Among the objections to the reality of objects of sense, there is one

which is derived from the apparent difference between matter as it

appears in physics and things as they appear in sensation. Men of

science, for the most part, are willing to condemn immediate data as

"merely subjective," while yet maintaining the truth of the physics

inferred from those data. But such an attitude, though it may be

_capable_ of justification, obviously stands in need of it; and the only

justification possible must be one which exhibits matter as a logical

construction from sense-data--unless, indeed, there were some wholly _a

priori_ principle by which unknown entities could be inferred from such

as are known. It is therefore necessary to find some way of bridging the

gulf between the world of physics and the world of sense, and it is this

problem which will occupy us in the present lecture. Physicists appear

to be unconscious of the gulf, while psychologists, who are conscious of

it, have not the mathematical knowledge required for spanning it. The

problem is difficult, and I do not know its solution in detail. All that

I can hope to do is to make the problem felt, and to indicate the kind

of methods by which a solution is to be sought.

Let us begin by a brief description of the two contrasted worlds. We

will take first the world of physics, for, though the other world is

given while the physical world is inferred, to us now the world of

physics is the more familiar, the world of pure sense having become

strange and difficult to rediscover. Physics started from the

common-sense belief in fairly permanent and fairly rigid bodies--tables

and chairs, stones, mountains, the earth and moon and sun. This

common-sense belief, it should be noticed, is a piece of audacious

metaphysical theorising; objects are not continually present to

sensation, and it may be doubted whether they are there when they are

not seen or felt. This problem, which has been acute since the time of

Berkeley, is ignored by common sense, and has therefore hitherto been

ignored by physicists. We have thus here a first departure from the

immediate data of sensation, though it is a departure merely by way of

extension, and was probably made by our savage ancestors in some very

remote prehistoric epoch.

But tables and chairs, stones and mountains, are not _quite_ permanent

or _quite_ rigid. Tables and chairs lose their legs, stones are split by

frost, and mountains are cleft by earthquakes and eruptions. Then there

are other things, which seem material, and yet present almost no

permanence or rigidity. Breath, smoke, clouds, are examples of such

things--so, in a lesser degree, are ice and snow; and rivers and seas,

though fairly permanent, are not in any degree rigid. Breath, smoke,

clouds, and generally things that can be seen but not touched, were

thought to be hardly real; to this day the usual mark of a ghost is that

it can be seen but not touched. Such objects were peculiar in the fact

that they seemed to disappear completely, not merely to be transformed

into something else. Ice and snow, when they disappear, are replaced by

water; and it required no great theoretical effort to invent the

hypothesis that the water was the same thing as the ice and snow, but in

a new form. Solid bodies, when they break, break into parts which are

practically the same in shape and size as they were before. A stone can

be hammered into a powder, but the powder consists of grains which

retain the character they had before the pounding. Thus the ideal of

absolutely rigid and absolutely permanent bodies, which early physicists

pursued throughout the changing appearances, seemed attainable by

supposing ordinary bodies to be composed of a vast number of tiny atoms.

This billiard-ball view of matter dominated the imagination of

physicists until quite modern times, until, in fact, it was replaced by

the electromagnetic theory, which in its turn is developing into a new

atomism. Apart from the special form of the atomic theory which was

invented for the needs of chemistry, some kind of atomism dominated the

whole of traditional dynamics, and was implied in every statement of its

laws and axioms.

The pictorial accounts which physicists give of the material world as

they conceive it undergo violent changes under the influence of

modifications in theory which are much slighter than the layman might

suppose from the alterations of the description. Certain features,

however, have remained fairly stable. It is always assumed that there is

_something_ indestructible which is capable of motion in space; what is

indestructible is always very small, but does not always occupy a mere

point in space. There is supposed to be one all-embracing space in which

the motion takes place, and until lately we might have assumed one

all-embracing time also. But the principle of relativity has given

prominence to the conception of "local time," and has somewhat

diminished men's confidence in the one even-flowing stream of time.

Without dogmatising as to the ultimate outcome of the principle of

relativity, however, we may safely say, I think, that it does not

destroy the possibility of correlating different local times, and does

not therefore have such far-reaching philosophical consequences as is

sometimes supposed. In fact, in spite of difficulties as to measurement,

the one all-embracing time still, I think, underlies all that physics

has to say about motion. We thus have still in physics, as we had in

Newton's time, a set of indestructible entities which may be called

particles, moving relatively to each other in a single space and a

single time.

The world of immediate data is quite different from this. Nothing is

permanent; even the things that we think are fairly permanent, such as

mountains, only become data when we see them, and are not immediately

given as existing at other moments. So far from one all-embracing space

being given, there are several spaces for each person, according to the

different senses which give relations that may be called spatial.

