There
are few day-to-day events that send me into a rage as quickly as a pair of
tangled earphones. As soon as I put them down, they somehow thread themselves
into an unholy mess. And don’t even think about putting them into your pocket
or bag. So how do headphones (and other stringy objects) get so knotted in such
a short time? To find out, these physicists started by tumbling strings of
different stiffness in a box. They found that “complex knots often form within
seconds” (so it’s not just my imagination!), and that stiffer strings are less
likely to get knotted up. They then used these data and computer simulations to
explain how the knots are likely formed (see figure below); basically, when
jostled, the strings tend to form coils, and then the loose end weaves through
the other strands, much like braiding or weaving. And voila! Tangled headphones
to make your day just that much angrier.
“It
is well known that a jostled string tends to become knotted; yet the factors
governing the “spontaneous” formation of various knots are unclear. We
performed experiments in which a string was tumbled inside a box and found that
complex knots often form within seconds. We used mathematical knot theory to
analyze the knots. Above a critical string length, the probability P of
knotting at first increased sharply with length but then saturated below 100%.
This behavior differs from that of mathematical self-avoiding random walks,
where P has been proven to approach 100%. Finite agitation time and jamming of
the string due to its stiffness result in lower probability, but P approaches
100% with long, flexible strings. We analyzed the knots by calculating their
Jones polynomials via computer analysis of digital photos of the string.
Remarkably, almost all were identified as prime knots: 120 different types,
having minimum crossing numbers up to 11, were observed in 3,415 trials. All
prime knots with up to seven crossings were observed. The relative probability
of forming a knot decreased exponentially with minimum crossing number and
Möbius energy, mathematical measures of knot complexity. Based on the
observation that long, stiff strings tend to form a coiled structure when
confined, we propose a simple model to describe the knot formation based on
random “braid moves” of the string end. Our model can qualitatively account for
the observed distribution of knots and dependence on agitation time and string
length.”
Schematic illustration of the simplified model for knot
formation. Because of its stiffness, the string tends to coil in the box, as
seen in Fig. 1, causing a number of parallel string segments to lie parallel
adjacent the end segment. As discussed in the text, we model knots as forming
due to a random series of braid moves of the end segment among the adjacent
segments (diagrams at bottom). The overall connectivity of the segments is
indicated by the dashed line.
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