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|    sci.physics.research    |    Current physics research. (Moderated)    |    17,516 messages    |
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|    Message 17,328 of 17,516    |
|    Richard Livingston to Luigi Fortunati    |
|    Re: Gravity and curvature    |
|    18 Dec 23 16:07:15    |
      From: richalivingston@gmail.com              On Monday, December 18, 2023 at 2:14:47 AM UTC-6, Luigi Fortunati wrote:       > Luigi Fortunati il 17/12/2023 09:29:50 ha scritto:       ...       > By gravity I mean the Newtonian force F directly proportional to the product       of the masses m1 and m2 and inversely proportional to the square of their       distance.       ...       > Does all this exclude that, in classical mechanics, gravity is a fundamental       force and, therefore, is necessarily a vector?       ...       > If there are many directions in the GR, why does the elastic sheet sink       *always and only* downwards, i.e. towards a single direction?       >       > Luigi Fortunati              As mentioned by the moderator, our current understanding of gravity is       considerably more complex and subtle than Newton's concept. Experimental       evidence has confirmed all this. In particular, thinking of gravity only as a       force is missing some        important phenomena.              The current understanding is that space time is not Euclidean everywhere, but       can be curved in various ways. The geometry of space-time is described by the       metric tensor, which is a 4x4 tensor with 10 unique parameters. The ways that       space-time can be        distorted is more complex than can be described by a simple vector. However,       with the metric tensor one can calculate how objects move from point to point       via the covariant derivative. This is an extension of the ordinary derivative       to a non-Euclidean        space-time. One of these derivatives can calculate what we commonly       experience as the "force of gravity", and that is a vector with direction and       magnitude. But that is only one of several gravitational effects that we now       understand.              To put that more clearly, gravity is not just an attractive force. There are       a multitude of effects we now understand to be due to gravity.              In general relativity gravity can manifest in ways other than a simple       attractive force. The gravitational red shift is one. Actually, what we       regard as a "force" is due to the variation in this red shift with radial       position. Geometrically, there is        a curvature of the time metric, g_00, in the radial direction. But GR also       shows that the radial metric varies in the radial direction. This is a       different kind of curvature and it does not result in a "force", but it does       affect the paths that free        objects follow. As an example. if you could somehow turn off the g_00       curvature (i.e. make g_00 = 1 everywhere), then objects could orbit a black       hole at the event horizon at any speed without falling in, and without       experiencing anything you would        call a force. That is, an object in a circular orbit will behave as if it is       going in a straight line, which geometrically it is, even though it returns to       the same place every orbit. This is not a force, yet it is a gravitational       effect.              Rich L.              --- SoupGate-Win32 v1.05        * Origin: you cannot sedate... all the things you hate (1:229/2)    |
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