation of the multitude of  heat transfer tests related to emergency core cooling.  This was true of the extensive FLECHT and related programs that began during the 1960s and is true of the continuing programs that are funded today.  One example (among several) of today’s efforts is the Rod Bundle Heat Transfer Testing (RBHT)at Pennsylvania State University.  Although millions of dollars are being expended on RBHT, that expenditure is likely insignificant in comparison with the total of other programs in the United States as well as the international community.  The very expensive nuclear powered tests in the Loss of Fluid Test (LOFT) were likewise discontinued without any recognition that the fouling that is commonplace in light water power reactors (LWRs) would have a significant impact.

7.2    Incomplete Codes

The common practice is to “calibrate” or otherwise certify computer codes that are employed in reactor safety analyses based on results of testing in programs such as FLECHT, PBF, SPERT, LOFT and a multitude of others.  A limited number of tests have also been conducted during the startup phases of commercial nuclear power reactors. Fortunes have been expended on so-called “test cases” and “round robin” exercises.  However, none of the codes ranging from the current RELAP, RETRAN, TRACE and countless others have been “calibrated” based on test results with fouled heat transfer surfaces.  It could be argued that all of the codes have the capability of modeling a range of heat transfer resistances that could be assigned to fouling.  It is a fact that this has not been done, and even if it was attempted, the results would have little credibility.

7.3    Deficient Regulation

Under the banners of  “realism” and “conservative realism” there are current moves to produce “risk informed” regulations.  Indeed, an opening panel discussion called  Risk Informing Emergency Core Cooling System (50.46) Requirements” is scheduled for the USNRC’s Regulatory Information Conference, March 2005. It is unlikely that the panel will discuss the deficiencies in the NRC’s regulations related to LOCAs.  The NRC and the DOE’s national laboratory, INEEL, avoid  realistic test programs  (Rankin, 2003, APPENDIX B).  They also avoid realistic code applications (Jacobsen, 2003, APPENDIX C). Initiatives that would derail deficient regulations are summarily rejected.



8.0  SUMMARY AND CHALLENGES





Fouling is ubiquitous.  A few of the cases of severe fouling in light water reactors over the past five decades, with power levels have ranging from tens to thousands of megawatts, have been described. 



        Fouling has a substantial thermal resistance.  Fouling leads to increased surface temperature of zirconium alloy cladding and this increases the rate of formation of layers of zirconium oxide. Values of thermal resistance of  present day fouling have not been reported.  However, at a modest heat flux of 100 W/cm2 the cladding temperature increases by 115 oC per 25 microns of zirconium dioxide.



        Fouling has a greater impact than burnup on reactivity insertion accidents (RIAs). There is an erroneous belief at the USNRC that fouling has only a minor role in the severity of RIAs.  The USNRC is preoccupied with the phenomenon of embrittlement. Even in the absence of cladding embrittlement, the thermal resistance of severe fouling will substantially increase the severity of an RIA.



        Fouling has a substantial impact on loss of coolant accidents (LOCAs).  With severe fouling, the cladding temperature at the start of the accident will be several hundred degrees higher than is the basis of LWR operating licenses.  The added impact of the resulting  layer of zirconium dioxide and the associated embrittlement adds to the adverse impact of the severe fouling.



        Very clearly, the current fouling of LWR fuel elements must be classified: thermal characteristics, composition, porosity, etc.  The characteristics of fouling must be added to the complex codes: RELAP, RETRAN, TRAC, TRACE and others.  This will place realism into licensing of LWRs.

REFERENCES


Breden, C. R. and Leyse, R. H., 1960.  Water Chemistry and Fuel Element Scale in the EBWR.  Report ANL-6136.  Argonne National Laboratory.



Frattini, P. L., et al., 2001.  Axial offset anomaly: coupling PWR primary chemistry with core design. Nuclear Energy, 40, 123 -133.



Hobson, D. O., and Rittenhouse, P. L., 1972.  Embrittlement of Zircaloy-Clad Fuel Rods by Steam During LOCA Transients. Report ORNL 4758. Oak Ridge National Laboratory.


King, R. J., 2000.  Thermally-Induced Accelerated Corrosion of BWR Fuel.  Licensee Event Report 50-458/99-016-00. Entergy.



Leyse, R. H., 1964.  Zircaloy-2 and Type 304 Stainless Steel at 2000oF in Water-Steam for Brief Times.  Report APED-4413. General Electric Co.



McAdams, W. H. 1942. Heat Transmission. Second edn. McGraw-Hill.



Rockwell, T. 2004. On the 50th Anniversary. Nuclear News, August 2004, 36-40.



Rusauskas, E. J., and Smith, D. L. 2004.  Fuel Failures During Cycle 11 at River Bend.  Proceedings of the 2004 International Meeting on LWR Fuel Performance.  American Nuclear Society.



Schneider, R. J., et al.,  2004.  Recent GNF BWR Fuel Performance.  Proceedings of the 2004 International Meeting on LWR Fuel Performance.  American Nuclear Society.



Thodani, A. C., 2004. An Assessment of   Postulated Reactivity Insertion  Accidents for Operating Reactors in the U. S. Research Information Letter No 401.  United States Nuclear Regulatory Commission.



Varrin, R. D. 2002.  United States Patent, US 6,396,892.























































































APPENDIX A



 


 


 


 


 


 


 


 


 


 


 


 




























 


 


 


 


 


 


 





























































APPENDIX B



The following letter shows that only initiatives from NRC or DOE are allowed at  INEEL.



