Free floating crystolecule - Revision history

Apm: /* High energy ejection out of machine phase into dystactic phase */ moved content over to page Overstretch pushout

2025-09-22T11:56:15Z

High energy ejection out of machine phase into dystactic phase: moved content over to page Overstretch pushout

@@ Line 42: / Line 42: @@
 [[File:Prototype-1-250-ps.gif|thumb|400px|right|Simulation by Philip Turner. '''Beware of [[misleading aspects in animations of diamondoid molecular machine elements]].''' Pauli repulsion pushes the piston out of the slightly too tight cylinder. The effect gets weaker with progressive push-out but still suffices for a final ejection. A bend snap makes for a sudden re-acceleration and for strong excitation of mechanical modes. As a side-note: There is also some significant conversion to kinetic energy. This is around tens to ~100m/s. '''More like a crystolecule cannon than a gentle push-out.''']]
-[[VdW suck-in and suck-on]] can accelerate a [[crystolecule]] enough <br>
+See main page: '''[[Overstretch pushout]]'''
 == Related ==

Apm: /* High energy ejection out of machine phase into dystactic phase */

2025-09-22T11:53:06Z

High energy ejection out of machine phase into dystactic phase

← Older revision		Revision as of 13:53, 22 September 2025
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	[[VdW suck-in and suck-on]] can accelerate a [[crystolecule]] enough <br>		[[VdW suck-in and suck-on]] can accelerate a [[crystolecule]] enough <br>
	such that it overshoots the end of its ~~unbostructed~~ superlubric rail and it escapes into free space.		such that it overshoots the end of its unobstructed [[superlubricity\|superlubric]] rail and it escapes into free space.

	High ebergy [[intercrystolecular snapping modes]] can cause <br>		High ebergy [[intercrystolecular snapping modes]] can cause <br>

Apm: /* Growing positional uncertainty from quantum dispersion and Brownian random walk */

2025-09-22T11:52:08Z

Growing positional uncertainty from quantum dispersion and Brownian random walk

← Older revision		Revision as of 13:52, 22 September 2025
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	In a gas they are diffused away to who knows where.		In a gas they are diffused away to who knows where.

	== Growing positional uncertainty from quantum dispersion and Brownian random walk ==		== Growing positional uncertainty from quantum dispersion and (if in gas) Brownian random walk ==

	For small crystolecules and typical machine speeds of mm/s quantum dispersion speed of position is relevant. <br>		For small crystolecules and typical machine speeds of mm/s quantum dispersion speed of position is relevant. <br>

Apm: /* Challenge if cool i.e. slow free space crystolecules */

2025-09-22T11:51:36Z

Challenge if cool i.e. slow free space crystolecules

← Older revision		Revision as of 13:51, 22 September 2025
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	Electric fields, magnetic fields, and optical traps. <br>		Electric fields, magnetic fields, and optical traps. <br>

	== Challenge if cool i.e. slow free space crystolecules ==		== Challenge of getting cool i.e. slow free space crystolecules ==

	Cooling them down aka slowing then down is possible so far that gravity acting on them can be observed. <br>		Cooling them down aka slowing then down is possible so far that gravity acting on them can be observed. <br>

Apm: Growing positional uncertainty from quantum dispersion and Brownian random walk

2025-09-22T11:51:15Z

Growing positional uncertainty from quantum dispersion and Brownian random walk

← Older revision		Revision as of 13:51, 22 September 2025
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	If charged they can be free-space manipulated with conventional techniques. <br>		If charged they can be free-space manipulated with conventional techniques. <br>
	Electric fields, magnetic fields, and optical traps. <br>		Electric fields, magnetic fields, and optical traps. <br>

			== Challenge if cool i.e. slow free space crystolecules ==

	Cooling them down aka slowing then down is possible so far that gravity acting on them can be observed. <br>		Cooling them down aka slowing then down is possible so far that gravity acting on them can be observed. <br>
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	they fall off and down by gravity locally at scale similar to their own size right after being fully pushed-out. <br>		they fall off and down by gravity locally at scale similar to their own size right after being fully pushed-out. <br>

	Crossing [[the heat-overpowers-gravity size-scale]] rather "fall" in a relative to their own size very large parabolic arc so far they are in a good vacuum. <br>		Crossing [[the heat-overpowers-gravity size-scale]] crystolecules rather "fall" in a <br>
	~~Or in~~ a gas they are diffused away to who knows where.		relative to their own size very large parabolic arc. That is so far they are in a good vacuum. <br>
			In a gas they are diffused away to who knows where.

