by Martin Probert
First posted February 2001, revised April 2001, June 2001. Under major revision August 2002.
String figures are defined as 'unknots under tension'. The concepts of 'motif' (a subset of string contacts) and 'look-alikes' (similar looking string figures) are introduced. It is shown how, by labelling the motifs of a string figure, the figure can be projected onto two dimensions so that the techniques of knot theory can be used to identify the look-alikes. A process of 'unravelling by motifs' is introduced which transforms one look-alike into another. Several conjectures are made concerning this unravelling process on the set of all look-alikes.
In 1920 the historian of mathematics W. W. Rouse Ball wrote of string figures that "What ... is striking, is the immense variety of well-defined patterns". Yet no mathematical result that applies equally to all string figures (two dimensional and three dimensional, symmetric and asymmetric) appears ever to have been published. This paper attempts to rectify the situation. With the exception only of the ethnographical figures and the use made in one paragraph of knot theory, the contents are due solely to the present author.
Part I defines string figures and introduces the concepts of look-alikes and motifs. Part II shows how look-alikes may be determined by knot theory and introduces a process by which one look-alike is converted into another. Part III uses the results derived to analyse a range of string figures. Part IV contains several conjectures concerning the partial unravelling of string figures.
From the viewpoint of knot theory every string figure - each one of the 2000 known figures and every figure yet to be invented - is the ‘trivial knot’, an unknotted loop of string. To differentiate between one string figure and another we shall take account of the effect of tension as the string figure is extended between a number of suspension points.
We emphasise the following characteristics of string figures:
It is unlikely that it is possible to produce a unique and simple mathematical description of a string figure. A string figure is an unknot under tension. Any description of the static final figure would need to take account of string contacts, points of support, tensions in the string segments, and the three dimensional nature of many figures. The tensions in particular are very subtle: a small change in tension can produce a significant change in the figure. A notation defining the two dimensional projection of a three dimensional figure would give insufficient information to allow the figure to be constructed. And a description based upon a method of construction would certainly not be unique, for there are many ways in which a string figure may be constructed.
‘Spot the difference’ is a familiar game from childhood: the challenge is to spot the difference in two similar pictures. A similar game may be played with string figures. What is the difference in the following two string figures?
|Fig. 1 - Stone Money
Caroline Islands 1902
|Fig. 2 - Star
The labelling indicates the points at which the figures differ. E, F, G and H (fig. 1) differ from e, f, g and h (fig. 2). Such similar looking figures will be called look-alikes. We shall study such figures in detail.
The substructure efgh (fig. 2) is the reflection of EFGH (fig. 1), the reflection taking place in the plane of the substructure.
We define a reflectible substructure as one with the following three characteristics:
A pair of reflectible substructures such as EFGH and efgh will be called substructures of opposite parity.
An examination of Stone Money (fig. 1) shows that A, B, C, D, E, F and G are all reflectible substructures. There are no smaller reflectible substructures than those labelled A to G. Such minimal reflectible substructures will be called motifs.
It is easily proved that the reflectible substructures of any string figure are partitioned into motifs. The proof, which follows from the definitions of reflectible substructures and motifs, is left to the reader.
If a motif is denoted by an upper case letter, then the substitution in a string figure of that motif by one of opposite parity will be denoted by a lower case letter (compare fig. 1 motif G with fig. 2 motif g). A set of motifs will be denoted by a succession of upper or lower case letters where each letter is the label of a motif (e.g. fig. 2 contains the set of motifs ABCDefgh).
Motifs occur at each point of support of a string figure but, in such a case as Stone Money (fig. 1) where a single string encircles each point of support, these motifs are trivial and have not been labelled.
A motif may contain a complex cluster of string contacts. Two or more string segments may, for example, twist and intertwine ropewise around one another. We shall only represent such clusters in terms of distinct string crossings when we discuss the projection of a figure onto two dimensions for analysis by knot theory. To justify certain processes involving the unravelling of a three dimensional string figure, we shall make use of the Deconstruction Theorem introduced in Part II.
Four motifs we shall meet frequently are illustrated in fig. 3. From left to right the four motifs will be referred to as a single-crossing, a double-crossing, a spiral triple-crossing and a triangular triple-crossing.
Infinitely many different motifs exist. For example, two segments of string might twist around one another in spiral fashion through any multiple of 180 degrees to create a motif.
Each motif of fig. 3 above together with the corresponding motif of fig. 4 below make up a pair of motifs of opposite parity.
String figure glossary
Construction: Insert the thumbs into the loop and separate the hands. Pass the index fingers into the thumb loop from above and pick up the near thumb string. Pass the right thumb to the left and, from below, pick up the string running from the left thumb to left index. Extend. With the teeth pick up, from the back of the right thumb, the lower loop, pulling the loop up over the upper loop and off the right thumb, but maintaining hold of the loop with the teeth. Adjust the figure so that the mouth loop lies symmetrically between the left and right hands. Pass the little fingers under the strings and up into the thumb loop from below, then push the far thumb string and near index string away from you and under the far index string, then with the little fingers hook the far index string to the palm. Release the mouth loop and extend.
The 3D framework is the set of all those contacts in a three-dimensional string figure in which the single segments of string diverging from the contact do not all lie in a single plane. The 3D framework in the Worm is made up of the contacts P1, P2, P3, P4, P5 and P6.
Motifs in corresponding positions in two look-alikes are equivalent if, without involving the supporting single strands, the interiors of the motifs may be manipulated into identical configurations. The motifs in fig. 6 are equivalent.
For the construction of a string figure possessing four such motifs, see Double Crow's Feet on this web site (Main Menu: Invented String Figures).
We are not here concerned with the identification of the motifs in a given string figure. Identification of the motifs is merely a process of establishing the minimal substructures with the reflectible properties listed earlier. We assume that the motifs have been identified and pursue the following questions:
Changing the parity of one or more motifs will result in one of two outcomes: a similar looking string figure, or an impossible figure (i.e. one that may not be constructed from an unknotted loop). How may the similar looking string figures be identified, and what relationships exist between them?
String Figure Mathematics - Part II
String Figures - Main Menu