 






















































































APPENDIX C



Following are excerpts from  the letter and the attachment that Leyse received from staff at INEEL dated June 17, 2003.  As the attachment reveals, the users of SCDAP/RELAP, MELCOR, and MAAP do not  consider fouling , “…because it has not been demonstrated conclusively that this effect should be considered.”  In response to this INEEL letter, Leyse submitted a revised approach and the slide presentation, “Unmet Challenges for SCDAP/RELAP5-3D: Analysis of Severe Accidents for Light Water Nuclear Reactors with Heavily Fouled Cores,” may be viewed via GOOGLE, enter Leyse Relap.  Of course, the USNRC and the USDOE have continued to spend millions of dollars annually on thermal hydraulic testing and code development.  Nevertheless, the impact of severe fouling is overlooked in the wide assortment of international activities. To this day (January 17, 2005) the impact of severe fouling on fuel element temperatures has not been considered in licensing of LWRs.    

  











AN UNMET CHALLENGE: CONSIDERATION OF HEAVY FOULING IN THE ANALYSIS OF SEVERE ACCIDENTS



Robert H. Leyse, CEO

Inz, Inc., PO BOX 2850, Sun Valley, ID 83353

bobleyse@aol.com

aBSTRACT


The impact of heavy fouling of fuel elements has not been considered in the analysis of severe accidents such as Reactivity Insertion Accidents and Loss of Coolant Accidents.  Operation of nuclear power reactors with significant fouling deposits is commonplace.  Fouling deposits have substantial thermal resistance. This has led to fuel element failures in several instances as the zirconium alloy cladding has failed due to high temperature corrosion.  Although the details of current fouling have not been disclosed, in several instances the deposits have been unusually heavy with clumpy formations.  Such heavy clumpy fouling is complex with substantial thermal resistance. Relatively straightforward fouling at the Experimental Boiling Water Reactor (EBWR)  during the late 1950s was classified in terms of the thickness and the thermal conductivity.  Thickness of the scale was 0.013 cm, the thermal conductivity was 0.008 W/cm-C; thus the heat transfer coefficient was 0.6 W/(cm2)(C).  The peak heat flux in today’s large light water reactors is in the range of 150 W/cm2 and the temperature gradient for EBWR-type fouling would be 250 C.  However, the effective heat transfer coefficient of the heavy, clumpy fouling in today’s reactors is likely substantially less than the EBWR case. The real heat transfer is thus vastly degraded in contrast to the clean cores of current safety analyses. 





1.    INTRODUCTION



The renowned heat transfer expert, W. H. McAdams once observed (McAdams, 1942, p. 316), “The small amount of scale necessary to reduce a high (heat transfer) coefficient by a substantial amount is not generally realized.”  More recently, at the 50th anniversary meeting of the American Nuclear Society, the prominent nuclear safety expert, Theodore Rockwell asserted (Rockwell, 2004, p.40), “There is a good realistic story to tell based on facts, knowledge, and understanding.  Rockwell was followed by Eltawila of the United States Nuclear Regulatory Commission who added, “Realism comes from using the best information you have from science, engineering, and operating experience.”

  

        The heat transfer characteristics of the fouling in today's LWRs have not been reported.  However, operational experience reveals that with fouling and corrosion the fuel pin heat transfer characteristics are vastly degraded in contrast to clean pins.  In several instances, the severe fouling has led to corrosion thicknesses sufficient to penetrate the cladding of many fuel pins.  At more than 20 units fouling has trapped boron and this led to offsets in the power distribution. In one case, control rod binding was traced to guide tubes that deformed when fouled fuel pins lengthened beyond end space limits and bent. At Paks Units 1-3, reduced flow restricted the power level. Several units now employ ultrasonic means to remove fouling.  The impact of fouling has not been considered in the evaluation of  reactivity insertion accidents RIAs, loss of coolant accidents or normal operation of water cooled and moderated nuclear power reactors.  . 

       

        Fouling at the Experimental Boiling Water Reactor during the late 1950s severly limited the experimental program, however the impact on potential accidents has never been disclosed.  The impact of fouling on the severity of the reactivity insertion accident at the  SL-1 boiling water reactor on January 3, 1961 has not been evaluated.



An assessment of postulated reactivity insertion accidents for operating reactors in the U. S. A.  was issued by the United States Nuclear Regulatory Commission (NRC) on March 31, 2004.  The lengthy report considers the results of test programs worldwide, but includes no consideration of the impact of fouling on severity of RIAs.  There is no thermal analysis of the impact of oxidation or fouling.



        The challenge for the licensees of nuclear power reactors is to produce thorough evaluations of the impact of heavy fouling on severe accidents.  Leyse has submitted several petitions to the NRC calling for the consideration of fouling in the evaluation of  RIAs, LOCAs and normal plant operation.  The NRC has denied that fouling is a significant safety issue.  In general, the NRC believes that fouling is more accurately described as crud, a very thin loose deposit that has no impact on the hydraulics and thermal hydraulics of operating reactors.  Moreover, all of the past and current thermal hydraulic experimental programs worldwide have not considered any impact of fouling,





2.    RECENT EXPERIENCE WITH FOULING IN NUCLEAR POWER REACTORS



Thick, tenacious fouling is ubiquitous among the fleet of nuclear power reactors in the U.S. A. and it also occurrs in reactors elsewhere.  Following are several examples.



