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On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

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Page 1: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

On the use of spatial eigenvalue spectra in transient polymeric

networks

Qualifying exam

Joris Billen

December 4th 2009

Page 2: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Overview

• Transient polymer networks

• Eigenvalue spectra for network reconstruction

• Spatial eigenvalue spectra

• Current work

Page 3: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Transient polymeric networks*

*’Numerical study of the gel transition in reversible associating polymers’, Arlette R. C. Baljon, Danny Flynn, and David Krawzsenek, J. Chem. Phys. 126, 044907 2007.

Page 4: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

TemperatureSol Gel

Transient polymeric networks• Reversible polymeric gels• Telechelic polymers

Concentration

Page 5: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

• Examples– PEG (polyethylene glycol) chains terminated by

hydrophobic moieties

– Poly-(N-isopropylacrylamide) (PNIPAM)

• Use:– laxatives, skin creams, tooth paste, Paintball fill,

preservative for objects salvaged from underwater, eye drops, print heads, spandex, foam cushions,…

– cytoskeleton

Telechelic polymers

Page 6: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

• Bead-spring model

• 1000 polymeric chains, 8 beads

• Reversible junctions between end groups

• Molecular Dynamics simulations

with Lennard-Jones interaction between beads and

FENE bonds model chain structure and junctions

• Monte Carlo moves to form and destroy junctions

• Temperature control (coupled to heat bath)

Hybrid MD / MC simulation

[drawing courtesyof Mark Wilson]

Page 7: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Transient polymeric network• Study of polymeric network

T=1.0only endgroupsshown

Page 8: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Network notations• Network definitions and notation

– Degree (e.g. k4=3)

– Average degree:– Degree distribution P(k)– Adjacency matrix– Spectral density:

k P(k)1 0

2 0.5

3 0.5

4 0

1

2

3

4

0 0 1 1

0 0 1 1

1 1 0 1

1 1 1 0

1

2

3

4

node 1 2 3 4

5.22

1

N

lkPkk i

N

ii

N

j=jλλδ

N=ρ(λ)

1

1

Page 9: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Degree distribution gel• Bimodal network:

Page 10: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Degree distribution gel (II)

• 2 sorts of nodes:– Peers– Superpeers

!!)(

k

ekN

k

ekNkP

PSkk

PP

kk

SS

Master thesis M. Wilson

Page 11: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

probabilities to form links?pSS

PPPSPSP

PPSSSSS

NpNpk

NpNpk

adjust :

pPP pPS

One degree of freedom!

Mimicking network

Page 12: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Mimicking network (II)

SimulatedGel

Model2 separatednetworkspps=0

Modelno linksbetween peersppp=0

Modelppp=0.002pps=0.009pss=0.04

‘Topological changes at the gel transition of a reversible polymeric network’, J. Billen, M. Wilson, A. Rabinovitch and A. R. C. Baljon, Europhys. Lett. 87 (2009) 68003.

Page 13: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Mimicking network (III)

[drawings courtesyof Mark Wilson]

lP

lS

lps

Page 14: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

• Proximity included

in mimicking gel

• Asymmetric spectrum

• Spectrum to estimate maximum connection length• Many real-life networks are spatial

– Internet, neural networks, airport networks, social networks, disease spreading, polymeric gel, …

Spatial networks

Page 15: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Eigenvalue spectra of spatial dependent networks*

* ’Eigenvalue spectra of spatial-dependent networks’, J. Billen, M. Wilson, A.R.C. Baljon, A. Rabinovitch, Phys. Rev. E 80, 046116 (2009).

