implementation of an analytical model accounting for sample inhomogeneities in refit k. kauwenberghs...

22
Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security and Safeguards (SN3S)

Upload: fay-carter

Post on 21-Jan-2016

216 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

Implementation of an analytical model accounting for sample

inhomogeneities in REFIT

K. Kauwenberghs

EC – JRC – IRMM

Standards for Nuclear Safety, Security and Safeguards (SN3S)

Page 2: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

Introduction (EC - JRC- IRMM)

Neutron Resonance Transmission and Capture Analysis

Motivation

Initial model validation

Experimental model validation

Summary

Outline

Page 3: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

JRC-IRMM major provider in Europe of ND for nuclear energy applications

GELINA

VdG

EC - JRC – IRMMneutron facilities

Page 4: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

GELINA Van de Graaff

White neutron source+

Time-of-flight (TOF)

99Tc(n,) cross section

Mono-energetic neutrons(cp,n) reactions

10-2 100 102 104 10610-4

10-2

100

102

104

(n,)

(n,)

/ bar

n

Neutron Energy / eV

99Tc + n

EC - JRC – IRMMneutron facilities

Page 5: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

Pulsed white neutron source

(10 meV < En < 20 MeV)

High resolution TOF measurements

Multi-user facility: 10 flight paths

Flight path lengths: 10 m – 400m

Measurement stations with special equipment to perform:

• Total cross section measurements• Partial cross section measurements

FLIGHT PATHS SOUTH

FLIGHT PATHS NORD

ELECTRON LINAC

TARGET HALL

Mondelaers and Schillebeeckx, Notizario 11 (2006) 19

EC - JRC – IRMMGELINA

Page 6: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

NEUTRONMODERATOR

ELECTRONBEAMLINE EXIT

NEUTRONTARGET

NEUTRONFLIGHT PATHS

e- accelerated to Ee-,max ≈ 140 MeV

Bremsstrahlung in U-target

(rotating & cooled with liquid Hg)

( , n) , ( , f ) in U-target

Low energy neutrons by moderation

(water moderator in Be-canning)

EC - JRC – IRMMGELINA

Page 7: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

Neutron Resonance Transmissionand Capture Analysis

CaptureTransmission

totn

tot

Y (1 e )

totneT

T : transmissionFraction of the neutron beam traversing the sample without any interaction

Y : capture yieldFraction of the neutron beam creating a (n,) reaction in the sample

Page 8: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

out

inexp C

CT

,exp

CY

totn

tot

Y (1 e )

totneT

CaptureTransmission

Schillebeeckx et al., Nuclear Data Sheets 113 (2012) 3054 - 3100

Neutron Resonance Transmissionand Capture Analysis

Page 9: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

,exp

CY

totn

tot

Y (1 e )

totneT

CaptureTransmission

Schillebeeckx et al., Nuclear Data Sheets 113 (2012) 3054 - 3100

out

inexp C

CT

Neutron Resonance Transmissionand Capture Analysis

Page 10: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

104 105 106 10710-2

10-1

100

101

102

103

W

Bi

Co

Ag

C'

out

B'

out

Re

spo

nse

/ (1

/ns)

Time Of Flight / ns

Na

104 105 106 10710-2

10-1

100

101

102

103

WAg

Bi

Co

Na

C'

in

B'

in

Re

spo

nse

/ (1

/ns)

Time Of Flight / ns

104 105 106 1070.0

0.2

0.4

0.6

0.8

1.0

1.2

Tra

nsm

issi

on

Time Of Flight / ns

Sample out Sample in

'out

'out

'in

'in

expBC

BCT

Schillebeeckx et al., Nuclear Data Sheets 113 (2012) 3054 - 3100

Neutron Resonance Transmissionand Capture Analysis

Page 11: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

Motivationgood geometry + homogeneous sample

out

inexp C

CT

dEe)E,t(R)t(T )E(nmmM

tot 0.1 1 10

0.2

0.4

0.6

0.8

1.0

Texp

TM

Tra

nsm

issi

on

Neutron energy / eVR(tm,E) response of TOF-spectrometer

REFIT, M. Moxon

241Am

inC

outC

Schillebeeckx et al., Nuclear Data Sheets 113 (2012) 3054 - 3100

Page 12: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

2.5 2.6 2.7 2.8

-4-3-2-101234

resi

dual

s

energy [eV]

300 K Pu-242 Simultaneuos Fit

0.5

0.6

0.7

0.8

0.9

1.0

Literature= 25 meV

n= 2.00 meV

FIT = 36.5 meV

n= 1.46 meVT

rans

mis

sion

Ignoring sample inhomogeneities:

• Underestimation of speak

• Overestimation of GG

Motivationheterogeneous sample

Page 13: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

Transmission + Capture data

sample properties

resonance parameters

Motivationgood geometry + homogeneous sample

Page 14: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

Expected transmission

• Homogeneous sample:

• Heterogeneous sample:

totneT

tottot

tot

)'dn)'n(p'n(n

'n

ee)n(T

'dn)'n(pe'dn)'n(p)'n(TT

p(n') : distribution of areal density1cm

From H. Uetsuka, et al., “Gamma Spectrometry of TMI-2 Debris” (written in Japanese), JAERI-Research 95-084.

