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popper-logic-scientific-discovery

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192<br />

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

being given a criterion of what is to be called ‘long’, we cannot know<br />

when, or whether, we have reached an approximation to the<br />

probability.<br />

(3) How can we know that the desired approximation has in fact been<br />

reached?<br />

Although I believe that these objections are justified, I nevertheless<br />

believe that we can retain the physicist’s definition. I shall support this<br />

belief by the arguments outlined in the previous section. These showed<br />

that probability hypotheses lose all informative content when they are<br />

allowed unlimited application. The physicist would never use them in<br />

this way. Following his example I shall disallow the unlimited application<br />

of probability hypotheses: I propose that we take the methodo<strong>logic</strong>al<br />

decision never to explain physical effects, i.e. reproducible regularities, as accumulations of<br />

accidents. This decision naturally modifies the concept of probability: it<br />

narrows it.* 2 Thus objection (1) does not affect my position, for I do<br />

not assert the identity of the physical and the mathematical concepts of<br />

probability at all; on the contrary, I deny it. But in place of (1), a new<br />

objection arises.<br />

(1′) When can we speak of ‘accumulated accidents’? Presumably in<br />

the case of a small probability. But when is a probability ‘small’? We<br />

may take it that the proposal which I have just submitted rules out the<br />

use of the method (discussed in the preceding section) of manufacturing<br />

an arbitrarily large probability out of a small one by changing the<br />

formulation of the mathematical problem. But in order to carry out the<br />

proposed decision, we have to know what we are to regard as small.<br />

In the following pages it will be shown that the proposed methodo<strong>logic</strong>al<br />

rule agrees with the physicist’s definition, and that the objections<br />

raised by questions (1′), (2), and (3) can be answered with its<br />

help. To begin with, I have in mind only one typical case of the application<br />

of the calculus of probability: I have in mind the case of certain<br />

reproducible macro effects which can be described with the help of<br />

precise (macro) laws—such as gas pressure—and which we interpret,<br />

or explain, as due to a very large accumulation of micro processes, such<br />

* 2 The methodo<strong>logic</strong>al decision or rule here formulated narrows the concept of<br />

probability—just as it is narrowed by the decision to adopt shortest random-like sequences<br />

as mathematical models of empirical sequences, cf. note *1 to section 65.

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