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Assuming that there is physical space, and that it does thus correspond |
to private spaces, what can we know about it? We can know _only_ what is |
required in order to secure the correspondence. That is to say, we can |
know nothing of what it is like in itself, but we can know the sort |
of arrangement of physical objects which results from their spatial |
relations. We can know, for example, that the earth and moon and sun |
are in one straight line during an eclipse, though we cannot know what |
a physical straight line is in itself, as we know the look of a straight |
line in our visual space. Thus we come to know much more about the |
_relations_ of distances in physical space than about the distances |
themselves; we may know that one distance is greater than another, or |
that it is along the same straight line as the other, but we cannot have |
that immediate acquaintance with physical distances that we have with |
distances in our private spaces, or with colours or sounds or other |
sense-data. We can know all those things about physical space which a |
man born blind might know through other people about the space of sight; |
but the kind of things which a man born blind could never know about the |
space of sight we also cannot know about physical space. We can know the |
properties of the relations required to preserve the correspondence with |
sense-data, but we cannot know the nature of the terms between which the |
relations hold. |
With regard to time, our _feeling_ of duration or of the lapse of time |
is notoriously an unsafe guide as to the time that has elapsed by the |
clock. Times when we are bored or suffering pain pass slowly, times when |
we are agreeably occupied pass quickly, and times when we are sleeping |
pass almost as if they did not exist. Thus, in so far as time is |
constituted by duration, there is the same necessity for distinguishing |
a public and a private time as there was in the case of space. But in so |
far as time consists in an _order_ of before and after, there is no need |
to make such a distinction; the time-order which events seem to have is, |
so far as we can see, the same as the time-order which they do have. At |
any rate no reason can be given for supposing that the two orders are |
not the same. The same is usually true of space: if a regiment of men |
are marching along a road, the shape of the regiment will look different |
from different points of view, but the men will appear arranged in the |
same order from all points of view. Hence we regard the order as true |
also in physical space, whereas the shape is only supposed to correspond |
to the physical space so far as is required for the preservation of the |
order. |
In saying that the time-order which events seem to have is the same as |
the time-order which they really have, it is necessary to guard against |
a possible misunderstanding. It must not be supposed that the various |
states of different physical objects have the same time-order as the |
sense-data which constitute the perceptions of those objects. Considered |
as physical objects, the thunder and lightning are simultaneous; that is |
to say, the lightning is simultaneous with the disturbance of the air in |
the place where the disturbance begins, namely, where the lightning |
is. But the sense-datum which we call hearing the thunder does not take |
place until the disturbance of the air has travelled as far as to where |
we are. Similarly, it takes about eight minutes for the sun's light |
to reach us; thus, when we see the sun we are seeing the sun of eight |
minutes ago. So far as our sense-data afford evidence as to the physical |
sun they afford evidence as to the physical sun of eight minutes ago; if |
the physical sun had ceased to exist within the last eight minutes, that |
would make no difference to the sense-data which we call 'seeing |
the sun'. This affords a fresh illustration of the necessity of |
distinguishing between sense-data and physical objects. |
What we have found as regards space is much the same as what we find |
in relation to the correspondence of the sense-data with their |
physical counterparts. If one object looks blue and another red, we may |
reasonably presume that there is some corresponding difference between |
the physical objects; if two objects both look blue, we may presume a |
corresponding similarity. But we cannot hope to be acquainted directly |
with the quality in the physical object which makes it look blue or red. |
Science tells us that this quality is a certain sort of wave-motion, and |
this sounds familiar, because we think of wave-motions in the space we |
see. But the wave-motions must really be in physical space, with which |
we have no direct acquaintance; thus the real wave-motions have not that |
familiarity which we might have supposed them to have. And what holds |
for colours is closely similar to what holds for other sense-data. Thus |
we find that, although the _relations_ of physical objects have all |
sorts of knowable properties, derived from their correspondence with the |
relations of sense-data, the physical objects themselves remain unknown |
in their intrinsic nature, so far at least as can be discovered by means |
of the senses. The question remains whether there is any other method of |
discovering the intrinsic nature of physical objects. |
The most natural, though not ultimately the most defensible, hypothesis |
to adopt in the first instance, at any rate as regards visual |
sense-data, would be that, though physical objects cannot, for the |
reasons we have been considering, be _exactly_ like sense-data, yet they |
may be more or less like. According to this view, physical objects will, |
for example, really have colours, and we might, by good luck, see an |
object as of the colour it really is. The colour which an object seems |
to have at any given moment will in general be very similar, though |
not quite the same, from many different points of view; we might thus |
suppose the 'real' colour to be a sort of medium colour, intermediate |
between the various shades which appear from the different points of |
view. |
Such a theory is perhaps not capable of being definitely refuted, but |
it can be shown to be groundless. To begin with, it is plain that the |
colour we see depends only upon the nature of the light-waves that |
strike the eye, and is therefore modified by the medium intervening |
between us and the object, as well as by the manner in which light is |
reflected from the object in the direction of the eye. The intervening |
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