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popper-logic-scientific-discovery

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(1,1)<br />

N(α.β.γ)<br />

N(α)<br />

N(α.β) N(α.β.γ)<br />

= ·<br />

N(α) N(α.β)<br />

which proves to be an identity after cancellation of ‘N(α.β)’. (Contrast<br />

with this proof, and with the proof of (2 s), by Reichenbach in<br />

Mathematische Zeitschrift 34, p. 593.)<br />

If we assume independence (cf. section 53), i.e.<br />

(1 s )<br />

α.βF″(γ) = αF″(γ)<br />

we obtain from (1) the special multiplication theorem<br />

(1 s)<br />

αF″(β.γ) = αF″(β). αF″(γ)<br />

With the help of the equivalence of (1) and (1′), the symmetry of the<br />

relation of independence can be proved (cf. note 4 to section 53).<br />

The addition theorems deal with the frequency of those elements which<br />

belong either to β or to γ. If we denote the disjunctive combination<br />

bination of these classes by the symbol ‘β + γ’, where the sign ‘ + ’, if<br />

placed between class designations, signifies not arithmetical addition but the<br />

non-exclusive ‘or’, then the general addition theorem is:<br />

(2)<br />

αF″(β + γ) = αF″(β) + αF″(γ) − αF″(β.γ)<br />

This statement follows from the definition in section 52 if we use<br />

the universally valid formula of the calculus of classes<br />

(2,2)<br />

α.(β + γ) = (α.β) + (α.γ),<br />

and the formula (which is also universally valid)<br />

(2,1)<br />

N(β + γ) = N(β) + N(γ) − N(β.γ)<br />

Under the assumption that, within α, β and γ have no member in<br />

common—a condition which can be symbolized by the formula<br />

(2 s )<br />

N(α.β.γ) = 0<br />

appendix ii 287

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