daniel yan
TRANSCRIPT
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Supercritical-Water-Cooled Reactor System - as one of the most
promising type of Generation IV Nuclear Reactor Systems
Davit Danielyan
November 24, 2003.
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EXECUTIVE SUMMARY
The supercritical water is interesting
and not yet deeply studied phenomena in
nature (pic.1). Critical parameters for thewater are 374C, 22.1 MPa. The supercritical
water-cooled reactor (SCWR) is one of the six
reactor technologies selected for research anddevelopment (R&D) under the Generation-IV
program. SCWRs are promising advanced
nuclear systems because of their high thermal
efficiency (i.e., about 45% vs. about 33%efficiency for current Light Water Reactors,
LWRs) and considerable plant simplification.
Picture1. Supercritical water in nature - Black Smoker
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TABLE OF CONTENTS
EXECUTIVE SUMMARY............................................................................................................. 2
TABLE OF CONTENTS................................................................................................................ 3
1. INTRODUCTION....................................................................................................................... 4
2. TECHNICAL PROGRESS IN SCWR R&D............................................................................72.1 Technology Base for the SCWR ................................................................................................. 7
2.1.1 Reactor Vessel........................................................................................................................... 7
2.1.2 Containment.............................................................................................................................. 7
2.2 NERI &INERI Projects................................................................................................................8
2.3 Technology Gaps for the SCWR................................................................................................. 82.4 Core and Fuel Assembly Design and Materials Selection.......................................................... 9
2.4.1 Corrosion and SCC.................................................................................................................. 10
2.4.2 Radiolysis and Water Chemistry. ............................................................................................ 11
2.4.3 Dimensional and Microstructural Stability. ............................................................................ 12
2.4.4 Stability Analysis...................................................................................................................... 12
2.4.5 Strength, Embrittlement, and Creep Resistance....................................................................... 13
2.5 SCWR Reactor Systems R&D..................................................................................................... 132.6 Balance of Plant (BoP).................................................................................................................13
2.7 SCWR Safety R&D..................................................................................................................... 13
2.8 Preliminary Analysis of Key Transients and Accidents.............................................................. 142.9 Flow Stability............................................................................................................................... 16
2.10 SCWR Design and Evaluation R&D......................................................................................... 16
2.11 Control Strategy......................................................................................................................... 16
2.12 SCWR Fuel Cycle R&D............................................................................................................ 17
5. CONCLUSIONS ......................................................................................................................... 18
6. REFERENCES............................................................................................................................. 18
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1. INTRODUCTION
SCWRs are basically LWRs operating at higher pressure and temperatures with a direct once-
through cycle (pic2.). Operation above the critical pressure eliminates coolant boiling, so the coolantremains single-phase throughout the system.
Thus the need for recirculation andjet pumps, pressurizer, steam
generators, steam separators anddryers is eliminated (pic.3). The
main mission of the SCWR is
generation of low-cost electricity.Thus the SCWR is also suited for
hydrogen generation with
electrolysis, and can support thedevelopment of the hydrogen
economy in the near term. It is
built upon two proventechnologies, LWRs, which are the
most commonly deployed power
generating reactors in the world,
and supercritical fossil-fired boilers, Picture 2. SCWR - simplified once-through direct cyclea large number of which is also in use around the world. The SCWR concept is being investigated by
32 organizations in 13 countries.
The objective of the multi-year SCWR program is to assess the technical viability of the SCWRconcept. Thus the focus is on establishing a conceptual design, assessing its safety and stability
characteristics, and identifying and testing candidate materials for all reactor components.
The US supercritical light water reactor (SCLWR) with a thermal spectrum will be in this report the
subject of the most development work and is the basis for much of the reference design.The reference design has been selected a for the SCWR system that focuses on a large-size, direct-
cycle, thermal-spectrum, light-water
cooled and moderated, low-enricheduranium fuelled, base-load operation
plant for electricity generation at low
capital and operating costs. Theoperating pressure and core inlet/outlet
temperatures are 25 MPa and
280/500oC, respectively. The coolant
density decreases from about 760
kg/m
3
at the core inlet to about 90kg/m3 at the core outlet. Thus, large
square water rods with down flow are
used to provide adequate moderation
in the core. The fuel pin design is
similar to that of a pressurized waterreactor (PWR), but with higher fill pressure and longer Picture 3. Simplifications in SCWR
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fission gas plenum. Candidate materials for all fuel assembly and vessel internal components include
ferritic-martensitic steels and low-swelling austenitic steels for the components exposed to highneutron doses, and high-strength austenitic steels and nickel-based alloys for low-dose components.
However, these materials are un-proven in the potentially aggressive SCWR environment, and their
performance will have to be tested. A materials development program has been prepared for this
purpose.Two traditional austenitic steels (304L and 316L) were tested for corrosion and stress-corrosion
cracking (SCC) susceptibility in supercritical water. It was found that both alloys are susceptible toSCC (316L less so than 304L) in both
deaerated and nondeaerated high-
temperature (>400oC) supercritical
water. Thus, these alloys cannot be
used for hightemperature components
in the SCWR. However, they could be
used for components operating in the280-350oC range (e.g., the lower core
plate, the control rod guide tubes),given their satisfactory behavior indeaerated water at these temperatures.
