PDF 5.2 a Taste of Reactor Physics-Part 2

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    1

    A Look at Nuclear Scienceand Technology

    Larry Foulke

    Module 5.2

    A Taste of Reactor Physics Part 2

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    NuclearEngineeringProgram

    Finite System Neutron Balance

    Production vs Absorption + Leakage

    f = a + Leakage

    Note: kkeff (To accommodate leakage)

    keff = k =Production

    Absorption + Leakage

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    NuclearEngineeringProgram

    Neutron Leakage Effect

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    NuclearEngineeringProgram

    States of criticalitykeff = 1 Critical

    keff > 1 Supercritical

    keff < 1 Subcritical

    No reactor can be constantly critical: Fuel depletion Fission product buildup (absorb neutrons) Temperature changes (changes cross section)

    Criticality

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    NuclearEngineeringProgram

    In order to keep an operating nuclear reactor criticalwe will need to adjust terms in the neutron balance

    Neutron balance controlled by: ProductionAbsorption Leakage

    Criticality Control

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    NuclearEngineeringProgram

    Criticality Control

    n Let us consider how we could adjust these parametersto achieve a target keff for two different applications

    n Nuclear Power PlantnTarget keff:

    nkeff= 1 for steady-state operationnkeff> 1 for start-up, keff< 1 for shutdown

    n Nuclear Fuel Processing FacilitynTarget keff:

    nkeff< 1 under all possible conditions (including accidents)

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    Criticality Control (Reactor)

    Nuclear ReactorProduction

    Determined by the total fissile content of the core Initial fuel loading Conversion of fertile nuclides (breeding) Refueling

    On-line

    ShutdownAbsorptionLeakage

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    Criticality Control (Reactor)

    Nuclear ReactorProductionAbsorption Fission-Product Absorbers

    Cladding, Structure, Coolant Control Rods Soluble Absorbers (poisons) Burnable Absorbers

    Leakage

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    Criticality Control (Reactor)

    n Nuclear ReactornProductionnAbsorption (Modern reactor designs):

    nMoveable control rods (CR) to change power level and maintainsteady state operation.

    nMovable safety rods (SR) to quickly shut down reactor andensure keff< 1.

    Soluble boron in reactor coolant (PWR only) toshim

    keff(liketrim control in an airplane) and fixed burnable poisons (boron or

    gadolinium) that deplete during operation to accommodate fuel

    burnup.

    nLeakage

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    Criticality Control (Reactor)

    Nuclear ReactorProduction

    Absorption

    Leakage Core size and shape Reflection of neutrons back into the core Density of core material(s)

    (temperature-dependent)

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    NuclearEngineeringProgram

    Water-Reflector

    Effect onMinimumCore Size

    11

    Image Source: See Note 1

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    NuclearEngineeringProgram

    Criticality Control (Reactor)

    Nuclear ReactorProduction

    Absorption

    LeakageModeration

    Controls how effectively neutrons can slow downto thermal energies.

    Determined by selection of moderator materialand pin dimensions (diameter and pitch).

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    NuclearEngineeringProgram

    Criticality Control (Reactor)

    Reactor Criticality Requirements Operation Modes

    Power Reactors (Startup / Steady-State / Shutdown) Some Research Reactors (Pulse Mode) All reactors have emergency shutdown (SCRAM) capability

    Routine adjustments to reactor criticality are required Account for power fluctuations and feedback effects

    Fuel depletion, density changes of moderator Small frequent adjustments: control rods (in PWR) Larger, planned, adjustments: soluble boron (in PWR) BWR reactors use control rods and coolant flow feedback to

    adjust criticality.

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    NuclearEngineeringProgram

    nFuel Facility:Always Subcritical!nDesigned subcritical

    nVerify that current configuration is subcriticalnConfirm that proposed changes will be subcritical

    nkeff< 1 under all conditions; must accountfor:

    nUncertainties in Experimental Data and CalculationsnNormal, Anticipated Abnormal & Credible Accident

    Scenarios

    Criticality Control (Fuel Facility)

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    NuclearEngineeringProgram

    Beyond keff

    When designing critical systems (reactors) weneed to know the spatial distribution of neutrons in

    the core, in addition to the multiplication factor.

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    NuclearEngineeringProgram

    The Exact Way (Hard)

    Write down a neutron balance equation over somedifferential volume element and then solve the resultingintegro-differential equation:

    Terms: 1)Time Variance, 2) Leakage, 3) Total Interaction Loss,

    4) Fission Source, 5) In-Scattering Source

    TR

    UTH!

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    NuclearEngineeringProgram

    Typical Core DesignFuel Assemblies

    Zoom In on

    these 4 assemblies

    Core SymmetryImage Source: See Note 2

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    NuclearEngineeringProgram

    Typical Assembly Design

    Fuel Pins

    Control Rods

    Assembly

    Symmetry

    Zoom In onQuarter Assembly

    Image Source: See Note 2

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    NuclearEngineeringProgram

    Typical, Simplified Assembly Model

    Simplified 2-D model of anAP600 quarter assembly.

    Contains UO2 fuel, boroncontrol rods, and B4Cburnable absorber rods.

    Reflecting boundaryconditions on all sides.

    Image Source: See Note 2

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    NuclearEngineeringProgram0 2 4 6 8

    0

    2

    4

    6

    8

    Quarter-Assembly, Control Rods Withdrawn

    0 2 4 6 8

    0

    2

    4

    6

    8

    k

    = 1.1630

    Image Source: See Note 2

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    NuclearEngineeringProgram0 2 4 6 8

    0

    2

    4

    6

    8

    Quarter-Assembly, Control Rods Inserted

    0 2 4 6 8

    0

    2

    4

    6

    8

    k

    = 0.93287

    Image Source: See Note 2

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    NuclearEngineeringProgram

    A More Approximate Way (Easier)

    Write down a neutron balance equation using DiffusionTheory with one energy group

    Time Variance, Fission Source, Absorption Loss, Leakage

    AL

    MOSTTRU

    TH!

    1

    v

    (

    r,t)

    t=

    f(

    r,t) a(

    r,t)+D2(

    r,t)

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    1. Reprinted with permission from the American Nuclear Society.Nuclear Engineering Theory and Technology of Commercial

    Nuclear Powerby Ronald Allen Knief, 2nd Edition. Copyright

    2008 by the American Nuclear Society, La Grange Park, Illinois.

    2. Reprinted with permission from David Griesheimer. FunctionalExpansion Tallies for Monte Carlo Simulations, PhD

    Dissertation, Nuclear Engineering and Radiological Sciences,

    University of Michigan (2005). ProQuest/UMI, AAT 3163808.

    Image Source Notes