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Registered Member #56
Joined: Thu Feb 09 2006, 05:02AM
Location: Southern Califorina, USA
Posts: 2445
Depends on the angle you start it at. Consider the limiting case of shooting the coin strait down into the hole - clearly all of the coins energy would be converted to kinetic energy and it would fall into the hole.
In the case of a lossless system where you started the trajectory exactly such that the centrifugal upward force balances the downward force from gravity then the coin would 'orbit' forever. I point out however that this is an unstable equilibrium (unlike planetary orbits), so practically the coin is always going to climb up the ramp (and slow down) or fall down the ramp (and speed up).
I would have to think about it, but it is conceivable that with a carefully designed cone shape you could make make the system stable, but then you would loose the entertaining bit where the coin slowly speeds up as it falls down toward the hole.
Registered Member #2529
Joined: Thu Dec 10 2009, 02:43AM
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Posts: 600
The correct answer is 1) but with caveats.
The caveat is that the surface must be perfectly smooth. If it isn't, even if you assume no losses, it can change the angular momentum, and the eccentricity will change over time and it will be virtually certain to either fall into the middle or get flung out the top of the funnel.
Registered Member #2939
Joined: Fri Jun 25 2010, 04:25AM
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No, the best way to prove it is with an analytical solution. Simulations are often not "lossless" as they are inevitably numerical solutions, with rounding errors and discrete steps in the simulation. It is entirely possible for a discrete step simulation to be unstable when the continuous system is not.
Registered Member #54278
Joined: Sat Jan 17 2015, 04:42AM
Location: Amite, La.
Posts: 367
2Spoons wrote ...
No, the best way to prove it is with an analytical solution. Simulations are often not "lossless" as they are inevitably numerical solutions, with rounding errors and discrete steps in the simulation. It is entirely possible for a discrete step simulation to be unstable when the continuous system is not.
I agree totally with this...SO MUCH!!!
I work almost exclusively with this method (ever since it was the --only-- method)---the work may be VERY difficult--and even sometimes simple (if you know and properly apply the *basic* laws), but the outcome is uniquely satisfying and virtually always includes a bonus or two!...IMHO
Consider a rotationally symmetric funnel with the symmetry axis vertical. Place a mass m on it with a circumferential (i.e. tangential) speed component v. Then the centrifugal force will be:
Fc = m * v^2 / r
when it rotates at radius r. The angular momentum J is given by
J = m * v * r
and it is a constant of motion, since the funnel is rotationally symmetric. We can then write Fc as:
Fc = 1/m * J^2 / r^3
The downward slope of the funnel causes an inward force. If that is smaller than the centrifugal force, the mass will be driven upward else it will continue down. The shape of the funnel defines a "force law", i.e. the inward force as a function of r. If e.g. it is an inverse square law such as the one in gravity, the centrifugal force will always become larger at low r since it rises a 1/r^3 as compared to the attractional force, which rises a 1/r^2. That prevents planets from falling into the sun. For funnels the force law can be different, so for some shapes the mass can spiral infinitely down into the funnel.
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