The SCWR core average power
density is about 70 kW/L, i.e., betweenthe power density of boiling water
reactors (BWRs) and PWRs. The reactor Picture 4. Operating cycle diagrams for SCWR
coolant system of the SCWR comprises the feedwater lines and main steam lines up to the outermost
set of containment isolation valves. Similar to a BWR, the SCWR uses two feedwater lines made ofcarbon steel. However it has been determined that because of its high-density steam, the SCWR needs
only two steam lines as opposed to four in a BWR of similar thermal power. This further adds to the
economic strength of the SCWR concept. The steam lines can be constructed out of ferritic steels suchas P91 and P92, which are currently used in supercritical fossil plant steam lines.
A pressure-suppression type containment with a condensation pool, essentially the same design as
modern BWRs, was selected. The dry and wet well volumes were calculated to limit the pressurebuild-up to typical BWR levels following a LOCA or a severe accident with core melting.
The condensation pool water inventory was designed to provide ample margin for residual heat
removal and meet the requirement that active safety systems are not needed during the first 24 hours
following an initiating event resulting in a severe accident. The very conservative European UtilityRequirements for mitigation of severe accidents were adopted in sizing the containment and a core
catcher was added to the design. Despite this conservative approach the SCWR containment is
somewhat smaller than that of an advanced BWR of similar thermal power, and thus significantlysmaller on a per unit electric power basis.
Thermal-hydraulic and thermal-nuclear coupled instabilities were investigated at ANL with a
frequency-domain linear stability analysis code based on single-channel thermal hydraulics, one-dimensional fuel heat conduction, and point-kinetics models. The BWR stability criteria were adopted
and it was found that the SCWR is stable against core-wide in-phase oscillations at normal operating
power and flow conditions.A critical review of the LWR abnormal events and their NRC classification has been performed with
the SCWR application in mind. Four events were singled out that could be potentially troublesome: (i)
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loss of feedwater flow, which in the once-through direct-cycle SCWR coincides with the loss of core
flow, (ii) turbine trip without steam bypass, which pressurizes the system and could result insignificant positive reactivity insertion because of the low density of the SCWR coolant, (iii) loss of
feedwater heating, which also results in the insertion of positive reactivitybecause of the lack of
feedwater mixing with hotter coolant in the vessel, and (iv) large break in the feedwater lines, which,
if unmitigated, results in coolant stagnation in the core and rapid overheating of the fuel. Apreliminary analysis of these four key events was performed at INEEL with a modified version of the
RELAP5 code. It was found that the SCWR behavior is relatively benign during the turbine tripwithout steam bypass, the loss of feedwater heating, and the large break in the feedwater lines.
On the other hand, survival of the total loss of feedwater will likely require the use of a high-capacity
high-pressure fast-acting auxiliary feedwater system. Design of such system will be a major challenge.The reference SCWR system has a power conversion cycle that is very similar to a supercritical coal-
fired plant, with the boiler replaced by the nuclear reactor. A conceptual study was performed by
BREI to identify an optimal configuration for the goals of thermal efficiency maximization and capital
cost minimization. The SCWR power conversion cycle uses a single-shaft turbine-generator, operatingat reduced speed (1,800 rpm), with one high-pressure/intermediate-pressure (HPT/IPT) turbine unit
and three low-pressure turbine (LPT) units with six flow paths, with a moisture separator reheaterbetween the HPT/IPT and the LPTs, eight feedwater heaters, steam-turbine-driven feedwater pumpsand natural draft cooling towers. The reference design generates 1,600 MWe with a thermal efficiency
(net electric power to the grid / fission power) of 44.8% versus about 35% for LWRs under equivalent
assumptions.A pre-conceptual design of the SCWR control system was also performed. The main characteristics
affecting the design of the SCWR control system are the relatively low vessel water inventory, the
nuclear/thermal-hydraulic coupling, the lack of level indication under supercritical conditions and the
absence of recirculation flow. The main variables to be controlled include the reactor power, the coreoutlet temperature during supercritical pressure operation (e.g., full power operation), the reactor
pressure, the reactor level during subcritical pressure operation (e.g., during start-up) and the
feedwater flow. Then, assuming base-load operation, the recommended approach for the SCWR is onein which the control rods accomplish the primary control of the thermal power, the turbine control
valve provides the control of the pressure, the feedwater flow (i.e., the feedwater pumps) provides the
primary control of the outlet temperature, and the control of the coolant inventory in the vessel isaccomplished by assuring that steam and feed flow are balanced while maintaining the correct core
outlet temperature.
Also, rather than an approach in which higher functions such as power or turbine valve control are in
manual with lower level control loops in automatic, the use of an integrated control approach, one inwhich all functions are in automatic, is deemed preferable due to the SCWRs expected fast response
to perturbations.
