Lecture 9 - Accident Analysis 9 - Accident Analysis.pdf · Lecture 9 -Accident Analysis.ppt Rev. 8...

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11/17/2009 6:28 PM Lecture 9 - Accident Analysis.ppt Rev. 8 vgs 1 Lecture 9 - Accident Analysis Dr. V.G. Snell Nuclear Reactor Safety Course McMaster University

Transcript of Lecture 9 - Accident Analysis 9 - Accident Analysis.pdf · Lecture 9 -Accident Analysis.ppt Rev. 8...

Page 1: Lecture 9 - Accident Analysis 9 - Accident Analysis.pdf · Lecture 9 -Accident Analysis.ppt Rev. 8 vgs 32 Acceptance Criteria -1 Dose to the most exposed individual in the critical

11/17/2009 6:28 PMLecture 9 - Accident Analysis.ppt

Rev. 8 vgs 1

Lecture 9 - Accident Analysis

Dr. V.G. Snell

Nuclear Reactor Safety Course

McMaster University

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Where We Are

Probabilistic RequirementsDeterministic Requirements

Design BasisAccidents

Plant safetyas operated

Safety GoalsExperience

CredibleAccidents

Plant safetyas designed

Safety CultureGood Operating

Practice

MitigatingSystems

ProbabilisticSafety Analysis

SafetyAnalysis

Chapter 2

Chapter 3

Chapter 1

Chapter 2

Chapter 4

Chapter 5

Chapter 6

Chapters 7 & 8

Chapter 9

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Objective

� How are data & assumptions chosen?

� How do we ensure that the answer is pessimistic?

� Is this good?

� Details specific to CANDU –methodology is general

� “Think Negatively”!

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Selection of Events by Pseudo-Frequency

02/21 /97 05:11 PM 12Licensing in C anada.ppt Rev. 0 vgs

AECB Consultative Document C-6 Criteria(Darlington*)1

10

10

10

10

10

1010 10 10 0.01 0.1 1

-1

-2

-5 -4

-3

-4

-5

-6

-3

W hole body dose (Sv)

* as app lied

Class 1

Class 2

Class 3

Class 4

Class 5

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Selection of Events by Phenomena - 1

1. Reactivity Accidents• Bulk Loss of Reactivity Control• Loss of Reactivity Control from Distorted Flux Shapes• Inadvertent Criticality

2. Decrease of Reactor Coolant Flow• Loss of Class IV Power• Partial Loss of Class IV Power• Single Pump Trip or Seizure

3. Increase of Reactor Coolant Pressure• Loss of Primary Pressure and Inventory Control (increase)

4. Decrease of Reactor Coolant Inventory• Large Heat Transport System LOCA• Small Heat Transport System LOCA

• Single Channel Events• Single Steam Generator Tube Rupture• Multiple Steam Generator Tube Rupture

• Loss of Primary Pressure and Inventory Control (decrease)

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Selection of Events by Phenomena - 25. Increase of Secondary Side Pressure

• Loss of Secondary Side Pressure Control (increase)6. Loss of Secondary Side Heat Removal

• Main Steam Line Break• Feedwater Line Break• Loss of Feedwater Pumps• Spurious Closure of Feedwater Valves• Loss of Secondary Side Pressure Control (decrease)• Loss of Shutdown Heat Sink

7. Moderator & Shield Cooling System Failures• Pipe Break• Loss of Forced Circulation• Loss of Heat Removal

8. Fuel Handling Accidents• Fuelling Machine On-Reactor• Fuelling Machine Off-Reactor

5. Increase of Secondary Side Pressure• Loss of Secondary Side Pressure Control (increase)

6. Loss of Secondary Side Heat Removal• Main Steam Line Break• Feedwater Line Break• Loss of Feedwater Pumps• Spurious Closure of Feedwater Valves• Loss of Secondary Side Pressure Control (decrease)• Loss of Shutdown Heat Sink

7. Moderator & Shield Cooling System Failures• Pipe Break• Loss of Forced Circulation• Loss of Heat Removal

8. Fuel Handling Accidents• Fuelling Machine On-Reactor• Fuelling Machine Off-Reactor

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Void &

tempe

rature

Accident Analysis Flow Chart

Fuel thermomechanical

Hot channel thermohydraulics

System Thermohydraulics

Fission product transportin fuel and HTS

Physics

Pow

erContainment thermohydraulics

Channelthermomechanical

Moderatorthermohydraulics

Atmospheric dispersion & dose

Steam

discharge

Leakage from containment

Channel integrity

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Models - 1

� Reactor physics� Transient 3D

� System thermohydraulics� Transient 2- or 3-fluid, 1D, non-equilibrium, network

� Fuel thermo-mechanical� Initial - strain, fuel-to-sheath heat transfer coefficient, fission gas release, temperatures