			== Growing positional uncertainty from quantum dispersion and Brownian random walk ==

			For small crystolecules and typical machine speeds of mm/s quantum dispersion speed of position is relevant. <br>
			{{wikitodo\|Ad a very crude caculation to show the scales.}} <br>

			Probably the case: In a gas the quantum dispersion more or less mixes with a statistical Brownian random walk. <br>
			Free floating crystolecule decoherence due to a collision with a gas molecule is not fully decohereing the free floating crystolecule relaive to the nanomachine bulk if the gas molecule itself has some degree of quantum dispersion relative to the nanomachine bulk. Relational quantum mechanics.

	== High energy ejection out of [[machine phase]] into [[dystactic phase]] ==		== High energy ejection out of [[machine phase]] into [[dystactic phase]] ==
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	* [[Accidental heatpump]]		* [[Accidental heatpump]]
	* [[VdW suck-in and suck-on]]		* [[VdW suck-in and suck-on]]

			== External links ==

			* https://en.wikipedia.org/wiki/Relational_quantum_mechanics

Apm: improvements

2025-09-22T11:39:38Z

improvements

← Older revision		Revision as of 13:39, 22 September 2025
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	{{stub}}		{{stub}}

	Getting [[crystolecule]]s into huge scale free space should afford some easily manageable conscious effort. <br>		Getting [[crystolecule]]s into huge scale free space <br>
	If charged they ~~than~~ can be manipulated with conventional techniques~~, electric~~ fields, magnetic fields, and optical traps. <br>		(larger than their won scale by several orders of magnitude) <br>
			should afford some easily manageable conscious effort. <br>
			If charged they can be free-space manipulated with conventional techniques. <br>
			Electric fields, magnetic fields, and optical traps. <br>

	Cooling them down aka slowing then down is possible so far that gravity acting on them can be observed. <br>		Cooling them down aka slowing then down is possible so far that gravity acting on them can be observed. <br>
			{{wikitodo\|Check that claim, there can be significant heat-up problems from the laser intensity.}} <br>
	But these crystolecules are far outside [[machine phase]] deep inside gas phase (or [[dystactic phase]]).		But these crystolecules are far outside [[machine phase]] deep inside gas phase (or [[dystactic phase]]).

	Instead ~~getting~~ crystolecules ~~down to low speed and~~ <br>		Instead, keeping crystolecules … <br>
	~~keeping them~~ close to the emitting source inside a small volume and <br>		– close to the emitting source and <br>
	having them without a charge is likely quite difficult. <br>		– inside a small volume not much bigger than their own size, and <br>
			– having them without a charge is likely quite difficult. <br>
			Requites getting crystolecules ejected at at typical nanomachine speeds of a few mm/s <br>
			(constant speed control, in mechanical analogy to constant current control). <br>
			Or requires to at least get them quickly cooled down again after high speed ejection.

	Due to [[intercrystolecular forces]] being many orders of magnitude bigger than gravity (at these small scales) <br>		Due to [[intercrystolecular forces]] being many orders of magnitude bigger than gravity (at these small scales) <br>
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	Crossing [[the heat-overpowers-gravity size-scale]] rather "fall" in a relative to their own size very large parabolic arc so far they are in a good vacuum. <br>		Crossing [[the heat-overpowers-gravity size-scale]] rather "fall" in a relative to their own size very large parabolic arc so far they are in a good vacuum. <br>
	Or in a gas they are diffused away to who knows where.		Or in a gas they are diffused away to who knows where.


	== High energy ejection out of [[machine phase]] into [[dystactic phase]] ==		== High energy ejection out of [[machine phase]] into [[dystactic phase]] ==

Apm: improvements

2025-09-22T11:28:24Z

improvements

← Older revision		Revision as of 13:28, 22 September 2025
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	Instead getting crystolecules down to low speed and <br>		Instead getting crystolecules down to low speed and <br>
	keeping them close to the emitting source in a small volume and <br>		keeping them close to the emitting source inside a small volume and <br>
	having them without a charge is likely ~~very~~ difficult. <br>		having them without a charge is likely quite difficult. <br>

