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If you haven't heard of Philip Ball before, it's about
time you did. Ball (who majored in chemistry at Oxford
University and received his Ph.D. in physics from Bristol University)
is emerging as one of the best of the science writers
specializing in presenting scientific material to the general, as well as
the scientifically literate, public. His first book,
Designing the Molecular World: Chemistry at the
Frontier (1994), and his second book, Made to Measure: New Materials for the
21st Century (1997), are wonderful presentations of the
exciting new developments in our field of chemistry. They are
written in a lucid style by an author who is not afraid to
(successfully) tackle the task of explaining difficult concepts. Topics
such as molecular and crystal structures, chemical reactions,
laser chemistry, organic conductors, biochemistry,
atmospheric chemistry, and the rapidly progressing field of materials
science (e.g., photonics, information storage, biomaterials,
polymers) are discussed from first principles to current
developments, with many references to both the primary and
secondary literature. For the readers of this
Journal, who have strong chemistry backgrounds, each of the chapters in these
two books can be read independently.
However, in spite of the excellent writing, profuse
and illustrative diagrams and photographs, and intelligent
selection of timely topics, these books do not compare with the
tour de force presented by Philip Ball in his latest book,
The Self-Made Tapestry: Pattern Formation in
Nature. This book, an expanded version of Chapter 9 of
Designing the Molecular World, is best read as a coherent unit from beginning to
end. It describes the formation of the many naturally
occurring patterns, from the spots on a leopard to the ripples on
sand dunes to the spirals found in oscillating chemical
reactions. Pattern formation in chemistry, biology, physics,
mathematics, geology, cosmology, urban planning, atmospheric
dynamics, and mineralogy are but some of the areas covered by
the author, who shows us how similar patterns arising in
different circumstances are interrelated.
We can ask "Where does the pattern come from? Is it
built into the system? How can the symmetry of the effect
differ from that of the cause? Why are some patterns
universal?" The main thesis of this book is that the formation of
patterns is due to the operation of basic scientific principles, but
the answers to these questions arise only partly from the
derivation of the mathematical equations that describe the
interaction of the variables in the system. Of equal importance is
the ability to solve these equations. Since many of them
are intractable, it is only recently, with the availability of
supercomputers, that reasonable solutions have been produced.
In many cases involving complex systems, the older
theoretical work is best understood in light of modern
computational analyses. The results reported by a phalanx of
scientists covering an amazing range of subjects have been
mastered by Ball and formed into a coherent whole. His elucidation
of these generalizations from the myriad of individual
units of research is quite spectacular, even if one wishes to
quibble over some aspect or other.
In his efforts to demonstrate the universality of
pattern formation, Ball has organized the book by the type
of pattern that is formed. The general principles governing
the development of a particular pattern are described and
followed by many examples, often presented in great detail, from
a wide range of disciplines. In this way we are shown
that the same underlying physical principles are responsible
for similar patterns in apparently disparate fields.
The introductory chapter, Patterns, discusses two
main topics. First, D'Arcy Thompson's 1917 thesis that
biology cannot afford to neglect physics, so that much of
Darwinian natural selection can be explained in terms of applied
basic physics (e.g., the effect of mechanical forces). Second,
symmetry breaking--a uniform, fully symmetrical gaseous
system consists of randomly disordered individual molecules
whose average features are symmetrical; that is, they show no
patterns. The most highly symmetrical systems are also the
most featureless, and patterns form when the high symmetry
engendered by randomness is reduced. Symmetry breaking
is responsible for the formation of patterns!
The chapter on Bubbles explains how
three-dimensional soap bubbles, froths, honeycombs, geodesic domes,
cell-packing, and space-filling models, as well as
two-dimensional surfactant films and layered silicas, all form under the
same set of rules: the need to form a minimal surface.
In the next chapter we find that the crucial
characteristic of a Wave is that the elements of the pattern--its symmetry,
its length scale, its rhythms--are set "not by an external
agency but by the internal dynamics of the system."
Oscillating chemical reactions of many types are described in terms of
the autocatalysis that occurs. The BZ reaction, reactions in
catalytic converters, Liesegang bands, patterns in rocks, heart
rhythms, and microbial chemoattractant reactions are all described.
In one of the most fascinating chapters in the
book, Bodies, we learn that Alan Turing (of computer fame)
published a paper in 1952 describing a hypothetical chemical
reaction that could generate spontaneous symmetry
breaking, leading to stable spatial patterns (Turing patterns), in an
initially uniform mixture of compounds. The paper, entitled
"The Chemical Basis of Morphogenesis", is one of the more
influential papers in theoretical biology. This phenomenon,
which is no longer hypothetical, is currently explained as being
due to a competition between activation by compound A
and inhibition by compound B, where B diffuses more
rapidly than A, thus differentiating between global and local
reactions. These activator-inhibitor systems are responsible for the
formation of patterns on animal pelts, seashells, and
butterfly wings and in various chemical reactions.