� Transient - fuel sheath strain, beryllium braze penetration, sheath embrittlement, athermalstrain, and excessive fuel energy content

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Acceptance Criteria

� Public dose as per siting guide or C-6 or RD-337

� Designers choose secondary targets

� Shutdown is special:

� Each shutdown system must be independently effective

� Two diverse trips on each system for each accident for operating plants

� RD-337 drops this requirement for direct trips

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Thermohydraulic Model� Non-equilibrium model

� 2-velocities,

� 2-temperatures

� 2-pressures

� plus noncondensables

� Flow regime dependent constitutive relations couple two-phase model

� Interfaces to other codes:

� Fuel Behaviour

� Plant Control

� Physics

Vapor

LiquidBundle Elements

Velocity

Axial Segment (node)

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Typical HTS Nodalization

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Fuel Failure Mechanisms• no excessive straining- 5% strain less than 1000oC

• no-oxide cracking- 2% strain greater than 1000oC

• no oxygen embrittlement

• no beryllium-braze penetration

• no fuel melting

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Models - 2

� Pressure-tube thermo-mechanical

� Moderator temperature & flow� 3D, steady state & transient

� Fission product transport� Within HTS; at break; within containment

� Containment thermohydraulics� 1D & 3D multi-fluid transient

� Atmospheric dispersion and dose� Gaussian plume; ICRP-60

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ModeratorExisting Reactors

Momentum & buoyancy forces opposing – higher

temperatures

ACR

Momentum & buoyancy forces same direction – lower temperatures

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Moderator Flow - ACR

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Moderator temperature

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Initial Conditions - 1Parameter Conservative

DirectionRationale

Reactor thermal power High Minimize time to useup cooling waterinventory, minimizemargins to critical heatflux, etc.

Reactor regulating system Normal operation orinactive, whichever isworse; setback isgenerally not creditedunless it tends to“blind” the trip

Choose so as to delayreactor trip

Radionuclide operating load in theHTS

Highest permissibleoperating iodineburden (and associatednoble gases) and end-of-life tritiumconcentration

Maximize radionucliderelease from stationand public dose

ParameterDirection

Rationale

Reactor thermal power High Minimize time to useup cooling waterinventory, minimizemargins to critical heatflux, etc.

Reactor regulating system Normal operation orinactive, whichever isworse; setback isgenerally not creditedunless it tends to“blind” the trip

Choose so as to delayreactor trip

Radionuclide operating load in theHTS

Highest permissibleoperating iodineburden (and associatednoble gases) and end-of-life tritiumconcentration

Maximize radionucliderelease from stationand public dose

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Initial Conditions - 2Steam generators Clean & fouled casesReduce reactor trip

effectiveness

Steam generator tube leak rate Maximum permittedduring operation, plusassessment of anyconsequential effectsdue to the accident

Increase radioactivityrelease

Pressure tube creep Largest value expectedReduce margins tocritical heat f lux andincrease voidreactivity

HTS flow Low Reduce margins tocritical heat f lux

HTS Instrumented channel flow High Reduce low flow tripeffectiveness

Steam generators Clean & fouled casesReduce reactor tripeffectiveness

Steam generator tube leak rate Maximum permittedduring operation, plusassessment of anyconsequential effectsdue to the accident

Increase radioactivityrelease

Pressure tube creep Largest value expectedReduce margins tocritical heat f lux andincrease voidreactivity

HTS flow Low Reduce margins tocritical heat f lux

HTS Instrumented channel flow High Reduce low flow tripeffectiveness

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Initial Conditions - 3Coolant void reactivity coeff icient High;

Low

Maximize overpowertrans ient;

De lay HTS highpressure trip

Fuel loading Equilibrium;

Fresh

Maximize fue ltemperatures,radioactivity releases;

Maximize overpowertrans ient

Shutdown system Backup trip on lesseffect ive shutdownsystem using the lastof threeinstrumentat ionchannels to tr ip

De lay shutdownsystem effect iveness

SDS2 injection nozzles Most effective nozzleunava ilable

Reduce shutdownsystem reactivity depth

Coolant void reactivity coeff icient High;

Low

Maximize overpowertrans ient;

De lay HTS highpressure trip

Fuel loading Equilibrium;

Fresh

Maximize fue ltemperatures,radioactivity releases;

Maximize overpowertrans ient

Shutdown system Backup trip on lesseffect ive shutdownsystem using the lastof threeinstrumentat ionchannels to tr ip

