They arise in any mechanical rotating sytem but only in it (as opposed to orbits under gravitational influence as explained below). The terminology is not unfortunate or confusing at all if one keeps strictly to mechanical rotating systems, its purpose is simply to let us know that we talk about the special case of circular (rotating) accelerated motion as opposed to linear one. It is a motion distinct enough to warrant its own special terminology (i.e., acceleration can easily be maintained indefinitely as opposed to linear acceleration.</DIV> </p><p>See above. One can use the tereminology if one chooses, and it does perhaps aid discussion. But don't let the terminology obscure the fundamentals.</p><p> </p><p>Replying to:<BR/><DIV CLASS='Discussion_PostQuote'>~~~~~~~~~~~~~~~~~~~~~~~~~~~Any confusion arises from misapplication of these forces to gravitationally bound system but then the confusion is due to misapplication, not because the terms are not in some way not kosher. When it comes to orbits under gravitational influence as opposed to mechanical rotating sytem, these two forces - action and reaction Newtonian forces - are not present or acting and that is where some confusion may come from. The reason is that gravitation is not the classical mechanical Newtonian force. Where the mechanical force acts on the body directly in the push/pull fashion and alters its motion that way by working against and overcoming its inertial resistance, the gravitation is a force which acts directly on the body's inertial properties so to speak, altering them and thus generating the acceleration of the body without it being mechanically pushed/pulled around. That is also why it is (correctly) said that gravitation is (really) not a force, at least not in the sense of the classical Newtonian force.</DIV></p><p>Huh? Gravity is easily formulated as a force, and that is precisely what is done in Newton's Theory of Universal Gravitation. In fact the fundamental reason that Newton developed his theory of mechanics, his theory of gravity and calculus was to provide and explanation in terms of basic and far-reaching principles for Kepler's laws of planetary motion. I have no idea where you got the idea that gravity is not a classical Newtonian force, but that idea is totally wrong both scientifically and historically.</p><p> </p><p>Replying to:<BR/><DIV CLASS='Discussion_PostQuote'>It might seem odd calling gravitational force non-Newtonian given that Newton was the one who 'discovered' it. That has to do with the fact that as he admited himself, he didn't understand how gravitation works, that is what is the machinery behind it. I call the gravitation non-Newtonian force to distinguish it from the classical Newtonian force acting in the F=ma formula. Perhaps there is a better way to make the distinction and I am open to ideas in that regard.</DIV></p><p>Gravity is as Newtonian as it gets. Newton absolutely did understand, to a very high degree of approximation, how gravity works. His understanding is still the basis for all modern calculation of satellite orbits as well as most orbits calulated in astrophysics. In some highly specializeds circumstances Newtonian calculations are replaced by the more difficult more more accurate calculations of general relativity. But Newton most assuredly did, by any reasonable definition, know HOW gravity works.</p><p>What Newton did not understand is WHY gravity works the way it does. Nobody does, Not then. Not now. He was originally hoping for an explanation of how gravity works similar the explanation of how a clock a works in terms of pendulums and gears. No one has such an explanation. That has nothing to do with the discussion as to whether gravity is a Newtonian force.</p><p> </p><p> Replying to:<BR/><DIV CLASS='Discussion_PostQuote'>~~~~~~~~~~~~~~~~~~~~~~~~~ The gravitation doesn't work against the body's inertia in the sense of overcoming it but rather it alters the inertia of a body itself, so that the body moves in accelerated fashion on its own.</DIV></p><p>Actually gravity works on a bodies mass. It is an experimental fact that the masses M and m that occur in the statement of universal gravitation F = G(Mm)/r^2 are the same masses that occur in F=ma. Inertial mass and gravitational mass are the same, to as many decimal places as we have been able to measure.</p><p> </p><p>Replying to:<BR/><DIV CLASS='Discussion_PostQuote'> Centripetal (pulling) force takes no part in the Moons orbital motion (for example) simply because there is no centrifugal (pull resisting) force to begin with and vice versa - that's because gravitation is not a mechanical Newtonian force as pointed out and is really not a force at all in a strict sense. In a sense the gravitational 'force' is the very opposite of the mechanical Newtonian force - the Moon is in a freefall towards the Earth's surface which it approaches at the rate of 9.8 m/second squared and if there were no gravitation and we wanted to achieve the same result, we would have to do some hard pushing to make it move that way. Now if we were instead somehow able to adjust the Moon's inertial properties the same way that gravitation does it, then the Moon would have acceleration as its normal and natural motion without us having to push it. But then instead we would have hard time holding it still suspended in the space above the Earth. In short the Moon's natural motion with such tweaked inertial properties would then want to accelerate all the time in some direction (of course the inertia of the Moon could be put into imbalance only in a certain direction at a time in respect to its body) as opposed to the usual way of staying put, moving with whatever velocity it had, if there were no other bodies in close proximity to influence it gravitationally.