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194<br />

some structural components of a theory of experience<br />

Thus (2), i.e. the question When is n sufficiently long? has been<br />

reduced to (1′), i.e. the question When is ε small? (and vice versa).<br />

But this means that all three questions could be answered if only we<br />

could decide what particular value of ε is to be neglected as ‘negligibly<br />

small’. Now our methodo<strong>logic</strong>al rule amounts to the decision to<br />

neglect small values of ε; but we shall hardly be prepared to commit<br />

ourselves for ever to a definite value of ε.<br />

If we put our question to a physicist, that is, if we ask him what ε he<br />

is prepared to neglect—0.001, or 0.000001, or . . . ? he will presumably<br />

answer that ε does not interest him at all; that he has chosen not ε<br />

but n; and that he has chosen n in such a way as to make the correlation<br />

between n and ∆p largely independent of any changes of the value ε which we<br />

might choose to make.<br />

The physicist’s answer is justified, because of the mathematical peculiarities<br />

of the Bernoullian distribution: it is possible to determine for<br />

every n the functional dependence between ε and ∆p.* 4 An examination<br />

of this function shows that for every (‘large’) n there exists a<br />

characteristic value of ∆p such that in the neighbourhood of this value<br />

∆p is highly insensitive to changes of ε. This insensitiveness increases<br />

with increasing n. If we take an n of an order of magnitude which we<br />

should expect in the case of extreme mass-phenomena, then, in the<br />

neighbourhood of its characteristic value, ∆p is so highly insensitive<br />

to changes of ε that ∆p hardly changes at all even if the order of<br />

* 4 The remarks that follow in this paragraph (and some of the discussions later in this<br />

section) are, I now believe, clarified and superseded by the considerations in appendix<br />

*ix; see especially points 8 ff of my Third Note. With the help of the methods there used,<br />

it can be shown that almost all possible statistical samples of large size n will strongly<br />

undermine a given probabilistic hypothesis, that is to say give it a high negative degree of<br />

corroboration; and we may decide to interpret this as refutation or falsification. Of the<br />

remaining samples, most will support the hypothesis, that is to say, give it a high positive<br />

degree of corroboration. Comparatively few samples of large size n will give a probabilistic<br />

hypothesis an undecisive degree of corroboration (whether positive or negative).<br />

Thus we can expect to be able to refute a probabilistic hypothesis, in the sense here<br />

indicated; and we can expect this perhaps even more confidently than in the case of a<br />

non-probabilistic hypothesis. The methodo<strong>logic</strong>al rule or decision to regard (for a large<br />

n) a negative degree of corroboration as a falsification is, of course, a specific case of the<br />

methodo<strong>logic</strong>al rule or decision discussed in the present section—that of neglecting<br />

certain extreme improbabilities.

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