Design of crystolecules: Difference between revisions
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For a definition of what they are see here: [[Gemstone-like molecular element|"What are crystolecules DMEs?"]] | For a definition of what they are see here: [[Gemstone-like molecular element|"What are crystolecules DMEs?"]] | ||
== Applicability of 3D FDM printing for Crystolecule Design | You might instead be interested in: '''[[Design for manufacturing for crystolecular systems]]'''. | ||
= Comared to macroscale machine parts made from metals = | |||
Comaring to macroscale machinery might bet be the best approach here <br> | |||
due to this being the area people have expertise in. <br> | |||
* '''The overlap/similarities:''' See: [[Scale agnostic mechanical design principles]] | |||
* '''The big differences:''' See chapters below. <br> | |||
== Design rules from [[superelasticity]] of the very hard and very tough material == | |||
Unlike macroscale metals nanoscale diamond and [[gemstone like compound]] allow for large fully reversible bending and stretching. <br> | |||
As a rule of thumb it's above 10% stretch before any damage so stayin below that is safe. <br> | |||
⚠️ '''But beware:''' This does not at all mean everyting is soft and wobbly <br> | |||
[[Misleading aspects in animations of diamondoid molecular machine elements|as molecular dynamics simulations migh misleadingly suggest]]. Oh no, it's quite the contrary. <br> | |||
It is more like hyper spring steel. See page: [[A better intuition for diamondoid nanomachinery than jelly]]. | |||
Large bending of diamond and similar stiff gems constitutes quite a high energy desnity nearing that of chemical energy storage. <br> | |||
Thus bending back and forth makes for quite high energy turnover and <br> | |||
even with quite high bening energy recuperation efficiencies <br> | |||
the small fraction of loss is still a quite big amount of thermalized energy. | |||
Thus designing crystolecules with large bending in operation should likely … <br> | |||
– better be reserved to one time actuated assembly (related to [[design for manufacturing]] and <br> | |||
– better be avoided for MHz operation fequencies after assembly (in bulk agglomerations of nanomachinery) <br> | |||
== Design rules from non-sharp surfaces at nanoscale == | |||
Macroscale surface contacts are like a Heaviside step-function. <br> | |||
They are perfectly approximated by a sharp step-function from no contact to (yes) contact. <br> | |||
Nanoscale machinery of just a few atoms diameter in comparison does not have that sharp surface contacting transition. <br> | |||
The repulsion exponentially ramps up. <br> | |||
And before that there is [[van der Waals attraction]] with a rough phenomenological analogy to macroscale magnetism. <br> | |||
Completely different underlying physics though. Dipole electrostatics rathe rthan magnetostatics. <br> | |||
=== Sort of surprisingly sharp surfaces again when looking at just mild surface pressure (variations) === | |||
⚠️ '''But beware:''' Just like with the interior of the material this does not mean surfaces are soft and all that forgiving. <br> | |||
Small everyday macroscale surface pressures (like presing the finger on a table) <br> | |||
would correspond to a very minute fraction of that elastic range. <br> | |||
[[todo|run some example numbers and put them here.]] <br> | |||
Again. High surface pressure variations (@ MHz) => high energy turnover => potential high heat losses. <br> | |||
One will want to avoid such variations. <br> | |||
=== Fine tuning of surface distances and pressures === | |||
Fine tuning of mating surfaces in chemistry, structure, and contact pressure <br> | |||
is ione of the hugest subtopics for crystolecule machinery design. <br> | |||
⚠️ Just plainly contacting surfaces already "suffer" from a very high preload merely from [[vdW forces]]. <br> | |||
As crude a rude of thumb It's about 1/00tth of covalent forces. <br> | |||
But diamond is enormously strong so even 1/100th of that is still huge. <br> | |||
These vdW attarction forces seem to be quite underestimated in common intuitive perception. <br> | |||
=== Negative pressure and maybe repusion === | |||
Designing systems with parts wedged between well spaced surface can allow for neurtralizing mor or less of that huge vdW preload. <br> | |||
😯 Interestingly (as acuriosity of the nanoscale) even permanent [[negative pressure bearings]] can be achived up to bunded negative pressure. <br> | |||
Don't be confused by the term "pressure". This about solid surface to surface pressing pressure. <br> | |||
No gasses here. And no liquid lubricants either. It'd just be molecular gravel at thsi scale.<br> | |||
