fuel burnup calculations and uncertainties

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2013-12-13 1 Fuel Burnup Calculations and Uncertainties International Atomic Energy Agency Page 2 Outline Review lattice physics methods Different approaches to burnup predictions Linkage to fuel safety criteria Sources of uncertainty Survey of available codes

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Page 1: Fuel Burnup Calculations and Uncertainties

2013-12-13

1

Fuel Burnup Calculations and Uncertainties

International Atomic Energy AgencyPage 2

Outline

� Review lattice physics methods

� Different approaches to burnup predictions

� Linkage to fuel safety criteria

� Sources of uncertainty

� Survey of available codes

Page 2: Fuel Burnup Calculations and Uncertainties

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International Atomic Energy AgencyPage 3

Reactor Physics Challenge

Go from here to � here without losing too much information

International Atomic Energy AgencyPage 4

Additional Complications

� Temperature (or doppler effects)

� Strong spatial discontinuities between materials• Water next to Zr and UO2

� Neutron scattering is non-linear in energy, angle and

space

� Time dependence• Neutron population

• Material properties and compositions

Page 3: Fuel Burnup Calculations and Uncertainties

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International Atomic Energy AgencyPage 5

Reactor Physics Computational Strategy

K. Smith, “Reactor Core Methods,” M&C 2003

Circa 1980

International Atomic Energy AgencyPage 6

Modern Approaches

K. Smith, “Reactor Core Methods,” M&C 2003

Page 4: Fuel Burnup Calculations and Uncertainties

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International Atomic Energy AgencyPage 7

Lattice to Whole Core Analyses

K. Smith, “Reactor Core Methods,” M&C 2003

International Atomic Energy AgencyPage 8

A Brute Force Approach … not possible

K. Smith, “Reactor Core Methods,” M&C 2003

Page 5: Fuel Burnup Calculations and Uncertainties

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International Atomic Energy AgencyPage 9

Different Approaches to Analyses

� Deterministic methods• Collision probabilities

• Discrete ordinate methods

• Method of characteristics

� Stochastic methods• Monte carlo

� The choice of method is dictated by computational

resources and desired accuracy• Note that this accuracy directly affects burnup calculations and error can

compound with time

International Atomic Energy AgencyPage 10

Collision Probabilities

� Integral method based on assumption that flux at a

point is dependent on the probability of a neutron

transiting a region in space

Page 6: Fuel Burnup Calculations and Uncertainties

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International Atomic Energy AgencyPage 11

Discrete Ordinates

� Refers to treatment of angular variable

� Spatial variable treatment varies• Finite difference type approach

• Characteristics based methods

International Atomic Energy AgencyPage 12

Methods of Characteristics

� Lagragian method that explicitly treats both spatial

and angular variables

� Scalar fluxes calculated by integrating along a series of

rays transiting through the problem domain

Page 7: Fuel Burnup Calculations and Uncertainties

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International Atomic Energy AgencyPage 13

The Burnup Problem

� Branching constants bi.j

are known

� Decay constants λj are

known

� Flux, φ, and cross

section, σ, derived from

lattice physics analyses

International Atomic Energy AgencyPage 14

Modeling Approaches

� Once again, choice

depends on desired

accuracy

� Modern approaches

predict burnup pin by

pin

� Historical approaches

perform calculations at

the lattice level

Page 8: Fuel Burnup Calculations and Uncertainties

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International Atomic Energy AgencyPage 15

Computational Strategy

� Historically core burnup

calculations have been

performed based on pre-

calculated cross section

libraries

• Account for all relevant

physics

� Fuel temperature

� Moderator conditions

� Exposure

� Xe/Sm

� Control rods

� etc.

International Atomic Energy AgencyPage 16

Lattice Physics Computational Flow

http://scale.ornl.gov/index.shtml

Page 9: Fuel Burnup Calculations and Uncertainties

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International Atomic Energy AgencyPage 17

Application to Reactor Problems

� Lattice physics

calculation applied to

fuel assembly

• Output reduced to library

� Whole core multi-group

diffusion simulation

accesses fuel specific

library

• This allows whole core

simulation to account for

changes in state variable

(Tf, Tm, Dm, etc.)