2.1    Fouling at the River Bend Boiling Water Reactor



 An analysis of fuel pin failure timing for severe accidents at the River Bend Station (RBS) would be revealing.  Entergy issued a Licensing Event Report that partially describes the severe fouling that occurred at RBS during 1998 (King, 2000).  Multiple fuel pin failures were attributed to "…an unusually heavy deposition of crud on the fuel bundles."  It was, "Determined that an insulating layer of crud caused accelerated fuel rod corrosion."  There is no quantitative disclosure of the effective thermal conductivity of the insulating layer of crud.  It is disclosed that "Measured zircaloy oxide thickness on high power unfailed HGE bundles was up to 6 mils at the 50" level where the perforations occurred."  However, there has been no public disclosure of the measured zircaloy oxide thickness on the  failed HGE bundles.



        Schneider, et al. (2004. p28) partially describe the River Bend event as follows.  An unusual water chemistry condition was encountered during 1988-99 at one plant (River Bend, Cycle 8) resulting in 7 fuel assembly failures.  Although the available water chemistry measurements indicated general conformance to the EPRI Water Chemistry Guidelines, the fule condition was observed to be highly unusual as characterized by an extremely thick, non-uunifirm layer of reactor system corrosion products (crud).  The observed failure mechanism at River Bend during cycle 8 was crud-induced accelerated oxidation of the cladding.  With the high thermal resistance provided by the the thick crud layer, elevated cladding temperatures were encountered which then resulted in oxidation to the point of  failure.  It is noted that another event, apparently similar to Cycle 8, occurred at the same plant in Cycle 11(2002-2003) and resulted in 8 fuel failures, this time in non-GNF first-cycle fuel.



        Entergy did not issue a Licensing Event Report describing the extensive fouling of Cycle 11.  However, Ruzauskas and Smith (2004) issued a somewhat detailed report of the fouling.  Following are excerpts from the abstract of this paper.  Examinations performed during the refueling outage indicated that Span 2 (the axial location between the second and third spacers form the assembly bottom) in both failed and unfailed one-cycle assemblies had an unusually thick and tenacious crud on peripheral rods.  The cause of failure was determined to be accelerated oxidation of the cladding in Span2 resulting from unusually heavy deposits of insulating tenacious crud. The most probable cause of the insulating tenacious crud was that copper and zinc were available in sufficient quantity to plug the normal wick boiling paths within the crud or clad oxide resulting in diminished heat transfer in local areas of the cladding surface. 



        The reference to wick boiling in the abstract is interesting; however, there is no reference to this in the body of the paper.  The paper includes ten figures that reveal several aspects of the severe fouling.  See Figure 1 for a typical photograph of the fouled rods and a discussion of the ten figures.




































































Figure 1:   This photograph and the captions are copied from the slide presentation by AREVA staff at the cited conference.  The heavy deposits were sufficient to bridge the gap between the two rods on the left side of the above illustration.   Other figures that are in the cited reference reveal (quoting from the captions) Heavy textured crud with nodules in Span 2 before brushing; Areas of spalling crud in Span 2 before brushing; Typical Appearance of Rods in Upper Spans of a Failed Assembly; On Some Assemblies Brushing Span 2 Removed all of the Tenacious Crud;  On Other Assemblies Brushing Removed Very Little of the Tenacious Crud in Lower Span 2; Examples of Tenacious Crud that Could not be Removed with Washing and Aggressive Brushing; Example of Rod Bowing in Span 2 on a Failed Assembly; Typical Crud Remaining After an Aggressive Cleaning Operation on Peripheral Rod in Span 2.     



        Although the severity of the fouling at River Bend has been most intense in limited regions, it is evident that fouling has been sufficient throughout the entire core to significantly impact reactivity insertion accidents, loss of coolant accidents, and the conduct of normal operations.  The investigators consistently refer to the high thermal resistance of the thick crud, but there is no thermal analysis.  And the vague inference that “good” crud, via wick boiling, may enhance heat transfer is unsubstantiated.

2.2     Fouling at the Columbia Generating Station Boiling Water Reactor









     

       

2.3    Fouling at other  Boiling Water Reactors



The experience at River Bend shows that even with severe fouling the amount of thermally induced fuel element failure has been modest.   According to Schneider, et al. (2004) fuel element failures have recently been very infrequent with GNF fuel at other at  BWRs.  Of course, this does not prove that fouling has not been sufficient to impact reactivity insertion accidents.  The authors refer to Increased Tenacious Crud Deposits on Fuel as a performance challenge.  However, this illustrates the lack of the thoroughness of the fuel reliability initiatives since no data are reported on the extent of the problem.  They report: Detailed post-irradiation examinations of fuel from the initial NobleChemTM application and a subsequent reapplication at the Duane Arnold plant were conducted at the GE Vallecitos hotcell facility.  These examination results largely show a thick Zn-rich tenacious crud layer with relatively little oxide growth.  The inspections confirmed that the observed spalling was due to the thick tenacious crud and was not oxide; corrosion in general was low.

     

2.4   Fouling at Paks Units 1-3       



An analysis of fuel pin failure timing for the Paks Units 1-3 would be revealing.  In a May 2003 report to the Chairman,  Hungarian AEC, the extensive fouling of the Paks units is candidly discussed. There is no description of the thermal resistance of the fouling or the amount of zircaloy corrosion.  However, the fouling (magentite)) has been extensive.  Quoting, "...magnetite deposits in the fuel assembles increased and the cooling water flow-rate decreased.  Consequently the power of Units 1-3 had to be decreased."  Chemical cleaning of fuel elements in batches of seven elements became routine.  In 2002, Framatome ANP expanded the cleaning process to 30 element batches.



