Point always moves either to some state at which it stops, or to



Some cycle around which it circulates indefinitely. Such a graph

Is like a map of a country’s water drainage, showing, if a drop of

Water or a representative point starts at any place, to what region

It will come eventually. These separate regions are the graph’s

Basins. These matters obviously have some relation to what is

Meant by “stability”, to which we shall come in Chapter 5.

Ex. 1: Draw the kinematic graphs of the transformations of A and B in Ex. 2/4/3.

Ex. 2: How can the graph of an identical transformation be recognised at a

Glance?

Ex. 3: Draw the graphs of some simple closed one-one transformations. What is

Their characteristic feature?

Ex. 4: Draw the graph of the transformation V in which n, is the third decimal

digit of log10(n + 20) and the operands are the ten digits 0, 1, . . ., 9.

Ex. 5: (Continued) From the graph of V read off at once what is V(8), V2(4),

V4(6), V84(5).

Ex. 6: If the transformation is one-one, can two arrows come to a single point?

Ex. 7: If the transformation is many-one, can two arrows come to a single point ?

Ex. 8: Form some closed single-valued transformations like T, draw their kine-

Matic graphs, and notice their characteristic features.

Ex. 9: If the transformation is single-valued, can one basin contain two cycles?

      B → AD ← E ← C

And so on. These different shapes are not regarded as different

Graphs, provided the internal connexions are identical.

The elements that occur when C is transformed cumulatively by

U (the series C, E, D, D, …) and the states encountered by a point

In the kinematic graph that starts at C and moves over only one

Arrow at a step, always moving in the direction of the arrow, are

Obviously always in correspondence. Since we can often follow

The movement of a point along a line very much more easily than

We can compute U(C), U2(C), etc., especially if the transforma-

Tion is complicated, the graph is often a most convenient represen-

Tation of the transformation in pictorial form. The moving point

Will be called the representative point.

22

23

TH E D ET ERM IN A TE MA C HI N E

Chapter

3

T H E D ET ERM I N A T E M A C H I N E

Having now established a clear set of ideas about transforma-

Tions, we can turn to their first application: the establishment of an

Exact parallelism between the properties of transformations, as

Developed here, and the properties of machines and dynamic sys-

Tems, as found in the real world.

About the best definition of “machine” there could of course be

Much dispute. A determinate machine is defined as that which

Behaves in the same way as does a closed single-valued transfor-

Mation. The justification is simply that the definition works— that

It gives us what we want, and nowhere runs grossly counter to

What we feel intuitively to be reasonable. The real justification

Does not consist of what is said in this section, but of what follows

In the remainder of the book, and, perhaps, in further develop-

Ments.

It should be noticed that the definition refers to a way of behav-

Ing, not to a material thing. We are concerned in this book with

Those aspects of systems that are determinate— that follow regular

And reproducible courses. It is the determinateness that we shall

Study, not the material substance. (The matter has been referred to

Before in Chapter 1.)

Throughout Part I, we shall consider determinate machines, and

The transformations to be related to them will all be single-valued.

Not until S.9/2 shall we consider the more general type that is

Determinate only in a statistical sense.

As a second restriction, this Chapter will deal only with the

Machine in isolation— the machine to which nothing actively is

Being done.

As a simple and typical example of a determinate machine, con-

Sider a heavy iron frame that contains a number of heavy beads

Joined to each other and to the frame by springs. If the circum-

Stances are constant, and the beads are repeatedly forced to some

Defined position and then released, the beads’ movements will on

Each occasion be the same, i.e. follow the same path. The whole

24

System, started at a given “state”, will thus repeatedly pass

Through the same succession of states


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