In summary, the research work during the first year of the Generation-IV SCWR program hasconfirmed the basic assumptions contained in the Generation-IV Roadmap Report regarding the
SCWR, and no new potential showstoppers have been found. The key feasibility issues for the SCWR
remain the development of in-core materials and the demonstration of adequate safety. Dynamicinstabilities appear to be less of a concern.
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2. TECHNICAL PROGRESS IN SCWR R&D
2.1 Technology Base for the SCWRMuch of the technology base for
the SCWR can be found in the
existing LWRs and incommercial supercritical-water-
cooled fossil-fired power plants
(pic.5). However, there are somerelatively immature areas. There
have been no prototype SCWRs
built and tested. For the reactor
primary system, there has beenvery little in-pile research done
on potential SCWR materials or
designs, although some SCWRin-pile research has been done
for defense programs in Russia
and the United States. Limiteddesign analysis has been
underway over the last 10 to 15 Picture 5. SCW in power industry
years in Japan, Canada, and Russia.
2.1.1 Reactor VesselThe SCLWR reactor vessel is similar in design to a PWR vessel (although the primary coolant system
is a direct-cycle, BWR-type system). High-pressure (25.0 MPa) coolant enters the vessel at 280C.The inlet flow splits, partly to a downcomer and partly to a plenum at the top of the core to flow down
through the core in special water rods.
2.1.2 ContainmentThe SCWR containment is a pressure-suppression type containment with a condensation pool
(essentially the same design as modern BWRs).The dry and wet well volumes were calculated to limit the pressure build-up to typical BWR levels
following a LOCA or a severe accident with core melting (hydrogen generation from cladding
oxidation was considered in the calculations). The concrete floors were designed to withstand suchloads. The condensation pool water inventory provides ample margin for residual heat removal andmeets the requirement that active safety systems are not needed during the first 24 hours following an
initiating event resulting in a severe accident. The blow-down pipes or vents are placed in the outer
cylindrical walls due to lack of space in the inner cylindrical walls.Compared to the advanced BWR containment designs, the SCWR containment drywell can be reduced
because:
The SCWR has only two steam and feedwater lines.
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The SCWR has a smaller diameter of the pressure vessel. The control rods enter the reactor pressure vessel from the top. Also, there are less control rod
drive installations needed and fewer areas needed for transportation of equipment. Also,installations for control rod drive maintenance are not needed below the pressure vessel.
There are no internal recirculation pumps.On the other hand, the SCWRcontainment drywell volume isincreased because of the high
temperature fluid moving from the
reactor to the turbine, sinceadditional cooling and thermal
expansion space are needed. Also,
the concrete must accommodatehigher temperatures during an
accident.
Furthermore the SCWR
containment is lower because thepressure vessel is lower. However,
this will tend to increase the
diameter of the containment andwill also lead to less space for
connections and floorings. When all Picture 6. Small Containment for SCWR
these effects are accounted for, theSCWR containment ends up being somewhat smaller than that of an advanced BWR of similar
thermal power, and thus significantly smaller on a per unit electric power basis (pic. 6).
2.2 NERI &INERI Projects
Number of non-Generation-IV SCWR activities in the U.S. include four NERI projects and two INERIprojects. While these projects have well-defined scope and budgets that pre-date the inception of the
Generation-IV program, an attempt has been made to coordinate their activities with the Generation-IV activities, so that DOE-NEs objective of assessing the feasibility of the SCWR concept can be
pursued effectively. The NERI and I-NERI projects are briefly presented next; however much more
information can be found in the progress reports that these projects produce quarterly and annually forDOE.
2.3 Technology Gaps for the SCWRIn this chapter will consider important SCW
technology gaps (pic.7). They are mainly in
the areas of: SCWR materials and structures, including
Corrosion and stress corrosion cracking(SCC)
Radiolysis and water chemistry
Dimensional and microstructural stability
Strength, embrittlement, and creep
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resistance Picture 7. Core materials
SCWR safety, including power-flow stability during operation
SCWR plant design.
Important viability issues are found within the first two areas, and performance issues are foundprimarily within the first and third areas.
2.4 Core and Fuel Assembly Design and Materials SelectionThe supercritical water (SCW) environment is unique and few data exist on the behavior of materials
in SCW under irradiation and in the temperature and pressure ranges of interest. At present, nocandidate alloy has been confirmed for use as either the cladding or structural material in thermal or
fast spectrum SCWRs (pic. 8).
Potential candidates include austenitic stainless steels, solid solution and precipitation-hardened alloys,
ferriticmartensitic alloys, and oxide dispersion-strengthened alloys.The fast SCWR design would result in greater doses to cladding and structural materials than in the
thermal design by a factor of 5 or more. The maximum doses for the core internals are in the 1030dpa range in the thermal design, andcould reach 100150 dpa in the fast
design. These doses will result in
greater demands on the structuralmaterials in terms of the need for
irradiation stability and effects of
irradiation on embrittlement, creep,
corrosion, and SCC. The generationof helium by transmutation of nickel
is also an important consideration in
both the thermal and fast designsbecause it can lead to swelling and
embrittlement at high temperatures.
