In physical knot theory, each realization of a link or knot has an associated ropelength. Intuitively this is the minimal length of an ideally flexible rope that is needed to tie a given link, or knot. Knots and links that minimize ropelength are called ideal knots and ideal links respectively.
The ropelength of a knotted curve
C
L(C)=\operatorname{Len}(C)/\tau(C)
\operatorname{Len}(C)
C
\tau(C)
C
Ropelength can be turned into a knot invariant by defining the ropelength of a knot
K
K
One of the earliest knot theory questions was posed in the following terms:
In terms of ropelength, this asks if there is a knot with ropelength
12
15.66
C1
An extensive search has been devoted to showing relations between ropelength and other knot invariants such as the crossing number of a knot. For every knot
K
K
\operatorname{Cr}(K)3/4
\operatorname{Cr}(K)
(k,k-1)
k
On the other hand, there also exist knots whose ropelength is larger, proportional to the crossing number itself rather than to a smaller power of it. This is nearly tight, as for every knot,The proof of this near-linear upper bound uses a divide-and-conquer argument to show that minimum projections of knots can be embedded as planar graphs in the cubic lattice. However, no one has yet observed a knot family with super-linear dependence of length on crossing number and it is conjectured that the tight upper bound should be linear.