K. Smith, “Reactor Core Methods,” M&C 2003

International Atomic Energy AgencyPage 18

Latest Developments

� Main difference is that lattice physics is embedded

into core diffusion code• Eliminates intermediate library

• Better captures real physics

Page 10: Fuel Burnup Calculations and Uncertainties

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International Atomic Energy AgencyPage 19

Linkages to Safety Criteria

� Input to fuel mechanical code

� Predict reactivity coefficients

� Peaking factors

� Fuel burnup

� Reactor operations

International Atomic Energy AgencyPage 20

Input to Fuel Mechanical Code

� Most fuel performance processes dependent upon

power

� Typically, a limiting power profile is chosen

� Core physics calculations needed to ensure that reality

is within assumed values

Page 11: Fuel Burnup Calculations and Uncertainties

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International Atomic Energy AgencyPage 21

Reactivity Coefficients

� Needed to ensure compliance with safety standards

� Reactivity coefficients are burnup dependent

� Calculation needed to assure proper values

throughout the entire operating cycle

International Atomic Energy AgencyPage 22

Peaking Factors

� Directly linked to AOO, LOCA and RIA fuel safety

criteria

� LHGR derived from AOO analysis typically constrains

power operation

� Similarly, LOCA calculation assume peaking factors

that constrain power operations

� RIA simulation imposes radial peaking limits to

constrain rod worth

Page 12: Fuel Burnup Calculations and Uncertainties

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International Atomic Energy AgencyPage 23

Fuel burnup

� Limits derived from fuel mechanical simulation• Imposed by regulatory authority

� Simulation needed to demonstrate compliance• Measurements difficult and uncertain

International Atomic Energy AgencyPage 24

Reactor Operations

� Modern online monitoring systems are coupled to 3-D

core simulator• Use pre-calculated cross section libraries

• Use simplified nodalization schemes to allow for real time results

� Operator aid to assess plant performance• Not used to actuate safety functions

Page 13: Fuel Burnup Calculations and Uncertainties

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International Atomic Energy AgencyPage 25

Sources of Uncertainty

� Mechanical

� Data

� Calculational error

� Stochastic error

International Atomic Energy AgencyPage 26

Mechanical Uncertainties

� Manufacturing processes are all conducted with

design tolerances• Fuel pellet radius diameter

• Cladding diameters

• Spacer pitch

• Channel thickness

� Material properties are never exact• UO2 density

• Cladding material specification

• Soluble poison specification

� Operational impacts• CRUD

• Rod bow

Page 14: Fuel Burnup Calculations and Uncertainties

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International Atomic Energy AgencyPage 27

Uncertainty in Data

� Cross section measurements not exact• Early techniques fairly uncertain for some materials

• Some of these measurements still in ENDF database

� Fe neutron transmission

� Thermal expansion coefficients

� Branching constants

� Decay constants

� Neutron yields

� Half life

International Atomic Energy AgencyPage 28

Calculation Errors

� All deterministic methods employ some type of

discretization scheme• Finite differences

• Angular quadrature

• Energy partitioning (i.e. multi-group assumption)

� Convergence errors caused by ill formed solution• Nodalization too coarse

• Bad quadrature weights

� Inherent errors from numerical methods• Event well converged solutions are not perfect

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International Atomic Energy AgencyPage 29

Stochastic Errors

� Generally refer to Monte Carlo methods

� Modern codes typically employ continuous energy

treatment• No multi-group errors

� Can exactly represent complex geometry• No finite difference errors

� Stochastic errors relate to under sampling• Not enough particle histories to have good statistics

• Problem domain not fully sampled

� Even for well sampled problems, uncertainty remains• Relates to the convolution of various probability distribution functions

International Atomic Energy AgencyPage 30

Treatment of Uncertainty

� Typically handled by sensitivity calculations

� Mechanical uncertainties addressed by biasing model

to extreme of tolerance

� Calculational uncertainties derived from assessment

and applied as a bias

� Stochastic uncertainty addressed by upper bound

95/95 limit

� All of these treatments manifest themselves as an

increase in margin between operating and safety

limits

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International Atomic Energy AgencyPage 31

Typical Uncertainties

K. Smith, “Reactor Core Methods,” M&C 2003

International Atomic Energy AgencyPage 32

So what is a Regulator to do?

� Take time to understand the physics and

manufacturing processes

� Ask good questions

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International Atomic Energy AgencyPage 33

Survey of the more Common Physics Codes

International Atomic Energy AgencyPage 34

WIMS

http://www.answerssoftwareservice.com/wims/

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International Atomic Energy AgencyPage 35

CASMO

http://www.studsvik.com/Documents/Product-sheets/Updated%20product%20sheets%20SSP/C5_2013-01_USA_R1.pdf

International Atomic Energy AgencyPage 36

HELIOS

http://www.studsvik.com/Documents/Product-sheets/Updated%20product%20sheets%20SSP/helios.a4_el.pdf

Page 19: Fuel Burnup Calculations and Uncertainties

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International Atomic Energy AgencyPage 37

MCU

http://mcuproject.ru/eabout.html

International Atomic Energy AgencyPage 38

SCALE

http://scale.ornl.gov/index.shtml