The reference SCWR core designhas 145 assemblies with an
equivalent diameter of about 3.9
meters. The average power density is Picture 8. Probable core designs
about 70 kW/L (or 30% higher thanBWRs and 35% lower than PWRs) with a total target power peaking factor of about 2.0. The average
and peak linear heat generation rates are similar to typical LWR values. The estimated core pressure
drop is also comparable with typical LWR pressure drops and inlet orifices are used to adjust the flowto each assembly based on its expected power.
However, the control rod worth calculations are not complete and it may be desirable to change the
number and/or size of the control elements, or it may be desirable to change the locations of thecontrol elements. Also, it is assumed that there is one instrumentation tube in each assembly at the
center fuel rod location. The number of the dimensions are tentative including the fuel bundle wall
thickness and the inter-assembly gap size, and the fuel pin spacers have yet to be designed.The reference fuel pin dimensions are typical of 1717 PWR fuel assembly pins, with the exception ofthe plenum length and fill pressure. Candidate materials have been identified by the ORNL materials
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experts for all the components of the fuel assembly. The structural materials recommended for these
components are primarily ferriticmartensitic steels, and low swelling variants of the austenitic stainlesssteels. Among the more advanced materials oxide-dispersion strengthene ferritic steels and ceramic
composites (e.g., SiC-SiC) should also be explored given their potential for superior high-temperature
strength. Many of these materials have been selected based on satisfactory unirradiated properties
and/or proven performance under irradiation.
2.4.1 Corrosion and SCC.The SCWR corrosion and SCC research activities should focus on obtaining the following
information:
Corrosion rates in SCW at temperatures between 280 and 620C (the corrosion should be measuredunder a wide range of oxygen and hydrogen contents to reflect the extremes in dissolved gasses)
Composition and structure of the corrosion films as a function of temperature and dissolved gasses
The effects of irradiation on corrosion as a function of dose, temperature, and water chemistry
SCC as a function of temperature, dissolved gasses, and water chemistry The effects of irradiation on SCC as a function of dose, temperature, and water chemistry.
The corrosion and SCC R&D activities will be organized into three parts: an extensive series of out-of-pile corrosion and SCC experiments on unirradiated alloys, companion out-of-pile corrosion andSCC experiments on irradiated alloys, and in-pile loop corrosion and SCC tests. It is envisioned that at
least two and maybe as many as four out-of-pile test loops would be used, some addressing the
corrosion issues and others addressing the SCC issues. At least two such loops should be built inside ahot cell in order to study preirradiated material. Facilities to preirradiate samples prior to corrosion and
SCC testing will be required.
The fourth NERI project (see 2.2) is titled Fundamental Understanding of Crack Growth in Structural
Components of Generation IV Supercritical Light Water Reactors and is conducted at the StanfordResearch Institute International. A test system for electrochemical and fracture mechanics studies in
supercritical water was built as part of this project. Controlled-distance electrochemistry is used to
measure the transport of ions or ionic defects in the oxide films on structural components made ofstainless steels and nickel base alloys at supercritical temperatures. Ionic transport is then correlated
with the susceptibility to cracking using fracture surface topography analysis of crack initiation and
growth.The first NERI project (see 2.2) is titled Feasibility Study of Supercritical Light Water Cooled
Reactors for Electric Power Production, is led by the INEEL, started in 2001 and includes
Westinghouse, the University of Michigan, and MIT. Activities at INEEL and Westinghouse include
the neutronic, thermal-hydraulic, and mechanical design of the SCWR fuel assembly, core and vesselinternals. As part of this project a new SCW loop was constructed at the University of Michigan to
investigate the susceptibility of candidate structural alloys to stress corrosion cracking in supercritical
water at various temperature, pressure, oxygen, pH and conductivity conditions.A second NERI project (see 2.2) is titled Supercritical Water Nuclear Steam Supply System:
Innovations in Materials, Neutronics and Thermal-Hydraulics, is led by the University of Wisconsin
at Madison and ANL, and also started in 2001. R&D activities include core and plant design with theemphasis on an innovative dual-spectrum core concept using a fast central region surrounded by a
thermal annular region.
The first I-NERI (see 2.2) is a collaboration with the Korean Atomic Energy Research Institute(KAERI) in South Korea, is titled Developing and Evaluating Candidate Materials for generation-IV
Supercritical Water Reactors, started in 2003 and includes the ANL-West as the lead organization,
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the INEEL, the University of Michigan and the University of Wisconsin at Madison. The scope of this
project includes a survey of commercial alloys for application to the SCWR, preparation of surface-treated coupons at the University of Wisconsin, testing of commercial and surface-treated alloys in the
SCW loop at the University of Michigan, as well as mechanical testing of advanced alloys at INEEL.
