international summer school on turbulence diffusion 2006 multifractal analysis in b&w soil...
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International Summer School on Turbulence Diffusion 2006
Multifractal Analysis in B&W Soil Images
Ana M. Tarquis
Dpto. de Matemática Aplicada
E.T.S.I. Agrónomos
Universidad Politécnica de Madrid
International Summer School on Turbulence Diffusion 2006
INDEX
• Problem: motivation and start point.
• Fractals and multifractals concepts.
• Porosity images: resolved?
• Configuration Entropy
• Griding Methods
International Summer School on Turbulence Diffusion 2006
CONSERVATION OF NATURAL RESOURCES
• Agriculture : soil degradation and water contamination.
• Sustainable agriculture
• Quantification of soil quality index?
International Summer School on Turbulence Diffusion 2006
Soil structure • Water, solutes and gas transport• Soil resistance• Roots morphology• Microorganism populations
PORE AND SOIL MATRIX GEOMETRY
International Summer School on Turbulence Diffusion 2006
• Fractal structure: structured distribution of pore (and/or soil) in the space such that at any resolution the set is the union of similar subset to the whole.
International Summer School on Turbulence Diffusion 2006
Measure techniques
• The number-size relation is used normally to measure the fractal dimension of the defined measure (number of white or black pixels), or counting objects:
• Or covering the object with regular geometric elements of variable size:
DN )(
DkrrN )(
International Summer School on Turbulence Diffusion 2006
“ Box-Counting”
-m = fractal dimension, D
1 n
Black, white or interface
International Summer School on Turbulence Diffusion 2006
• Multifractal analysis consider the number of black pixels in each box (pore density=m).
International Summer School on Turbulence Diffusion 2006
• Multifractal: density has an structured distribution in the space such that at any resolution the set is the union of similar subsets to the whole. But the scale factor at different parts of the set is not the same.
• More than one dimension is needed => the measure consider (M) is characterized by the union of fractal sets, each one with a fractal dimension.
International Summer School on Turbulence Diffusion 2006
1 n
q
δn
1ii
iqii
m
mPδq,
δlog
δ1,logδ1,limD
δn
1iii
0δ1
Dq
q
)log()],(log[
lim)( 0 q
q
)log()],(log[
lim)1(
1)1(
)(0
qqq
qDq
International Summer School on Turbulence Diffusion 2006
Numerical Analysis of Multifractal Spectrum on 2-D Black and White Images
p1 p2
p3 p4
p1 p2
p3 p4
p1p2 p1p4
p1p1 p1p3
p2p2
p2p4
p2p1
p2p3
p3p2
p3p4
p3p1
p3p3 p4p1p4p2
p4p1p4p4
p1p2 p1p4
p1p1 p1p3
p2p2
p2p4
p2p1
p2p3
p3p2
p3p4
p3p1
p3p3 p4p1p4p2
p4p1p4p4
1 2 3 … 8
256
1
8
1
}4,3,2,1{.i
ik
kji mmjwithpmm
m (number of black pixels)m (number of black pixels)
p1 p2
p3 p4
p1 p2
p3 p4
p1p2 p1p4
p1p1 p1p3
p2p2
p2p4
p2p1
p2p3
p3p2
p3p4
p3p1
p3p3 p4p1p4p2
p4p1p4p4
p1p2 p1p4
p1p1 p1p3
p2p2
p2p4
p2p1
p2p3
p3p2
p3p4
p3p1
p3p3 p4p1p4p2
p4p1p4p4
1 2 3 … 8
256
1
8
1
}4,3,2,1{.i
ik
kji mmjwithpmm
m (number of black pixels)m (number of black pixels)
International Summer School on Turbulence Diffusion 2006
RANDOM AND MULTIFRACTAL IMAGES
• In this way a hierarchical probability tree was built generating an image of 1024x1024 pixels (ten subdivisions), as the soil images are normally analyzed.
• Probabilistic parameters are: { p1, p2, p3, p4 }• Random images : p1= p2 = p3 = p4 = 25%• Multifractal images: p1= 50%, p2= 5%, p3= 25%
and p4= 20% (by random arrangements or not).
