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Section 21 of 67
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Page 27 of 46
CHAPTER XIII MATTER AND SPACE
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Chapter XIII — MATTER AND SPACE
Central question
How should matter and space be related in the new physics?
Main argument
Russell argues that matter is not a little thing sitting in space; it is a structured set...
AI Summary
The Analysis of Matter
Section 21 of 67
Chapter XIII — MATTER AND SPACE
Central question
How should matter and space be related in the new physics?
Main argument
Russell argues that matter is not a little thing sitting in space; it is a structured set of events whose spatial relations are themselves part of the theory. Geometry and matter co-determine each other. This chapter is a major step toward seeing matter as a logical construction rather than a substance.
Key ideas
Matter is tied to event-structure.
Space is not an empty container.
Geometry and physics are intertwined.
The old substance picture is too coarse.
Key takeaway
Matter and space are mutually defined within a single structural account.
Missing dictionary data:
1 unique word is not in the dictionary data yet. Amber marks show where it appears.
finitely extended events will form the subject of the next chapter .
Nor do I assign a maximum to the duration of an event ,
though I hold that any event ,
in the broad sense ,
which lasts for more [Pg 287]
than about a second can ,
if it is a percept ,
be analyzed into a structure of events .
But this is a merely empirical fact .
There are certain purely logical principles which are useful in regard to structure .
When we are dealing with inferred entities ,
as to which ,
as explained in Part II.,
we know nothing beyond structure ,
we may be said to know the equations ,
but not what they mean :
so long as they lead to the same results as regards percepts ,
all interpretations are equally legitimate .
Let us take an example .
Suppose we have a set of propositions about an electron which we will call .
According to the subject-predicate logic ,
and according to the view that matter is a substance ,
there is a certain entity which is mentioned in all statements about this electron .
According to the view which resolves an electron into a series of events ,
the propositions in question will be differently analyzed .
Assuming a certain schematic simplicity ,
we might set the matter out as follows :
there is a certain relation which sometimes holds between events ,
and when it holds between and ,
and are said to be events in the biography of the same electron .
If belongs to the field of , "
the electron to which belongs "
will mean the relation with its field limited to terms belonging to the -
family of ;
and the -
family of consists of together with the terms which have the relation to and the terms to which has the relation . "
This electron "
will mean "
the electron to which this belongs ." "
An electron "
will mean "
a series such that there is an such that the series is the electron to which belongs ."
In order to mention some particular electron ,
we must be able to mention some event connected with it ,
e .g.
the scintillation when it hits a certain screen .
Thus ,
instead of saying "
the event happened to the electron "
we shall say "
the event happened to the electron to which happened ,"
or ,
more simply , "
belongs to the -
family of ."
The formal properties of the propositional function "
belongs to the -
family [Pg 288]
of " (
being constant )
are the same as those of "
belongs to the electron ."
If we want any two electrons to be mutually exclusive ,
in the sense that no event can happen to both ,
we can insure it by assuming that if has the relation (
or the converse relation )
to both and ,
then belongs to the -
family of .
If we do not want this ,
we do not make this assumption about .
It is because of the identity in formal properties that the one propositional function can be substituted for the other .
Whenever we suggest a new view as to structure ,
we have to make sure that it does not falsify any of the old formulæ ,
though it may give them a new interpretation .
Another illustration ,
more purely logical ,
may be useful .
It seems natural to say that any given shade of colour is a quality ,
i .
e .
that when we say "
this is red ,"
we are saying that "
this "
has a characteristic which we cannot express otherwise than by a predicate —
assuming ,
for the moment ,
that "
red "
stands for just one shade of colour .
But although this may be the right view ,
there is no logical necessity for supposing that it is .
We might define one shade of colour as "
all the coloured surfaces which have exact colour-similarity
to a given surface ."
Thus "
this has the colour "
is replaced by "
this is one of the class of entities that have exact colour-similarity
with ";
and "
is a colour "
will be replaced by "
is the class of all entities having exact colour-similarity
with a given entity ."
In this case ,
no facts can be conceived which would give reason for preferring one form of statement to the other ,
since any ascertainable fact can be interpreted equally well on either theory .
We have ,
in fact ,
something more or less analogous to the arbitrariness of co-ordinates in the general theory of relativity .
Provided our symbols have the same interpretation when they apply to percepts ,
their interpretation elsewhere is arbitrary ,
since ,
so long as the formulæ remain the same ,
the structure [Pg 289]
asserted is the same whatever interpretation we give .
Structure ,
and nothing else ,
is just what is asserted by formulæ in which the meaning of the terms is unknown ,
but the purely ,
logical symbols have definite meanings (
see Chapter XVII.).
Even the purely logical symbols are arbitrary to a certain limited extent ,
as we saw in the above example of colours .
But often ,
when facts from different regions have to be brought into connection ,
one interpretation is much simpler than another .
Often ,
also ,
one interpretation involves less inference than another ,
and is therefore less likely to be wrong .
These are the main motives governing any suggested interpretation of the symbols which occur in mathematical physics .
FOOTNOTES : [58] Dr C.
D .
Broad ,
in The Mind and its Place in Nature ,
lays stress upon what he calls "
emergent "
properties of complexes —
i .
e .
such as cannot be inferred from the properties and relations of the parts .
I believe that "
emergent "
properties represent merely scientific incompleteness ,
which would not exist in the ideal physics .