😯 As side-note: There is an interesting exotic repusive part of vdW forces that is [[repuslive keesom forces]]. <br> | |||
It's repulsively opposed real dipoles that are rotation constrained from escaping this unfavorable alignment. <br> | |||
Nitrogen monolayer pasivated Si(111) facing each other may have taht situation going on. <br> | |||
{{Todo|[[Superlubric groove slider simulations]] needed, to check for changed equilibrium distance.}} <br> | |||
=== Surface distance and pressure fine tuning stratregies === | |||
The discrete steps of size makes fitting linear rods in load channels via the naive approach quite limited. <br> | |||
It jumps from way too tight to way too loose with huge likelyhood. <br> | |||
Strained shell bearings give a bit mre options but these are hard to make needing jigs. <br> | |||
See: [[Design fro manufacturing for crystilecular systems]] <br> | |||
Best results might be gained by a method like: <br> | |||
Wedging sliding rods betwen two V or W groove self centering channels that on both cntact sides <br> | |||
set a finely adjusted contact distance and almost equivalently a fineyl set contact pressure. <br> | |||
Speculating: The repulsive keesome forces may be usable to increase contact distance without going changing forces. <br> | |||
See: [[Fine tuning crystolecule slider bearing pressure by self-center wedging]] <br> | |||
=== [[Design for superlubricity]] === | |||
Low or negative presure bearings may have such low magnitute remnant wavyiness sliding energy barriers <br> | |||
that they turn out [[supercritically superlubric]] even for interfaces that <br> | |||
were not designed for [[superlubricity from incommensurate alignment]]. <br> | |||
[[todo|Investigate via first principles simulations.]] <br> | |||
See: [[superlubricity from large contact distance bearings]] <br> | |||
See also [[Design for superlubricity]]. <br> | |||
=== Avoid sliding contacts in first pace if possible. === | |||
Also remember: '''The best contact is no contact.''' <br> | |||
Go for fee moving chains that stretch over long ranges <br> | |||
not contacting anything over long stretches if avodiable. | |||
= Applicability of 3D FDM printing for Crystolecule Design = | |||
Main article: [[applicability of macro 3D printing for nanomachine prototyping]] | Main article: [[applicability of macro 3D printing for nanomachine prototyping]] | ||
| Line 17: | Line 115: | ||
One needs to look out for those in the judgment whether bulk macroscale designs could be ported over to nanoscale crystolecule designs. | One needs to look out for those in the judgment whether bulk macroscale designs could be ported over to nanoscale crystolecule designs. | ||
== physical models for visualization only == | |||
Non functional models purely for visualization that have all their surface atoms visible and color coded require more expensive full color powder printing. (Hard brittle and rough material) | Non functional models purely for visualization that have all their surface atoms visible and color coded require more expensive full color powder printing. (Hard brittle and rough material) | ||
== demos of principles == | |||
The author of this Wiki [[APM:About|(about)]] conducts a meta project that aims to build up a collection of 3D-printable 3D-models (mainly in ''atom aware bulk limit'') that will hopefully turn out to be useful in the development and understanding of advanced nanofactories. See main article: [[The DAPMAT demo project]] | The author of this Wiki [[APM:About|(about)]] conducts a meta project that aims to build up a collection of 3D-printable 3D-models (mainly in ''atom aware bulk limit'') that will hopefully turn out to be useful in the development and understanding of advanced nanofactories. See main article: [[The DAPMAT demo project]] | ||
= Some things to take care of = | |||
== avoid quartz like solid CO<sub>2</sub> or the like == | |||
Too much oxygen must not be brought in direct bonding contact with carbon atoms since this may practically represent solid CO<sub>2</sub> which will likely behave like an highly potent explosive. The same goes for other combinations that are known to be highly energetic from normal cemistry. | Too much oxygen must not be brought in direct bonding contact with carbon atoms since this may practically represent solid CO<sub>2</sub> which will likely behave like an highly potent explosive. The same goes for other combinations that are known to be highly energetic from normal cemistry. | ||
Some examples: room temperature solid nitrogen (in sp3 hybridisation), oxygen chains, ... | Some examples: room temperature solid nitrogen (in sp3 hybridisation), oxygen chains, ... | ||