International Summer School on Turbulence Diffusion 2006
Random
multifractal
International Summer School on Turbulence Diffusion 2006
-40.0
-32.0
-24.0
-16.0
-8.0
0.0
8.0
16.0
-12 -8 -4 0 4 8 12
q
(q)
1.00
1.25
1.50
1.75
2.00
2.25
2.50
2.75
3.00
3.25
3.50
-12 -8 -4 0 4 8 12
q
Dq
p1=0.40 p2=0.10
p1=0.33 p2=0.17
Generalized dimensions (Dq) obtained for two different distributions based on Stanley and Meakin (1988) formulas with
their respective -(q) curves.
International Summer School on Turbulence Diffusion 2006
Most common parameters calculated
• D0 q=0 box counting dimension
• D1 q=1 entropy dimension
• D2 q=2 correlation dimension
International Summer School on Turbulence Diffusion 2006
Singularities of the measure ()
For a given there is a fractal dimension f() of the set that support the singularity. At each area the relation number-size is applied:
dqqd )(
)()( fN
f()
)())(()( qqqfq
International Summer School on Turbulence Diffusion 2006
f()
Multifractal Spectrum
wf
w
International Summer School on Turbulence Diffusion 2006
ADS 375X250 PIXELS
VOIDSCIRCULARPOLARIZED
TRANSMITTED
International Summer School on Turbulence Diffusion 2006
INTER DENNY
ABOK MUNCHONG
1500x1000 pixels
International Summer School on Turbulence Diffusion 2006
-120
-70
-20
30
80
130
0 1 2 3 4 5 6 7
log r
log
(r
,q)
-10
-8
-6
-4
-2
0
2
4
6
8
10
¿How many points?
International Summer School on Turbulence Diffusion 2006
1,9900
1,9950
2,0000
2,0050
2,0100
2,0150
2,0200
-11 -9 -7 -5 -3 -1 1 3 5 7 9 11
0,0000
0,5000
1,0000
1,5000
2,0000
2,5000
3,0000
3,5000
-11 -9 -7 -5 -3 -1 1 3 5 7 9 11
0,0000
1,0000
2,0000
3,0000
4,0000
5,0000
-11 -9 -7 -5 -3 -1 1 3 5 7 9 11
ADS
BUSO
EHV1
International Summer School on Turbulence Diffusion 2006
We have to compare
1,5000
2,0000
2,5000
3,0000
3,5000
4,0000
4,5000
5,0000
-11 -9 -7 -5 -3 -1 1 3 5 7 9 11
ADS
BUSO
EVH1
International Summer School on Turbulence Diffusion 2006
0,0%
10,0%
20,0%
30,0%
40,0%
50,0%
60,0%
1,50 1,55 1,60 1,65 1,70 1,75 1,80 1,85 1,90 1,95 2,00
D0
Po
rosi
ty (
%)
1,0%
11,0%
21,0%
31,0%
41,0%
51,0%
61,0%
1,1000 1,3000 1,5000 1,7000 1,9000D1
Po
r. (
%)
1,0%
11,0%
21,0%
31,0%
41,0%
51,0%
61,0%
1,1000 1,3000 1,5000 1,7000 1,9000 2,1000
D2
Po
r. (
%)
International Summer School on Turbulence Diffusion 2006
Obtaining Dq por. q=-3
-20,0000
0,0000
20,0000
40,0000
60,0000
0,0000
2,0000
4,0000
6,0000
8,0000
log(r)
log(
S(r
))
lower
upper
por. q=0
-5,0000
0,0000
5,0000
10,0000
15,0000
0,0000
2,0000
4,0000
6,0000
8,0000
log(r)
log(
S(r
))
lower
upper
por. q=1
-15,0000
-10,0000
-5,0000
0,0000
5,0000
0,0000
2,0000
4,0000
6,0000
8,0000
log(r)
log(
S(r
))
lower
upper
Ehv1, porosity 46,7%