        On 10 April 2003, while the assemblies were being cleaned for Unit 2, severe damage occurred to an entire batch.    The state of the fuel prior to the accident has not been disclosed. But as this data including the extent of fouling become available, it is likely that analysis will yield further insights on the impact of fouling on severe accidents.  The cleaning process for the 30 element batch was designed by Framatom ANP.  V. Asmolov, the Director of the Kurchatov Institute observed, "... it was a hand-made accident caused by those who, mildly speaking, clumsily thrust where they shouldn't. This is a precious experience." 



2.5  Axial Offset Anomaly (AOA)



More than 20 LWR's have had power distribution shifts caused by boron-loaded fouling.  EPRI reports, The root cause of AOA is corrosion product deposition in the upper spans of fuel assemblies as a result of sub-cooled nucleate boiling.  EPRI does not report the thermal conductivity of the deposits or the extent of zirconium oxidation.  Deposits were scraped from several fuel assemblies following a cycle that experienced AOA.  The thickness of the samples was in the range of 125 microns, however, that likely does not include zirconium oxides that are integral with the base cladding.  Again, it is clear that the deposits constitute a significant thermal resistance that should be incorporated in analyses of reactor accidents



        Frattini, P. L., et al., 2001, have apparently described a relationship between PWR primary chemistry and  axial offset anomaly.  However, the report is copyrighted and apparently has not been publicly disclosed to the regulatory authorities and is thus not detailed here.

      

        NRC Information Notice 97-85 clarifies AOA:  Axial offset (AO) is a measure of the difference between power in the upper and lower portions of the core.  This difference must remain within limits established in the technical specifications to ensure that both SDM and clad local peaking factors are not exceeded.  Exceeding these limits could result in the reactor fuel exceeding 10 CFR 50.46 limits on fuel clad temperature (1204C).  If the reactor approaches these limits, compensatory measures, including a power reduction, must be taken to maintain the reactor within its operational limits.



        However, the Notice does not include any discussion of the very substantial temperature increase of the limiting fuel pins that results from the same fouling that leads to the AOA.  This temperature increase likely exceeds 250C, however the consequent increase beyond the 1204C limit during loss of collant accidents is far greater than 250C because the fuel rods bend, distort and burst during the accident.  There is a simultaneous set of physical and chemical occurrences.  The fouling layers and the zirconium oxide layers become cracked, broken, shocked and loosened while zirconium-water reactions proceed at accelerating rates as additional zirconium is exposed to the water steam conditions at increasing temperatures.  .  



2.6  Ultrasonic Fuel Cleaning



Operators of several pressurized water reactors and one boiling water reactor have  deployed ultrasonic fuel cleaning (Varrin, 2002) for mitigation of axial offset anomaly via crud removal.  The patent owner, EPRI, promotes the process as follows:  Ultrasonic fuel cleaning is a patented EPRI technology that removes deposited corrosion products from nuclear fuel pin surfaces by emitting radially distributed ultrasonic waves through the fuel pin bundle, followed by the use of water to carry crud from the fuel to the filters. The industry has used the technology with great success at several pressurized water reactor (PWR) nuclear power plants for mitigation of axial offset anomaly as well as the ancillary benefit of radiation field reduction.





3.    EARLY EXPERIENCE WITH FOULING AT LOW POWER BWRs



During the late 1950s and early 1960s corrosion of aluminum structures led to severe fouling probems at two low powered boiling water reactors that were developed at the Argonne National laboratory.



3.1    Experimental Boiling Water Reactor  (EBWR)



The Experimental Boiling Water Reactor (EBWR) was designed and operated by Argonne National Laboratory during the late 1950s and early 1960s.  An unfortunate selection of aluminum alloy for core filler pieces led to deposits of hydrated alumina on the zirconium clad fuel elements.  Thickness of the fouling was 0.013 cm, the thermal conductivity was 0.008 W/cm-C; thus the heat transfer coefficient was 0.6 W/(cm2)(C).  The peak heat flux in today’s large light water reactors is in the range of 150 W/cm2 and the temperature gradient for EBWR-type fouling would be 250 C.  However, the heat transfer coefficient for the combined fouling and zircaloy oxide of today's units is likely substantially less than the EBWR case.



3.2    Argonne Low Power Reactor (SL-1)



The SL-1 was destroyed in a Reactivity Insertion Accident (RIA) on January 3, 1961.  Fouling of the aluminum clad fuel plates likely intensified the severity of the accident.  However, fouling was not considered by the analysts who investigated this RIA.  Here is a quote from GE Report, Additional Analysis of the SL-1 Excursion, Report IDO-19313, 1962: The thickness of the cladding has an important effect on the magnitude of the excursion.  Because of the extremely short period, this 0.89 mm cladding became an effective thermal insulator and impeded the flow of heat to the reactor water where it could initiate shutdown of the reactor.  Now, inasmuch as the thermal conductivity of aluminum is  about 200 times greater than the corrosion on the fuel plate, a corrosion layer only 0.00445 millimeters thick would have the same temperature gradient as 0.89 mm of aluminum cladding. Alternatively, the measured corrosion product thickness of 0.09 mm has 20 times the temperature gradient of the aluminum cladding.  Ignoring the corrosion thus yields a grossly incomplete analysis in determining turnaround characteristics.





4.0    FOULING AND RUNAWAY



There has never been a runaway zirconium water chemical reaction in a nuclear power reactor that was induced by fouling.  However, there have been cases of rapid zirconium (zirconium alloy) reactions with water.  One case was the rapid oxidation that occurred during the Chernobyl accident.  And, during the accident at Three Mile Island there were likely times during which the cladding reaction  was relatively rapid.  As is clear from the River Bend experience, severe fouling leads to extensive corrosion of the cladding.  At River Bend, there was no runaway zirconium water reaction.  However, with the very thick deposits, it is not clear that limited runaway was not imminent. Following are two experiences with runaway that occurred during documented test programs.