== avoid too high interface pressure in sleeve bearings == | |||
If the fit gets too tight the atom "teeth" may spontaneously jump back with thermal speeds instead of lowly bend back with machine speeds | If the fit gets too tight the atom "teeth" may spontaneously jump back with thermal speeds instead of lowly bend back with machine speeds | ||
the induced snap back overshoot vibrations will be fully dissipated and not, as desired, almost fully recuperated. Instead as a bearing the device will work as friction unit. | the induced snap back overshoot vibrations will be fully dissipated and not, as desired, almost fully recuperated. Instead as a bearing the device will work as friction unit. | ||
== check for too strained spots in auto-generated passivation layers == | |||
Concave edges passivated with hydrogen sometimes causes the hydrogen atoms to massively overlap. | Concave edges passivated with hydrogen sometimes causes the hydrogen atoms to massively overlap. | ||
| Line 45: | Line 143: | ||
{{wikitodo| collect some tricks here how this can be made easier}} | {{wikitodo| collect some tricks here how this can be made easier}} | ||
== avoid situations where poisonous molecules may be released on thermal or chemical attack == | |||
{{wikitodo|elaborate on this}} | {{wikitodo|elaborate on this}} | ||
| Line 57: | Line 155: | ||
Thus one can very effectively protect internal materials from chemical attack. | Thus one can very effectively protect internal materials from chemical attack. | ||
= Regarding molecular dynamics = | |||
Main article: [[Molecular dynamics simulation]] | Main article: [[Molecular dynamics simulation]] | ||
== Avoid elements to the left of the carbon group – at least for now == | |||
Electron deficiency bonds are misrepresented nanoengineer-1's current force field models. | Electron deficiency bonds are misrepresented nanoengineer-1's current force field models. | ||
| Line 67: | Line 165: | ||
A safe way to go is to not use them yet in crystolecule designs. | A safe way to go is to not use them yet in crystolecule designs. | ||
== Equilibration method == | |||
Nanoenginer-1 {{todo|version?|add latest nanoengineer-1 version 2015}} seems to use a rather naive force field equilibration method of just iteratively equilibrating all the atoms one after another and applying the changes all at once (not sure if this is the case - {{todo|check code|look into nanoengineer-1 code and check out the used equilibration method - is there documentation beside the code?}}) | Nanoenginer-1 {{todo|version?|add latest nanoengineer-1 version 2015}} seems to use a rather naive force field equilibration method of just iteratively equilibrating all the atoms one after another and applying the changes all at once (not sure if this is the case - {{todo|check code|look into nanoengineer-1 code and check out the used equilibration method - is there documentation beside the code?}}) | ||
| Line 74: | Line 172: | ||
{{todo|IIRC there where news of a new faster equilibration method - find it and link it here}} | {{todo|IIRC there where news of a new faster equilibration method - find it and link it here}} | ||
= The three levels of stability - chemical, thermal, mechanical = | |||
Stability against chemical attacks is hardest to achieve followed by stability against thermal loads (high temperatures). | Stability against chemical attacks is hardest to achieve followed by stability against thermal loads (high temperatures). | ||
| Line 97: | Line 195: | ||
Weak or extremely strained bonds may limit heat resistance. | Weak or extremely strained bonds may limit heat resistance. | ||
= Avoidance of toxicity = | |||
A good design software should constantly look at which elements are put near each other and in which bond topologies. | A good design software should constantly look at which elements are put near each other and in which bond topologies. | ||
| Line 106: | Line 204: | ||
Also sometimes problematic: fluorine, boron, ... | Also sometimes problematic: fluorine, boron, ... | ||
= Related = | |||
Intended working environment: vacuum / aggressive medium | Intended working environment: vacuum / aggressive medium | ||
| Line 127: | Line 225: | ||
* '''[[Scale agnostic design principles]]''' | * '''[[Scale agnostic design principles]]''' | ||
= External links = | |||
* molecular dynamics: {{WikipediaLink|https://en.wikipedia.org/wiki/Molecular_dynamics}} | * molecular dynamics: {{WikipediaLink|https://en.wikipedia.org/wiki/Molecular_dynamics}} | ||
Latest revision as of 18:17, 3 May 2026
This page is about issues with the design of crystolecules / DMEs.