Page 16: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Spatial dependent networks: construction (I)

• Erdös-Rényi (ER)

Regular ER random network Spatial dependent ER

qconnect

constant qconnect

~ distance

ijij dq ~

measure forspatial dependence

Page 17: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Spatial dependent networks: construction (II)

1.Create lowest cost network

2.Rewire each link with p

>p

<p

Rewiring probability p

0 1

Lo

wes

t co

st

ER

SD

ER

if rewired connection probability qij~dij

-

• Small-world network

Page 18: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

4

Spatial dependent networks: construction (III)

• Scale-free network

Regular scalefreeRich get richer

Spatial dependent scalefree:Rich get richer... when they are close

qconnect

~degree k qconnect

~(degree k,distance dij)

1

5

1

1

1

1

2

1

4

1

1

11

22

ijjji dkq )1(~

Page 19: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Spatial dependent networks: spectra

Observed effects for high :– fat tail to the right– peak shifts to left– peak at -1

Page 20: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

• Quantification tools:– mth central moment about mean:

– Skewness:

– Number of directed paths that return to starting vertex after s steps:

Analysis of spectra

Page 21: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Skewness

Page 22: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Directed paths

N

j=

kjk λ=D

1

• Spectrum contains info on graph’s topology:

Tree:D2=4(1-2-1)(2-1-2)(1-3-1)(3-1-3)

D3=0

1

2 3

TriangleD2=6D3=6

32

1

# of directed paths of k steps returning to the same node in the graph

Page 23: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Directed paths (II)

Page 24: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Number of triangles

• Skewness S related to number of triangles T

ER spatial ER 2Dtriangular lattice

• T and S increase for spatial network15

1

90

1

2

1

2

kkS

kkNT

N

kkS

kkT

1

6

1

2

1

2

3

6

NT

S

Page 25: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

System size dependence

Page 26: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Relation skewness and clustering coefficient (I)

• Clustering coefficient = # connected neighbors

# possible connections

• Average clustering coefficient

Spatial ER

Page 27: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Anti-spatial network• Reduction of triangles

• More negative eigenvalues

• Skewness goes to zero for high negative

Page 28: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Conclusions

• Contribution 1: Spectral density of polymer simulation– Spectrum tool for network reconstruction– Spectral density can be used to quantify spatial

dependence in polymer

• Contribution 2: Insight in spectral density of spatial networks– Asymmetry caused by increase in triangles– Clustering and skewed spectrum related

Page 29: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Current work

Page 30: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Current work (I)

• Polymer system under shear

Page 31: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Current work (II)

stress versusshear:plateau

velocityprofile:shear banding

Sprakel et al.,Phys Rev. E, 79,056306(2009).

preliminary results

Page 32: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Current work (III)• Changes in topology?

Page 33: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Acknowledgements

• Prof. Baljon

• Mark Wilson

• Prof. Avinoam Rabinovitch

• Committee members

Page 34: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Emergency slide I

• Spatial smallworld

Page 35: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Emergency slide II

• How does the mimicking work?– Get N=Ns+Np from simulation– Determine Ns and Np from fits of bimodal– Determine ls / lp / lps so that

0

)(k

AA kpNN

0

)(k

BB kpNN

Page 36: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Equation of Motion

)(tWrUr iiij

iji

FENEij

LJijij UUU

K. Kremer and G. S. Grest. Dynamics of entangled linear polymer melts: Amolecular-dynamics simulation. Journal of Chemical Physics, 92:5057, 1990.

W

•Interaction energy

•Friction constant

•Heat bath coupling – all complicated interactions

•Gaussian white noise

Page 37: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

• Skewness related to number of triangles T

• P (node and 2 neighbours form a triangle) =

possible combinations to pick 2 neighbours X

total number of links / all possible links

ER spatial ER

Number of triangles

Page 38: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

• Relation skewness and clustering:

however only valid for high <k> when <ki(ki-1)> ~ ki(ki-1)

can be approximated

by

Spatial dependent networks: discussion (IV)

Page 39: On the use of spatial eigenvalue spectra in transient polymeric networks Qualifying exam Joris Billen December 4 th 2009

Shear banding

S. Fielding, Soft Matter 2007,3, 1262.