International Summer School on Turbulence Diffusion 2006
Calculating Dq
ADS, porosity 5,7%por. q=-3
-20,000000
-10,000000
0,000000
10,000000
20,000000
30,000000
40,000000
50,000000
0,000000 2,000000 4,000000 6,000000 8,000000
log(r)
log
(S(r
))
lower
upper
por. q=0
-4
-2
0
2
4
6
8
10
12
0,000000 2,000000 4,000000 6,000000 8,000000
log(r)
log
(S(r
))
lower
upper
por. q=1
-16
-14
-12
-10
-8
-6
-4
-2
0
2
4
0,000000 2,000000 4,000000 6,000000 8,000000
log(r)
log
(S(r
))
lower
upper
International Summer School on Turbulence Diffusion 2006
scale and put stde
multifractal? Yes, quite sure 10 points 10 points
difference in the difference in the number of points number of pointsfor the regression line for the regression line
multifractal? No, quite sure 8 points 8 points
scale and put stde
1,74
1,76
1,78
1,80
1,82
1,84
1,86
1,88
-5 -3 -1 1 3 5
q
Dq
1,93
1,94
1,95
1,96
1,97
1,98
1,99
2,00
-5 -3 -1 1 3 5q
Dq
1,601,651,701,751,801,851,901,952,002,05
-5 -3 -1 1 3 5q
Dq
1,601,701,801,902,002,102,202,302,40
-5 -3 -1 1 3 5q
Dq
International Summer School on Turbulence Diffusion 2006
Continuos line = random structure
Dashed line = mfract structure
Filled Square = values from image soils
1,0%
11,0%
21,0%
31,0%
41,0%
51,0%
61,0%
1,1000 1,3000 1,5000 1,7000 1,9000 2,1000
D0
Po
ros
ity
(%)
1,0%
11,0%
21,0%
31,0%
41,0%
51,0%
61,0%
1,1000 1,3000 1,5000 1,7000 1,9000 2,1000
D1
Po
ros
ity
(%)
1,0%
11,0%
21,0%
31,0%
41,0%
51,0%
61,0%
1,1000 1,3000 1,5000 1,7000 1,9000 2,1000
D2
Po
ros
ity
(%)
A
B
C
International Summer School on Turbulence Diffusion 2006
Considerations on Dq calculations
• Several authors have shown that the exact value of the generalized dimension is not an easy calculation to do . Vicsek proposed practical methods to compute the generalized dimension
• The main difficulty in using the multifractal formalism lies in the fact that the ideal limit cannot be reached in practice
International Summer School on Turbulence Diffusion 2006
RESULTS AND DISCUSSION (1)
• For all of the soil images with different porosity we obtain convincing straight-line fits to the data having all of them r2 higher than 0.98,
International Summer School on Turbulence Diffusion 2006
RESULTS AND DISCUSSION
• Finally, a comparison among the different images in each dimension is showed .
• In all of them, the points corresponding to porosities higher than 30% lie on the line representing the Dq calculated for the random generated images.
• Observing the difference between the fractal dimensions coming from multifractal and random images (discontinue line and continue line respectively) it is obvious that decreases when porosity increases in the images.
