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Gregory
Buck Selected
Publications |
Department of
Mathematics Saint Anselm
College |
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The
self-induced motion of filaments Filaments are ubiquitous -- they appear on
every scale studied by science. We present here a new system of equations for
the self induced motion for an attracting or
repelling filament or filamentary distribution of matter. The equations allow
us to solve several natural problems involving filaments of varying shape
and/or varying mass or charge density. Applications include celestial
distributions such as spiral arms of galaxies, charged strings, and biofilaments such as DNA. |
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Galactic
spiral arms can be sustained by self-gravity Using an equation of motion for a
self-gravitating filament, we show how galactic spiral arms might be created and
sustained. We find that the combination of differential rotation of the
galactic disk and the self-gravity of the arm (as given by the equation)
leads to a rotating spiral structure. Moreover, using this analysis, we find
a differential equation that explicitly relates this spiral structure to the
rotation curve of the galaxy. In particular, the equation connects spiral
shape to pattern speed. We also describe a simple many-body numerical
experiment that supports our approach. The findings are with consistent with
observational evidence concerning arm structure and rotation curves,
including leading arm structures. |
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The
Wondrous Mathematics of Winter Éwhen winter comes I think of PlatoÕs theory of ideal
forms. If I say circle or square, you know what I mean, though in some sense
you have never seen a circle—the shape in the plane where all the
points are exactly equidistant from the center—because in reality
everything is always at least a little off. Plato thought truth ought to work
this way, that what we understand as truth is always an approximation to an
ideal form. Winter
is the PlatonistÕs seasonÉ
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The
spectrum of filament entanglement complexity and an entanglement phase
transition G. Buck and J. Simon DNA, hair, shoelaces, vortex lines, rope, proteins,
integral curves, thread, magnetic flux tubes, cosmic strings and extension
cords; filaments come in all sizes and with diverse qualities. Filaments
tangle, with profound results: DNA replication is halted, field energy is
stored, polymer materials acquire their remarkable properties, textiles are
created and shoes stay on feet. We classify entanglement patterns by the rate
with which entanglement complexity grows with the length of the filament. We
show which rates are possible and which are expected in arbitrary
circumstances. We identify a fundamental phase transition between linear and
nonlinear entanglement rates. We also find (perhaps surprising) relationships
between total curvature, bending energy and entanglement. |
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A
Mathematician Goes to the Beach Like everyone else I know, when I go to the
beach I think mathematics. Archimedes, my favorite mathematician, did too --
his perhaps best-known work is the 'Sand Reckoner,' wherein he counts the
grains of sand it would take to fill the universe. He must have been at the
beach when he thought how to do it. I'm not sure Archimedes picked the most
interesting thing about the beach for analysis, but he might be forgiven --
because the ancient Greeks didn't wear swimsuits. Swimsuits often remind me of Carl Friedrich
Gauss, a superb nineteenth-century mathematician who really understood a
curved surface... |
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G. Buck, R. Scharein,
J. Schnick, J. Simon We introduce
a measure of complexity, an energy, for any
conformation of filaments. It is the occlusion, the portion hidden when
viewed from an arbitrary exterior point. By inverting we get the exposure, a
first approximation of the accessibility of the filaments. Assuming the
filament is a source, we get the self-irradiation, which leads to both an
interpretation as the temperature and a visualization technique: ray tracing
as a virtual laboratory. There is a wide variety of applications, from enzyme
action on and radiation damage of biopolymers, to the geometry of light bulb
filaments. Energy minimization provides automatic detangling, resulting in
symmetric and pleasing conformations. |
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DNA
disentangling by type-2 topoisomerases G.
Buck and
E. Zechiedrich A type-2 topoisomerase cleaves
a DNA strand, passes another through the break, and then rejoins the severed
ends. Because it appears that this action is as likely to increase as to
decrease entanglements, the question is: how are entanglements removed? We
argue that type-2 topoisomerases have evolved to act at ÒhookedÓ
juxtapositions of strands (where the strands are curved toward each other).
This type of juxtaposition is a natural consequence of entangled long
strands. Our model accounts for the observed preference for unlinking and
unknotting of short DNA plasmids by type-2 topoisomerases and well explains experimental
observations. |
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Most
smooth closed space curves contain an approximate solution to the N-body
problem The determination
of the exact trajectories of mutually interacting masses (the n-body
problem) is apparently intractable for n greater than or equal to 3, when the generic solutions become
chaotic. A few special solutions are known, which require the masses to be in
certain initial positions; these are known as 'central configurations' (an example is the equilateral
triangle formed by the Sun, Jupiter and Trojan asteroids). The configurations
are usually found by symmetry arguments. Here I report a generalization of
the central-configuration approach which leads to
large continuous families of approximate solutions. I consider the uniform
motion of equidistributed masses on closed space
curves, in the limit when the number of particles tends to infinity. In this
situation, the gravitational force on each particle is proportional to the
local curvature, and may be calculated using an integral closely related to
the Biot–Savart
integral. Approximate solutions are possible for certain (constant) values of
the particle speed, determined by equating this integral to the mass times
the centrifugal acceleration. Most smooth, closed space curves contain such
approximate solutions, because only the local curvature is involved.
Moreover, the theory also holds for sets of closed curves, allowing
approximate solutions for knotted and linked configurations. |
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Four-thirds
power law for knots and links Physical knot theory has recently
been applied to polymer dynamics, and specifically to gel electrophoresis of
DNA. Knot energies measure the complexity of a knot
conformation; minimum energy conformations are considered canonical or
'ideal' conformations. The rope length of a knot is one such measure of
energy and an approximately linear relationship between rope length and the
average crossing number for minimum rope-length conformations of simple knots
has been reported. Here I show that a linear relationship cannot hold in
general: the rope length required to tie an N-crossing knot or link
varies at least between ~N 3/4 and ~N. Since it is known that there are only
a finite number of knots for any given finite N number of crossings, this
result gives a bound on the number of different knots that can be tied in a
finite length of rope. |
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