</DIV></p><p>That is a rather confused and confusing explanation. If you go back to my derivation of the acceleration and force required for simple circular motion then the force necessary to provide the necessary acceleratin is simply that of the gravity of the Earth. And it is most certainly a Newtonian force.</p><p>The Moon does experience an acceleration towards the center of motion, which is the center of the Earth. But that acceleration is NOT 9.8 m/s^2 because the Moon is sufficiently far from the Earth that calculation of the gravitational acceleration is materially affected by the distance-squared term in the denominator of Newton's law of universal gravitation. It is however, completely consistent with the w^2*R term in my derivation above.</p><p> </p><p> </p><p> Replying to:<BR/><DIV CLASS='Discussion_PostQuote'> ~~~~~~~~~~~~~~~~~~~~~~~~~~That's how gravitation works and that's why it behaves differently from the classical Newtonian forces (F=ma) and why the forces of action and reaction (or centri-petal/fugal when it comes to rotation) don't apply when it is the gravitation that acts.</DIV></p><p>No that is not how gravitation works in classical Newtonian theory. It works precisely according the mathematics that I showed you. </p><p>Replying to:<BR/><DIV CLASS='Discussion_PostQuote'> That is also the reason why in the GR the gravitation is not a force. In the classical Newtonian context also, the gravitation is not a force (should not be taken as such) if one wants to be strict with terminology employed, given that one is using today's insight into gravitation.</DIV></p><p>What is going on in general relativity is more subtle than what you seem to realize.</p><p>In Newtonian mechanics an object in motion tends to stay in uniform linear motion unless acted upon by a force. That is in fact why it takes an acceleration to cause a body to move in a circle. I showed how to derive the necessary force, using Newtonian mechanics, in the case of uniform circular motion.</p><p>It is important to recognize that Newtonian mechanics assumes that everything is happening against the backdrop of an ordinary Euclidean space. In Euclidean space the shortest distance between two points is a straight line. The geodesics of Euclidean space are straight lines.</p><p>General relativity replaces the backdrop of Euclidean space with a non-Euclidean curved version of space -- a Lorentzian 4-manifold called space-time. Mass causes curvature of space-time, and curvature results in geodesics that are not ordinary straight lines.</p><p>Newton's law that objects follow geodesics unless acted upon by a force continues to hold in general relativity. But those geodesics are no longer ordinary straight lines, but are affected by the curvature of space-time that results from the pressence of massive objects. What we perceive as gravity in general relativity is simply bodies following geodesics in space-time (not just in space). In that sense gravity is no longer a force in general relativity, but is rather a phenomena that results from motion in a curved space-time in the absence of force.</p><p>One ought be very careful to clearly state whether one is working with Newtonian mechanics or general relativity and not confuse the two. Either, in almost all (but not the most extreme) situations can produce extremely accurate predictions. But if you mix the two inappropriately you get gibberish.</p><p>Replying to:<BR/><DIV CLASS='Discussion_PostQuote'>Of course, in Newton's time there were no such insights and one equated ma=G[(mm)/r*r] without scruples. The danger is that confusion can develop with such usage which mixes the two kinds of forces freely. As explained, the F=ma force achieves acceleration by acting against the body's inertial properties - that is it seeks to overcome them. In contrast the gravitation instead acts to alter these inertial properties themselves so as to achieve the acceleration of the body in question without forcing it in any way. In short it is like the difference between hand pushing a recalcitrant stuck-in-place ox (oxen?) to make it go someplace instead of suspending a carrot on a stick and dangling it in front of its nose which it then naturally follows of its own will without any pushing being necessary. Alas we can only wish we were able to influence a body's inertia the same way we can influence the ox's because then all our problems would be solved. Like Sartre or some other philosopher said, quoting from memory of a quote - if a man has ten cows, all his problems are solved. Constructive criticism is welcomed (welcome?) <br />Posted by vandivx</DIV></p><p>You have more or less stated the case for general relativity, although it does not alter inertial properties of masses, but rather provides an altered view of space and time. But you are trying to mix the Newtonian perspective and Einstein's relativistic perspective inappropriately. The result is confusion.</p><p>Newton's mechanics works extremely well in almost all common situations. Einstein's general relativity works more broadly and more accurately. But you should not and cannot accurately combime the perspectives of the two in the manner that you are doing. They are distinct mathematical models, one simpler and accurate in almost all cases, the other more complex. more accurate, and more broadly applicable. <br /></p> <div class="Discussion_UserSignature"> </div>