4.1  Runaway During a Severe Fuel Damage Scoping Test



On Feb. 22, 1983, MacDonald of Idaho National Engineering Laboratory (INEL), in testimony to the Advisory Committee on  Reactor Safety (ACRS) discussed a destructive test in the Power Burst Facility (PBF).   A 32 rod array of PWR 17x17 fuel, 36 inches long, was heated to high temperature with fission heating and then exposed to a steam/water mix.  MacDonald stated, "We observed rapid oxidation of the lower portion of the bundle.  It wasn't expected.  It cannot be calculated with existing models. It is a flame-front phenomenon which is not addressed in the existing models.  It will probably be addressed in the coming months or years. ... Think of a sparkler.  That kind of phenomenon.  One of the problems with the existing models, all the axial loadings are extremely course.  They just do not deal with the spread of a zircaloy fire."  This was a case of substantial and unexpected runaway, and contrary to MacDonald’s forecast, the problem has not been addressed.



4.2    Runaway During FLECHT Run 9573



A series of experiments called Full Length Emergency Cooling Heat Tansfer (FLECHT) was initiated during the late 1960s and continues to this day under multiple programs at many laboratories.  The early tests were conducted with simulated fuel element assemblies.  A 7 by 7 array of  electrically powered stainless steel clad heaters, 12 feet long, was preheated to temperature in the range of 1000 to 1300 oC and then bottom-flooded with cooling water.  Temperatures along the test rods were monitored with thermocouples that were mounted internally.  A limited number of tests were run with zircaloy clad heaters.

       

        The extensive failure of the FLECHT assembly at 18 seconds after reflood was not anticipated.  (Limited runaway.) This may be fertile territory for SCDAP/RELAP5-3D.  Tasks would include analysis of Run 9573 as well as design and analysis of further tests. 



        In issuing its document, “Acceptance Criteria for Emergency Core Cooling Systems for Light-Water Cooled Nuclear Reactors-Opinion of the Commission,” Docket No. RM50-1, December 28, 1973, the Commission concluded, “It is apparent , however, that more experiments with zircaloy cladding are needed to overcome the impression left from run 9573.”  It is a fact that more experiments of the type called for have not been conducted.

4.3  Runaway Discussions at the Advisory Committee for Reactor Safeguards (ACRS)



The USNRC is currently working on revisions to rule 10 CFR 50.46 concerning emergency core cooling systems for reactors.  The process is called  risk-informing the regulation.  The ACRS discussions of Friday, May 31, 2002, are revealing in that several aspects of the revisions were discussed, however, the ubiquitous fouling of today’s LWRs was not considered.  This was a combined meeting of three of the most influential subcommittees of the ACRS: Materials and Metallurgy; Thermal Hydraulic Phenomena & Reliability and Probabilistic Risk Assessment

        Member Graham B. Wallis was especially enraged by the limited approaches to fuel integrity under LOCA conditions.  In response to detailed descriptions of fracture of corroded specimens of cladding from irradiated power reactor fuel he asserted:  It seems to be that both these coursing tests and hitting tests, impact tests and the squeezing tests are not really typical of the loads imposed on the real cladding.. I keep wondering what the relevance of all these tests are to the real truth.”  He also reacted to the discussions of  runaway,  “I think when you come back and talk about run-away to this committee you better have a criterion for run-away and not this sort of vagueness about heat transfer.”


        S. Bajorek of the NRC staff described Non-Conservatisms in the present day  Appendix K (10 CFR 50.46): “Now the processes that we've identified over the last few months which are strong candidates that need to be corrected are downcomer boiling, reflood ECC bypass and fuel relocation. Bajorek discussed fuel relocation as follows: “The issue of relocation has been around for several years. We hope to get better information in some of the newer tests that are being devised right now.  They are going to be running some tests with better instrumentation on the nuclear rods to try to get at fuel relocation which has been observed in tests in Germany, France and the U.S.  When we get this ballooning that occurs in the rod, it's possible that these fragmented pellets due to the vibrations can migrate down into the burst and rupture zone. The typical assumption in Appendix K is that these pellets remain as a concentric stack. Now I was talking to Dr. Ford who said why is this cladding temperature going down after it swells. It's good because you've swollen the cladding away from its heat source. If you are at low temperatures and zirc-water doesn't make any difference, this is a fin.  It's not a fin if you consider fuel relocation. It becomes much worse if there is a rupture involved and you have zirc-water reaction because now you've relocated the pellets, your local power is increased, you have very good communication now between the pellet fragments and the cladding itself. I have lost that fin effect. You see varying estimates on this. But we are identifying this as something that needs to be accounted for in future models.”



        The direct quotes from Bajorek are revealing.  The impact of fuel relocation on cladding heat transfer, temperatures, and oxidation reactions is emphasized.  However, the very definite impact of fouling on the course of a LOCA is not considered.  This is the case even though fouling is known to significantly impact the properties of the fuel pins at the beginning of LOCA.  .  The current 10 CFR 50.46 limits the calculated cladding temperature to 1200 oC.  With severe fouling, the cladding temperature during steady state power operation could exceed the starting temperature values in present LOCA documents by several hundred oC.  





