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Probability and Relative Frequency

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Abstract

The concept of probability seems to have been inexplicable since its invention in the seventeenth century. In its use in science, probability is closely related with relative frequency. So the task seems to be interpreting that relation. In this paper, we start with predicted relative frequency and show that its structure is the same as that of probability. I propose to call that the ‘prediction interpretation’ of probability. The consequences of that definition are discussed. The “ladder”-structure of the probability calculus is analyzed. The expectation of the relative frequency is shown to be equal to the predicted relative frequency. Probability is shown to be the most general empirically testable prediction.

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Notes

  1. I am grateful for many suggestions from the work of and discussions with von Weizsäcker. He introduced the idea of the importance of the structure of time for philosophy in general and especially for the philosophy of physics, as well as the idea of probability being the quantification of possibility, and possibility in turn relating to the future. Cf. the collections of texts [5, 6]; cf. also [7].

  2. von Weizsäcker calls that an ‘n-fold alternative’. This is actually a very general way of characterizing a (finite) observable as it is used in physics.

  3. cf. Appendix.

References

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  2. Kolmogoroff, A.N.: Grundbegriffe der Wahrscheinlichkeitsrechnung. Springer, Berlin (1933)

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  5. von Weizsäcker, C.F.: The Unity of Physics. Farrar/Straus/Giroux, New York (1971)

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Correspondence to Michael Drieschner.

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This paper deals with the philosophical question of how probability and relative frequency are related in empirical science. Its main point will be introducing and making plausible the “prediction interpretation” of probability. I will not ask any of the questions discussed today about objectivity or empirical sources or admissible distributions of probability, etc. The purpose of this paper is rather making clear the importance of predictions and showing how the rather intricate structure of probability—the “probability ladder”—is derivable from considering predictions of relative frequency. I conclude with two remarks on the probability of single results, and on the generality of probability statements.

Appendix: Derivation of the Predicted Variance

Appendix: Derivation of the Predicted Variance

The predicted variance \(\sigma ^{2}\) of the relative frequency is

$$\begin{aligned} \sigma ^2&:=\,E\left( {\left( \frac{k}{N}-p\right) ^2}\right) =E\left( {\left( {\frac{k}{N}}\right) ^2-2\frac{k}{N}\cdot p+p^2}\right) \\&=\,E\left( \left( {\frac{k}{N}}\right) ^2\right) -2\cdot E\left( {\frac{k}{N}}\right) \cdot p+p^2=E\left( \left( {\frac{k}{N}}\right) ^2\right) -p^2, \end{aligned}$$

since (cf. Eq. 7) \(E( {\frac{k}{N}})=p.\) Using Eq. (6) we get,

$$\begin{aligned}&E\left( \left( {\frac{k}{N}}\right) ^2\right) =\sum \limits _{k=0}^N {\left( {\frac{k}{N}}\right) ^2\cdot p(A_k^N )}\\&\quad =\,\sum \limits _{k=0}^N {\left( {\frac{k}{N}}\right) ^2\cdot ( {_k^N })\cdot p^k\cdot (1-p)^{N-k}}\\&\quad =\,\sum \limits _{k=1}^N {\frac{k}{N}\cdot \frac{k}{N}\cdot \frac{N!}{k!(N-k)!}\cdot p^k\cdot (1-p)^{N-k}}\\&\quad =\,\frac{1}{N}\sum \limits _{k=1}^N {k\cdot \frac{(N-1)!}{(k-1)!(N-k)!}\cdot p^k\cdot (1-p)^{N-k}} . \end{aligned}$$

Replacing the factor k by the sum of k–1 and 1, we get the sum of two terms, \(T_{1 }\)and \(T_{2}\):

$$\begin{aligned} E\left( \left( {\frac{k}{N}}\right) ^2\right)&=\frac{1}{N}\sum \limits _{k=1}^N {(k-1)\cdot \frac{(N-1)!}{(k-1)!(N-k)!}\cdot p^k\cdot (1-p)^{N-k}}\\&\quad +\,\frac{1}{N}\sum \limits _{k=1}^N {\frac{(N-1)!}{(k-1)!(N-k)!}\cdot p^k\cdot (1-p)^{N-k}} \\&=T_1 +T_2 . \end{aligned}$$

In \(T_1\) the summand with k = 1 is zero. Thus:

$$\begin{aligned} T_1 =\frac{p^2\cdot (N-1)}{N}\cdot \sum \limits _{k=2}^N {\frac{(N-2)!}{(k-2)!(N-k)!}\cdot p^{k-2}\cdot (1-p)^{N-k}} . \end{aligned}$$

Substituting in the sum, l for k–2 and M for N–2 we get a binomial form:

$$\begin{aligned} T_1&=\,\frac{p^2\cdot (N-1)}{N}\cdot \sum \limits _{l=0}^M {\frac{(M)!}{l!(M-l)!}\cdot p^l\cdot (1-p)^{M-l}}\\&=\,\frac{p^2\cdot (N-1)}{N}\cdot (p+(1-p))^M=\frac{p^2\cdot (N-1)}{N}. \end{aligned}$$

Similarly we transform \(T_{2}\), substituting l for k–1 and M for N–1:

$$\begin{aligned} T_2&=\,\frac{p}{N}\cdot \sum \limits _{k=1}^N {\frac{(N-1)!}{(k-1)!(N-k)!}\cdot p^{k-1}\cdot (1-p)^{N-k}}\\&=\,\frac{p}{N}\cdot \sum \limits _{l=0}^M {\frac{(M)!}{l!(M-l)!}\cdot p^l\cdot (1-p)^{M-l}=} \frac{p}{N}. \end{aligned}$$

Thus

$$\begin{aligned} E\left( \left( {\frac{k}{N}}\right) ^2\right) =\frac{p^2\cdot (N-1)}{N}+\frac{p}{N}=p^2-\frac{p^2}{N}+\frac{p}{N}=p^2+\frac{p\cdot (1-p)}{N}. \end{aligned}$$

So we get the variance

$$\begin{aligned} \sigma ^2=E\left( \left( {\frac{k}{N}}\right) ^2\right) -p^2=\frac{p\cdot (1-p)}{N}. \end{aligned}$$

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Drieschner, M. Probability and Relative Frequency. Found Phys 46, 28–43 (2016). https://doi.org/10.1007/s10701-015-9955-9

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