For a definition of what they are see here: "What are crystolecules DMEs?"
You might instead be interested in: Design for manufacturing for crystolecular systems.
Comared to macroscale machine parts made from metals
Comaring to macroscale machinery might bet be the best approach here
due to this being the area people have expertise in.
- The overlap/similarities: See: Scale agnostic mechanical design principles
- The big differences: See chapters below.
Design rules from superelasticity of the very hard and very tough material
Unlike macroscale metals nanoscale diamond and gemstone like compound allow for large fully reversible bending and stretching.
As a rule of thumb it's above 10% stretch before any damage so stayin below that is safe.
⚠️ But beware: This does not at all mean everyting is soft and wobbly
as molecular dynamics simulations migh misleadingly suggest. Oh no, it's quite the contrary.
It is more like hyper spring steel. See page: A better intuition for diamondoid nanomachinery than jelly.
Large bending of diamond and similar stiff gems constitutes quite a high energy desnity nearing that of chemical energy storage.
Thus bending back and forth makes for quite high energy turnover and
even with quite high bening energy recuperation efficiencies
the small fraction of loss is still a quite big amount of thermalized energy.
Thus designing crystolecules with large bending in operation should likely …
– better be reserved to one time actuated assembly (related to design for manufacturing and
– better be avoided for MHz operation fequencies after assembly (in bulk agglomerations of nanomachinery)
Design rules from non-sharp surfaces at nanoscale
Macroscale surface contacts are like a Heaviside step-function.
They are perfectly approximated by a sharp step-function from no contact to (yes) contact.
Nanoscale machinery of just a few atoms diameter in comparison does not have that sharp surface contacting transition.
The repulsion exponentially ramps up.
And before that there is van der Waals attraction with a rough phenomenological analogy to macroscale magnetism.
Completely different underlying physics though. Dipole electrostatics rathe rthan magnetostatics.
Sort of surprisingly sharp surfaces again when looking at just mild surface pressure (variations)
⚠️ But beware: Just like with the interior of the material this does not mean surfaces are soft and all that forgiving.
Small everyday macroscale surface pressures (like presing the finger on a table)
would correspond to a very minute fraction of that elastic range.
run some example numbers and put them here.
Again. High surface pressure variations (@ MHz) => high energy turnover => potential high heat losses.
One will want to avoid such variations.
Fine tuning of surface distances and pressures
Fine tuning of mating surfaces in chemistry, structure, and contact pressure
is ione of the hugest subtopics for crystolecule machinery design.
⚠️ Just plainly contacting surfaces already "suffer" from a very high preload merely from vdW forces.
As crude a rude of thumb It's about 1/00tth of covalent forces.
But diamond is enormously strong so even 1/100th of that is still huge.
These vdW attarction forces seem to be quite underestimated in common intuitive perception.
Negative pressure and maybe repusion
Designing systems with parts wedged between well spaced surface can allow for neurtralizing mor or less of that huge vdW preload.
😯 Interestingly (as acuriosity of the nanoscale) even permanent negative pressure bearings can be achived up to bunded negative pressure.
Don't be confused by the term "pressure". This about solid surface to surface pressing pressure.
No gasses here. And no liquid lubricants either. It'd just be molecular gravel at thsi scale.
😯 As side-note: There is an interesting exotic repusive part of vdW forces that is repuslive keesom forces.
It's repulsively opposed real dipoles that are rotation constrained from escaping this unfavorable alignment.
Nitrogen monolayer pasivated Si(111) facing each other may have taht situation going on.
(TODO: Superlubric groove slider simulations needed, to check for changed equilibrium distance.)
Surface distance and pressure fine tuning stratregies
The discrete steps of size makes fitting linear rods in load channels via the naive approach quite limited.
It jumps from way too tight to way too loose with huge likelyhood.