5.  THE  IMPACT OF FOULING ON SEVERITY OF REACTIVITY INITIATED ACCIDENTS (RIAs) HAS BEEN OVERLOOKED



The U. S. nuclear power industry and the U. S. NRC have focused on the severity of RIAs in studies that are directed to extending burnup limits for PWR and BWR fuel.  These studies have not considered the impact of fouling on the severity of RIAs even though fouling is ubiquitous among the worldwide fleet of PWRs and BWRs.  A few years ago the NRC listed seven activities on high-burnup fuel research.  The following quotation is from the NRC’s then available document called HIGH-BURNUP FUEL RESEARCH.

“ A list of current NRC research activities on high-burnup fuel is shown below.

1. ANL (NRC) Hot Cell LOCA Tests of Fuel Rods and Mechanical Properties of Cladding

2. PNNL (NRC) Steady-State and Transient Fuel Rod Codes and Analysis

3. BNL (NRC) Neutron Kinetic Codes and Analysis of Plant Transients

4. Halden (Norway) Reactor Tests of Fuel Rods in Steady State and Mild Transients

5. Cabri (France) Reactivity Accident Tests of Fuel Rods and Related Programs

6. NSRR (Japan) Reactivity Accident Tests of Fuel Rods and Related Programs

7. IGR (Russia) Reactivity Accident Tests of Fuel Rods and Related Programs”



        Then, on June 12, 2002, the U. S. nuclear industry lobby organization, the Nuclear Energy Institute, provided the NRC with EPRI Report 1002865, Topical Report on Reactivity Initiated Accidents: Bases for RIA Fuel Rod Failures and Core Coolability Criteria.  This report purports to provide, “Revised acceptance criteria (that) have been developed for the response of light water reactor (LWR) fuel under reactivity initiated accidents (RIA).  Development of these revisions is part of an industry effort to extend burnup levels beyond currently licensed limits.  The revised criteria are proposed for use in licensing burnup extensions or new fuel designs.”  Clearly, the thrust of EPRI Report 1002865 is to extend burnup levels.  There is no consideration of fouling as a significant factor in the severity of RIAs.



        Next, on March 31, 2004, the NRC (Thadani, 2004) issued Research Information Letter No. 0401, “An Assessment of Postulated Reactivity-Initiated Accidents for Operating Reactors in the U. S.”  In the final paragraph of its cover letter to RIL 0401, the NRC states:  “We hope the attached assessment will provide NRR with independent information that will help in the review of EPRI Report 1002865, ‘Topical Report on Reactivity Initiated Accidents: Bases for RIA Fuel Rod Failures and Core Cool ability Criteria.’  The RES staff are available to assist NRR with that review, and RES is prepared to subsequently revise Regulatory Guide 1.77 on RIA safety analysis as indicated in the updated program plan,” In another paragraph of this cover letter, the NRC, for the first time ever, asserts that, “It should be noted that cladding failure thresholds vary only weakly with burnup level.  Cladding corrosion (oxidation) which might differ widely for different cladding materials at the same burnup was found to be the most important variable.”



        In a clarifying letter to Leyse (Paperiello, 2004, APPENDIX A) the NRC asserts that there is no need to account for crud deposits in the analysis of RIAs.  In paragraph 4, the NRC explains, “Going one level deeper in technical detail, we can draw a further distinction between the effects of oxide and crud.  Specifically, the oxidation process releases hydrogen, some of which is absorbed by the zirconium-based cladding alloy, where it embrittles the cladding and could lead to cladding failure during an RIA power transient.  By contrast, crud sits on top of the oxide and does not produce any embrittling products that migrate into the cladding metal.  Therefore, crud has only a secondary effect, as it provides some insulation and leads to slightly higher cladding temperatures that accelerate oxidation.  Nonetheless, the correlation of RIL-0401 explicitly accounts for total oxidation, so crud has no additional effect and there was no need to account for crud deposits in that analysis.”   It is noteworthy that Paperiello refers to hydrogen absorption as a cause of embrittlement of the cladding alloy, however, he makes no mention of  dissolved oxygen in the zirconium alloy as described by Leyse, 1964, Hobson and Rittenhouse, 1972, and very likely, others.  Hobson and Rittenhouse present correlations that relate the degree of embrittlement of  Zircaloy tubing to the amount of oxide on the surface and the additional dissolved oxygen gradient into the wall.  



        The NRC does not address the heat transfer characteristics of the oxide or the crud or the combination of the oxide and the crud.  The NRC regards the amount of oxide as a measure of the embrittlement of the cladding.  That embrittlement could then lead to cladding failure during an RIA power transient.  The NRC asserts that crud provides some insulation and leads to slightly higher cladding temperatures that accelerate oxidation, and that since RIL-0401 explicitly accounts for total oxidation, there is no need to account for crud deposits.  As the NRC’s incomplete analyses reveal, the impact of fouling on the severity of  RIAs has been overlooked.



6. THE IMPACT OF FOULING AND OXIDATION ON FUEL CLADDING                   OPERATING TEMPERATURES



Fouling leads to substantially higher cladding temperatures during normal operation of the nuclear power plant.  Fouling also leads to higher power levels during RIAs.  The heat transfer characterists of the fouling in the worldwide fleet of today’s LWRs have not been openly reported.  However, the thermal resistance of fuel element scale deposits at the Experimental Boiling Water Reactor (EBWR) has been documented.  The impact of the EBWR deposits on its fuel element dimensional changes has also been recorded.  More recently, there have been allusions to boiling chimneys within the fouling of today’s LWRs. 



