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International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 1
Construction of Maximum Tortuosity of
Single Fluid Path in Grid-based 2-d
System (5×20) and 3-d system (5×20×3)
S. Viridi1
, F. D. E. Latief2
, S. N. Khotimah3
Physics Department, Institut Teknologi Bandung
Jalan Ganesha 10, Bandung 40132, Indonesia
1
dudung@fi.itb.ac.id, 2
fourier@fi.itb.ac.id, 3
nurul@fi.itb.ac.id
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 2
Outline
• Introduction
• Model
• Results and discussion
• Summary
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 3
Introduction
Porosity
• Porosity ϕ is fraction of void space VV in
material with total volume VT
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 4
R. Hilfer, Phys. Rev. B 45 7115 (1992)
φ =
VV
VT
VT
VV
Tortuosity
• Hydraulic tortuosity T is ratio of averaged fluid
path λavg and geometrical distance L between
two points
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 5
M. Matyka, A. Khalili, Z. Koza, Phys. Rev E 78 026306 (2008)
L
T
avg
λ
=
L
λavg
Specific surface area
• Specific surface area S is defined as
with N is number of channels per cross-
sectional area and lavg is average peripheral
length of each pore, which could be simply
circumference of a pore
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 6
S =
Nlavg
1−φ
F.A. Schwertz, J. Am. Ceram. Soc. 32 390 (1949)
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 7
Model
L
W
H
• Imitating CDI-like
construction
Model
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 8
.
A. Hemmatifar, M. Stadermann, J.G. Santiago, J. Phys. Chem. C 119 24681 (2015)
capacitive
deionization
(CDI)
Model: Simplification
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 9
Model: Connected grids
• It should be perpendicular connected
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 10
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 11
Results and discussion
Some microstates
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 12
Thermodynamics probability
• Thermodynamics probability for certain
porosity ϕ
with the term 2NL is from side walls
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 13
.
Wφ =
N − 2NL( )!
Nϕ( )! N − 2NL − Nϕ( )!
Thermodynamics prob.. (cont.)
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 14
Averaged tortuosity
• Assume W = 1 for all tortuosity T smaller then
Tmax
where path with Tmax is found visually and
intuitively
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 15
φφ W
T
dT
W
T
T 11 max
1
avg
max −
=≈ ∫
Averaged tortuosity (cont.)
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 16
ϕ = 0.28, WT > 1
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 17
ϕ = 0.28, WT > 1 (cont.)
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 18
ϕ = 0.28, WT > 1 (cont.)
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 19
ϕ = 0.28, not connected voids
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 20
ϕ = 0.28, 3-d system (5×20×3)
• It can be understood that porosity between
0.253 and 0.280 will have the same value of
Tmax, since the 8 unconnected voids do not give
any contribution to Tmax
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 21
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 22
Summary
Summary
• System for modeling tortuosity of single
channel fluid path has been developed
• Thermodynamics probability of a certain
porosity value to produce a tortuous channel
is very small, in order of 10-17
• The postulate only is not sufficient to predict
how such channel can be formed in nature,
other mechanism is required
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 23
.
Acknowledgements
• Part of this work is supported by RIK ITB with
contract number 006q/I1.C01/PL/2016
• This presentation is supported by ICES 2016
Committee and Faculty of Mathematics and
Natural Sciences, Institut Teknologi Bandung
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 24
International Conference on
Energy Sciences (ICES)
25-7 July 2016, Bandung, Indonesia 25
Thank you

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Construction of Maximum Tortuosity of Single Fluid Path in Grid-based 2-d System (5×20) and 3-d system (5×20×3)

  • 1. International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 1 Construction of Maximum Tortuosity of Single Fluid Path in Grid-based 2-d System (5×20) and 3-d system (5×20×3) S. Viridi1 , F. D. E. Latief2 , S. N. Khotimah3 Physics Department, Institut Teknologi Bandung Jalan Ganesha 10, Bandung 40132, Indonesia 1 dudung@fi.itb.ac.id, 2 fourier@fi.itb.ac.id, 3 nurul@fi.itb.ac.id
  • 2. International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 2 Outline • Introduction • Model • Results and discussion • Summary
  • 3. International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 3 Introduction
  • 4. Porosity • Porosity ϕ is fraction of void space VV in material with total volume VT International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 4 R. Hilfer, Phys. Rev. B 45 7115 (1992) φ = VV VT VT VV
  • 5. Tortuosity • Hydraulic tortuosity T is ratio of averaged fluid path λavg and geometrical distance L between two points International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 5 M. Matyka, A. Khalili, Z. Koza, Phys. Rev E 78 026306 (2008) L T avg λ = L λavg
  • 6. Specific surface area • Specific surface area S is defined as with N is number of channels per cross- sectional area and lavg is average peripheral length of each pore, which could be simply circumference of a pore International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 6 S = Nlavg 1−φ F.A. Schwertz, J. Am. Ceram. Soc. 32 390 (1949)
  • 7. International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 7 Model
  • 8. L W H • Imitating CDI-like construction Model International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 8 . A. Hemmatifar, M. Stadermann, J.G. Santiago, J. Phys. Chem. C 119 24681 (2015) capacitive deionization (CDI)
  • 9. Model: Simplification International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 9
  • 10. Model: Connected grids • It should be perpendicular connected International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 10
  • 11. International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 11 Results and discussion
  • 12. Some microstates International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 12
  • 13. Thermodynamics probability • Thermodynamics probability for certain porosity ϕ with the term 2NL is from side walls International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 13 . Wφ = N − 2NL( )! Nϕ( )! N − 2NL − Nϕ( )!
  • 14. Thermodynamics prob.. (cont.) International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 14
  • 15. Averaged tortuosity • Assume W = 1 for all tortuosity T smaller then Tmax where path with Tmax is found visually and intuitively International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 15 φφ W T dT W T T 11 max 1 avg max − =≈ ∫
  • 16. Averaged tortuosity (cont.) International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 16
  • 17. ϕ = 0.28, WT > 1 International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 17
  • 18. ϕ = 0.28, WT > 1 (cont.) International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 18
  • 19. ϕ = 0.28, WT > 1 (cont.) International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 19
  • 20. ϕ = 0.28, not connected voids International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 20
  • 21. ϕ = 0.28, 3-d system (5×20×3) • It can be understood that porosity between 0.253 and 0.280 will have the same value of Tmax, since the 8 unconnected voids do not give any contribution to Tmax International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 21
  • 22. International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 22 Summary
  • 23. Summary • System for modeling tortuosity of single channel fluid path has been developed • Thermodynamics probability of a certain porosity value to produce a tortuous channel is very small, in order of 10-17 • The postulate only is not sufficient to predict how such channel can be formed in nature, other mechanism is required International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 23 .
  • 24. Acknowledgements • Part of this work is supported by RIK ITB with contract number 006q/I1.C01/PL/2016 • This presentation is supported by ICES 2016 Committee and Faculty of Mathematics and Natural Sciences, Institut Teknologi Bandung International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 24
  • 25. International Conference on Energy Sciences (ICES) 25-7 July 2016, Bandung, Indonesia 25 Thank you