Strained shell bearings give a bit mre options but these are hard to make needing jigs.
See: Design fro manufacturing for crystilecular systems
Best results might be gained by a method like:
Wedging sliding rods betwen two V or W groove self centering channels that on both cntact sides
set a finely adjusted contact distance and almost equivalently a fineyl set contact pressure.
Speculating: The repulsive keesome forces may be usable to increase contact distance without going changing forces.
See: Fine tuning crystolecule slider bearing pressure by self-center wedging
Design for superlubricity
Low or negative presure bearings may have such low magnitute remnant wavyiness sliding energy barriers
that they turn out supercritically superlubric even for interfaces that
were not designed for superlubricity from incommensurate alignment.
Investigate via first principles simulations.
See: superlubricity from large contact distance bearings
See also Design for superlubricity.
Avoid sliding contacts in first pace if possible.
Also remember: The best contact is no contact.
Go for fee moving chains that stretch over long ranges
not contacting anything over long stretches if avodiable.
Applicability of 3D FDM printing for Crystolecule Design
Main article: applicability of macro 3D printing for nanomachine prototyping
Some strong limitations for plastic FDM 3D-printing also hold for mechanosynthesis of crystolecules. (FDM ... fused deposition modelling i.e. printing with molten plastic from a nozzle) Thus, in the context of these limitations, if something works for FDM 3D-printing then chances are that the tested mechanical concept in question will work for mechanosynthesis of crystolecules too. (Not quite exploratory engineering but conservative design.)
Of course there clearly are limitations in the mechanosynthesis of crystolecules that are not present in FDM 3D-printing. One needs to look out for those in the judgment whether bulk macroscale designs could be ported over to nanoscale crystolecule designs.
physical models for visualization only
Non functional models purely for visualization that have all their surface atoms visible and color coded require more expensive full color powder printing. (Hard brittle and rough material)
demos of principles
The author of this Wiki (about) conducts a meta project that aims to build up a collection of 3D-printable 3D-models (mainly in atom aware bulk limit) that will hopefully turn out to be useful in the development and understanding of advanced nanofactories. See main article: The DAPMAT demo project
Some things to take care of
avoid quartz like solid CO2 or the like
Too much oxygen must not be brought in direct bonding contact with carbon atoms since this may practically represent solid CO2 which will likely behave like an highly potent explosive. The same goes for other combinations that are known to be highly energetic from normal cemistry. Some examples: room temperature solid nitrogen (in sp3 hybridisation), oxygen chains, ...
avoid too high interface pressure in sleeve bearings
If the fit gets too tight the atom "teeth" may spontaneously jump back with thermal speeds instead of lowly bend back with machine speeds the induced snap back overshoot vibrations will be fully dissipated and not, as desired, almost fully recuperated. Instead as a bearing the device will work as friction unit.
check for too strained spots in auto-generated passivation layers
Concave edges passivated with hydrogen sometimes causes the hydrogen atoms to massively overlap. Sometimes two hydrogens can be replaced by a oxygen bridge but this introduces tension that may detrimentally deform the crystolecule. Alternating with oxygen with its bigger cousin sulfur or nitrogen with phosphor might help in some cases.
Since passivation atoms add thickness it can be tricky to create parts complementary in shape.
(wiki-TODO: collect some tricks here how this can be made easier)
avoid situations where poisonous molecules may be released on thermal or chemical attack
(wiki-TODO: elaborate on this)
- Cyanides
- organophosphorus compounds (leave to Wikipedia - please come back again)
- Halogenides
- Small polyaromatic molecules - organic pigments (leave to Wikipedia - please come back again) have usually low toxicity but also low biodegradability - related: color emulation
Designing mechanical metamaterials in such a way that in case of overload they do only break at predeterimined internal surfacts allow one to keep internal machinery as isolated as possible. Thus one can very effectively protect internal materials from chemical attack.
Regarding molecular dynamics
Main article: Molecular dynamics simulation
Avoid elements to the left of the carbon group – at least for now
Electron deficiency bonds are misrepresented nanoengineer-1's current force field models. A nitrogen atom adjacent to a boron atom embedded in a diamond crystal shouldn't strongly repel each other but instead behave almost like carbon atoms since the boron has the space for the nitrogens excess electron. Since aluminium is to an electron deficient element it is likely to misbehave the same way as boron does in the NanoEngineer-1 model. A safe way to go is to not use them yet in crystolecule designs.
