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and (see page 346)<br />

(3)<br />

a = lim a<br />

n →∞<br />

n<br />

p(a) = limp(a<br />

n →∞<br />

n )<br />

It is clear that we may interpret a n as the assertion that, within the finite<br />

sequence of elements k 1, k 2, ... k n, all elements possess the property A. This<br />

makes it easy to apply the classical definition to the evaluation of p(a n ).<br />

There is only one possibility that is favourable to the assertion a n : it is the<br />

possibility that all the n individuals, k i without exception, possess the<br />

property A rather than the property non-A. But there are in all 2 n<br />

possibilities, since we must assume that it is possible for any individual<br />

k i, either to possess the property A or the property non-A. Accordingly,<br />

the classical theory gives<br />

(4 c )<br />

p(a n ) = 1/2 n<br />

appendix *vii 377<br />

But from (3) and (4 c ), we obtain immediately (1).<br />

The ‘classical’ argument leading to (4 c ) is not entirely adequate,<br />

although it is, I believe, essentially correct.<br />

The inadequacy lies merely in the assumption that A and non-A are<br />

equally probable. For it may be argued—correctly, I believe—that since<br />

a is supposed to describe a law of nature, the various a i are instantiation<br />

statements, and thus more probable than their negations which are<br />

potential falsifiers. (Cf. note *1 to section 28). This objection however,<br />

relates to an inessential part of the argument. For whatever<br />

probability—short of unity—we attribute to A, the infinite product a<br />

will have zero probability (assuming independence, which will be<br />

discussed later on). Indeed, we have struck here a particularly trivial<br />

case of the one-or-zero law of probability (which we may also call, with an<br />

allusion to neuro-physiology, ‘the all-or-nothing principle’). In this<br />

case it may be formulated thus: if a is the infinite product of a 1, a 2, ...,<br />

where p(a i) = p(a j), and where every a i is independent of all others, then<br />

the following holds:

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