International Summer School on Turbulence Diffusion 2006
Configuration Entropy H()
The maximum value of j is x and the minimum value is 0 (Andraud et al., 1989)
1 i
n() = boxes of size from = 1 to = w /4
w
Nj = number of boxes with j black pixels inside
International Summer School on Turbulence Diffusion 2006
Configuration Entropy H()
The probability associated with a case of j black pixels in a box of size (pj())
)(
)()(
n
Np jj
))(plog()(p ) ( j0j
j
x
H
) (
) ( ) (*
max
H
HH )1log( ) ( 2
max H
International Summer School on Turbulence Diffusion 2006
Configuration Entropy H()
(pixels)
H*()
0
1
1 w/4
H*(L)
L
International Summer School on Turbulence Diffusion 2006
Methods: gliding, random walks, randomly
•Box size
•Jump step length
•Number of jumps
International Summer School on Turbulence Diffusion 2006
Thank you for your attention
International Summer School on Turbulence Diffusion 2006
Multifractal Analysis on a Matrix
Ana M. Tarquis
Dpto. de Matemática Aplicada
E.T.S.I. Agrónomos
Universidad Politécnica de Madrid
International Summer School on Turbulence Diffusion 2006
INDEX
• Field Percolation
• Soil Roughness
• Satellite images
• Time series
International Summer School on Turbulence Diffusion 2006
Z= 10 cm Z = 20 cm Z = 30 cm
Z = 40 cm Z = 50 cm Z = 60 cm
International Summer School on Turbulence Diffusion 2006
0
10
20
30
40
50
60
70
80
0 20 40 60 80 100Dye Tracer (%)
Dep
th (
cm
)
% of blue vs. depth
50%
15 cm
International Summer School on Turbulence Diffusion 2006
-120
-70
-20
30
80
130
0 1 2 3 4 5 6 7
log r
log
(r,q
)
-10
-8
-6
-4
-2
0
2
4
6
8
10
Z = 25 cm blue staining 28,95%
International Summer School on Turbulence Diffusion 2006
Dye Tracer Distribution
1
C1
0
50
100
150
200
250
Dye Tracer
X
Y
International Summer School on Turbulence Diffusion 2006
Multifractal Analysis of the Dye Tracer Distribution
1,830000
1,930000
2,030000
2,130000
2,230000
2,330000
-12 -9 -6 -3 0 3 6 9 12
qD
q
0,00
0,50
1,00
1,50
2,00
1,60 1,80 2,00 2,20 2,40 2,60
f(
)
A B
B) Generalized dimensions
A) f() spectrum
International Summer School on Turbulence Diffusion 2006
•Multispectral Satellite Images
International Summer School on Turbulence Diffusion 2006
0.45 m - 0.52 m
0.5
0.7
0.9
1.1
1.3
1.5
1.7
1.9
2.1
1.6 1.7 1.8 1.9 2 2.1 2.2 2.3
f(
)
Landsat-7 Ikonos (32 m)
0.52 m - 0.60 m
0.5
0.7
0.9
1.1
1.3
1.5
1.7
1.9
2.1
1.6 1.7 1.8 1.9 2 2.1 2.2 2.3
f(
)
Ikonos (32 m) Landsat-7
0.63 m - 0.69 m
0.5
0.7
0.9
1.1
1.3
1.5
1.7
1.9
2.1
1.6 1.7 1.8 1.9 2 2.1 2.2 2.3
f(
)
Ikonos (32 m) Landsat-7
0.76 m - 0.90 m
0.5
0.7
0.9
1.1
1.3
1.5
1.7
1.9
2.1
1.6 1.7 1.8 1.9 2 2.1 2.2 2.3
f(
)
Ikonos (32 m) Landsat-7
International Summer School on Turbulence Diffusion 2006
Soil Rougness• Roughness indices normally are based on
transects data. One of the most used is the Random Roughness (RR).
• RR is the standard deviation of the soil heights readings from the transect. This implies that there is not an spatial component.
• Several authors have applied fractal dimensions to this type of data. Burrough (1989), Bertuzzi et al. (1990), Huang and Bradford (1992),
International Summer School on Turbulence Diffusion 2006
INTRODUCTION
• The aim of this work is to study soil height readings with multifractal analysis in the context of soil roughness.
• Several soils, with different textures, with different tillage methods have been analysed to compare their multifractal spectrum.
International Summer School on Turbulence Diffusion 2006
Soil measurements
• Three different soils with different textures.
• Three different treatments applying tillage: chisel, moldboard, seedbeds.
• Height measures of 2x2 m2 plot area.
• Resolution of the measure each 2 cm
International Summer School on Turbulence Diffusion 2006
International Summer School on Turbulence Diffusion 2006
%Sand %Silt %ClayM.O. (%)
2.59
1.49 P_3
TextureCode
50.49 21.2 28.3
P_1
20.7 40.8 38.5 P_2
1.76 30.6 52.3 17.1
La Higueruela C.S.I.C.
