https://relap53d.inl.gov/seminars/westyellowstone2003/Shared%20Documents/leyse.pdf
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.”
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.
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.”
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.
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 tex tured
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 ur anium
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 Po wer 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 “cali brate”
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 “cali brated”
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 tex tured
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 ur anium
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 Po wer 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 “cali brate”
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 “cali brated”
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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