Motivationheterogeneous sample

Page 15: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

Analytical models to account for inhomogeneities of a powder sample:• Kopecky et al. (ND2007)

• LP Model (Levermore, Pomraning et al., J. Math. Phys. 27, 2526, 1986)

• …

Comparison with transmission spectra produced by stochastic calculations (MC simulations)

LP model performs the best

35th ESARDA 2013Becker et al., "Particle size inhomogeneity effect on NRD"

Initial model validation

Page 16: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

35th ESARDA 2013Becker et al., "Particle size inhomogeneity effect on NRD"

Initial model validation

Kopecky et al.:• Macroscopic model to describe the variation of the thickness

Kopecky et al., ND2007 , Nice , pp. 623 – 626; Schillebeeckx et al., NDS 113 (2012) 3054 - 3100

LP Model:• Microscopic model

Levermore, Pomraning et al., J. Math. Phys. 27, 2526, 1986

2

22

2 2

)2/(lnexp

2

1)(

s

sx

sxxp

h

k'k f1

nn

hh

En

ffdxxpeT kktotk

)1()()(,

'

𝑇=¿~Σ=𝑝 𝛽 𝜆𝛼+𝑝𝛼 𝜆𝛽+𝜆𝛼

−1+𝜆𝛽−1

2𝑟±=Σ+~Σ±√ (Σ−~Σ )2+4θ

θ=(Σ𝛼−Σ𝛽 )2𝑝𝛼𝑝𝛽

Page 17: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

Experimental validation of the model

= based on capture and transmission measurements at GELINA:

• Cu powder samples with known grain size distribution• W powder samples with known grain size distribution

35th ESARDA 2013Becker et al., "Particle size inhomogeneity effect on NRD"

Experimental model validation

Page 18: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

54th INMM 2013Schillebeeckx et al., "Contribution of the JRC to the development of NRD"

1 10 100 100010-5

10-4

10-3

10-2

10-1

Cin

Bin

Cou

nts

/ (1/s

)

TOF / s

natW-metal disc (80 cm diameter, 14 g natW)

natW-powder mixed with natS-powder(80 cm diameter, 14 g natW, 3.5 g natS)

1 10 100 100010-5

10-4

10-3

10-2

10-1

Cin

Bin

Cou

nts

/ (1/

s)

TOF / s

Experimental model validation

Page 19: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

0.0

0.4

0.8

Texp

TM (hom.)

Tra

nsm

issi

on

10 20 30 40 50-10

-5

0

5

10

Res

idua

l

Neutron energy / eV

natW-metal disc (80 cm diameter, 14 g natW)

54th INMM 2013Schillebeeckx et al., "Contribution of the JRC to the development of NRD"

Experimental model validation

Page 20: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

0.0

0.4

0.8

Texp

TM (hom.)

TM (in-hom.)

Tra

nsm

issi

on

10 20 30 40 50-10

-5

0

5

10

Res

idua

l

Neutron energy / eV

natW-powder mixed with natS-powder(80 cm diameter, 14 g natW, 3.5 g natS)

54th INMM 2013Schillebeeckx et al., "Contribution of the JRC to the development of NRD"

0.0

0.4

0.8

Texp

TM (hom.)

Tra

nsm

issi

on

10 20 30 40 50-10

-5

0

5

10

Res

idua

l

Neutron energy / eV

Experimental model validation

Page 21: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

Model accounting for inhomogeneities of a powder sample is implemented in REFIT

Initial validation of possible models with MC simulations

LP Model performs the best

Experimental validation of the model with capture and transmission measurements at GELINA

W powder samples with known grain size distribution

Summary

Page 22: Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security

Contributors:

B. Becker, F. Emiliani, S. Kopecky, P. SchillebeeckxEC – JRC – IRMM, Geel (B)

H. Harada F. Kitatani, M. Koizumi, H. TsuchiyaJAEA, Tokai-mura (Japan)

Acknowledgement:

This work was supported by the European Commission within the Seventh Framework Programme through ERINDA (FP7 – 269499).