La Higueruela C.S.I.C.
Place
E.T.S.I.A. Experimental fields
Soil texture
International Summer School on Turbulence Diffusion 2006
International Summer School on Turbulence Diffusion 2006
moldboard
seedbedschisel
International Summer School on Turbulence Diffusion 2006
moldboard
seedbeds
chisel
International Summer School on Turbulence Diffusion 2006
1
n
Box counting method
Number of boxes depends on i
20.4 20.2 13.0 58.7 20.5 21.9 22.7 22.4 22.1 21.1 22.0 21.0 22.4 21.6 37.5 21.2 20.520.8 20.0 20.6 20.6 20.0 14.8 22.3 23.4 22.7 21.5 21.9 41.3 22.2 22.0 22.2 21.3 37.127.5 19.3 20.3 22.7 20.9 21.4 21.4 23.3 22.6 21.8 21.5 21.1 21.5 21.9 22.2 22.4 20.822.1 19.3 20.1 21.6 22.0 21.5 22.0 21.9 22.4 21.5 21.6 22.2 21.6 22.1 22.6 22.3 22.123.5 19.0 19.4 20.0 21.5 20.3 23.2 20.5 22.4 22.1 21.4 21.6 21.2 21.1 21.4 22.0 22.123.0 19.1 18.3 19.5 19.8 19.8 19.9 25.0 22.0 21.8 22.1 21.1 21.0 21.9 21.6 22.0 22.620.3 18.9 20.3 19.2 19.4 19.5 19.4 24.6 23.1 21.6 22.8 21.6 21.0 22.7 21.5 22.4 22.719.7 18.8 19.4 18.8 18.3 18.2 19.9 20.1 25.5 22.9 22.4 72.9 20.4 21.3 21.8 22.9 22.519.1 18.4 19.5 19.3 18.8 18.1 18.5 18.9 18.5 24.3 23.1 23.9 19.9 20.2 22.1 22.2 22.718.2 18.4 17.9 19.8 18.9 18.4 18.7 18.6 18.7 18.6 24.5 21.7 20.0 20.5 21.9 21.8 22.317.2 18.5 17.8 18.4 19.3 18.9 18.1 18.8 19.0 18.4 18.6 18.7 20.4 21.4 21.6 21.4 22.217.3 17.1 17.7 17.8 19.4 19.0 18.4 19.6 19.3 19.5 18.3 18.2 18.3 20.2 23.2 21.0 21.917.8 17.2 17.2 17.9 18.9 19.1 19.2 19.3 19.0 18.2 19.5 18.3 18.9 13.0 22.3 20.8 21.0
20.4 20.2 13.0 58.7 20.5 21.9 22.7 22.4 22.1 21.1 22.0 21.0 22.4 21.6 37.5 21.2 20.520.8 20.0 20.6 20.6 20.0 14.8 22.3 23.4 22.7 21.5 21.9 41.3 22.2 22.0 22.2 21.3 37.127.5 19.3 20.3 22.7 20.9 21.4 21.4 23.3 22.6 21.8 21.5 21.1 21.5 21.9 22.2 22.4 20.822.1 19.3 20.1 21.6 22.0 21.5 22.0 21.9 22.4 21.5 21.6 22.2 21.6 22.1 22.6 22.3 22.123.5 19.0 19.4 20.0 21.5 20.3 23.2 20.5 22.4 22.1 21.4 21.6 21.2 21.1 21.4 22.0 22.123.0 19.1 18.3 19.5 19.8 19.8 19.9 25.0 22.0 21.8 22.1 21.1 21.0 21.9 21.6 22.0 22.620.3 18.9 20.3 19.2 19.4 19.5 19.4 24.6 23.1 21.6 22.8 21.6 21.0 22.7 21.5 22.4 22.719.7 18.8 19.4 18.8 18.3 18.2 19.9 20.1 25.5 22.9 22.4 72.9 20.4 21.3 