De lay shutdownsystem effect iveness

SDS2 injection nozzles Most effective nozzleunava ilable

Reduce shutdownsystem reactivity depth

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Initial Conditions - 4SDS1 shutoff rods Two most effective

rods unavailableReduce shutdownsystem reactivity ‘bite’and depth

Maximum channel/bundle power High Maximize fuel &sheath temperature

Reactor decay power High Minimize time to useup cooling waterinventory

Initial flux tilt High Maximize fuel &sheath temperature

Moderator initial local maximumsubcooling

Low Minimize margin tocritical heat flux oncalandria tube

SDS1 shutoff rods Two most effectiverods unavailable

Reduce shutdownsystem reactivity ‘bite’and depth

Maximum channel/bundle power High Maximize fuel &sheath temperature

Reactor decay power High Minimize time to useup cooling waterinventory

Initial flux tilt High Maximize fuel &sheath temperature

Moderator initial local maximumsubcooling

Low Minimize margin tocritical heat flux oncalandria tube

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Initial Conditions - 5Number of operating containmentair coolers and other heat sinks

Low;

High

Maximize containmentpressure;

Delay high pressuretrip and maximizelikelihood of hydrogencombustion

Number of containment dousingspray headers

Low (typically 4 outof 6);

High

Maximize short-termcontainment pressure;

Maximize long-termcontainment pressureand leak-rate,maximize likelihood oflong-term hydrogencombustion

Containment leak rate High (typically 2x to10x design leak rate);

Low

Maximize public dose;

Maximize containmentpressure

Number of operating containmentair coolers and other heat sinks

Low;

High

Maximize containmentpressure;

Delay high pressuretrip and maximizelikelihood of hydrogencombustion

Number of containment dousingspray headers

Low (typically 4 outof 6);

High

Maximize short-termcontainment pressure;

Maximize long-termcontainment pressureand leak-rate,maximize likelihood oflong-term hydrogencombustion

Containment leak rate High (typically 2x to10x design leak rate);

Low

Maximize public dose;

Maximize containmentpressure

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Initial Conditions - 6Containment bypass leakage Pre-existing steam

generator tube leakMaximize public dose

Weather Least dispersiveweather occurring>10% of the time

Maximize public dose

Operator Actions Not credited before 15minutes after a clearindication of the event,for actions that can bedone from the controlroom; and not creditedbefore 30 minutes, foractions that must bedone “in the field”

Ensure adequate timefor diagnosis

Containment bypass leakage Pre-existing steamgenerator tube leak

Maximize public dose

Weather Least dispersiveweather occurring>10% of the time

Maximize public dose

Operator Actions Not credited before 15minutes after a clearindication of the event,for actions that can bedone from the controlroom; and not creditedbefore 30 minutes, foractions that must bedone “in the field”

Ensure adequate timefor diagnosis

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Large LOCA – Initiating Event

� Instantaneous break up to 2X area of largest pipe

� Large pipes all above core

� RIH, ROH, PSH

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Break Locations

1) Pump Suction1) Pump Suction

2) Inlet Header2) Inlet Header

3) Outlet Header3) Outlet Header

HTS PumpsHTS Pumps

Steam GeneratorsSteam Generators

FeedersFeeders

Reactor/Fuel ChannelsReactor/Fuel Channels

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Sequence of Events - 1

� Large break occurs discharging steam to containment

� Coolant voids, reactivity increases

� Reactor power increases

� Reactor is shutdown on a neutronic trip

� HTS flow decreases fastest in the core pass downstream of the break

� Power pulse & fuel dryout result in an increase in fuel temperature

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But for ACR…

� On large LOCA, gross reactivity initially increases due to “checkerboard voiding”, then decreases slowly

� Power increases, then decreases slowly

� Reactor trips on process parameter e.g. low flow

� Fuel temperature increases due to loss of heat removal and redistribution of stored heat

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Sequence of Events - 2

� HTS pressure reduces to the ECC activation setpoint & ECC is activated; two loops (where relevant) are isolated, crash cool-down

� Containment pressure rises, building isolates, dousing sprays turn pressure over

� Some fuel fails, fission products released to containment, some small leakage

� Loops refill, fuel temperature falls

� Long-term ECC recirculation

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Time Scale of Large LOCA

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Safety Aspects

� Jet forces & pipe whip

� Flow decrease downstream of break

� Power increase & neutronic trip

� Fuel heatup and sheath strain

� Pressure-tube heatup, strain to contact with calandria tube

� Heat transfer to moderator

� Containment pressure increase

� Leakage of radioisotopes

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Stagnation BreakCoolant Flow at Center of Downstream Core Pass (RIH)