	Due to [[intercrystolecular forces]] being many orders of magnitude bigger than gravity (at these small scales) <br>		Due to [[intercrystolecular forces]] being many orders of magnitude bigger than gravity (at these small scales) <br>
	either they stick like very strongly or they fly off very fast with a lot of kinetic energy. <br>		either they stick like very strongly or they fly off very fast with a lot of kinetic energy. <br>
	There is no pushing them out and they fall off by gravity locally at ~~small~~ scale.		There is no easy pushing them off a surface (or out of a tube) gently and <br>
			they fall off and down by gravity locally at scale similar to their own size right after being fully pushed-out. <br>

			Crossing [[the heat-overpowers-gravity size-scale]] rather "fall" in a relative to their own size very large parabolic arc so far they are in a good vacuum. <br>
			Or in a gas they are diffused away to who knows where.

	~~Crossing [[the heat-overpowers-gravity size-scale]] they fall in a large parabolic arc in a good vacuum. <br>~~
	~~Or are diffused away to who knows where in a gas.~~

	== High energy ejection out of [[machine phase]] into [[dystactic phase]] ==		== High energy ejection out of [[machine phase]] into [[dystactic phase]] ==

Apm at 11:22, 22 September 2025

2025-09-22T11:22:40Z

← Older revision		Revision as of 13:22, 22 September 2025
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	Due to [[intercrystolecular forces]] being many orders of magnitude bigger than gravity (at these small scales) <br>		Due to [[intercrystolecular forces]] being many orders of magnitude bigger than gravity (at these small scales) <br>
	either they stick like very strongly or they fly off ~~like~~ very fast with a lot of kinetic energy. <br>		either they stick like very strongly or they fly off very fast with a lot of kinetic energy. <br>
	There is no pushing them out and they fall off by gravity locally at small scale.		There is no pushing them out and they fall off by gravity locally at small scale.

Apm at 11:22, 22 September 2025

2025-09-22T11:22:26Z

← Older revision		Revision as of 13:22, 22 September 2025
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	having them without a charge is likely very difficult. <br>		having them without a charge is likely very difficult. <br>

	Due to [[intercrystolecular forces]] being many orders of magnitude bigger than gravity <br>		Due to [[intercrystolecular forces]] being many orders of magnitude bigger than gravity (at these small scales) <br>
	either they stick like very strongly or they fly off like very fast with a lot of kinetic energy. <br>		either they stick like very strongly or they fly off like very fast with a lot of kinetic energy. <br>
	There is no pushing them out and they fall off by gravity locally at small scale.		There is no pushing them out and they fall off by gravity locally at small scale.

Apm: /* High energy ejection out of machine phase into dystactic phase */ fixed some typos and added note on this being more a cannon/gun than a gentle push-out

2025-09-22T11:19:57Z

High energy ejection out of machine phase into dystactic phase: fixed some typos and added note on this being more a cannon/gun than a gentle push-out

← Older revision		Revision as of 13:19, 22 September 2025
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	== High energy ejection out of [[machine phase]] into [[dystactic phase]] ==		== High energy ejection out of [[machine phase]] into [[dystactic phase]] ==

	[[File:Prototype-1-250-ps.gif\|thumb\|400px\|right\|Simulation by Philip Turner. '''Beware of [[misleading aspects in animations of diamondoid molecular machine elements]].''' Pauli ~~repulstion~~ pushes the piston out of the ~~slihtly~~ too ~~thight~~ cylinder. The effect gets weaker with progressive push-out but still suffices for a final ejection. A bend snap makes for a sudden ~~reacceleration~~ and for strong excitation of mechanical modes. As a side-note: There is also some significant conversion to kinetic energy. This is around tens to ~100m/s.]]		[[File:Prototype-1-250-ps.gif\|thumb\|400px\|right\|Simulation by Philip Turner. '''Beware of [[misleading aspects in animations of diamondoid molecular machine elements]].''' Pauli repulsion pushes the piston out of the slightly too tight cylinder. The effect gets weaker with progressive push-out but still suffices for a final ejection. A bend snap makes for a sudden re-acceleration and for strong excitation of mechanical modes. As a side-note: There is also some significant conversion to kinetic energy. This is around tens to ~100m/s. '''More like a crystolecule cannon than a gentle push-out.''']]

	[[VdW suck-in and suck-on]] can accelerate a [[crystolecule]] enough <br>		[[VdW suck-in and suck-on]] can accelerate a [[crystolecule]] enough <br>