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Computational Models of Measurement and Hempel’s Axiomatization

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Part of the book series: Theory and Decision Library A: ((TDLA,volume 46))

Abstract

We have developed a mathematical theory about using physical experiments as oracles to Turing machines. We suppose that an experiment makes measurements according to a physical theory and that the queries to the oracle allow the Turing machine to read the value being measured bit by bit. Using this theory of physical oracles, an experimenter performing an experiment can be modelled as a Turing machine governing an oracle that is the experiment. We consider this computational model of physical measurement in terms of the theory of measurement of Hempel and Carnap (see Fundamentals of Concept, Formation in Empirical Science, vol 2, International Encylopedia of Unified Science, University of chicago press, 1952; Philosophical Foundations of Physics, Basic Book, New York, 1928). We note that once a physical quantity is given a real value, Hempel’s axioms of measurement involve undecidabilities. To solve this problem, we introduce time into Hempel’s axiomatization. Focussing on a dynamical experiment for measuring mass, as in Beggs et al. (Proc R Soc Ser A 464(2098): 2777–2801, 2009; 465(2105): 1453–1465; Technical Report; Accepted for presentation in Studia, Logica International conference on logic and the foundations of physics: space, time and quanta (Trends in Logic VI), Belgium, Brussels, 11–12 December 2008; Bull Euro Assoc Theor Comp. Sci 17: 137–151, 2009), we show that the computational model of measurement satisfies our generalization of Hempel’s axioms. Our analysis also explains undecidability in measurement and that quantities are not always measurable.

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Notes

  1. 1.

    Why should the balance be in a vacuum? It is not because of friction. It is because there are substances in the atmosphere that have “negative weight” such as hydrogen and helium.

  2. 2.

    This is done by considering a semigroup of objects \(\mathcal{O} =\langle \mathcal{O},\circ ; 1\rangle\), with the distinguished element 1 called the unit, and some internal structure to generate fractions and multiples of the unit.

  3. 3.

    There can be further structure for the map M, e.g., depending on the fact that the attribute considered is either extensive (e.g., mass) or intensive (e.g., temperature).

  4. 4.

    This error margin in the initial speed of the proof particle of mass m means that precision in speed does not matter for this experiment.

  5. 5.

    Let f and g be total maps with signature \(\mathbb{N} \rightarrow \mathbb{N}\). We say that fΩ(g) if there exists a constant \(k \in \mathbb{R}\) such that, for an infinite number of values of \(n \in \mathbb{N},\ f(n) > \mathit{kg}(n)\).

  6. 6.

    The reference frame of the stars is a good inertial frame for experiments carried out on Earth.

  7. 7.

    To Aristotle the force applied is the cause and in some way the velocity is the effect. Since uniform motion in a straight line does not need any explanation, Newton searched for the variation of uniform motion in a straight line as the required effect.

  8. 8.

    In the Principia, Newton defined force as change of momentum, i.e., \(\mathbf{\mathit{f }} = \frac{d\mathbf{\mathit{p}}} {\mathit{dt}}.\)

  9. 9.

    Compare the context of Geroch and Hartle (1986) and Beggs et al. (2008a, c, 2009a).

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Correspondence to Edwin Beggs .

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Beggs, E., Costa, J.F., Tucker, J.V. (2010). Computational Models of Measurement and Hempel’s Axiomatization. In: Carsetti, A. (eds) Causality, Meaningful Complexity and Embodied Cognition. Theory and Decision Library A:, vol 46. Springer, Dordrecht. https://doi.org/10.1007/978-90-481-3529-5_9

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