File:0415tenseBear.gif - Revision history

Apm at 15:45, 5 November 2023

2023-11-05T15:45:07Z

← Older revision		Revision as of 17:45, 5 November 2023
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	Operation in the stable attractive-force regime reduces bearing stiffness (which falls to zero at the threshold of instability), but also reduces the interatomic couplings that produce dynamic drag.		Operation in the stable attractive-force regime reduces bearing stiffness (which falls to zero at the threshold of instability), but also reduces the interatomic couplings that produce dynamic drag.

			----
			'''How can large interatomic repulsions increase static friction and energy dissipation?''' <br>
			🔘 [https://web.archive.org/web/20160314100841/http://e-drexler.com/p/04/02/0315pairSnap.html Softly supported sliding atoms can undergo abrupt transitions in energy (via internet archive)]
			----
			'''Bearing stiffness, dynamic energy dissipation:''' <br>
			Drexler, K. E. (1992) Nanosystems: Molecular Machinery, Manufacturing, and Computation. Wiley/Interscience, pp.289-293.

			= Related here on this wiki =

			* [[Negative pressure bearings]]
			* [[Levitation]]
			* [[Snapback]]

Apm: added original text

2021-09-17T22:39:12Z

added original text

← Older revision		Revision as of 00:39, 18 September 2021
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	Source: https://web.archive.org/web/20160314130257/http://e-drexler.com/p/04/03/0322nonrepulsive.html <br> Author: Eric K. Drexler		Source: https://web.archive.org/web/20160314130257/http://e-drexler.com/p/04/03/0322nonrepulsive.html <br> Author: Eric K. Drexler

			"attractive interfaces"

			= Associated text from Eric's Website =

			== Bearings can be stable despite attractive interactions between their surfaces ==

			Intuitively, it might seem that a shaft-in-sleeve bearing can be stable only if the surfaces repel one another, pushing the shaft to the center of the sleeve. A closer examination shows that this condition is not necessary.

			Consider a shaft centered in a sleeve (here illustrated in schematic cross-section '''A'''). By symmetry, the forces on the shaft cancel, but stability requires something more — that the potential energy as a function of displacement have a positive curvature, creating positive mechanical stiffness. This will obviously be the case when the surfaces are at their equilibrium separation (at a minimum of the intersurface potential) or closer (as shown in '''A''').

			The situation at greater separations becomes clear when one considers that the potential for displacement of the shaft equals the sum of the potentials for the opposed surfaces, as illustrated in the diagrams on the right. Where this combined potential retains a positive curvature (as shown in '''B'''), the centered position remains stable, even though the net intersurface force is attractive. (At still greater separations, as shown in '''C''', the potential well bifurcates and the centered postion becomes unstable.)

			Operation in the stable attractive-force regime reduces bearing stiffness (which falls to zero at the threshold of instability), but also reduces the interatomic couplings that produce dynamic drag.

Apm: Source: https://web.archive.org/web/20160314130257/http://e-drexler.com/p/04/03/0322nonrepulsive.html
Author: Eric K. Drexler

2021-09-17T22:35:46Z

Source: https://web.archive.org/web/20160314130257/http://e-drexler.com/p/04/03/0322nonrepulsive.html <br> Author: Eric K. Drexler

New page

Source: https://web.archive.org/web/20160314130257/http://e-drexler.com/p/04/03/0322nonrepulsive.html <br> Author: Eric K. Drexler

File:0415tenseBear.gif - Revision history

Apm at 15:45, 5 November 2023

Apm: added original text

Apm: Source: https://web.archive.org/web/20160314130257/http://e-drexler.com/p/04/03/0322nonrepulsive.html Author: Eric K. Drexler

Apm: Source: https://web.archive.org/web/20160314130257/http://e-drexler.com/p/04/03/0322nonrepulsive.html
Author: Eric K. Drexler