21.8 22.9 22.519.1 18.4 19.5 19.3 18.8 18.1 18.5 18.9 18.5 24.3 23.1 23.9 19.9 20.2 22.1 22.2 22.718.2 18.4 17.9 19.8 18.9 18.4 18.7 18.6 18.7 18.6 24.5 21.7 20.0 20.5 21.9 21.8 22.317.2 18.5 17.8 18.4 19.3 18.9 18.1 18.8 19.0 18.4 18.6 18.7 20.4 21.4 21.6 21.4 22.217.3 17.1 17.7 17.8 19.4 19.0 18.4 19.6 19.3 19.5 18.3 18.2 18.3 20.2 23.2 21.0 21.917.8 17.2 17.2 17.9 18.9 19.1 19.2 19.3 19.0 18.2 19.5 18.3 18.9 13.0 22.3 20.8 21.0
2
20.4 20.2 13.0 58.7 20.5 21.9 22.7 22.4 22.1 21.1 22.0 21.0 22.4 21.6 37.5 21.2 20.520.8 20.0 20.6 20.6 20.0 14.8 22.3 23.4 22.7 21.5 21.9 41.3 22.2 22.0 22.2 21.3 37.127.5 19.3 20.3 22.7 20.9 21.4 21.4 23.3 22.6 21.8 21.5 21.1 21.5 21.9 22.2 22.4 20.822.1 19.3 20.1 21.6 22.0 21.5 22.0 21.9 22.4 21.5 21.6 22.2 21.6 22.1 22.6 22.3 22.123.5 19.0 19.4 20.0 21.5 20.3 23.2 20.5 22.4 22.1 21.4 21.6 21.2 21.1 21.4 22.0 22.123.0 19.1 18.3 19.5 19.8 19.8 19.9 25.0 22.0 21.8 22.1 21.1 21.0 21.9 21.6 22.0 22.620.3 18.9 20.3 19.2 19.4 19.5 19.4 24.6 23.1 21.6 22.8 21.6 21.0 22.7 21.5 22.4 22.719.7 18.8 19.4 18.8 18.3 18.2 19.9 20.1 25.5 22.9 22.4 72.9 20.4 21.3 21.8 22.9 22.519.1 18.4 19.5 19.3 18.8 18.1 18.5 18.9 18.5 24.3 23.1 23.9 19.9 20.2 22.1 22.2 22.718.2 18.4 17.9 19.8 18.9 18.4 18.7 18.6 18.7 18.6 24.5 21.7 20.0 20.5 21.9 21.8 22.317.2 18.5 17.8 18.4 19.3 18.9 18.1 18.8 19.0 18.4 18.6 18.7 20.4 21.4 21.6 21.4 22.217.3 17.1 17.7 17.8 19.4 19.0 18.4 19.6 19.3 19.5 18.3 18.2 18.3 20.2 23.2 21.0 21.917.8 17.2 17.2 17.9 18.9 19.1 19.2 19.3 19.0 18.2 19.5 18.3 18.9 13.0 22.3 20.8 21.0
3
International Summer School on Turbulence Diffusion 2006
MF analysis of Height Distribution (HD)
),(
),( )(q, i
i
q
q
log
,1log,lim 1
0
n
iii q
q
δlog
δq,logδq,limqf
δn
1iii
0δ
Chhabra and Jenssen method
q
δn
1ii
iqii
m
mPδq,
International Summer School on Turbulence Diffusion 2006
f()
Multifractal Spectrum
wf
w
International Summer School on Turbulence Diffusion 2006
Considerations on MF calculations
• Height readings have been corrected for slope and tillage tool marks.
• The linearity in the function were found in all cases from =1 to =64 cm.
• The range of q values used were from –5 to +5 with increments of 0.5.
