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|    sci.physics.research    |    Current physics research. (Moderated)    |    17,516 messages    |
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|    Message 15,712 of 17,516    |
|    rockbrentwood@gmail.com to rockbr...@gmail.com    |
|    Re: Mathematics of physical units and di    |
|    21 Jul 17 20:29:09    |
      On Wednesday, July 19, 2017 at 12:13:12 AM UTC-5, rockbr...@gmail.com wrote:       > It is not so much the question of what *additional* axioms are       > needed, but which ones need to be removed. Physical quantities are       > not numbers, so that not all the infrastructure of a field (or more       > generally: of the number system) has physical meaning with them;       > both rather only a substructure thereof.              On subsequent thought it's suddenly clear what the nature of those       restrictions are. It's something that's clear to any programmer.       Physical quantities form a TYPED ALGEBRA.              The system of types form an Abelian group with the identity 1       standing for the type of dimensionless quantities              A type judgement e: T means quantity e has type T, which in dimensional       analysis means [e] = T.              Addition and subtraction are subject to type-restriction: e + f and       e - f are only defined if e:T and f:T, in which case (e +/- f): T.              For comparison (if applicable): the same restriction applies, e and       f can only be compared if they have the same type: e < f and e = f       are only defined if e: T and f: T.              The 0 is a polymorphic constant (0: T for all types T). Alternatively       one may have a zero 0_T for each type.              Dimensionless numbers all have type 1.              Multiplication, division and reciprocals have the expected types:       if e: T and f: U then ef: TU and e/f: T/U; and 1/e: 1/T (and 1/f:       1/U).              Additional structure is required to do calculus. The system of types       becomes localized at each space-time point: a copy for each point.       One then needs a kind of "connection" to be able to compare quantities       of a given type between different points. This leads to the potential       of the comparison, itself being path dependent.              In such a case, hypotheses phrased like "c is constant" would be       utterly devoid of any meaning. Instead, one would need to replace       it with an hypothesis that makes no reference to constancy or       variability (e.g. that the chronogeometry representing the space-time       manifold is locally Lorentzian).              I'll have more to say, time permitting, on the issue of the       electromagnetic field and its units -- particularly in the context       of a metric like that given by the time element       ds^2 = dt^2 - K t (dx^2 + dy^2 + dz^2), where K > 0.              This geometry is locally Lorentzian ONLY for t > 0. At t = 0, there       is a so-called "null surface" (i.e. a 3D slice of Newton-Cartan       geometry, where c is infinite!) and for t < 0, it is locally Euclidean       (i.e. a 4-dimensional timeless space).              Such a geometry is radiation dominant near t = 0 and having a null       surface at t = 0 is also an essential condition to accord with the       ability to predict Inflation (which arises as a consequence of the       junction conditions required to join the t < 0 with the t > 0       sector); a' la Mansouri. This is something that is normally only       "written in by hand", rather than predicted.              For this geometry, the notion of c being used as a "constant" for       eliminating dimensions is completely undercut (and this also shows       by way of example why it's wrong for the literature to Sapir-Worf       away such physically interesting cases like this by its wrong       convention of taking "c = 1"). One does not Sapir-Worf away physical       postulates. That leads to dogma.              --- SoupGate-Win32 v1.05        * Origin: you cannot sedate... all the things you hate (1:229/2)    |
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