From clusters of particles to 2D bubble clusters

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Edwin Flikkema, ICMS, Edinburgh, March 2012 From clusters of particles to From clusters of particles to 2D bubble clusters 2D bubble clusters Edwin Flikkema, Simon Cox IMAPS, Aberystwyth University, UK

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From clusters of particles to 2D bubble clusters. Edwin Flikkema, Simon Cox IMAPS, Aberystwyth University, UK. Introduction and overview. Introduction: The minimal perimeter problem for 2D equal area bubble clusters. Systems of interacting particles Global optimisation - PowerPoint PPT Presentation

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Page 1: From clusters of particles to 2D bubble clusters

Edwin Flikkema, ICMS, Edinburgh, March 2012

From clusters of particles to 2D bubble From clusters of particles to 2D bubble clustersclusters

Edwin Flikkema, Simon Cox IMAPS, Aberystwyth University, UK

Page 2: From clusters of particles to 2D bubble clusters

Edwin Flikkema, ICMS, Edinburgh, March 2012

Introduction and overviewIntroduction and overview

Introduction:The minimal perimeter problem for 2D equal area bubble

clusters.Systems of interacting particlesGlobal optimisation

2D particle clusters to 2D bubble clustersVoronoi construction

2D particle systems: -log(r) or 1/rp repulsive potentialHarmonic or polygonal confining potentials

Results

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Edwin Flikkema, ICMS, Edinburgh, March 2012

2D bubble clusters2D bubble clusters• Minimal perimeter problem:

2D cluster of N bubbles. All bubbles have equal area. Free or confined to the interior of a circle or polygon. Minimize total perimeter (internal + external).

• Objective: apply techniques used in interacting particle clusters to this minimal perimeter problem.

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Edwin Flikkema, ICMS, Edinburgh, March 2012

Systems of interacting particlesSystems of interacting particles● System energy:● Usually:● Example:

...,,,

kjikjiijkji

jiij

iii rrrVrrVrVU

||||, jijiij rrVrrV

612

11rr

rV

Lennard-Jones potential:

LJ13: Ar13

● Used in: Molecular Dynamics, Monte Carlo, Energy landscapes

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Edwin Flikkema, ICMS, Edinburgh, March 2012

Energy landscapesEnergy landscapes● Stationary points of U: zero net force on each particle● Minima of U correspond to (meta-)stable states.● Global minimum is the most stable state.● Local optimisation (finding a nearby minimum) relatively easy:

● Steepest descent, L-BFGS, Powell, etc.● Global optimisation: hard.

Energy vs coordinate

Local optimisation

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Edwin Flikkema, ICMS, Edinburgh, March 2012

Global optimisation methodsGlobal optimisation methods• Inspired by simulated annealing:

Basin hopping Minima hopping

• Evolutionary algorithms: Genetic algorithm

• Other: Covariance matrix adaption Simply starting from many random geometries

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Edwin Flikkema, ICMS, Edinburgh, March 2012

2D particle systems2D particle systems• Energy:

• Repulsive inter-particle potential:

• Confining potential:

i

iconfi ij

jirep rVrrVU

)log(rrVrep or prep rrV 1

2

21 rKrVconf harmonic

polygonal 2

max21

kkconf urKrV

,...2,1p

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Edwin Flikkema, ICMS, Edinburgh, March 2012

2D particle clusters2D particle clusters• Pictures of particle clusters: e.g. N=41, bottom 3 in energy

-945.421319 -945.419781 -945.419508

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Edwin Flikkema, ICMS, Edinburgh, March 2012

Particles to bubblesParticles to bubbles

particle cluster Voronoi cells optimized perimeter

Qhull Surface Evolver

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Edwin Flikkema, ICMS, Edinburgh, March 2012

2D particle clusters2D particle clusters• Polygonal confining potential: e.g. triangular

1u2u

3u

2

max21

kkconf urKrV contour lines

discontinuous gradient: smoothing needed?

unit vectors

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Edwin Flikkema, ICMS, Edinburgh, March 2012

Technical detailsTechnical details• List of unique 2D geometries produced

• Problem: permutational isomers.

• Distinguishing by energy U not sufficient: Spectrum of inter-particle distances compared.

• Gradient-based local optimisers have difficulty with polygonal potential due to discontinuous gradient

Smoothing needed? Use gradient-less optimisers (e.g. Powell)?

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Edwin Flikkema, ICMS, Edinburgh, March 2012

N=31-37

Results: bubble clusters: Results: bubble clusters: Free, circle, hexagonFree, circle, hexagon

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Edwin Flikkema, ICMS, Edinburgh, March 2012

N=31-37

Results: bubble clusters: Results: bubble clusters: pentagon, square, trianglepentagon, square, triangle

Elec. J. Combinatorics 17:R45 (2010)

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Edwin Flikkema, ICMS, Edinburgh, March 2012

ConclusionsConclusions• Optimal geometries of clusters of interacting particles can

be used as candidates for the minimal perimeter problem.

• Various potentials have been tried. 1/r seems to work slightly better than –log(r).

• Using multiple potentials is recommended.

• Polygonal potentials have been introduced to represent confinement to a polygon

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Edwin Flikkema, ICMS, Edinburgh, March 2012

AcknowledgementsAcknowledgements• Simon Cox

• Adil Mughal

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Edwin Flikkema, ICMS, Edinburgh, March 2012

Energy landscapesEnergy landscapes● Stationary points of U: zero net force on each particle● Minima of U correspond to (meta-)stable states.● Global minimum is the most stable state.● Saddle points (first order): transition states● Network of minima connected by transition states● Local optimisation (finding a nearby minimum) relatively easy:

● L-BFGS, Powell, etc.● Global optimisation: hard.

Energy vs coordinate

Local optimisation

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Edwin Flikkema, ICMS, Edinburgh, March 2012

2D clusters: perimeter

is fit to data for free clusters