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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.