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Felix Klein developed the idea that a geometry was defined in terms of its
invariant properties. Euclidean geometry has dominated classical thinking, for
it is the geometry constructed from the invariants of translation and rotations.
That is, Euclidean geometry is the geometry of rigid body motion. Two obvious
invariants are size and shape, but there are others. Such processes of
translation and rotations are defined as diffeomorphisms.
Consider now an elastic object, say a rubber notebook sheet of paper with three
holes in it. Certainly rigid motions of rotation and translation do not change
the size and shape of the object. However bending of the sheet changes it shape,
but not its size. Uniform expansion changes it size but not its shape. A general
stretching can change both size and shape, but all of these things leave one
property invariant. The number of holes does not change.
The number of holes, not their size or shape, is a topological property. A
topological property is an invariant of a smooth deformation (no tearing apart
or glueing together is permitted). Such processes are defined as homeomorphisms.
The key idea is that such processes that preserve topological properties are
continous, and have an inverse which is continuous.
The great bulk of classical physics is restricted to the study of geometric
properties. Classic Tensor analysis assumes a domain that is covered by
diffeomorphisms. Almost all of classical mechanics studies systems of invariant
topology. In almost every case, the highly developed theories are REVERSIBLE.
The parts of science that are controversial involve explanations of events where
the topology of the initial state is not the same as the topology of the final
state; where the process does not have a inverse. If the scientific objective
is to understand the real irreversible world, then
WHAT ARE THE LAWS OF TOPOLOGICAL EVOLUTION?
Cartan's theory of exterior differential forms can give part of the answer, for
it appears that Cartan's methods can be applied to problems of continuous
topological evolution. Such problems do not have unique continuous inverses.
Yet, by using the methods of functional substitution and the pullback
(RETRODICTION) some headway can be made in the understanding of irreversible
phenomena. For example, Cartan's methods may be used to say something about the
decay of turbulence, as a continuous irreversible process (think glueing
together). The creation of turbulence (think discontinuous punctures or tearing
into parts) is as of yet beyond current knowledge.
The idea is to learn about topology and topological properties, for when it is
recognized that topology has changed during a process, then a signal has been
given that such a process is irreversible in a thermodynamic sense.
Irreversibility, up to now, has eluded physical theories, except in a
statistical sense.
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