Equilibration method
Nanoenginer-1 (TODO: version?) seems to use a rather naive force field equilibration method of just iteratively equilibrating all the atoms one after another and applying the changes all at once (not sure if this is the case - (TODO: check code)) that does not scale well. A self adapting (TODO: add implementation ideas) 6D space Fourier space deformation method might be implementable to speed up equilibration massively. (TODO: IIRC there where news of a new faster equilibration method - find it and link it here)
The three levels of stability - chemical, thermal, mechanical
Stability against chemical attacks is hardest to achieve followed by stability against thermal loads (high temperatures). Stability against mechanical loads is easiest to achieve.
A good design software should keep track of high energy bonds. Bonds can carry high energies either due to chemical instability (weak bonds that could form strong ones if rearranged) or due to very high strain. Some local spots / nests of high energy bonds may be ok but the products as a whole should not become explosive or a fire hazard.
Silicon (or metals) as fire quenching agent:
Materials that contain a lot of energy when located in an oxygen atmosphere (like on earth) are not necessarily a fire hazard.
Physical processes can stop a runaway chain reaction (a blazing major fire).
In nature on earth there's the quenching agent is water (which unfortunately can evaporate and lead to very dangerous situations)
In advanced gem-gum products of large scale (e.g. cities on Earth or balloons on Venus) one could use silicon as quenching agent. By replacing half of the carbon atoms in diamond (or lonsdaleite or other sp3 carbon compounds) one gets various forms of moissanite (SiC) which is ridiculously hard to burn.
Very quickly a protection layer of glassy slack forms which very effectively prevents further oxygen from reaching more of the moissanite.
Due to the possibility of sealing most of the nano-machinery in into a highly inert internal environment (practically perfect vacuum) the strongest restriction (chemical stability) can for the most part be lifted. (For everything not facing weather exposed surfaces). Water soluble compounds and even compounds that moderately react with water can be considered for usage.
For thermal stability one needs to mind "consistent design for external limiting factors". Weak or extremely strained bonds may limit heat resistance.
Avoidance of toxicity
A good design software should constantly look at which elements are put near each other and in which bond topologies. When advanced gem-gum products are attempted to be burned (which one may want to avoid in most cases - see: diamondoid waste incineration) then certain configurations are likely to undergo thermally induced reconstructions (and oxidations / nitrations) that lead to products compounds that can be slightly to highly toxic. There's a huge amount of knowledge about simple compounds and their toxicity and environmental impact. Even on the "surface" of the web (wikipedia) alone. This needs to be unified for a standard software interface.
Two abundant elements that are especially prone to create problematic compounds are phosphorus and chlorine. Also sometimes problematic: fluorine, boron, ...
Related
Intended working environment: vacuum / aggressive medium
At any time the accessible crystolecule structures are given by the available capabilities of Mechanosynthesis.
- Design levels
- Limits of construction kit analogy
- Pseudo phase diagram
- Isostructural bending
- 3D modeling
- The DAPMAT demo project
- Applicability of macro 3D printing for nanomachine prototyping
- Mass and spring molecular modelling
- Design of kaehler brackets
- Crystolecules can already be designed and analyzed in great detail but they cannot yet be built.
This is one area where a theoretical overhang can build up.
- The capabilities of the mechanosynthesis cores give design restrictions.
External links
- molecular dynamics: (leave to Wikipedia - please come back again)
Software:
- NanoEngineer-1
Here some active development continues to happen:
(Umbrella brand: MDS Molecular Dynamics Studio)
The new focus though seems to go more in the direction of science than engineering.
Situations to avoid or at least to be aware of:
- https://en.wikipedia.org/wiki/Fluxional_molecule
- https://en.wikipedia.org/wiki/Tautomer
- https://en.wikipedia.org/wiki/Fast_ion_conductor
- water exchanges its hydrogen atoms mixing H2O and D2O produces HDO - https://en.wikipedia.org/wiki/Heavy_water