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1 Studies in the History of Statistics and Probability ... - Sheynin, Oscar

1 Studies in the History of Statistics and Probability ... - Sheynin, Oscar

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is energy?) from chapter 4 <strong>of</strong> Feynman (1963). In an excellent stylebut, regrettably <strong>in</strong> a passage too long for be<strong>in</strong>g quoted, it is stated <strong>the</strong>rethat <strong>the</strong> law <strong>of</strong> conservation <strong>of</strong> energy can be corroborated <strong>in</strong> eachconcrete case by f<strong>in</strong>d<strong>in</strong>g out where did energy go, but that modernphysics has no general concept <strong>of</strong> energy. This does not prevent usfrom be<strong>in</strong>g so sure <strong>in</strong> that law that we make a laugh<strong>in</strong>g-stock <strong>of</strong>anyone tell<strong>in</strong>g us that <strong>in</strong> a certa<strong>in</strong> case <strong>the</strong> efficiency was greater than100%. Many conclusions derived by apply<strong>in</strong>g stochastic methods tosome statistical ensembles are not less certa<strong>in</strong> than <strong>the</strong> law <strong>of</strong>conservation <strong>of</strong> energy.The circumstances are quite different for apply<strong>in</strong>g <strong>the</strong> <strong>the</strong>ory <strong>of</strong>probability when <strong>the</strong>re certa<strong>in</strong>ly exists no statistical ensemble or itsexistence is doubtful. In such cases modern science generally denies<strong>the</strong> possibility <strong>of</strong> those applications, but temptation is <strong>of</strong>ten strong...Let us first consider <strong>the</strong> reason why.1.2. The restrictiveness <strong>of</strong> <strong>the</strong> concept <strong>of</strong> statistical ensemble(statistical homogeneity). The reason is that that concept is ra<strong>the</strong>rrestrictive. Consider <strong>the</strong> examples cited above: co<strong>in</strong> toss<strong>in</strong>g, pass<strong>in</strong>g anexam<strong>in</strong>ation, ra<strong>in</strong>fall. The existence <strong>of</strong> an ensemble is only doubtless<strong>in</strong> <strong>the</strong> first <strong>of</strong> those. The bus<strong>in</strong>ess is much worse <strong>in</strong> <strong>the</strong> o<strong>the</strong>r twoexamples. We may discuss <strong>the</strong> probability <strong>of</strong> a successful pass<strong>in</strong>g <strong>of</strong>an exam<strong>in</strong>ation by a r<strong>and</strong>omly chosen student (better, by that student<strong>in</strong> a r<strong>and</strong>omly chosen <strong>in</strong>stitute <strong>and</strong> discipl<strong>in</strong>e <strong>and</strong> exam<strong>in</strong>ed by ar<strong>and</strong>omly chosen <strong>in</strong>structor). R<strong>and</strong>omly chosen means chosen <strong>in</strong> anexperiment from a statistical ensemble <strong>of</strong> experiments. Here, however,that ensemble consists <strong>of</strong> exactly one non-reproducible experiment <strong>and</strong>we can not consider that probability.It is possible to discuss <strong>the</strong> probability <strong>of</strong> ra<strong>in</strong>fall dur<strong>in</strong>g a givenday, 11 May, say, <strong>of</strong> a r<strong>and</strong>omly chosen year, but not <strong>of</strong> its happen<strong>in</strong>g<strong>in</strong> <strong>the</strong> even<strong>in</strong>g today. In such a case, when consider<strong>in</strong>g that probability<strong>in</strong> <strong>the</strong> same morn<strong>in</strong>g, we ought to allow for all <strong>the</strong> wea<strong>the</strong>rcircumstances, <strong>and</strong> we certa<strong>in</strong>ly will not f<strong>in</strong>d any o<strong>the</strong>r day with <strong>the</strong>mbe<strong>in</strong>g exactly <strong>the</strong> same, for example, with <strong>the</strong> same synoptic chart, atleast dur<strong>in</strong>g <strong>the</strong> period when meteorological observations have beenmade.Many contributions on apply<strong>in</strong>g <strong>the</strong> concept <strong>of</strong> stochastic processhave appeared recently. It should describe ensembles <strong>of</strong> suchexperiments whose outcome is not an event, or even a measurement(that is, not a s<strong>in</strong>gle number), but a function, for example a path <strong>of</strong> aBrownian motion. We will not discuss <strong>the</strong> scope <strong>of</strong> that concept evenif <strong>the</strong> existence <strong>of</strong> a statistical ensemble is certa<strong>in</strong> but consider <strong>the</strong>opposite case. Or, we will cite two concrete problems.The first one concerns manufactur<strong>in</strong>g. We observe <strong>the</strong> value <strong>of</strong>some economic <strong>in</strong>dicator, labour productivity, say, dur<strong>in</strong>g a number <strong>of</strong>years (months, days) <strong>and</strong> wish to forecast its values. It is tempt<strong>in</strong>g toapply <strong>the</strong> <strong>the</strong>ory <strong>of</strong> forecast<strong>in</strong>g stochastic processes. However, ourexperiment only provides <strong>the</strong> observed values <strong>and</strong> is not <strong>in</strong> pr<strong>in</strong>ciplereproducible, <strong>and</strong> <strong>the</strong>re is no statistical ensemble.The o<strong>the</strong>r problem is geological. We measured <strong>the</strong> content <strong>of</strong> auseful component <strong>in</strong> some test po<strong>in</strong>ts <strong>of</strong> a deposit <strong>and</strong> wish todeterm<strong>in</strong>e its mean content, <strong>and</strong> thus <strong>the</strong> reserves if <strong>the</strong> configuration9

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