Experience teaches us to obtain one space from these by correlation, and

experience, together with instinctive theorising, teaches us to

correlate our spaces with those which we believe to exist in the

sensible worlds of other people. The construction of a single time

offers less difficulty so long as we confine ourselves to one person's

private world, but the correlation of one private time with another is a

matter of great difficulty. Thus, apart from any of the fluctuating

hypotheses of physics, three main problems arise in connecting the world

of physics with the world of sense, namely (1) the construction of

permanent "things," (2) the construction of a single space, and (3) the

construction of a single time. We will consider these three problems in

succession.

(1) The belief in indestructible "things" very early took the form of

atomism. The underlying motive in atomism was not, I think, any

empirical success in interpreting phenomena, but rather an instinctive

belief that beneath all the changes of the sensible world there must be

something permanent and unchanging. This belief was, no doubt, fostered

and nourished by its practical successes, culminating in the

conservation of mass; but it was not produced by these successes. On the

contrary, they were produced by it. Philosophical writers on physics

sometimes speak as though the conservation of something or other were

essential to the possibility of science, but this, I believe, is an

entirely erroneous opinion. If the _a priori_ belief in permanence had

not existed, the same laws which are now formulated in terms of this

belief might just as well have been formulated without it. Why should we

suppose that, when ice melts, the water which replaces it is the same

thing in a new form? Merely because this supposition enables us to state

the phenomena in a way which is consonant with our prejudices. What we

really know is that, under certain conditions of temperature, the

appearance we call ice is replaced by the appearance we call water. We

can give laws according to which the one appearance will be succeeded by

the other, but there is no reason except prejudice for regarding both as

appearances of the same substance.

One task, if what has just been said is correct, which confronts us in

trying to connect the world of sense with the world of physics, is the

task of reconstructing the conception of matter without the _a priori_

beliefs which historically gave rise to it. In spite of the

revolutionary results of modern physics, the empirical successes of the

conception of matter show that there must be some legitimate conception

which fulfils roughly the same functions. The time has hardly come when

we can state precisely what this legitimate conception is, but we can

see in a general way what it must be like. For this purpose, it is only

necessary to take our ordinary common-sense statements and reword them

without the assumption of permanent substance. We say, for example, that

things change gradually--sometimes very quickly, but not without passing

through a continuous series of intermediate states. What this means is

that, given any sensible appearance, there will usually be, _if we

watch_, a continuous series of appearances connected with the given one,

leading on by imperceptible gradations to the new appearances which

common-sense regards as those of the same thing. Thus a thing may be

defined as a certain series of appearances, connected with each other by

continuity and by certain causal laws. In the case of slowly changing

things, this is easily seen. Consider, say, a wall-paper which fades in

the course of years. It is an effort not to conceive of it as one

"thing" whose colour is slightly different at one time from what it is

at another. But what do we really _know_ about it? We know that under

suitable circumstances--_i.e._ when we are, as is said, "in the

room"--we perceive certain colours in a certain pattern: not always

precisely the same colours, but sufficiently similar to feel familiar.

If we can state the laws according to which the colour varies, we can

state all that is empirically verifiable; the assumption that there is a

constant entity, the wall-paper, which "has" these various colours at

various times, is a piece of gratuitous metaphysics. We may, if we like,

_define_ the wall-paper as the series of its aspects. These are

collected together by the same motives which led us to regard the

wall-paper as one thing, namely a combination of sensible continuity and

causal connection. More generally, a "thing" will be defined as a

certain series of aspects, namely those which would commonly be said to

be _of_ the thing. To say that a certain aspect is an aspect _of_ a

certain thing will merely mean that it is one of those which, taken

serially, _are_ the thing. Everything will then proceed as before:

whatever was verifiable is unchanged, but our language is so interpreted

as to avoid an unnecessary metaphysical assumption of permanence.

The above extrusion of permanent things affords an example of the maxim

which inspires all scientific philosophising, namely "Occam's razor":

_Entities are not to be multiplied without necessity._ In other words,

in dealing with any subject-matter, find out what entities are

undeniably involved, and state everything in terms of these entities.

Very often the resulting statement is more complicated and difficult

than one which, like common sense and most philosophy, assumes

hypothetical entities whose existence there is no good reason to believe

in. We find it easier to imagine a wall-paper with changing colours than

to think merely of the series of colours; but it is a mistake to suppose

that what is easy and natural in thought is what is most free from

unwarrantable assumptions, as the case of "things" very aptly

illustrates.

The above summary account of the genesis of "things," though it may be

correct in outline, has omitted some serious difficulties which it is

necessary briefly to consider. Starting from a world of helter-skelter

sense-data, we wish to collect them into series, each of which can be

regarded as consisting of the successive appearances of one "thing."

