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APS 2015 19-20 Agustus 2015, Bandung, Indonesia 1
Two-Dimension Granular Fission Toy
Model and Evolution of Granular
Compaction
Sparisoma Viridi*, Rizal Kurniadi, and Abdul Waris
Nuclear Physics and Biophysics Research Division
Institut Teknologi Bandung, Jalan Ganesha 10, Bandung 40132, Indonesia
*dudung@gmail.com
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 2
Outline
• Previous studies
• Interactions
• Molecular dynamics method
• Simulation parameters
• Results and discussion
• Summaries
Previous study
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 3
Viridi et al., AIP-CP 2012
Previous study (cont.)
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 4
Viridi et al., JPFSM 2015
Interactions
• Repulsive force
• Attractive force
• Electrostatic force
• Center force
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 5
Interactions: Repulsive force
• Linear spring dash-pot model
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 6
ijNijijNij vrkF ˆˆ γξ −=

( )ijij rD −= ,0maxξ
ijijijij
ij
ij
ij rrrr
r
r
r


⋅=== ,ˆ
ijijijij
ij
ij
ij vvvv
v
v
v


⋅=== ,ˆ
Interactions: Attractive force
• Gravitational-like force
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 7
ij
ij
Gij r
r
m
kG ˆ2
2
−=

Interactions: Electrostatic force
• Coulomb-like force
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 8
ij
ij
ji
Qij r
r
qq
kQ ˆ2
=

Interactions: Center force
• Near earth gravitation-like force
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 9
( )
ci
ci
gi
rr
rr
mkF 

−
−
−=
Molecular dynamics method
• Newton second law of motion
• Euler algorithm
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 10








+++= ∑≠ij
ijijijii GQFF
m
a

1
1
( ) ( ) tatvttv ∆+=∆+

( ) ( ) tvtrttr ∆+=∆+

Simulation parameters
• kN = 5×103
, γN = 0
• kG = 0.5
• kQ = 1
• kg = 100, rc± =
• D = 0.5, m = 1, qi = 0
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 11
)1,1(22 ±±
Simulation parameters (cont.)
• L = 2, 3, 4, 5
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 12
Results and discussion
• Initial and final configurations
• Evolution of compaction
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 13
Initial and final config.. (L = 2)
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 14
Initial and final config.. (L = 3)
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 15
Initial and final config.. (L = 4)
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 16
Initial and final config.. (L = 5)
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 17
Evolution of compaction
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 18
Summaries
• Considered forces and chosen parameters 
fission-like process for 2-d spherical granular
configuration
• Compaction tends to form 2-d hexagonal close
packed (HCP) system under influence of the
forces
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 19
Future plan
• Formulation to quantify compaction for multi-
center compaction
• Introduce charged particles
• Add probabilistic factor
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 20
Acknowledgement
• This work is supported by Riset Inovasi Batch II
with contract number 1763/I1.B04.1/KU/2015
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 21
APS 2015 19-20 Agustus 2015, Bandung, Indonesia 22
Thank you

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Two-Dimension Granular Fission Toy Model and Evolution of Granular Compaction

  • 1. APS 2015 19-20 Agustus 2015, Bandung, Indonesia 1 Two-Dimension Granular Fission Toy Model and Evolution of Granular Compaction Sparisoma Viridi*, Rizal Kurniadi, and Abdul Waris Nuclear Physics and Biophysics Research Division Institut Teknologi Bandung, Jalan Ganesha 10, Bandung 40132, Indonesia *dudung@gmail.com
  • 2. APS 2015 19-20 Agustus 2015, Bandung, Indonesia 2 Outline • Previous studies • Interactions • Molecular dynamics method • Simulation parameters • Results and discussion • Summaries
  • 3. Previous study APS 2015 19-20 Agustus 2015, Bandung, Indonesia 3 Viridi et al., AIP-CP 2012
  • 4. Previous study (cont.) APS 2015 19-20 Agustus 2015, Bandung, Indonesia 4 Viridi et al., JPFSM 2015
  • 5. Interactions • Repulsive force • Attractive force • Electrostatic force • Center force APS 2015 19-20 Agustus 2015, Bandung, Indonesia 5
  • 6. Interactions: Repulsive force • Linear spring dash-pot model APS 2015 19-20 Agustus 2015, Bandung, Indonesia 6 ijNijijNij vrkF ˆˆ γξ −=  ( )ijij rD −= ,0maxξ ijijijij ij ij ij rrrr r r r   ⋅=== ,ˆ ijijijij ij ij ij vvvv v v v   ⋅=== ,ˆ
  • 7. Interactions: Attractive force • Gravitational-like force APS 2015 19-20 Agustus 2015, Bandung, Indonesia 7 ij ij Gij r r m kG ˆ2 2 −= 
  • 8. Interactions: Electrostatic force • Coulomb-like force APS 2015 19-20 Agustus 2015, Bandung, Indonesia 8 ij ij ji Qij r r qq kQ ˆ2 = 
  • 9. Interactions: Center force • Near earth gravitation-like force APS 2015 19-20 Agustus 2015, Bandung, Indonesia 9 ( ) ci ci gi rr rr mkF   − − −=
  • 10. Molecular dynamics method • Newton second law of motion • Euler algorithm APS 2015 19-20 Agustus 2015, Bandung, Indonesia 10         +++= ∑≠ij ijijijii GQFF m a  1 1 ( ) ( ) tatvttv ∆+=∆+  ( ) ( ) tvtrttr ∆+=∆+ 
  • 11. Simulation parameters • kN = 5×103 , γN = 0 • kG = 0.5 • kQ = 1 • kg = 100, rc± = • D = 0.5, m = 1, qi = 0 APS 2015 19-20 Agustus 2015, Bandung, Indonesia 11 )1,1(22 ±±
  • 12. Simulation parameters (cont.) • L = 2, 3, 4, 5 APS 2015 19-20 Agustus 2015, Bandung, Indonesia 12
  • 13. Results and discussion • Initial and final configurations • Evolution of compaction APS 2015 19-20 Agustus 2015, Bandung, Indonesia 13
  • 14. Initial and final config.. (L = 2) APS 2015 19-20 Agustus 2015, Bandung, Indonesia 14
  • 15. Initial and final config.. (L = 3) APS 2015 19-20 Agustus 2015, Bandung, Indonesia 15
  • 16. Initial and final config.. (L = 4) APS 2015 19-20 Agustus 2015, Bandung, Indonesia 16
  • 17. Initial and final config.. (L = 5) APS 2015 19-20 Agustus 2015, Bandung, Indonesia 17
  • 18. Evolution of compaction APS 2015 19-20 Agustus 2015, Bandung, Indonesia 18
  • 19. Summaries • Considered forces and chosen parameters  fission-like process for 2-d spherical granular configuration • Compaction tends to form 2-d hexagonal close packed (HCP) system under influence of the forces APS 2015 19-20 Agustus 2015, Bandung, Indonesia 19
  • 20. Future plan • Formulation to quantify compaction for multi- center compaction • Introduce charged particles • Add probabilistic factor APS 2015 19-20 Agustus 2015, Bandung, Indonesia 20
  • 21. Acknowledgement • This work is supported by Riset Inovasi Batch II with contract number 1763/I1.B04.1/KU/2015 APS 2015 19-20 Agustus 2015, Bandung, Indonesia 21
  • 22. APS 2015 19-20 Agustus 2015, Bandung, Indonesia 22 Thank you