-500-400-300-200-100

0100200

0 10 20 30 40 50

Time (s)

Flo

w (

kg/s

)

20% RIH 25% RIH 30% RIH

35% RIH 40% RIH 100% RIH

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Iodine Transport

I−−−−, I3−−−−, HOI, IOx

−−−−

I(con)

Iaq(ad)

Ig(ad)

I2(aq) RI(aq)

I2(g) RI(g)

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Acceptance Criteria - 1

� Dose to the most exposed individual in the critical group is below relevant limit

� Class 3 for C-6, single failure for siting guide, DBA for RD-337

� Pipe whip is limited so that:

� no impairment of either of the shutdown systems below their minimal allowable performance standards

� no break induced in the piping of the other HTS loop

� no shearing off of large numbers of feeder pipes

� no damage to the containment boundary

� no break induced in ECC piping

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Acceptance Criteria - 2

� Channel geometry must remain coolable

� amount of fuel sheath oxidation must not embrittle the sheaths on rewet

� amount of sheath strain must be limited so that coolant can flow through the channel.

� Channel integrity is maintained.

� no fuel melting

� no sheath melting

� no constrained axial expansion of the fuel string

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Acceptance Criteria - 3

� If the pressure tube strains or sags

� the pressure tube does not fail prior to contacting the calandria tube (ε < 100%)

� the calandria tube remains intact after pressure tube contact (no prolonged film boiling)

� Pressure within containment is below design pressure.

� Pressure within containment compartments does not cause internal structural failures.

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Three Classification Schemes

� Siting guide� Single process failure

� Dual failure (process system failure + safety system failure)

� C-6 Rev. 0� 5 accident classes

� RD-337� AOO, DBA, BDBA – Severe Accidents

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RD-337

� Anticipated Operational Occurrence (AOO)—a deviation from normal operation that is expected to occur once or several times during the operating lifetime of the NPP but which, in view of the appropriate design provisions, does not cause any significant damage to items important to safety, nor lead to accident conditions.;

� Design Basis Accident (DBA)—accident conditions for which an NPPis designed according to established design criteria, and for which damage to the fuel and the release of radioactive material are kept within regulated limits;and

� Beyond Design Basis Accident (BDBA)—accident conditions less frequent and more severe than a design basis accident. A BDBA may or may not involve core degradation.

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RD-337 Dose Acceptance Criteria

Dose Acceptance CriteriaAOOs DBAs

0.5 mSv 20.0 mSv

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Summary of Acceptance Criteria

C-6 (Darlington)

Siting Guide (BA/BB/PN/PL/G2)

RD-310/RD-337 Event Frequency (occ/yr)

Event

Classes

Dose

Limits (mSv)

Categories Dose

Limits (mSv)

Class

es

Dose

Limits (mSv)

> 10-2 Class 1 0.5 Single Failure 5 AOO 0.5

10-2 to 10-3 Class 2 5 Single Failure 5

10-3 to 10-4 Class 3 30 Single Failure 5

10-4 to 10-5 Class 4 100 Dual Failure 250

DBA 20

10-5 to 10-7 Class 5 250 Dual Failure 250 BDBA ---

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Event Combinations - ECC

� ECC Impairments� Failure of injection

� Failure of crash cooldown

� Failure of loop isolation

� Moderator required as a heat sink

� Low steam flow to channel� Metal water reaction

� Hydrogen production & transport

� Cooling of broken loop

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Fuel in LOCA + LOECC

PrePre--Test Configuration (radial)Test Configuration (radial)PostPost--Test Configuration (radial)Test Configuration (radial)

37-

ELEMENT

BUNDLE

PostPost--Test Test

Configuration (axial)Configuration (axial)

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Sensitivity to Steam Flow

3 STAGES:

1) Initial heatup2) Exothermic steam-Zircaloy reaction 3) Cool down to

steady-state

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Graphite HeaterPressure Tube

Calandria Tube

950 mm

Spacer RingInsulation VoltageTap

BusbarBusbar

Pressure Tube Ballooning Experiments

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Quenching (Nucleate Boiling)After PT/CT Contact

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Rev. 8 vgs 44

Film Boiling

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Effect of CT surface

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Subcooled Boiling Map

550 650 750 850 950 1050 1150Pressure-Tube Contact Temperature (°C)

40

35

30

25

20

15

10

5

Sub

cool

ing

of W

ater

(°C

)

