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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 CONCLUSIONS
2   TECHNICAL DEVELOPMENTSBefore developing the two
rival theories, it is useful to clarify the issues by making some simple
technical developments. The first is to generalise McTaggart’s two qualitative
series. Both of them can be extended to quantitative series with the structure
of the real line: A-series: x
seconds ago - now - in x
seconds time B-series: x
seconds earlier than - simultaneous with - x
seconds later than
for all real
x greater than zero. Since McTaggart initially
introduces the A-series as “that series of positions which runs from the
far past through the near past to the present, and then from the present
through the near future to the far future ...”, this generalisation to
a continuous series is consistent with the development of his thoughts
about time. By using
zero and negative reals we can reduce the terms in each series to a single
family of terms parametrised by real numbers: for
all positive x
: x seconds ago = in
(-x) seconds time , and x seconds earlier than = (-x) seconds later than ; now = in
0 seconds time simultaneous
with =
0 seconds later than. The second
terms in each of the series is just the same as the corresponding item
in the original qualitative series. The first and third terms in the qualitative
series can be reconstructed using the operation of continuous disjunction
- if coherent sense can be made of this operation. Informally at least,
we can write, for example future =
and similarly
for “past”, “earlier than” and “later than”. Next we have to look in more detail at what the
terms in each series actually are. They appear in the form of one-place
predicates (A-series) or two-place predicates (B-series). The expressions
which go in their argument places are the names of events. Let us introduce
the following abbreviated notation for each of these. Tense-xs (x) = x occurs in x seconds time Later-xs (x,h) = x occurs x seconds
later than h. It is a simple
matter within B-theory to produce a family of one-place predicates referring
to events, analogous to the tenses of A-theory. Once chooses an arbitrary
event to be the zero of our calendar, and defines the attribution of a
date to an event relative to this choice of calendar as: If one starts
B-theory from dates, then the “later” relation can be reconstructed from
the difference between the dates, a feature which is calendar independent.
It is worth noting at this point that here we
have used the words “tense” and “date” with senses somewhat generalised
from their usage in normal English. Normally we use the word “tense” to
denote the three forms of the verb, corresponding to the three terms in
McTaggart’s original qualitative A-series. Here we have made two changes.
The first is replacing the three tenses by a continuum of them. The second
is interpreting the verb modification in terms of a predicate qualifying
event names. In normal English the word “date” is reserved for a location
in time with a limit of resolution of a day, and is expressed in terms
of day-of-the-month, month-of-the-year and year. Any finer resolution
is expressed in terms of time-of-day, denominated in yet other units.
This conventional representation can readily be replaced by a single scale
denominated in a single unit. The choice of the word “date” for this single
measure is a little eccentric, but the more natural English choice, “time”,
is a word whose usage is so badly ambiguous that it cannot have a place
in serious philosophical analysis. For example, when talking about “the
A-theory of time”, the word “time” refers vaguely to the generality of
temporal phenomena. This analysis
exposes a fundamental difference between A- and B-theory. In the latter
the choice of a zero for the calendar is arbitrary. The fundamental items
in the theory are the temporal relations between events. In A-theory the
zero, namely the present, is a fundamental feature of reality. But trying
to say just what this feature is leads us to McTaggart’s paradox. How
this happens, and how we can escape paradox is the main subject matter
of this essay. Before proceeding
though, it should be noted that what has been given above is one particular
Fregean analysis of temporal statements. It is the one suggested most
directly by the choice of terms in the original McTaggart series, and
has been adopted here entirely uncritically. Whether it is the correct
analysis, and whether therefore we are right to adopt the concomitant
ontology of events, is a serious question, which is beyond the scope of
the present essay, apart from the comment that while the ontology of events
is natural for B-theory, it is far more problematic in the A-theoretic
context. This separation of issues is based on the assumption that the
two issues: A-theory versus B-theory, and the Fregean analysis of temporal
expressions, can be solved independently of each other, and more specifically
that if one can solve the problem raised by McTaggart’s paradox using
this analysis, then the solution can be transferred to another one. Yet another
matter of Fregean analysis should also be mentioned. When we have a family
of predicates with the structure of the real line (except the multiplicative
identity, and in some cases without the additive identity as well), can
we continue the analysis and extract the name of the real numbers? Are
we then committed to an ontology of numbers? These questions are not exclusive
to the philosophy of time, but arise generally whenever real-valued quantities
occur in physics.
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