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Title: Cellular Automata Models of Crystals and Hexlife


1
Cellular Automata Models of Crystals and Hexlife
  • CS240 Software Project
  • Spring 2003
  • Gauri Nadkarni

2
Outline
  • Background
  • Description of crystals
  • Packards CA model
  • A 3D CA model
  • Hexlife
  • Summary

3
Background
  • What is a Cellular Automaton (CA)?
  • State
  • Neighborhood
  • Program
  • What are crystals?
  • Solidification of fluid, vapors, solutions
  • Relation of CA and crystals
  • Similar structure

4
History of Crystals
  • Crystals comes from the greek word meaning
    clear ice
  • Came into existence in the late 1600s
  • The first synthetic gemstones were made in the
    mid-1800s
  • Crucial to semi-conductor industry since
    mid-1970s

5
Categories of Crystals
  • Hopper crystals
  • Polycrystalline materials
  • Quasicrystals
  • Amorphous materials
  • Snow crystals and snowflakes

6
Hopper Crystals
  • These have more rapid growth at the edge of each
    face than at the center
  • Examples rose quartz, gold, salt and ice

7
Polycrystalline materials
  • Composed of many crystalline grains not aligned
    with each other
  • Modeled by a CA which starts from several
    separated seeds
  • Crystals grow at random locations with random
    orientations
  • Results in interstitial region

Growth process of polycrystalline materials
8
Quasicrystals
  • Crystals composed of periodic arrangement of
    identical unit cells
  • Only 2-,3-,4-, and 6-fold rotational symmetries
    are possible for periodic crystals
  • Shechtman observed new symmetry while performing
    an electron diffraction experiment on an alloy of
    aluminium and manganese
  • The alloy had a symmetry of icosahedron
    containing a 5-fold symmetry. Thus quasicrystals
    were born

9
Quasicrystals
  • They are different from periodic crystals
  • To this date, quasicrystals have symmetry of
    tetrahedron, a cube and an icosahedron

Some forms of quasicrystals
10
Amorphous Materials
  • Do not have a well-ordered structure
  • Lack distinctive crystalline shape
  • Cooling process is very rapid
  • Ex Amorphous silicon, glasses and plastics
  • Amorphous silicon used in solar cells and thin
    film transistors

11
Snow crystals
  • Individual , single ice crystals
  • Have six-fold symmetry
  • Grow directly from condensing water vapor in the
    air
  • Typical sizes range from microscopic to at most a
    few millimeters in diameter

12
Growth process of snow crystals
  • A dust particle absorbs water molecules that form
    a nucleus
  • The newborn crystal quickly grows into a tiny
    hexagonal prism
  • The corners sprout tiny arms that grow further
  • Crystal growth depends on surrounding temperature

13
Growth process of snow crystals
  • Variation in temperature creates different growth
    conditions
  • Two dominant mechanisms that govern the growth
    rate
  • Diffusion the way water molecules diffuse to
    reach crystal surface
  • Surface physics of ice efficiency with which
    water molecules attach to the lattice

14
Snowflakes
  • One of the well-known examples of crystal
    formation
  • Collections of snow crystals loosely bound
    together
  • Structure depends on the temperature and humidity
    of the environment and length of time it spends

15
Different Snowflake Forms
Dendritic Sectored Plate
Simple Sectored Plate
Fern-like Stellar Dendrite
16
Packards CA Model
  • Computer simulations for idealized models for
    growth processes have become an important tool in
    studying solidification
  • Packard presents a new class of models
    representing solidification

17
Packards CA Model
  • Begin with simple models containing few
    elements.Then add physical elements gradually.
  • Goal is to find those aspects that are
    responsible for particular features of growth

18
Description of the model
  • A 2D CA with 2 states per cell and a transition
    rule
  • The states denote presence or absence of solid.
  • The rules depend on their neighbors only through
    their sum

19
Description of the model
  • Four Types of behavior
  • No growth
  • Plate structure reflecting the lattice structure
  • Dendritic structure with side branches growing
    along lattice directions
  • Growth of an amorphous, asymptotically circular
    form