4

HP218

3 D1

1915

SC2

HP12

HP4

HP3

HP9

QM1

HP1HP106M3

HP55

87

SC1

HP18

HP11HP13

9

12F2 F1

16

11

66M4

17210

F4

F3

20

hockey.sgr

1

Immediate QuenchSmall PatchesPatchyExtensiveTotal

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Safety Requirements – LOECC

� Dose limits from siting guide and C6, frequency limits from RD-337

� No limit on fuel damage

� Prevent channel failure

� No fuel melting, adequate moderator subcooling

� No hydrogen detonation or fast flame

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Event Combinations -Containment

� Containment impairments� loss of air coolers, loss of dousing, open ventilation dampers, deflated airlock door seals, (open airlock doors)

� partial or total loss of vacuum, failure of the instrumented containment pressure relief valves to open or close, failure of one bank of self-actuating containment pressure relief valves

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In-Core Break: Bubble Growth

� Hot-pressurized water is discharged into the cool moderator water

� Coolant flashing occurs

� Steam bubble formation

� Bubble expands/contracts

� Pressurization of surrounding water

� Loading in-core structures

� Short term transient on order of milliseconds

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Small-Scale Burst Test Facility

Burst Tests -− Designed to assess

consequences of an in-core FC rupture

− ~ 1/10 scale

− Tests in water with various channel configurations

− Data supports code development and understanding of large-scale tests

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Bubble DynamicsBurst Tests -

− ~ 1/10 scale

− Saturated water ~10 MPa

− Tests done with and without neighbouring channels

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5 x 5 Array

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In-Core Break: Safety Issues

� Damage to reactivity mechanisms

� Propagation of the break to other channels

� Calandria overpressure

� Detection signals

� Displacement of moderator poison

� Fission product washout

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Full Scale Channel Tests

� Full scale Zr-2.5Nb PT in Zr-2 CT burst channel and target channels

� 9 channel array (3x3), burst channel location variable

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Calandria Tubes Absorb Energy

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End-Fitting Ejection

� Fuel bundle ejection into oxidizing atmosphere

� Cooling by water sprays?

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Flow Blockage

� Molten fuel moderator interaction

� How much melt is present when the channel fails?

� Does the interaction depend on the amount of molten fuel?

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Molten Fuel – Channel Interaction

Molten Material

Small quantities of molten material from an overheated

bundle have been shown to be sufficient to rupture a fuel

channel at high system pressure in existing CANDUs

Failure

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Flow Blockage Channel Rupture Tests

Y

Subcooled Water

Pressure TubeC alandria Tube

Pressurized Argon Zr-4 Ingot

Graphite Heater

Bus Bar

Alumina Insulators

PouringSpout

LVDT

LVDT

LVDT

LVDTSeal Ring

C

C

L

L

Water Tank

NorthSouth

Busb arFixed

C O Annulus2

Test Apparatus

Post-test view of bottom of calandria tube

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Flow Blockage Test

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Molten Fuel Moderator Interaction

• During a single channel severe flow blockage event, it is postulated that

molten material may be generated in the channel, which would subsequently

be ejected into the moderator

• A test program has confirmed the dominant mechanism of interaction

between molten fuel (ejected at operating pressure) and the moderator

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Confinement Vessel

Inner Vessel

Steam Injection Vessel

Test SectionDummy Channels

Honey Comb

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Results

� Completed ejection tests – e.g. for 23kg. test:� Melt temperature ~2400°C� Melt ejection pressure ~3 MPa

� Steam injection lines (@10 MPa) opened ~30 ms after PT rupture

� No “steam explosion” noted

� Fine fragmentation of melt (<1 mm diameter)

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Poisoned Moderator

� Used during startup after a long shutdown

� Displacement of poisoned moderator by coolant

� Mixing modes

Piston model Perfect Mixing

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Reactivity BalanceParameter Conservative

DirectionRationale

Initial reactor operating state Startup after a longshutdown

Maximize reactivitydue to decay ofneutron absorbers inthe fuel

Fuel burnup Plutonium peak Maximize fuelreactivity requiringcompensation;maximize voidreactivity

Moderator poison load High Maximize reactivitydue to displacedmoderator

Coolant isotopic purity High Maximize reactivitydue to moderatorreplacement

Failed channel location Near most effectiveshutoff rods

Maximize loss ofshutoff rod reactivity

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ACR

� How would the use of light-water coolant in ACR affect the safety concerns?

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In-Class Assignment

Go back again to the ZED-2 reactor and consider a loss of reactivity control caused by an unexpected moderator pump up. Identify as many of the key systems and parameters as you can for this accident; and for each, list the ‘conservative’ assumptions that you would use to ensure your answer (reasonably) overestimates the consequences.