There is, to begin with, some conflict between what common sense regards

as one thing, and what physics regards an unchanging collection of

particles. To common sense, a human body is one thing, but to science

the matter composing it is continually changing. This conflict, however,

is not very serious, and may, for our rough preliminary purpose, be

largely ignored. The problem is: by what principles shall we select

certain data from the chaos, and call them all appearances of the same

thing?

A rough and approximate answer to this question is not very difficult.

There are certain fairly stable collections of appearances, such as

landscapes, the furniture of rooms, the faces of acquaintances. In these

cases, we have little hesitation in regarding them on successive

occasions as appearances of one thing or collection of things. But, as

the _Comedy of Errors_ illustrates, we may be led astray if we judge by

mere resemblance. This shows that something more is involved, for two

different things may have any degree of likeness up to exact similarity.

Another insufficient criterion of one thing is _continuity_. As we have

already seen, if we watch what we regard as one changing thing, we

usually find its changes to be continuous so far as our senses can

perceive. We are thus led to assume that, if we see two finitely

different appearances at two different times, and if we have reason to

regard them as belonging to the same thing, then there was a continuous

series of intermediate states of that thing during the time when we were

not observing it. And so it comes to be thought that continuity of

change is necessary and sufficient to constitute one thing. But in fact

it is neither. It is not _necessary_, because the unobserved states, in

the case where our attention has not been concentrated on the thing

throughout, are purely hypothetical, and cannot possibly be our ground

for supposing the earlier and later appearances to belong to the same

thing; on the contrary, it is because we suppose this that we assume

intermediate unobserved states. Continuity is also not sufficient, since

we can, for example, pass by sensibly continuous gradations from any one

drop of the sea to any other drop. The utmost we can say is that

discontinuity during uninterrupted observation is as a rule a mark of

difference between things, though even this cannot be said in such cases

as sudden explosions.

The assumption of continuity is, however, successfully made in physics.

This proves something, though not anything of very obvious utility to

our present problem: it proves that nothing in the known world is

inconsistent with the hypothesis that all changes are really continuous,

though from too great rapidity or from our lack of observation they may

not always appear continuous. In this hypothetical sense, continuity may

be allowed to be a _necessary_ condition if two appearances are to be

classed as appearances of the same thing. But it is not a _sufficient_

condition, as appears from the instance of the drops in the sea. Thus

something more must be sought before we can give even the roughest

definition of a "thing."

What is wanted further seems to be something in the nature of fulfilment

of causal laws. This statement, as it stands, is very vague, but we will

endeavour to give it precision. When I speak of "causal laws," I mean

any laws which connect events at different times, or even, as a limiting

case, events at the same time provided the connection is not logically

demonstrable. In this very general sense, the laws of dynamics are

causal laws, and so are the laws correlating the simultaneous

appearances of one "thing" to different senses. The question is: How do

such laws help in the definition of a "thing"?

To answer this question, we must consider what it is that is proved by

the empirical success of physics. What is proved is that its hypotheses,

though unverifiable where they go beyond sense-data, are at no point in

contradiction with sense-data, but, on the contrary, are ideally such as

to render all sense-data calculable from a sufficient collection of data

all belonging to a given period of time. Now physics has found it

empirically possible to collect sense-data into series, each series

being regarded as belonging to one "thing," and behaving, with regard to

the laws of physics, in a way in which series not belonging to one thing

would in general not behave. If it is to be unambiguous whether two

appearances belong to the same thing or not, there must be only one way

of grouping appearances so that the resulting things obey the laws of

physics. It would be very difficult to prove that this is the case, but

for our present purposes we may let this point pass, and assume that

there is only one way. We must include in our definition of a "thing"

those of its aspects, if any, which are not observed. Thus we may lay

down the following definition: _Things are those series of aspects which

obey the laws of physics._ That such series exist is an empirical fact,

which constitutes the verifiability of physics.

It may still be objected that the "matter" of physics is something other

than series of sense-data. Sense-data, it may be said, belong to

psychology and are, at any rate in some sense, subjective, whereas

physics is quite independent of psychological considerations, and does

not assume that its matter only exists when it is perceived.

To this objection there are two answers, both of some importance.

(a) We have been considering, in the above account, the question of the

_verifiability_ of physics. Now verifiability is by no means the same

thing as truth; it is, in fact, something far more subjective and

psychological. For a proposition to be verifiable, it is not enough that

it should be true, but it must also be such as we can _discover_ to be

true. Thus verifiability depends upon our capacity for acquiring

knowledge, and not only upon the objective truth. In physics, as

ordinarily set forth, there is much that is unverifiable: there are

hypotheses as to (A) how things would appear to a spectator in a place

where, as it happens, there is no spectator; (B) how things would appear

at times when, in fact, they are not appearing to anyone; (C) things

which never appear at all. All these are introduced to simplify the

statement of the causal laws, but none of them form an integral part of

what is _known_ to be true in physics. This brings us to our second

answer.

