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CONTENTS1   INTRODUCTION2   TECHNICAL DEVELOPMENTS3   B-THEORY: EXPOSITION4   A-THEORY: EXPOSITION AND PARADOX5   ARGUMENTS FOR A-THEORY6 A-THEORY: REVISED EXPOSITION7 TIME AND ASSERTION8 THE PAST-FUTURE ASYMMETRY9 CONCLUSIONS8   THE PAST-FUTURE ASYMMETRYWe should
also resist the temptation to say that in A-theory the future is open,
indeterminate, while the past is closed, determined. It is essential to
A-theory that future tensed statements have determinate truth-value just
like present and past tensed statements, however hard the future truth-values
may be to know. The truth about the future that we try (in vain) to express
by saying that each future moment will, in due course, be present entails
the determinate nature of the truth-value of future tensed sentences.
It is the very truth-value that the corresponding present tensed sentences
will, in the fullness of time, have. This ontological result indicates
the way out of epistemological difficulties with the future. There is
a perfectly good method of finding out about the future, one which is
quite unavailable for the past. It is called the wait-and-see method.
All you have to do is stay alive long enough to find out was happens.
None of this
entails the world should be deterministic in the causal sense, whereby
the future is determined by the present. The truth-value of future tensed
sentences is determinate, because it is determined by the way things will
be. It may be that we can not know now what the future will be because
these things are presently strictly unknowable. The whole present world
may not “know” the future - which is a way of saying that the laws of
motion of the world are not deterministic - in which case no person within
that world can know the future. But we still know that there is some state
to be ascribed, using the future tense, to the world in the future (unless
sense can be made of the possibility that time might stop, beyond which
point there is no future). Similarly
the logical determinacy of the future does not preclude the possibility
of free action. It does not entail a logical fatalism. The tautology “Que
será, será” still leaves open the possibility that what will be will
have been the result of my free choice and action. Even if there were
an omniscient God who knew what I would choose long before I even existed
(I take it that the quantification in “omniscient” extends over all time
- a strongly B-theoretic notion), when it comes to the point of choosing
and causing the future state in question, the choice and the cause will
be mine. God, as omniscient, would have known that all along. Conversely
although the past seems fixed to us (and is logically determinate, in
a past tensed way), it can become epistemologically detached from us.
It is quite possible that all physical records of large parts of the past
have simply been, either in practice or indeed in principle, destroyed.
It may never be possible to know the colour of dinosaurs or the what Jesus
did as a child. With the lost past, le temps perdu, we do not even have the
wait-and-see method available for the future. (The question of the retention
or erasure of records of the past turns out to have important causal significance
in quantum mechanics.) There is
certainly an epistemological asymmetry between past and future which creates
the impression of closed past and open future. We are much better at remembering
the past than we are at anticipating the future. Certainly, our access
to the past is much enhanced now that we have a long tradition of keeping
records, and have developed the sciences of interpreting physical records.