The second I-NERI (see 2.2) is also a collaboration with South Korea (Seoul National University and
KAIST), is titled Advanced Computational Thermal Fluid Physics (CTFP) and its Assessment forLight Water Reactors and Supercritical Reactors and involves INEEL as the lead organization, Iowa
State University, the University of Maryland, and Pennsylvania State University. This basic thermalfluids research applies first principles approaches (direct numerical simulation and large eddy
simulation) coupled with experimentation (heat transfer and fluid mechanics measurements) to
develop reliable computational tools for modeling of transport phenomena in supercritical fluids incomplex geometries such as the core of a SCWR. The experimental work is performed at the INEELs
Matched-Index-of- Refraction flow system while the development of the computational methods is
performed at the universities.
2.4.2 Radiolysis and Water Chemistry.
The SCWR water chemistry research program should focus on obtaining the following information: The complete radiolysis mechanism in SCW as a function of temperature and fluid density The chemical potential of H2, O2, and various radicals in SCW over a range of temperatures (280
620C)
Recombination rates of various radicals, H2, and O2 in SCW over a range of temperatures (280620C)
Effect of radiation type: neutrons, gammas, as well as flux on radiolysis yields
Formation and reaction of other species by radiolytic processes
Impurities introduced into the primary system.
Two research avenues are envisioned to obtain this information. First, beam ports and accelerators can
be used to irradiate SCW chemistries and study the characteristics of the recombination processes insome detail.
This information will be integrated into a model of the water radiolysis mechanism. Second, water
chemistry control studies can be performed using the in-pile test loops needed for the corrosion andSCC research discussed above.
A third NERI project (see 2.2) is titled Neutron and Beta/Gamma Radiolysis of Supercritical Water,
and is performed at ANL, the University of Wisconsin and Notre Dame University. This project
started in 1999 and was renewed in 2002. During the first phase of the project ANL used anaccelerator-based pulse radiolysis approach to measure the yields and recombination rates of key
radiolytic species in supercritical water. In the second phase the team has built a SCW loop inside the
TRIGA reactor at the University of Wisconsin to directly measure the concentration of radiolyticspecies in supercritical water under neutron irradiation. Also, means to suppress radiolysis such as
hydrogen injection are being investigated.
2.4.3 Dimensional and Microstructural Stability.The SCWR dimensional and microstructural research activities should focus on obtaining the
following information: Void nucleation and growth, and the effect of He production, on void stability and growth, and He
bubble nucleation and growth as a function of dose and temperature
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Development of the dislocation and precipitate microstructure and radiation-induced segregation as a
function of dose and temperature Knowledge of irradiation growth or irradiation induced distortion as a function of dose and
temperature
Knowledge of irradiation-induced stress relaxation as a function of tension, stress, material, and
dose.While many of the test specimens for this work will be irradiated in the corrosion and SCC in-pile
loops discussed above, accelerator-based irradiation offers a rapid and low-cost alternative to thehandling and analysis of neutron-irradiated material.
2.4.4 Stability AnalysisConsistent with the U.S. NRC approach to BWR licensing, the licensing of SCWRs will probably
require, at a minimum, demonstration of the ability to predict the onset of instabilities. This can be
done by means of a linear analysis. Prediction of the actual magnitude of the unstable oscillations
beyond onset, although scientifically interesting and relevant to beyond-design-basis accidents, willlikely not be required for licensing and can be delayed to a second phase of the SCWR development.
Following the standard approach for BWR stability analysis, the system stability was estimated usingthe decay ratio, which is determined by searching the dominant root of the system characteristicequation directly in the complex plane. Preliminary stability analyses were performed for the reference
SCWR concept. It was found that the core-wide in-phase oscillations would decay quickly at normal
operating power and flow conditions.
2.4.5 Strength, Embrittlement, and Creep Resistance.
The SCWR strength, embrittlement, and creep resistance research activities should focus on obtaining
the following information: Tensile properties as a function of dose and temperature
Creep rates and creep rupture mechanisms as a function of stress, dose, and temperature
Creep-fatigue as a function of loading frequency, dose, and temperature Time dependence of plasticity and high-temperature plasticity
Fracture toughness as a function of irradiation temperature and dose
Ductile-to-brittle transition temperature (DBTT) and helium embrittlement as a function of dose andirradiation temperature
Changes in microstructure and mechanical properties following design basis accidents.
The research should aim at high-temperature performance of both irradiated and unirradiated alloys
and also at low-temperature performance of irradiated alloys.High-temperature testing will include yield property determination, time dependent (creep)
experiments, and also the effect of fatigue loading with a high mean stress.
2.5 SCWR Reactor Systems R&DA number of reactor system alternatives have been developed for both vessel and pressure tube
versions of the SCWR. Significant additional work in this area is not needed.
