Difference between revisions of "Lagrangian mechanics for nanomechanical circuits"
m |
(added instructions with help of AI) |
||
| Line 8: | Line 8: | ||
See: [[The mechanoelectrical correspondence]] | See: [[The mechanoelectrical correspondence]] | ||
| − | {{wikitodo| | + | {{wikitodo|Add graphic with example system showing: equivalent circuit diagram, and some numbers.}} |
| + | |||
| + | Very complex mechanical systems can be easily mathematically modeled for simulation. | ||
| + | Like e.g. The [[Drive system]] of a [[gem-gum factory]] linking | ||
| + | * many [[chemomechanical converters]] | ||
| + | * across temporary elastic buffer storage springs | ||
| + | * to the many [[mechanosynthetic core]]s | ||
| + | via mechanical differentials that act (in analogy to electrical wire-junctions) as distribution nodes | ||
| + | to and from common transmission lines | ||
| + | * reducing losses and | ||
| + | * increasing system stiffness | ||
| + | * allowing for [[exothermy offloading]] and eventually even for [[dissipation sharing]] | ||
| + | |||
| + | Systems descriptions (typically coupled second order differential equations) <br> | ||
| + | can be split into a number of decoupled first order differential equations. <br> | ||
| + | So long they are not non-holonomic. | ||
== Springs are dominant over flywheels == | == Springs are dominant over flywheels == | ||
| Line 22: | Line 37: | ||
Other strategies like [[mechanical pulse width modulation]] maybe employable. | Other strategies like [[mechanical pulse width modulation]] maybe employable. | ||
| + | |||
| + | == Instructions for usage == | ||
| + | |||
| + | Used ChatGPT to jog my memory here. Seems plausible. | ||
| + | |||
| + | === Using Lagrangian Formalism for Simulating Complex Mechanical Systems === | ||
| + | |||
| + | The Lagrangian formalism is a powerful approach for simulating complex mechanical systems. Here's a step-by-step guide: | ||
| + | |||
| + | # Define the Lagrangian of the system as the difference between the kinetic energy and potential energy. | ||
| + | # Identify the generalized coordinates, denoted as ''q = (q1, q2, ..., qn)'', and their time derivatives, ''q̇''. | ||
| + | # Apply the Euler-Lagrange equations to derive the equations of motion. | ||
| + | # Introduce new variables ''u = (u1, u2, ..., un)'' representing the generalized velocities. | ||
| + | # Express the time derivatives of the generalized coordinates ''q̇'' in terms of the variables ''u''. | ||
| + | # Substitute the expressions for ''q̇'' into the original equations of motion. | ||
| + | # Rewrite the resulting coupled second-order differential equations as a set of decoupled first-order differential equations in terms of ''q'' and ''u''. | ||
| + | # Use the state-space representation of the system for numerical simulation and analysis. | ||
| + | |||
| + | '''Note''': Nonholonomic systems may require additional considerations and may not be able to be decoupled into first-order differential equations. | ||
== Advantages Lagrangian == | == Advantages Lagrangian == | ||
| Line 49: | Line 83: | ||
* [[https://en.wikipedia.org/wiki/Lagrangian_mechanics Lagrangian mechanics]] | * [[https://en.wikipedia.org/wiki/Lagrangian_mechanics Lagrangian mechanics]] | ||
| + | * [https://en.wikipedia.org/wiki/Euler%E2%80%93Lagrange_equation Euler–Lagrange equation] | ||
Revision as of 11:07, 9 June 2023
When thinking about nanotechnology one usually thinks about quantum mechanics and Hamiltonian mechanics.
But because nanomechanics is barely mechanical quantummechanics (it rather behaves quite classical)
the Lagrangian mechanics formalism is the one fitting to the problem.
Basically a classical network of axles, gears, springs, masses, and differentials taking the role of branching points.
See: The mechanoelectrical correspondence
(wiki-TODO: Add graphic with example system showing: equivalent circuit diagram, and some numbers.)
Very complex mechanical systems can be easily mathematically modeled for simulation. Like e.g. The Drive system of a gem-gum factory linking
- many chemomechanical converters
- across temporary elastic buffer storage springs
- to the many mechanosynthetic cores
via mechanical differentials that act (in analogy to electrical wire-junctions) as distribution nodes to and from common transmission lines
- reducing losses and
- increasing system stiffness
- allowing for exothermy offloading and eventually even for dissipation sharing
Systems descriptions (typically coupled second order differential equations)
can be split into a number of decoupled first order differential equations.
So long they are not non-holonomic.
Contents
Springs are dominant over flywheels
Operation frequencies are mainly determined by going slow to keeping friction losses
rather than being determined by deflections and vibrations from accelerations.
(See relatedpage: Same relative deflections across scales)
Proposed typical speeds are around ~1Mhz & ~5mm/s (see related page atomplacement frequency]]).
In free swinging unhampered spring-flywheel resonators without giant flywheels
the natural frequencies would be ways too high due to a lack of inertial mass of small flywheels.
You want a soft spring and a high flywheel inertia for a low frequency.
Other strategies like mechanical pulse width modulation maybe employable.
Instructions for usage
Used ChatGPT to jog my memory here. Seems plausible.
Using Lagrangian Formalism for Simulating Complex Mechanical Systems
The Lagrangian formalism is a powerful approach for simulating complex mechanical systems. Here's a step-by-step guide:
- Define the Lagrangian of the system as the difference between the kinetic energy and potential energy.
- Identify the generalized coordinates, denoted as q = (q1, q2, ..., qn), and their time derivatives, q̇.
- Apply the Euler-Lagrange equations to derive the equations of motion.
- Introduce new variables u = (u1, u2, ..., un) representing the generalized velocities.
- Express the time derivatives of the generalized coordinates q̇ in terms of the variables u.
- Substitute the expressions for q̇ into the original equations of motion.
- Rewrite the resulting coupled second-order differential equations as a set of decoupled first-order differential equations in terms of q and u.
- Use the state-space representation of the system for numerical simulation and analysis.
Note: Nonholonomic systems may require additional considerations and may not be able to be decoupled into first-order differential equations.
Advantages Lagrangian
- Ability to model non-conservative systems with dissipative systems and or non-potential forces (non gradient force-fields with nonzero rotor)
- Singular systems or systems with degeneracies in their configuration space systems with constraints
- may offer a more robust and versatile approach in pathological or chaotic systems
Why not Lagrangian for quantum mechanics
- Loss of (differential) operator formalism and commutation relations:
Commutation relations between operators determine the uncertainty relations.
What is measurable simultaneously and what is not. Complete sets of eigenvalues that are the observables and the result of wave collapse in a measurement process. - Non-conservative systems can be described but there are none. Everything is reversible at the smallest scales.
Related
- Mechanical-electrical analogies
- Nanomechanic circuits
- Mechanical circuit element
- Mechanical pulse width modulation
- Nanomechanics is barely mechanical quantummechanics