After three millennia of continuous literacy, half a millennium of printing,
two centuries of systematic palaeontology and archaeology, and now living
in an age saturated with means of recording information, we perhaps underestimate
how difficult memory is to bare unaccommodated man. Nevertheless we have
made no such great strides in the technology of anticipation. Much of
the immediate future is opaque to us while the immediate past is documented
in minute detail. I conjecture
that this asymmetry derives from the fundamental asymmetry between Self
and Other. The Self is small and the Other is large. My knowledge of past
things derives from the influence the Other has on me. To know about the
Other I have to have received messages from it - this includes the limiting
case of that very particular Other, my past Self. Conversely I have knowledge
of the future precisely to the extent I can influence things. Suppose
I predict that in one minute’s time, the cup on my desk is going to move
into the kitchen. One minute later I carry the cup into the kitchen, and
claim a successful prediction. I am likely to be accused of cheating,
because I was the one who moved the cup, and at the time of making the
prediction I fully intended to move it. Instead of cheating, I am merely
demonstrating the circumstances under which I have reliable knowledge
of the future. Because the rest of the world is bigger than me, and influences
me more than I can influence it, I have a bigger store of this reliable
knowledge about the past than I have about the future. This attempt
to explain the epistemological asymmetry between past and future points
us towards the underlying asymmetry, that with respect to causation and
agency. When the world influences me, for example in a way which gives
me knowledge about it, then its past creates my future. When I influence
the world my past intentions create its future. I can not now bring about
the past because it is intrinsic to the notion of “bring about” that what
is being brought about is a future state. We can not say what “happening”
is, or what the past-future distinction is, but we can know that the two
are different aspects of the same thing. While the future is not open
in the logical sense, it is logical in the sense that, to the (strictly
limited) extent I can influence the world, I can choose the way I want
the future to be. There
is much talk among physicists, most of whom, if they think about the issue
at all, are incorrigible and unreflecting B-theorists, about the “Arrow
of Time”. The valid and important question of physics is whether physical
processes are reversible. Unfortunately this question is given the confusing
name of “time-reversal symmetry”, which suggests that what is at issue
is whether it is possible to travel backwards in time or not. If we speak
in slightly less tendentious terms of T-reversal, then the symmetry claim
in deterministic physics says that if a process A®B is possible, then so is B®A. In probabilistic physics the statement is that the two processes
have the same probability. If the symmetry does not hold, at least some
changes in the world will be irreversible. In the deterministic case,
once we go from A to B we can not get back. But in all cases, whether
the symmetry principle holds or not, the processes go from past to future
- as argued above, this is intrinsic to the notion of “process” and the
past-future distinction. Indeed, without a distinction between past and
future prior to any mention of the contents of time, the two processes
would be identical (i.e. there would actually be only one process) and
T-reversal symmetry would no longer be a substantive law of physics. Put another way, if the processes in my body were
T-reversed, in forty years time I would be a child again. I would be in
the same state I was in 1958, but the date would be 2038. This is quite
different from travelling back in time to 1958 - a notion, at least within
A-theory, of dubious coherence. Of course if the clocks were likewise
T-reversed, at the end of the process they would read “1958”, but, according
to A-theory, this very T-reversal would render them invalid as clocks.
In B-theory
by contrast there is no intrinsic direction to the temporal manifold.
We then have to look to the contents of the manifold to give it an extrinsic
direction. If for example we have an asymmetry in the way thermodynamic
processes change the entropy of an isolated system, we can use this as
an extrinsic “arrow of time” and say that the higher entropy states are
later than the lower entropy ones. In this case the principle of entropy
increase is not a law of physics, but rather a definition of the time-ordering
word “increase”. Of course in the world of our experience, away from the
fancies of B-theory, we start with a past-future asymmetry, and then notice
that the higher entropy states are always later, as a contingent law of
physics. 9 CONCLUSIONThe strongest
argument to this conclusion is that of McTaggart. When we try to express
the things which we experience to be true of temporal passage, we encounter
contradictions. McTaggart concluded that time, which he identified with
passage must be unreal. The problem
with McTaggart’s argument is that it proves to much. If valid, it proves
that even the illusion of passage is impossible. The sensation of passage,
at least as an illusion, is one of the most fundamental and intimate parts
of our experience. If this were unreliable as a source of knowledge then
we could rely on nothing. Therefore there must be a way around McTaggart’s
argument. The conclusion
argued for here is that what McTaggart has in fact shown is that there
exists a fundamental limitation on our ability to express the known truths
about time in language. This result is quite as startling as McTaggart’s
own conclusion that time is unreal. I conjecture that time is an example
of a “radical multiplicity”, the existence of which prevents us using
the normal assertoric mechanisms of language. We know the facts about
passage as well as we can know anything, and can point to them using words,
but we can not use words to express this knowledge as articulated understanding.
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The other argument against
the physical reality of passage is that from Special Relativity. The argument
from experience shows that there must be a way to reconcile our experience
with relativistic reality, but producing such a reconciliation is a task
left to another essay. Click here to return to the start of the essay.
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