• All the R2 obtained were higher than 0.97
International Summer School on Turbulence Diffusion 2006
HD Multifractal Spectrum
soil P-1
1,000
1,200
1,400
1,600
1,800
2,000
1,500 1,750 2,000 2,250 2,500
f(
)
chisel
seedbeds
moldboard
International Summer School on Turbulence Diffusion 2006
HD Multifractal Spectrum
soil P-2
1,95
1,96
1,97
1,98
1,99
2,00
2,01
1,90 1,95 2,00 2,05 2,10
f(
)
chisel
seedbeds
moldboard
International Summer School on Turbulence Diffusion 2006
HD Multifractal Spectrum
soil P-3
1,95
1,96
1,97
1,98
1,99
2,00
2,01
1,90 1,95 2,00 2,05 2,10
f(
)
chisel
seedbeds
moldboard
International Summer School on Turbulence Diffusion 2006
Results from the multifractal analysis
Code Treatment max f(max)
min f(min) w wf
Chisel 2.020 1.970 1.980 1.690 0.040 0.280Seedbeds 2.020 1.120 1.730 1.160 0.290 -0.040Moldboard 2.090 1.900 1.690 1.220 0.400 0.680Chisel 2.010 1.990 2.000 1.990 0.010 0.000Seedbeds 2.010 1.990 2.000 1.990 0.010 0.000Moldboard 2.010 1.970 1.990 1.970 0.020 0.000Chisel 2.003 1.990 1.998 1.990 0.006 0.000Seedbeds 2.004 1.990 1.997 1.990 0.007 0.000Moldboard 2.005 1.990 1.996 1.990 0.009 0.000
P_1
P_2
P_3
International Summer School on Turbulence Diffusion 2006
AV= 26.98 SD =14.90
1.051.151.251.351.451.551.651.751.851.952.05
1.5 1.7 1.9 2.1
f(
)random
Chisel
RR
International Summer School on Turbulence Diffusion 2006
AV= 21.89 SD =6.62
1.05
1.15
1.25
1.35
1.45
1.55
1.65
1.75
1.85
1.95
2.05
1.5 1.7 1.9 2.1
f(
)
random
Seedbeds
International Summer School on Turbulence Diffusion 2006
AV= 25.83 SD =8.92
1.05
1.15
1.25
1.35
1.45
1.55
1.65
1.75
1.85
1.95
2.05
1.5 1.7 1.9 2.1
f(
)
random
Moldboard
International Summer School on Turbulence Diffusion 2006
1,95
1,96
1,97
1,98
1,99
2,00
2,01
1,90 2,00 2,10
f(
)
random S.D. 2,84
seedbeds
1,95
1,96
1,97
1,98
1,99
2,00
2,01
1,90 2,00 2,10
f(
)
random S.D. 5,70
moldboard
1,95
1,96
1,97
1,98
1,99
2,00
2,01
1,90 2,00 2,10
f(
)
random S.D. 3,14
chiselsoil P-2
soil P-2
soil P-2
1,95
1,96
1,97
1,98
1,99
2,00
2,01
1,90 2,00 2,10
f(
)
random S.D. 3,34
chisel
1,95
1,96
1,97
1,98
1,99
2,00
2,01
1,90 2,00 2,10
f(
)
random S.D. 2,15
seedbeds
1,95
1,96
1,97
1,98
1,99
2,00
2,01
1,90 2,00 2,10
f(
)
random S.D. 2,47
moldboard
soil P-3
soil P-3
soil P-3
International Summer School on Turbulence Diffusion 2006
CONCLUSIONS
• Fractal dimensions estimated from MF analyses of HD are useful descriptors.
• Multifractal parameters seem to be correlated depending on soil texture properties.
• Comparison between data structure and a random structure can be used to get a complementary index to RR.
International Summer School on Turbulence Diffusion 2006
Further research
• More work on correlating parameters from multifractal analysis to soil properties: we need to understand what represent each parameter.
• More work on application of multifractal parameters to the prediction of processes related to soil erosion.
International Summer School on Turbulence Diffusion 2006
WIND FLUCTUATIONS• The study of wind-speed (w) is aimed at greenhouse
control (heating and ventilation), since wind velocity influences both types of control. Wind increases heat losses in winter nights, so it is of interest to regulate the heating as a function of wind-speed and its realistic simulation is an important task in modeling and system design.
• To study the multifractal nature of this series and to fully characterize the dynamical system that supports it is the first step before any simulation could be successfully achieved.