6.1   Thermal Resistance and Impact of EBWR Scale



The Experimental Boiling Water Reactor (EBWR) was built and operated at the Argonne National Laboratory (ANL) near Chicago during the late 1950’s and early 1960’s. The initial power level was 20 megawatts.  The operating pressure was 40 atmospheres and the expected surface temperature of the zirconium-clad flat plate nuclear fuel elements was in the range of 255 degrees centigrade over a wide range of heat fluxes.  However, plans to operate the EBWR at substantially higher power levels were significantly impacted when significant scale deposits were discovered on the nuclear fuel elements. Scale deposits were most pronounced in the central regions of the reactor core where the maximum heat flux was in the range of 50 W/cm2.  These deposits were mainly aluminum oxide that was exfoliated from allegedly corrosion resistant aluminum alloy structures that were incorporated in peripheral locations of the reactor core.  The scale was extremely adherent to the zirconium heat transfer surfaces until the thickness reached the range of 0.013 centimeters, at which point some of the scale flaked off and entered the flow of boiling water.

      

Breden and Leyse, 1960, reported a range of activities.  An overall fuel inspection was performed during April,1959.  Fuel element ET-51 which operated in a relatively high flux location since startup was examined in the Argonne  hot cell.  A substantial amount of scale flaked off during the handling.  (See Figure 2.) Thickness was about 0.013 cm.  Density was 2.5 gm/cm3 based on weight and volume. The scale was attracted by a magnet.  Composition based on wet chemical, spectrographic and X-ray diffraction measurements yielded the following: boehmite, 80.6 %; nickel oxide, 12.6 %; iron oxide, 5.1%; silicon dioxide 1.6%.  Thermal conductivity of the flat (planar) scale was 0.008 W/(cm2)(oC). 























 


 


 



Figure 2.  Assembly of the EBWR plate-type fuel element and a hot cell photograph of one section of plate fuel. The scale is peeling away from the zirconium cladding.  The scale was very adherent to the cladding until it reached a thickness in the range of 125 microns when peeling began.  The zirconium clad enriched uranium metal plate type fuel elements were extremely robust, however, the thick scale led to fuel plate temperatures beyond design.  Therefore, the fuel plates expanded longitudinally beyond design limits when the EBWR was operated at elevated power levels for brief times (a few hours).  With no fouling of the fuel plates, the operating temperature of the fuel plates in the boiling water system would increase relatively little as heat flux (reactor power) was increased.  However, with the extra longitudinal growth of the fouled fuel plates, the side plates were stretched.  During inspections of the core, the perforated side plates were then found to be bowed between the assembly spot welds.  Clearly, the fouling had no “boiling chimneys” that enhanced heat transfer.



6.2   Boiling Chimneys



At times, there are inferences that crud deposits enhance heat transfer.  Mr. Deshon of EPRI referred to “boiling chimneys”  during his presentation to the U. S. NRC’s ACRS Reactor Fuels Subcommittee, September 30, 2003.  On page 132 of the transcript of this meeting,  Deshon asserts that these boiling chimneys enhance heat transfer from the cladding to the coolant when the thickness of the fouling is up to a thickness of 20 microns.  Next, on page 133, he refers to a flake with a thickness of 125 microns with “… very large voids in the crud, representing these boiling chimneys.”   Now, it is unlikely that a chimnied layer having a thickness of 20 microns will enhance the heat transfer from the cladding to the cooling water, and it  is very unlikely that a porous layer of 125 microns will be anything other than a significant barrier to heat transfer.  Deshon presented no experimental data to prove the enhancement of heat transfer.



        Now, wick boiling has been discussed by many investigators as a means of improving the performance of heat pipes.  In those applications, the fluid is highly pure and the wick geometry is fixed by controlled means (wire mesh structures, specific chemical vapor deposition and perhaps others).  However, the crud formations on nuclear power plants will not have the prescribed boiling channels.  Even if an optimum boiling chimney array is built into the surface of the cladding, the lifetime of any enhancement would be nil as magnetite and other deposits ruin the system.

7.0  INCOMPLETE TESTING, INCOMPLETE CODES, DEFICIENT REGULATION      

Although billions of dollars have been expended on testing and code production, the products are grossly deficient in terms of producing the realistic bases for current regulation of water cooled nuclear power plants.  Moreover, there is a dearth of undirected exploratory research that could bear on the technology.

7.1    Incomplete Testing and Analysis of Test Data

During the last five decades there have been hordes of test programs.  Many have been significant and useful, but the preponderance of the work has been incomplete.  The Borax experiments of the 1950’s were an impressive exploration into the inherent safety light water reactors, but the work was incomplete when the approaches were abandoned.  Further Borax-type experiments in the 1960’s followed the destructive reactivity insertion accident at SL-1, but again, the work, Special Power Excursion Reactor Tests (SPERT) was abandoned before it was complete.  The common thread of inadequacy of these programs was the total disregard of the significant impact of fouling on the results and conclusions.  The work in the Power Burst Facility (PBF) was abandoned with no regard for the impact of fouling. 

        Fouling has been ignored in the design, conduct, and interpretation of the multitude of  heat transfer tests related to emergency core cooling.  This was true of the extensive FLECHT and related programs that began during the 1960s and is true of the continuing programs that are funded today.  One example (among several) of today’s efforts is the Rod Bundle Heat Transfer Testing (RBHT)at Pennsylvania State University.  Although millions of dollars are being expended on RBHT, that expenditure is likely insignificant in comparison with the total of other programs in the United States as well as the international community.  The very expensive nuclear powered tests in the Loss of Fluid Test (LOFT) were likewise discontinued without any recognition that the fouling that is commonplace in light water power reactors (LWRs) would have a significant impact.