It is difficult to advance any conclusive argument on either side as to the ultimate character of apparently "
emergent "
properties ,
but I think my view is supported by such examples as the explanation of chemistry in terms of physics by means of the Rutherford-Bohr
theory of atomic structure .
[Pg 290]
CHAPTER XXVIII
THE CONSTRUCTION OF POINTS [59]
THE subject of this chapter is one which has been treated with wonderful ingenuity by Dr Whitehead,
to whom is due the whole conception of a method which arrives at "
points "
as systems of finitely-extended
events .
In advocating this method ,
it is not necessary to maintain that mathematical points are impossible as simple entities (
or "
particulars ");
all that it is necessary to maintain is that we have no good ground for regarding them as such .
What we know about points is that they are useful technically —
so useful that we must seek an interpretation of the propositions in which ,
symbolically ,
they occur .
But there is no ground for denying structure to a point ;
on the contrary ,
there are two grounds for assigning structure to a point .
One is the familiar argument of Occam's
razor :
we can make structures having the mathematical properties of points ,
and to suppose that there are points in any other sense is an inference which is useless to science and not warranted by any principle ,
logical or scientific .
The other argument is much more difficult to state ,
but the more one studies logical construction the more weight one feels inclined to attach to it .
It rests upon a maxim which might be enunciated as a supplement to Occam's
razor : "
What is logically convenient is likely to be artificial ."
To me personally ,
the first example of this maxim was the definition of real numbers .
Mathematicians found it convenient to suppose that all series of rationals have limits ,
while nevertheless [Pg 291]
some do not have rational limits .
They therefore postulated irrational limits ,
supposed to be homogeneous with the rationals .
Although the method of Dedekind
cuts was familiar ,
nobody thought of saying :
An irrational is a Dedekind
cut ,
or at least its inferior portion .
Yet this definition solves all difficulties .
We have now first ratios (
which cannot be irrational ),
then segments of the series of ratios .
Segments which have a limit are rational ,
segments which have no limit are irrational .
The square root of 2
is the class of ratios whose square is less than 2.
Segments of the series of ratios are real numbers the series of real numbers has both Dedekindian
and Cantorian
continuity .
Thus it is mathematically convenient ;
but its logical structure is more complex than that of the series of ratios .
The logical analysis of mathematics affords many examples of this procedure ,
such as the construction of "
ideal "
points ,
lines ,
and planes alluded to in Chapter XX.
It will be seen that the phrase "
what is logically convenient is artificial "
does not express what is meant with as much precision as is to be desired .
What we mean is this :
Given a set of terms having properties which suggest certain general mathematical (
or logical )
properties ,
but are subject to exceptions in regard to these properties ,
it is a mistake to postulate other terms ,
logically homogeneous with the original set ,
and such as to remove the exceptions ;
the proper procedure is to look for logical structures composed of the original terms ,
and such that these structures always have the mathematical properties in question .
It will be found that ,
where the assumption of such properties has proved fruitful ,
this procedure is usually possible .
Starting from events ,
there are many ways of reaching points .
One is the method adopted by Dr Whitehead,
in which we consider "enclosure-series."
Speaking roughly ,
we may say that this method defines a point as all the volumes [Pg 292]
which contain the point . (
The niceties of the method are required to prevent this definition from being circular ;
also to distinguish a set of volumes having only a point in common from such as have a line or surface in common .)
As a piece of logic ,
this method is faultless .
But as a method which aims at starting with the actual constituents of the world it seems to me to have certain defects . Dr Whitehead
assumes that every event encloses and is enclosed by other events .
There is ,
therefore ,
for him ,
no lower limit or minimum ,
and no upper limit or maximum ,
to the size of events .
Each of these assumptions demands consideration .
Let us begin with the absence of a lower limit or minimum .
Here we are confronted with a question of fact ,
which might conceivably be decided against Dr Whitehead,
but could not conceivably be decided in his favour .
The events which we can perceive all have a certain duration ,
i .
e .
they are simultaneous with events which are not simultaneous with each other .
Not only are they all ,
in this sense ,
finite ,
but they are all above an assignable limit .
I do not know what is the shortest perceptible event ,
but this is the sort of question which a psychological laboratory could answer .
We have not ,
therefore ,
direct empirical evidence that there is no minimum to events .
Nor can we have indirect empirical evidence ,
since a process which proceeds by very small finite differences is sensibly indistinguishable from a continuous process ,
as the cinema shows .
Per contra ,
there might be empirical evidence ,
as in the quantum theory ,
that events could not have less than a certain minimum spatio-temporal extent . Dr Whitehead's
assumption ,
therefore ,
seems rash .
At the same time ,
there is a confusion to be avoided :
space-time may be continuous even if there is a lower limit to events .
Suppose every elementary event filled a four-dimensional cube ,
e .g.
a cubic centimetre lasting for the time that light takes to travel a centimetre ;
and suppose ,
conversely ,
that every such four-dimensional [Pg 293]
cube was occupied by an event .
The space-time of such a world would be continuous ,
given suitable axioms ,
although events had a minimum .
And ,
conversely ,
the absence of a minimum to events does not insure spatio-temporal continuity .
The two questions are thus wholly distinct .
I conclude that there is at present no means of knowing whether events have a minimum or not ;
that there never can be conclusive evidence against their having a minimum ;
but that conceivably evidence may hereafter be found in favour of a minimum .
It remains to consider the question of a maximum .
On the question of a maximum to events ,
the arguments are rather logical than empirical .
In a certain sense ,
any series of events may be called one event ;
the Battle of Waterloo,
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