• Time series data from 2004 were used in this study. Every ten minutes, the station recorded mean values of the wind velocity in m/s. Thus we handle in each yearly analysis a series of 105.408 data points, and in the monthly analysis a minimum of 4.176 values (February) and a maximum of 4.464.
International Summer School on Turbulence Diffusion 2006
Stochastic process: fBm2
)()()( ii twtwCov
•The minimum and maximum lag values are normally chosen.
•If the series is self-similar then:
22)( HCCov Hurst exponent
•H = 0.5 => random structure
•H > 0.5 => persistant structure
•H < 0.5 => anti-persistant structure
International Summer School on Turbulence Diffusion 2006
Multifractal Analysis (MF)• Multiscaling analysis determines the
dependence of the statistical moments (and not only the covariance) of the time series on the resolution with which the data are examined.
• Different moments different exponent in the increments (q).
• Structure Function (Mq)
International Summer School on Turbulence Diffusion 2006
Generalized Hurst exponent H(q)
•The minimum and maximum lag values are normally chosen.
•If the series is self-similar or self-affine then:
q
iiq twtwM )()()( 21
)()( qqq CM
monotonically non-decreasing function of q
q
qqH
)()(
International Summer School on Turbulence Diffusion 2006
CASES
• stationary processes have scale-independent increments and show invariance under translation => H(q)=0
• non-stationary and monofractal processes => constant H(q)
• non-stationary and multifractal => non constant H(q)
International Summer School on Turbulence Diffusion 2006
Wind velocity time series
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
0:00
0:00
0:00
0:00
0:00
0:00
0:00
0:00
0:00
0:00
0:00
0:00
time
win
d (
m/s
)FEBRUARY 2004
0
0.5
1
1.5
2
2.5
3
time
win
d (
m/s
)JULY 2004
0
0.5
1
1.5
2
2.5
3
3.5
4
time
win
d (
m/s
)DECEMBER 2004
International Summer School on Turbulence Diffusion 2006
-1
-0.5
0
0.5
1
1.5
0:00
0:00
0:00
0:00
0:00
0:00
0:00
0:00
0:00
0:00
0:00
0:00
time
win
d f
luct
uat
ion
(m
/s)
FEBRUARY 2004
-1.5
-1
-0.5
0
0.5
1
0:00 0:00 0:00 0:00 0:00 0:00 0:00 0:00 0:00 0:00 0:00 0:00 0:00
timew
ind
flu
ctu
atio
n (
m/s
)
JULY 2004
-1.5
-1
-0.5
0
0.5
1
1.5
2
0:00 0:00 0:00 0:00 0:00 0:00 0:00 0:00 0:00 0:00 0:00 0:00 0:00
time
win
d f
luct
uat
ion
(m
/s)
DECEMBER 2004
International Summer School on Turbulence Diffusion 2006
Histograms of wind fluctuations
International Summer School on Turbulence Diffusion 2006
Structure Functions (M) for February of 2004.
-6
-4
-2
0
2
4
6
8
10
12
-8 -6 -4 -2 0
ln( /max)
ln(M
q)
2
4
6
8
10
12
International Summer School on Turbulence Diffusion 2006
(q) and the corresponding H(q) functionMonth (q) H(q) july y = -0.0156x2 + 0.4004x
R2 = 0.9881
0
1
2
3
4
5
6
7
0 2 4 6 8 10 12 14q
(q)
International Summer School on Turbulence Diffusion 2006
COMMENTS AND CONLUSION
• There are several steps as number of data and lag values range chosen that influence the numerical results.
• February shows a different behavior from the other months, however the q values used are much higher that it is normally found in the literature.
• July shows a clear multiscaling pattern with a non constant H(q). December shows an almost constant H(q)
• All of them, as the annual time series analysis, show an anti-persistent character.
• Structure Functions is a way to usefully characterizing this multiscale heterogeneity. Based on this modeling simulation of wind fluctuations can be done in easy way and being realistic.
International Summer School on Turbulence Diffusion 2006
Thank you for your attention