In the chapter on Branches we find detailed
descriptions of dendritic growth of crystals, formation of snowflakes,
tree-branch growth, and bacterial colony formation presented
in terms of diffusion-limited aggregation (DLA) and
fractal geometry. DLA describes systems in which the "rate of
growth is governed by the rate of diffusion of particles. It differs
from the way regular, faceted crystals grow, in that there is no
opportunity for the impinging particles to rearrange themselves
so that they pack together most efficiently. Since this takes
place at the surface of the growing crystal, it soon becomes jagged
and disorderly."
The details of the final shape are a function of the
kinetics of crystal growth, where the branched clusters are
nonequilibrium structures. The fractal dimension is a measure of
how densely packed the branches are and is a property that
is precise, reproducible, and characteristic of the
apparently irregular, branched objects. We also learn that the
algorithms used to describe the shape of a tree are much more
complex than one would imagine; several examples are described.
In Breakdowns, which in some ways is a
continuation of the previous chapter, glass fracture, electrical
discharges, earthquake-induced crustal fractures, and landscape
evolution are analyzed in terms of fractal geometry. The pattern
developed as a river forms from its converging streams is described
best by a fractal scaling law that is characteristic of most
branched networks including cracks and DLA clusters.
In the discussion of Fluids we find that smooth
flow, patterned flow, and turbulence are described by several
basic theories covering flow through a pipe, convection in
Earth's mantle, shapes of clouds, and interactions of fluids of
various viscosities and compositions. We learn that even
chaotically turbulent flows have some general discernible patterns.
The section on Grains teaches us that sand dunes,
grain elevators, landslides, and avalanches all have something
in common with the gas-liquid critical point. Specifically,
density fluctuations lead into the phenomenon of self-organized
criticality (SOC). "The addition of even a single grain to a
sand pile can induce a landslide of any magnitude.
This scale-invariant behavior is characteristic of turbulent flows as
well and indicates that the sand pile is constantly seeking the
least stable state. States like these, which are susceptible to
fluctuations on all scales at the slightest provocation, are
called critical states. Every liquid achieves a critical state at a
well-defined temperature and pressure, called the critical point.
A fluid, at its critical point, undergoes density fluctuations on
all length scales and is unstable to even the slightest
disturbance. Sand piles, unlike fluids, seem to seek a return to the
critical state." This phenomenon has been termed SOC,
reflecting the fact that the critical state seems to organize itself into
this unstable configuration. This concept of SOC has been
applied in many fields.
In Communities the patterns of ecocycles,
population growth, game theory, and urban spread are modeled
using the principles described above--oscillations,
autocatalysis, self-organization, activation-inhibitor interactions,
fractal dendritic growth, and computer modeling.
As mentioned earlier, the author has assembled
and assimilated an amazing amount of information from
an astonishingly large number of research areas. He
presents these in a carefully planned sequence of chapters, in such
a way that maximum benefit will be obtained if the book is
read from beginning to end. Then when you think you have
learned all there is to know about pattern formation in nature, the
last chapter, Principles, recasts everything in terms of a
beautiful discussion of irreversible thermodynamics. Pattern
formation, which is the point at which a nonequilibrium system is
driven across a particular threshold, is the result of competing
forces, symmetry breaking, formation of dissipative structures,
phase-space attractors, instabilities, scale invariance,
bifurcations, and higher-order phase transitions. The experimental
and computational results of these analyses all contribute to our
understanding of how patterns form in nature, even if we
have not yet reached the level of understanding why a
particular pattern develops. It is worth reading the whole book just
to be able to understand and appreciate this final chapter.
(If you find, when you are finished reading it, that you
are motivated to study the subject in more detail, you
might start with An Introduction to Nonlinear Chemical
Dynamics: Oscillations, Waves, Patterns, and
Chaos, by I. R. Epstein and J. A. Pojman, 1998, also published by Oxford University
Press and reviewed by Field in this issue of J. Chem.
Educ. Or, you can look at the use of Mathematica in
studying oscillations, complexity, and chaos in chemical kinetics in this
Journal : J. Chem. Educ.
1999, 76, 861, and references cited therein.)
After his presentation of the principles guiding the
natural formation of patterns, Ball concludes "I believe it is one
of the principal messages of this book that we can map
many of nature's tapestries onto some universal blueprint, in
which specifics cease to matter."
As in his other books, there are many and excellent
photographs and diagrams, a section of beautiful color plates,
and references to the primary and secondary literature.
Finally, there are detailed instructions in the appendix for
preparing and studying seven different experiments that
demonstrate the material described in the text.
This book, with its many broad generalizations
accompanied by detailed examples, is well worth the time and
effort it takes to read it. It should be available to everyone
teaching in the sciences. The author, who was a senior editor for
Nature for 11 years, is now a consulting editor for them and
devotes his time to free-lance writing.
His next book, due out in the spring of 2000, is
titled H2O: A Biography of Water.
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