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|    sci.physics.research    |    Current physics research. (Moderated)    |    17,520 messages    |
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|    Message 15,844 of 17,520    |
|    Tom Roberts to Luigi Fortunati    |
|    Re: Newton vs. Einstein    |
|    23 Sep 17 12:54:27    |
      From: tjroberts137@sbcglobal.net              On 9/22/17 9/22/17 12:42 AM, Luigi Fortunati wrote:       > Tom Roberts giovedà 21/09/2017 alle ore 15:53:32 ha scritto:       >>> Newton claims that gravity is a force, Einstein denies it: for him it is       >>> not a force (it is something else).       >>       >> Yes, in GR gravity is an aspect of the geometry of spacetime -- it can       >> masquerade as a fictitious "force", like "centrifugal and Coriolis force",       >> due to choice of coordinates.       >       > How can a different choice of coordinates have some influence on the       > "measurement" of a force?              For a real force, coordinates don't matter. But for a "fictitious force"       that is explicitly coordinate dependent, they do. That's why I put       "gravitational force", "centrifugal force", and "Coriolis force" in       quotes -- they aren't really forces at all, it's just that their       historical names contain the word inappropriately. They are really       FUDGES that permit one to act as if accelerated coordinates were       inertial, so Newton's laws are valid in them.              With the hindsight of GR, we understand why Newton thought there was a       "force of gravity" -- he was unknowingly using coordinates that were       themselves accelerated, and attributed the acceleration of free objects       relative to them to a "force". In retrospect, those free objects were       moving inertially, and the coordinates were accelerated.              > Force is the one exercised in its "point of application" and is       unique. But neither "gravity" nor "centrifugal force" nor "Coriolis       force" have any "POINT of application" -- they all apply equally to all       points of an object.               Real forces, in the sense of "a push or a pull", do indeed have        a point of application. (Electrical and magnetic forces have        a point of application at each charged particle.)              > If the bleacher exerts a force of 600 N on the scaffolding (and vice versa),       > that force is always equal to 600 N for everyone!              Sure.              But a freefalling ball above them feels no force at all (neglecting       air). The forces on scaffolding and bleachers are real, contact forces,       which are diverting the bleachers from their inertial path (which would       of course be falling downward).              > Otherwise tell me in what other reference system the bleacher could exert on       > the scaffold a force other than 600 N or even nothing.              You are using the wrong situation -- real forces like that are not       coordinate dependent. Look at the freefalling ball above the bleachers,       neglecting air -- it feels no force. It is accelerating relative to       coordinates fixed to the ground simply because the latter are       accelerating.               Consider a baseball thrown straight up and in the air for 4        seconds: it goes up ~ 64 feet and comes back down. Using        coordinates fixed to the earth, its trajectory through        spacetime extends for 744,000 miles along the time        coordinate and 64 feet in space -- very nearly a straight        line, because near earth the curvature of the manifold is        quite small. (metric: 1,200,000 km and 20 meters.)              General Relativity is a whole new way of looking at the world, compared       to Newtonian mechanics. A newsgroup like this is not a good place to       learn it -- get a good textbook.              Tom Roberts              --- SoupGate-Win32 v1.05        * Origin: you cannot sedate... all the things you hate (1:229/2)    |
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