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2.6 Balance of Plant (BoP)
The SCWRs can utilize the existing technology from the secondary side of the supercritical water-cooled fossilfired plants (pic. 9). Significant research in this area is not needed.The reference SCWR system has a power conversion cycle that is very similar to a supercritical coal-
fired plant, with the boiler replaced by the nuclear reactor. BREI has performed a conceptual study of
the power conversion cycle for the SCWR to identify an optimal configuration for the goals of thermalefficiency and electric power output
maximization and capital costminimization. Particular attention was
also given to ensure that all components
are either commercially available orwithin current design capabilities. The
following trade-offs affecting the goals
were considered: full vs. reduced speed
of the turbine-generator module, single-shaft vs. multi-shaft arrangement of the
turbine-generator module, steam-turbine-driven vs. motor-drivenfeedwater pumps. The following design
choices should be noted:
Reduced rotation speed, 1800rpm
Single-shaft turbine-generator Picture 9. Balance of Plant One high-pressure/intermediate-pressure turbine (HPT/IPT) unit and three low-pressure turbine
(LPT) units with six flow paths
Moisture separator reheater between the HPT/IPT and the LPTs Eight feedwater heaters raising the feedwater temperature to 280oC Steam-turbine-driven feedwater pumps operating at about 190oC Heat rejection in natural draft cooling towers
The reference design generates 1,600 MWe with a thermal efficiency (net electric power to the grid /
fission power) of 44.8%. BREI has also sized the feedwater heaters, pumps, cooling tower, steam
lines, condenser, etc. Note that, due to the higher steam density, only two small steam lines are neededfor this large size SCWR vs. four lines for an LWR of comparable power, which further adds to the
capital cost savings of the SCWR.
2.7 SCWR Safety R&D
An SCWR safety research activity is recommended, organized around the following topics:
Reduced uncertainty in SCW transport properties Further development of appropriate fuel cladding to coolant heat transfer correlations for SCWRs
under a range of fuel rod geometries
SCW critical flow measurements, as well as models and correlations
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Measurement of integral loss-of-coolant
accident (LOCA) thermal-hydraulicphenomena in SCWRs and related computer
code validation
Fuel rod cladding ballooning during
LOCAs SCWR design optimization studies,
including investigations to establish thereliability and system cost impacts of
passive safety systems
Power-flow stability assessments.
Picture 10. SCWR safety R&D
2.8 Preliminary Analysis of Key Transients and AccidentsThe integral SCWR LOCA thermal-hydraulic experiments would be similar to the Semiscale
experiments previously conducted for the U.S. Nuclear Regulatory Commission to investigate LOCA
phenomena for the current LWRs. A test series and the related computer code development would takeabout 10 years. It may be possible to design this facility to accommodate the heat transfer research
discussed above as well as the needed LOCA testing, and even some thermal-hydraulic instability
testing.Fuel rod cladding ballooning is an important phenomenon that may occur during a rapid
depressurization.
Although considerable work has been done to measure and model the ballooning of Zircaloy clad fuelrods during LOCAs, little is known about the ballooning behavior of austenitic or ferritic-martensitic
stainless steel or nickel-based alloy clad fuel rods during a LOCA.
All of the known accident scenarios must be carefully evaluated. These include large- and small-break
LOCAs, reactivity insertion accidents (RIAs), loss of flow, main steam isolation valve closure, overcooling events, anticipated transients without scram, and highand low-pressure boil off.
Westinghouse and INEEL performed a critical review of the LWR abnormal events and their NRCclassification with respect to the SCWR application. The objective was to identify potentially
troublesome events on which to focus the R&D attention as early in the program as possible. The
following four events were singled out:
Total loss of feedwater flow. Because the SCWR is a once-through direct cycle without coolantrecirculation, a loss of feedwater flow immediately causes a loss of core flow and results in rapid
undercooling of the core.
Turbine trip without steam bypass. The average coolant density is low in the SCWR core andpressurization events (such as the turbine trip without stem bypass or the accidental closure ofthe main steam isolation valves) result in significant positive reactivity insertion and increase
in reactor power.
Loss of feedwater heating. When a feedwater heater is lost, relatively cold water enters the coreresulting in the insertion of positive reactivity. The difference between the behavior of aSCWR and a BWR is that the effect is expected to be more pronounced, because the feedwater
is not mixed with hotter water before entering the core.
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Large break in the feedwater lines (or cold-leg large-break LOCA). Because the SCWRcoolant path is once-through without recirculation in the vessel, an unmitigated large break inthe feedwater lines results in coolant stagnation in the core and rapid overheating of the fuel.
Because at supercritical conditions the boiling crisis does not occur, the traditional CHF criterion to
assess the margin to failure cannot be used. Maximum allowable cladding temperatures are specified
instead for both transients and accidents. The following limits are also assumed for the SCWR fuel,and are identical to those used in BWRs: no centerline melting under transient overpower, and radial-
averaged fuel enthalpy (at any location in the core) below 0.711 kJ/g during transients and below 1.17
kJ/g during accidents.A preliminary analysis of the SCWR response to the four events mentioned above was performed at
the INEEL. The purpose of the analysis was to characterize the time constants of the system so that the
required response times and capacities for various safety systems could be determined. The analysiswas performed using a modified version of RELAP5-3D, specifically improved to support analysis of
the SCWR. The improvements included changes of the water properties interpolations around the
critical point, modification of the solution scheme in the supercritical region, and addition of heattransfer and wall friction correlations applicable to supercritical conditions.
