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|    sci.physics.research    |    Current physics research. (Moderated)    |    17,516 messages    |
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|    Message 15,922 of 17,516    |
|    Tom Roberts to Luigi Fortunati    |
|    Re: The "apparent" forces    |
|    15 Nov 17 08:16:36    |
      From: tjroberts137@sbcglobal.net              On 11/12/17 11/12/17 11:58 PM, Luigi Fortunati wrote:       > Centrifugal force is an "apparent" force.              Hmmmm. Rather than "apparent", say "fictitious", because that's what it is -- a       FICTION that permits one to apply Newton's laws in rotating coordinates.              Remember that Newton's laws only apply in an inertial frame. This is ESSENTIAL,       and the confusions in this thread are due to people forgetting it.              Historically people wanted to apply Newton's laws in coordinates fixed to the       earth's surface. As the earth rotates, "centrifugal and Coriolis forces" were       invented to account for the rotation; they are only important on large scales       (> a few km), and were initially invented for long-range artillery.               I put "centrifugal and Coriolis forces" in quotes, because        the names are a misnomer -- they are not forces, they are        mathematical conveniences. With the hindsight of GR we        recognize they are certain components of the geometrical        connection projected onto rotating coordinates.              Here is how you can avoid going wrong about such things: coordinates are human       fabrications used for convenience in describing physical phenomena. They are       ARBITRARY. As arbitrary human constructs, they cannot possibly affect any real,       physical phenomena. That implies that any real phenomena must be modeled by       coordinate-independent mathematical quantities (such as scalars, vectors,       tensors...) -- any coordinate-dependent quantity cannot possibly be real. Both       "centrifugal and Coriolis forces" depend on the coordinates used, and vanish in       an inertial frame, so they cannot be real.              Here's another way to avoid going wrong: for any real force you can figure some       way to measure it via a spring scale. For instance, put the scale in line with       the rope and measure its tension. For "centrifugal and Coriolis forces' there       is       no place to put the scale -- it is impossible to measure them.               Note this also applies to the "force of gravity" -- there's no        place to put the scale. A bathroom scale measures the force of        the earth pushing you upward, but you cannot measure the "force        of gravity" pulling you down. With the hindsight of GR we        recognize that the "force of gravity" is also fictitious, just        like "centrifugal and Coriolis forces" (i.e. it, too, is certain        components of the connection in non-inertial coordinates).        Note the context of this post is Newtonian mechanics, and you        cannot apply all of what I say here to GR.              > The sling rotates and the hand exerts a real centripetal force on the rope.              Yes. The rope transfers it to the stone in the sling, which consequently does       not follow a uniform straight line, but rather goes around in a circle. Here       I'm       implicitly using coordinates fixed to the ground, and the rotation of the earth       is negligible, so these are inertial coordinates -- there is no "centrifugal       force".               If there were a "centrifugal force" in these coordinates, it        would cancel the tension in the rope pulling on the stone, the        stone would have zero net force on it, and would go in a straight        line. But it goes around in a circle.              You MUST keep track of which coordinates you are using, and which forces you       are discussing. You confused yourself by not doing that.              > For the third principle, even the rope exerts an equal and opposite force       > (hence centrifuge) on the hand.              Yes. But this is NOT "centrifugal force", this is a force of tension in the       rope. (More about "centrifugal force" on the hand below.)              > How is possible that the two opposing forces, one is real and the other       > apparent?              You must keep track of which forces you are discussing. The rope exerts tension       on the stone, and tension on the hand -- both are real. In these coordinates       fixed to the ground there simply is no "centrifugal force". So the problem       you think you see does not really exist.              If you use coordinates in which the rope and stone are at rest, then a       "centrifugal force" arises in these rotating coordinates, it cancels the force       of tension on the stone, and the stone does follow a uniform straight line in       these rotating coordinates (it remains at rest). This is due purely to the use       of non-inertial, rotating coordinates.              In these rotating coordinates, how about a "centrifugal force" on the hand       holding the rope? For the case in which the hand remains at rest at the center       of the rotating coordinates as the stone revolves around it, "centrifugal       force"       is zero because it is proportional to radius from the rotation center.              Other people have added to the confusion:              Gerry Quinn said:       > In a rotating reference frame [...], centrifugal force exists.              This is a PUN on "exists". We normally use that word for real, physical objects       or phenomena. But "centrifugal force' is a purely mathematical construct, and       is       not "real" in any sense of the word.              > ["centrifugal force"] causes objects to move away from the centre of rotation       > when they are not subject to any other force.              This is not true. A mathematical fiction cannot "cause" anything. An object not       subject to any force moves in a uniform straight line (Newton's first law,       implicitly relative to an inertial frame) -- that is what happens. It's just       that such a uniform straight line, when observed via rotating coordinates,       LOOKS       like accelerated motion attributable to a magic "centrifugal force" (it's magic       because an inertial observer does not see it).              > We can also look at the situation in terms of an inertial reference frame       > [...]. Then we see the the centrifugal force as the reaction to a       > centripetal force that is causing a body to move non-inertially.              This is very confused. In an inertial reference frame, there is no "centrifugal       force". The reaction to the centripetal force of the above rope pulling on the       stone is simply the tension of the rope pulling on the hand. The stone has an       unbalanced force (tension of the rope), and thus does not move in a uniform       straight line. As I said above, if there were a "centrifugal force" in inertial       coordinates, the above stone would have no net force and would NOT go around in       a circle -- BUT IT DOES.              Douglas Eagleson mentioned       > oscillative action of the hand [...] airplanes              This is getting bogged down in details. Your entire post was so focused on       minutiae and other physical situations that it is not feasible for me to       respond       to it. But you also seem to be confused about the reality of "centrifugal       force"       and the utter impossibility of it to "cause" anything.              Tom Roberts              --- SoupGate-Win32 v1.05        * Origin: you cannot sedate... all the things you hate (1:229/2)    |
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