(b) If physics is to consist wholly of propositions known to be true, or

at least capable of being proved or disproved, the three kinds of

hypothetical entities we have just enumerated must all be capable of

being exhibited as logical functions of sense-data. In order to show how

this might possibly be done, let us recall the hypothetical Leibnizian

universe of Lecture III. In that universe, we had a number of

perspectives, two of which never had any entity in common, but often

contained entities which could be sufficiently correlated to be regarded

as belonging to the same thing. We will call one of these an "actual"

private world when there is an actual spectator to which it appears, and

"ideal" when it is merely constructed on principles of continuity. A

physical thing consists, at each instant, of the whole set of its

aspects at that instant, in all the different worlds; thus a momentary

state of a thing is a whole set of aspects. An "ideal" appearance will

be an aspect merely calculated, but not actually perceived by any

spectator. An "ideal" state of a thing will be a state at a moment when

all its appearances are ideal. An ideal thing will be one whose states

at all times are ideal. Ideal appearances, states, and things, since

they are calculated, must be functions of actual appearances, states,

and things; in fact, ultimately, they must be functions of actual

appearances. Thus it is unnecessary, for the enunciation of the laws of

physics, to assign any reality to ideal elements: it is enough to accept

them as logical constructions, provided we have means of knowing how to

determine when they become actual. This, in fact, we have with some

degree of approximation; the starry heaven, for instance, becomes actual

whenever we choose to look at it. It is open to us to believe that the

ideal elements exist, and there can be no reason for _dis_believing

this; but unless in virtue of some _a priori_ law we cannot _know_ it,

for empirical knowledge is confined to what we actually observe.

(2) The three main conceptions of physics are space, time, and matter.

Some of the problems raised by the conception of matter have been

indicated in the above discussion of "things." But space and time also

raise difficult problems of much the same kind, namely, difficulties in

reducing the haphazard untidy world of immediate sensation to the smooth

orderly world of geometry and kinematics. Let us begin with the

consideration of space.

People who have never read any psychology seldom realise how much mental

labour has gone into the construction of the one all-embracing space

into which all sensible objects are supposed to fit. Kant, who was

unusually ignorant of psychology, described space as "an infinite given

whole," whereas a moment's psychological reflection shows that a space

which is infinite is not given, while a space which can be called given

is not infinite. What the nature of "given" space really is, is a

difficult question, upon which psychologists are by no means agreed. But

some general remarks may be made, which will suffice to show the

problems, without taking sides on any psychological issue still in

debate.

The first thing to notice is that different senses have different

spaces. The space of sight is quite different from the space of touch:

it is only by experience in infancy that we learn to correlate them. In

later life, when we see an object within reach, we know how to touch it,

and more or less what it will feel like; if we touch an object with our

eyes shut, we know where we should have to look for it, and more or less

what it would look like. But this knowledge is derived from early

experience of the correlation of certain kinds of touch-sensations with

certain kinds of sight-sensations. The one space into which both kinds

of sensations fit is an intellectual construction, not a datum. And

besides touch and sight, there are other kinds of sensation which give

other, though less important spaces: these also have to be fitted into

the one space by means of experienced correlations. And as in the case

of things, so here: the one all-embracing space, though convenient as a

way of speaking, need not be supposed really to exist. All that

experience makes certain is the several spaces of the several senses,

correlated by empirically discovered laws. The one space may turn out to

be valid as a logical construction, compounded of the several spaces,

but there is no good reason to assume its independent metaphysical

reality.

Another respect in which the spaces of immediate experience differ from

the space of geometry and physics is in regard to _points_. The space of

geometry and physics consists of an infinite number of points, but no

one has ever seen or touched a point. If there are points in a sensible

space, they must be an inference. It is not easy to see any way in

which, as independent entities, they could be validly inferred from the

data; thus here again, we shall have, if possible, to find some logical

construction, some complex assemblage of immediately given objects,

which will have the geometrical properties required of points. It is

customary to think of points as simple and infinitely small, but

geometry in no way demands that we should think of them in this way. All

that is necessary for geometry is that they should have mutual relations

possessing certain enumerated abstract properties, and it may be that an

assemblage of data of sensation will serve this purpose. Exactly how

this is to be done, I do not yet know, but it seems fairly certain that

it can be done.

Our Knowledge of the External World as a Field for Scientific Method in Philosophy · 第 7 / 17 段