The effect of the main feedwater (MFW) pumps coastdown time, scram delay time and auxiliaryfeedwater (AFW) flow rate was evaluated for the total loss of feedwater. From obtained results it was
shown that the SCWR meets the transient peak cladding temperature criterion with the followingassumptions: a MFW pump coastdown of 5 s, AFW flow is initiated at 4.25 s and corresponds to 15%
of the initial MFW flow, the reactor scram signal is generated at 0.5 s, triggered by a 10% reduction in
MFW flow, the control rods begin moving 0.8 s later and are fully inserted 2.5 s later, the reactorpressure is assumed to remain constant due to the operation of turbine bypass valves. Thus, the SCWR
will likely need an AFW system that is fast acting and of relatively high capacity; this will be a
significant design challenge.The analysis also showed that the turbine trip without steam bypass is fairly benign because the high-
capacity steam relief valves open quickly and prevent over-pressurization of the system, i.e., the
inherent behavior of the SCWR is very similar to a BWR. However, the reactivity insertion is not ashigh as in the BWR because most of the moderation in the SCWR core is obtained from liquid coolant(in the water rods), which is not affected by pressurization. As a result the fuel is not overheated. The
reactor scram, triggered by the turbine trip, quickly terminates the event.
The loss of feedwater heating has been studied. The cladding and the fuel are not overheated becauseof the lower temperature coolant and the Doppler feedback effect, respectively. The assumptions are
as follows: the event is initiated by a 30oC step decrease in feedwater temperature (corresponding to
the loss of the last heater on the high-pressure feedwater train), the MFW mass flow is held constantduring the transient, scram is not assumed, and the turbine bypass valves are assumed to hold the
reactor pressure constant.
As far as the cold-leg large-break LOCA is concerned, the calculations were performed withoutemergency core coolant and automatic depressurization systems to provide an indication of the time
available for these systems to operate. A 100% feedwater line break is assumed. Scram is not needed
as the reactivity feedback due to the decrease in moderator density is able to quickly shut down the
reactor.
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2.9 Flow Stability
The objective of the power-flow stability R&D is better understanding of instability phenomena inSCWRs, identification of the important variables affecting these phenomena, and, ultimately, the
generation of maps identifying the stable operating conditions of the different SCWRs designs.
Consistent with the U.S. Nuclear Regulatory Commission approach to BWRs licensing, the licensing
of SCWRs will probably require, at a minimum, demonstration of the ability to predict the onset ofinstabilities. This can be done by means of a frequency-domain linear analysis.
Both analytical and experimental stability studies need to be carried out for the conditions expectedduring the different operational modes and accidents. The analytical studies can obviously be more
extensive and cover both works in the frequency domain, as well as direct simulations. These studies
can consider the effect of important variables such as axial and radial power profile, moderator densityand fuel temperature reactivity feedback, fuel rod thermal characteristics, coolant channel hydraulic
characteristics, heat transfer phenomena, and core boundary conditions. Mitigating effects such as
orificing, insertion of control rods, and fuel modifications to obtain appropriate thermal and/or
neutronic response time constants can also be assessed using analytical simulations. Instabilityexperiments could be conducted at the multipurpose SCW thermal hydraulic facility recommended for
the safety experimentation discussed above. The test section should be designed to accommodate asingle bundle, as well as multiple bundles. This will enable studying in-phase and out-of-phase densitywave oscillations. Moreover, the facility will provide a natural circulation flow path for the coolant to
study buoyancy loop instabilities
2.10 SCWR Design and Evaluation R&DMany of the major systems that can potentially be used in a SCWR were developed for the current
BWRs, PWRs, and SCW fossil plants. Therefore, the major plant design and development needs that
are unique for SCWRs are primarily found in their design optimization, as well as their performanceand reliability assurance under SCWR neutronic and thermo-hydraulic conditions.
Two major differences in conditions are the stresses due to the high SCWR operating pressure (25
MPa) and the large coolant temperature and density change (approximately 280 to 500C or more, 800to 80 kg/m3, respectively) along the core under the radiation field.
2.11 Control StrategyBREI has reviewed the general characteristics, standards and regulations for the control system in
existing nuclear power plants in view of the SCWR application. The SCWR presents several
similarities and differences with the BWR and PWR systems that affect the control strategy. The BWR
similarities are associated with the direct cycle with feedwater flow entering directly into the reactorvessel and steam flow going directly to the turbine. A balance between feed and steam is required to
maintain the water inventory in the vessel. Also, soluble poisons such as boric acid cannot be used for
reactivity control.The PWR similarities are associated with the high operating pressure, the single-phase conditions at
the core outlet and a core outlet temperature that is a function of power and coolant flow. Unique
aspects of the SCWR that influence the control concept include the elimination of the recirculationpumps, the low water inventory in the RPV, the large change in coolant density across the core, the
absence of a coolant level under supercritical conditions.