20
Description of the model
  • Two important ingredients are
  • Flow of heat modeled by addition of a
    continuous variable at each lattice site to
    represent temperature
  • Effect of solidification on the temperature field
    when solid is added to a growing seed, latent
    heat of solidification must be radiated away

21
Simulations
  • Temperature is set to a constant high value when
    new solid is added
  • Hybrid of discrete and continuum elements
  • Different parameters used
  • diffusion rate
  • latent heat added upon solidification
  • local temperature threshold

22
Different Macroscopic Forms
Tendril growth dominated by tip splitting
Strong anisotropy, stable parabolic tip with
side branching
Amorphous fractal growth
23
A 3D CA model of free dendritic growth
  • Proposed by S. Brown and N. Bruce
  • A dendrite is a branching structure that freezes
    such that dendrite arms grow in particular
    crystallographic directions
  • free dendrites form individually and grow in
    super-cooled liquid
  • Both pure materials and alloys can display free
    dendritic growth behavior

24
The CA Model
  • A 100x100x100 element grid is used with an
    initial nucleus of 3x3x3 elements placed at the
    center
  • Each element of the nucleus is set to value of 1
    (solid)
  • All other elements are set to value of 0 (liquid)
  • Temperatures of all sites are set to an initial
    predetermined value representing supercooling.

25
Rules and Conditions
  • A liquid site may transform to a solid if cx gt 3
    and/or cy gt 3 and/or cz gt3
  • Growth occurs if the temperature of the liquid
    site lt Tcrit
  • Tcrit -? ( f(cx) f(cy) f(cz) )
  • where f(ci) 1/ ci ci gt 1
  • f(ci) 0 ci lt 1
  • (? is a constant)

26
Rules and Conditions
  • If a liquid element transforms to a solid , then
    temperature of the element is raised to a fixed
    value to simulate the release of latent heat
  • At each time step, the temperature of each
    element is updated

27
Results and Observations
  • ? is set to value of 20 for all simulations
  • The initial liquid supercoolings are varied in
    the range 60 to 32
  • Different dendritic shapes are produced
  • The growth is observed until number of solid
    sites grown from center towards the edge was 45
    along any axes.

28
Results and Observations
  • With judicious choice of parameters , it is
    possible to simulate growth of highly complex 3-D
    dendritic morphology
  • For larger initial supercoolings, compact
    structures were produced
  • As the supercooling was reduced, a plate-like
    growth was observed
  • When decreased further, a more spherical growth
    pattern with tip-splitting was observed

29
Results and Observations
  • Results showed remarkable similarity to
    experimentally observed dendrites
  • Simulated dendrites produced, evolved from a
    single nucleus, but experimentally observed
    growth patterns comprised several
    interpenetrating dendrites

30
Hexlife
  • A model of Conways Game of Life on a hexagonal
    grid
  • Each cell has six neighbors. These are called the
    first tier neighbors.
  • The hexlife rule looks at twelve neighbors, six
    belonging to the first tier and remaining six
    belonging to the second tier

31
Hexlife
V1
The first tier six neighbors are marked by red
color. The second tier six neighbors considered
are marked by blue color.
32
Hexlife - Rule
  • The live cells out of the twelve neighbors are
    added up each generation.
  • live 2nd tier neighbors are only weighted as 0.3
    in this sum whereas live 1st tier neighbors are
    weighted as 1.0
  • A cell becomes live if this sum falls within the
    range of 2.3 - 2.9, otherwise remains dead
  • A live cell survives to the next generation if
    this sum falls within the range of 2.0 - 3.3.
    Otherwise it dies (becomes an empty space)

33
Summary
  • Crystals have been known since the sixteenth
    century.
  • There are many different kinds of crystals seen
    in nature
  • It is very fascinating to see the different
    intricate and complex forms that one sees during
    crystal growth
  • CA models have been successfully used to simulate
    different growth behavior of crystals

34
Summary
  • Hexlife is modeled on Conways game of life on a
    hexagonal grid
  • Hexlife considers the sum of 12 neighbors as
    opposed to 8 neighbors considered on Conways
    game of life
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