Ch 4 Nuclear Reactors

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    Nuclear Power Plants

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    Fission

    QuickTime an d a

    TIFF (Uncompressed) decompressorare needed to see this picture.

    http://www.chm.bris.ac.uk/motm/uf6/fission.gif

    Moderator

    Slow

    neutron

    Uranium-235

    fission

    Moderator

    U-235

    Control

    rods

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    Concepts

    Review

    Prompt neutrons vs Delayed neutron

    Capture to Fission ratio a

    New

    Multiplication factor - k the number ofneutrons in this generation/number of

    neutrons in the previous generationk

    or keff

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    Neutron cycle in a reactor

    100 fission

    259 neutrons produced

    59 lost

    Activation

    products

    100

    absorbed

    in

    Fuel

    no fission

    100

    absorbed

    in

    Fuelfission

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    Multiplication factor

    Four factor formula - Reactor of infinite size

    Reproduction factor, number of nts releasedin fission per nts absorbed

    f Thermal utilization, thermal nts absorbed infuel per thermal nts absorbed in fuel +thermal nts absorbed in everything else

    e Fast fission factor, fast nts produced per fastneutron from thermal fission

    p resonance escape probability, fraction of ntsnot captured while slowing down.

    kfep

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    Neutron Cycle - infinite reactor

    Fast Fission

    e

    ep

    Resonance

    absorption

    Thermal

    absorption

    epf Neutronproduction

    epf = k

    Captured

    Absorbed

    non fuel

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    Real reactors

    Four factors become 6

    Fast non-leakage Lf

    Thermal non-leakage Lt L=LfLt

    keff fepLfLt

    keff fepL

    keff kL

    QuickTime and a

    TIFF (Uncompressed) decompressorare needed to see this picture.

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    Neutron Cycle - finite reactor

    Fast Fission e

    eLfp

    Slowing

    Thermal

    absorptionepfL

    Neutron

    productionepfL

    Fast leak

    e(1-Lf)

    Absorbed

    non fuel

    Resonance

    absorption

    eLf

    Captured

    eLf(1-p)

    Diffusion

    Thermal

    leak

    eLfpLt

    eLfp(1-Lt)

    eLp(1-f)

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    Basic Components

    Fuel

    Controlrod

    Steam

    generato

    r

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    Control Rods

    Used to control the chain reaction

    Materials that have larger cross-

    sections than fuel

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    Typical cross sections

    Thermal neutron sf=572 b

    U-235 B-10

    sc=3000 b

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    Coolant Flow q=w(hout-hin)

    Steam

    Tout

    Water

    Tin

    Tin

    Tout

    q

    q

    Recirculating

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    Pressurized Water Reactor

    PWR

    150 bar 2200 psia

    Light water coolant/moderator

    ~ 3-4 % enriched

    Steam

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    Boiling Water Reactor

    BWR

    No separate steamgenerator

    70 bar 1000 psia

    10% of converted tosteam

    steam

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    Comparison PWR-BWR

    BWR core power density 1/2 of the PWR butstill greater than Gas cooled

    Steam generators for PWR requires moreupkeep

    PWR coolant loop is more contained

    Corrosion in the turbine can pass directly to

    the BWR causing activation and higherexposures to the operating staff

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    Comparison Continued

    PWR have high decay heat requirecooling even when shut down

    SS piping in BWR is more susceptibleto cracks

    PWR have a similar issue with the

    steam generator

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    LOCA

    Address component breakdown or acombination of component breakdowns

    that lead to interruption of normalcooling

    When an interruption occurs, the fission

    process is terminated, however heatgeneration continues

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    Classifications of operation

    Normal

    Operational transients

    UpsetsEmergencies

    Limiting Fault Conditions includes

    Design basis accident DBA

    Unprotected or beyond DBA

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    Engineered Safety Systems

    The actions aredone as a result ofinstrument signals

    Reliability

    Duplication

    Diversity

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    Most common ESS

    Alternate cooling

    SCRAM - Tripping - insert control rods

    to stop fission

    Control

    Cool

    Contain

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    Environmental Release

    Acid Rain Contribution

    1000 MWe

    Nuclear

    SO2 - 0

    Coal (1.5% S)

    SO2 - 90,900 tons

    Fuel oil (0.37%S)

    SO2 - 22,496 tons

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    Gen IV Program (INL.gov)

    Gas-Cooled Fast Reactor(GFR) features a fast-neutron-spectrum, helium-cooled reactor andclosed fuel cycle

    Very-High-Temperature Reactor(VHTR) agraphite-moderated, helium-cooled reactor with aonce-through uranium fuel cycle

    Supercritical-Water-Cooled Reactor(SCWR) a

    high-temperature, high-pressure water-cooledreactor that operates above the thermodynamiccritical point of water

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    Gen IV Program

    Sodium-Cooled Fast Reactor(SFR) features a fast-spectrum, sodium-cooled reactor and closed fuel cycle forefficient management of actinides and conversion of fertile

    uranium

    Lead-Cooled Fast Reactor(LFR) features a fast-spectrum lead of lead/bismuth eutectic liquid metal-cooledreactor and a closed fuel cycle for efficient conversion offertile uranium and management of actinides

    Molten Salt Reactor(MSR) produces fission power in acirculating molten salt fuel mixture with an epithermal-

    spectrum reactor and a full actinide recycle fuel cycle

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    Gas-cooled fast reactor GFR

    He

    600 MW th

    48% net eff

    Coolant

    Inlet 490C

    Outlet 850C

    Pressure 90 bar

    Ave power density100 MWth/m3

    Burn-up 5%

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    Very High Temperature Reactor

    H

    production

    He

    Core outlet 1000 C

    600 Mw t

    Water

    O2 H2

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    Super Critical Water Cooled

    Operates above thethermodynamiccritical point ( 374 C

    22.1 MPa

    1700 MWe

    Pressure 25 MPa

    T outlet is 550C

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    Sodium cooled fast

    T out 550 C

    Mixed oxide fuel

    Two sizes 150-500 MWe

    500 - 1500 Mwe

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    Lead Cooled Fast

    300 to 1200 MWe

    T outlet 550 - 800 C

    Fuel is metal ornitride based

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    Molten Salt

    1000 MWe

    T outlet 700-800 C

    Molten salt fuel

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    Questions