1 Challenge the future Fractal structure of nuclear graphite from nm to mm : a neutron’s view Z....
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Transcript of 1 Challenge the future Fractal structure of nuclear graphite from nm to mm : a neutron’s view Z....
1Challenge the future
Fractal structure of nuclear graphite from nm to mm :a neutron’s view
Z. Zhou*1, W.G. Bouwman1, H. Schut1, C. Pappas1
S. Desert2, J. Jestin2
S. Hartman3
1: Delft University of Technology, The Netherlands
2: Laboratoire Léon Brillouin, France
3: Paul Scherrer Institute, Switzerland
2Challenge the future
Fractal
Nuclear graphite ?
Self-similar in different scales
West Lake, Hangzhou
3Challenge the future
Neutron techniques
Small angle scattered neutrons
Transmitted neutrons
Neutrons
Structure of pores
Neutron imaging
Visible structural information in
real space
Small Angle Neutron Scattering
SANSSpin-Echo Small Angle Neutron Scattering
SESANS
4Challenge the future
Study on graphite
1 Å 1 nm 1 μm 1 mm
SESANS Imaging
Size range (real space)
Q range (reciprocal space)
1 nm-1 10-3 nm-110 nm-1
2Q
l
SANS
PGA graphite sample
5Challenge the future
4sinQ
Small Angle Neutron Scattering (SANS)
Neutrons
Transmitted beam
Scattered beamSample
2D detector
Scattering vectorQ$$$$$$$$$$$$$$
PAXE and TPA in LLB, Saclay
6Challenge the future
SANS of PGA
Multiple scatteringPower law
7Challenge the future
* DFR Mildner, PL Hall, J. Phys. D: Appl. Phys. 19 (1986) 1535
Schematic diagram of scattering from fractal ojects*
dimensionality of interfaces
The interface is sensed as smooth on
a distance smaller than
dimensionality of clusters
Power laws measured by SANS
8Challenge the future
SANS on PGA
Surface fractal dimension6 3.45 2.55sD
3I Q
4I Q
9Challenge the future
32 2
1( )
(1 ( ) )H
I q
qa
Random two phase media model
SANS simulation of the model
slope (3 2 )H
(6 ) (3 2 )
3 2
(3 ) / 2
Ds H
Ds H
H Ds
SANS of PGA2.55
0.225
Ds
H
10Challenge the future
1 Å 1 nm 1 μm 1 mm
SANS
Surface fractal
Ds = 2.55
SESANS
mon
ochr
omat
orm
agne
t 1
field
ste
pper
anal
yser
dete
ctor
pola
riser
guid
e fie
ld
Realisation SESANS @ TUD
sam
ple
pola
rise
r
pola
rise
r
M. Theo Rekveldt, Jeroen Plomp, Wim G. Bouwman, et al., Rev. Sci. Instrum. 2005
SESANS sensitive 30 nm – 20 um
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gas
liquid
glass
crystal
SESANS probes density correlationE.g. colloidal phases as function of concentration
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SESANS on PGA
1
2
1
22
( ) ( ) ( )1 2( )2
( ) exp( ( ( ) 1
0 5
)
.2
)
2
H
H
t
z zG z K
a aH
P z
H
z G
Surface fractal dimension
2. 53 52sD H
14Challenge the future
1 Å 1 nm 1 μm 1 mm
SANS
Surface fractal
Ds = 2.55
SESANS
Surface fractal
Ds = 2.55
Imaging
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Neutrons
Imaging with Cold neutrons (ICON), PSI
Neutron imaging
Sample Detector
Neutron transmission image of PGA
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Binary image obtained by thresholding the original image
Labelled pores which can be measured by DIPimage (a toolbox under Matlab)
Perimeter-area relation
2pDP AP is the contour perimeter length.
A is the enclosed area.
Dp is the fractal dimension of the bounding contour.
Relation between contour fractal dimension and surface fractal dimension of the object
1s pD D
Dp is the fractal dimension of the bounding contour.
Ds is the surface fractal dimension of the object.
Fractal analysis on image
17Challenge the future
Perimeter-area relationship
21.552
2.552 0.01.
08289
1
p
s
D
D Dp
Surface fractal dimension
18Challenge the future
1 Å 1 nm 1 μm 1 mm
SANS
Surface fractal
Ds = 2.55
SESANS
Surface fractal
Ds = 2.55
Imaging
Perimeter-area relation
Surface fractal Ds = 2.552
19Challenge the future
2D-Fourier Transform on image
2D Fourier transform3
2 2
1( )
(1 ( ) )
0.225
H
H
I q
qa
3I Q
Mass fractal dimension
(3 2
2. 5
)
5m
m
H D
D
20Challenge the future
1 Å 1 nm 1 μm 1 mm
SANS
Surface fractal
Ds = 2.55
SESANS
Surface fractal
Ds = 2.55
Imaging
Perimeter-area relation
Surface fractal Ds = 2.552
2D-Fourier transform
Mass fractal Dm = 2.55
21Challenge the future
Q (Å-1)
Sca
tte
ring
In
ten
sity
Data in Q-space over 7 orders of magnitude
Imaging
SANS
SESANS
22Challenge the future
Imaging
SANS
SESANS
Conclusion
Porosity of PGA graphite has a surface fractal structure with a
single fractal dimension Ds=2.55 over 7 orders of magnitude in
length scale. This is remarkable, which can provide complementary
information for modelling the structure of nuclear graphite.
Sca
tterin
g In
tens
ity
Q (Å-1)
23Challenge the future
Zhengcao Li Tadashi Maruyama
Acknowledge
M. Haverty
P. Mummery