The major systems to be controlled in the SCWR are the reactor coolant system, the feedwater andcondensate system, the steam system, and the turbine generator system. The main variables to be
controlled include the reactor power, the core outlet temperature during supercritical pressure
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operation (e.g., during full power operation), the reactor pressure, the reactor level during subcritical
pressure operation (e.g., during start-up) and the feedwater flow.Assuming that the SCWR will be operated in a base load rather than a load follow manner, and
considering the general characteristics of the SCWR plant, BREI has made the following two
recommendations for the SCWR control system:
Control of the main reactor variables. The control rods accomplish the primary control of thethermal power. The turbine control valve provides the control of the pressure, and the
feedwater flow (i.e., the feedwater pumps) provides the primary control of the outlet
temperature. The control of the coolant inventory in the vessel is accomplished by assuring thatsteam and feed flow are balanced while maintaining the correct core outlet temperature.
Integrated control system approach. Rather than an approach in which higher functions such aspower or turbine valve control are in manual with lower level control loops in automatic, a
coordinated control in which all functions are in automatic is proposed. The relatively smallvessel water inventory, the nuclear/thermal-hydraulic coupling, the lack of level indication
under supercritical conditions and the absence of recirculation flow makes control more
challenging.
Thus, the use of an integrated control would allow the system to anticipate changes and reactaccordingly.
An example of how the SCWR integrated control system will function is provided next. Assume thatthe reactor is operating at 100% power and the operator decides to lower the power to 95%; then the
following sequence will follow:
2.12 SCWR Fuel Cycle R&DThe thermal spectrum SCWR option will use conventional LEU fuel. The fuel itself is developed;
however, new cladding materials and fuel bundle designs will be needed. The designs for the thermal
spectrum SCWR will need significant additional moderator, i.e., water rods or solid moderation. Thedesigns for the fast spectrum SCWRs will require a tight pitch, but high neutron leakage to create a
negative density coefficient. The fast spectrum SCWR option uses mixed plutonium-uranium oxidefuel with advanced aqueous reprocessing.
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5. COCLUSIONS
The research work during the first years of the Generation-IV SCWR program has established that:
1. The SCWR can make substantial use of existing LWR technology in the nuclear island. Forexample, the design and materials of the SCWR reactor pressure vessel and containment are similar to
the PWRs and BWRs, respectively.2. The SCWR can achieve high thermal efficiencies making extensive use of available supercriticalfossil plant technology in the balance of plant. For example, the materials and design of the power
conversion cycle as well as the start-up and shutdown procedures and equipment can be drawn from
fossil plants with only minor modifications.3. Based on preliminary one-dimensional analyses, the SCWR appears to be stable with respect to
thermal-hydraulic and thermal/nuclear oscillations because of its relatively low coolant reactivity
feedback coefficient.4. The importance of the loss of feedwater as a key abnormal event has been recognized. The design of
a suitable high-pressure high-capacity fast-acting auxiliary feedwater system will be a major challenge
in proving the viability of the SCWR.
5. Limited corrosion and stress-corrosion testing of traditional stainless steels in high-temperaturewater has shown that finding materials that would perform satisfactorily in the SCWR environment
will be a challenge. However, classes of materials with promising mechanical properties and corrosion
resistance have been identified and will be tested.In summary, the basic assumptions contained in the Generation-IV Roadmap Report have been
confirmed. The key feasibility issues for the SCWR remain the development of in-core materials and
the demonstration of an adequate safety level.
6. REFERENCES
[1] A Technology Roadmap for Generation IV Nuclear Energy Systems, U.S. DOE Nuclear Energy
Research Advisory Committe, December 2002.[2] BREI, Burns & Roe Enterprises Inc., Supercritical Water Reactor (SCWR), Study of Power
Conversion Cycle, Control Strategy and Start-up Procedures, September 2003.
[3] BUONGIORNO, J., W. Corwin, P. MacDonald, L. Mansur, R. Nanstad, R. Swindeman, A.
Rowcliffe, G. Was, D. Wilson, I. Wright, Supercritical Water Reactor (SCWR), Survey of Materials
Experience and R&D Needs to Assess Viability, INEEL/EXT-03-00693 (Rev. 1), Idaho National
Engineering and Environmental Laboratory, September 2003(a).
[4] BUONGIORNO, J., K. G. Condie, G. E. McCreery, D. M. McEligot, M. E. Nitzel, J. E. OBrien,
The INEEL Heat Transfer Flow Loop for Development of Supercritical-Water-Cooled Reactors,
INEEL/PRO-03-00565 (Rev. 1), Idaho National Engineering and Environmental Laboratory, June
2003(b).
[5] KATAOKA, K. et al. Development Project of Supercritical-water Cooled Power Reactor,Proceedings of ICAPP-2002, Hollywood, Florida, June 9-13, 2002.
[6] JONSSON, N. O., U. Bredolt, T. A. Dolck, A. Johanson, T. Ohlin, L. Oriani, L. Conway, SCWR -
Design Review and Design of Safety Systems and Containment Status, September 2003, SE-03-044(Rev. 0), September 2003.
[7] YANG, W. S., N. Zavaljevski, Preliminary Stability Analysis for Supercritical Water Reactor,
Proceedings of Global 2003, New Orleans, November 16-20, 2003.