7.2    Incomplete Codes

The common practice is to “calibrate” or otherwise certify computer codes that are employed in reactor safety analyses based on results of testing in programs such as FLECHT, PBF, SPERT, LOFT and a multitude of others.  A limited number of tests have also been conducted during the startup phases of commercial nuclear power reactors. Fortunes have been expended on so-called “test cases” and “round robin” exercises.  However, none of the codes ranging from the current RELAP, RETRAN, TRACE and countless others have been “calibrated” based on test results with fouled heat transfer surfaces.  It could be argued that all of the codes have the capability of modeling a range of heat transfer resistances that could be assigned to fouling.  It is a fact that this has not been done, and even if it was attempted, the results would have little credibility.

7.3    Deficient Regulation

Under the banners of  “realism” and “conservative realism” there are current moves to produce “risk informed” regulations.  Indeed, an opening panel discussion called  Risk Informing Emergency Core Cooling System (50.46) Requirements” is scheduled for the USNRC’s Regulatory Information Conference, March 2005. It is unlikely that the panel will discuss the deficiencies in the NRC’s regulations related to LOCAs.  The NRC and the DOE’s national laboratory, INEEL, avoid  realistic test programs  (Rankin, 2003, APPENDIX B).  They also avoid realistic code applications (Jacobsen, 2003, APPENDIX C). Initiatives that would derail deficient regulations are summarily rejected.



8.0  SUMMARY AND CHALLENGES





Fouling is ubiquitous.  A few of the cases of severe fouling in light water reactors over the past five decades, with power levels have ranging from tens to thousands of megawatts, have been described. 



        Fouling has a substantial thermal resistance.  Fouling leads to increased surface temperature of zirconium alloy cladding and this increases the rate of formation of layers of zirconium oxide. Values of thermal resistance of  present day fouling have not been reported.  However, at a modest heat flux of 100 W/cm2 the cladding temperature increases by 115 oC per 25 microns of zirconium dioxide.



        Fouling has a greater impact than burnup on reactivity insertion accidents (RIAs). There is an erroneous belief at the USNRC that fouling has only a minor role in the severity of RIAs.  The USNRC is preoccupied with the phenomenon of embrittlement. Even in the absence of cladding embrittlement, the thermal resistance of severe fouling will substantially increase the severity of an RIA.



        Fouling has a substantial impact on loss of coolant accidents (LOCAs).  With severe fouling, the cladding temperature at the start of the accident will be several hundred degrees higher than is the basis of LWR operating licenses.  The added impact of the resulting  layer of zirconium dioxide and the associated embrittlement adds to the adverse impact of the severe fouling.



        Very clearly, the current fouling of LWR fuel elements must be classified: thermal characteristics, composition, porosity, etc.  The characteristics of fouling must be added to the complex codes: RELAP, RETRAN, TRAC, TRACE and others.  This will place realism into licensing of LWRs.

REFERENCES


Breden, C. R. and Leyse, R. H., 1960.  Water Chemistry and Fuel Element Scale in the EBWR.  Report ANL-6136.  Argonne National Laboratory.



Frattini, P. L., et al., 2001.  Axial offset anomaly: coupling PWR primary chemistry with core design. Nuclear Energy, 40, 123 -133.



Hobson, D. O., and Rittenhouse, P. L., 1972.  Embrittlement of Zircaloy-Clad Fuel Rods by Steam During LOCA Transients. Report ORNL 4758. Oak Ridge National Laboratory.


King, R. J., 2000.  Thermally-Induced Accelerated Corrosion of BWR Fuel.  Licensee Event Report 50-458/99-016-00. Entergy.



Leyse, R. H., 1964.  Zircaloy-2 and Type 304 Stainless Steel at 2000oF in Water-Steam for Brief Times.  Report APED-4413. General Electric Co.



McAdams, W. H. 1942. Heat Transmission. Second edn. McGraw-Hill.



Rockwell, T. 2004. On the 50th Anniversary. Nuclear News, August 2004, 36-40.



Rusauskas, E. J., and Smith, D. L. 2004.  Fuel Failures During Cycle 11 at River Bend.  Proceedings of the 2004 International Meeting on LWR Fuel Performance.  American Nuclear Society.



Schneider, R. J., et al.,  2004.  Recent GNF BWR Fuel Performance.  Proceedings of the 2004 International Meeting on LWR Fuel Performance.  American Nuclear Society.



Thodani, A. C., 2004. An Assessment of   Postulated Reactivity Insertion  Accidents for Operating Reactors in the U. S. Research Information Letter No 401.  United States Nuclear Regulatory Commission.



Varrin, R. D. 2002.  United States Patent, US 6,396,892.























































































APPENDIX A



 


 


 


 


 


 


 


 


 


 


 


 




























 


 


 


 


 


 


 





























































APPENDIX B



The following letter shows that only initiatives from NRC or DOE are allowed at  INEEL.



 






















































































APPENDIX C



Following are excerpts from  the letter and the attachment that Leyse received from staff at INEEL dated June 17, 2003.  As the attachment reveals, the users of SCDAP/RELAP, MELCOR, and MAAP do not  consider fouling , “…because it has not been demonstrated conclusively that this effect should be considered.”  In response to this INEEL letter, Leyse submitted a revised approach and the slide presentation, “Unmet Challenges for SCDAP/RELAP5-3D: Analysis of Severe Accidents for Light Water Nuclear Reactors with Heavily Fouled Cores,” may be viewed via GOOGLE, enter Leyse Relap.  Of course, the USNRC and the USDOE have continued to spend millions of dollars annually on thermal hydraulic testing and code development.  Nevertheless, the impact of severe fouling is overlooked in the wide assortment of international activities. To this day (January 17, 2005) the impact of severe fouling on fuel element temperatures has not been considered in licensing of LWRs.    

  










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