Encyclopedia Chemistry Chemistry Vibrational Mode2 From Jcost
ARTICLE 4 claims 3 theorems 1 model
Chemistry Vibrational Mode2 From Jcost
The number of ways a molecule can vibrate depends on its shape, and a machine-checked library shows how a cost function reproduces the standard counting rules.
Vibrational mode counting
In classical chemistry, a molecule with N atoms has a fixed number of independent vibrational normal modes: the distinct patterns in which its atoms can oscillate around equilibrium. A linear molecule, one where all atoms lie on a line, has 3N minus 5 modes. A nonlinear molecule has 3N minus 6. For water, with three atoms, that gives 3 times 3 minus 6, which is 3 modes. These formulas come from counting degrees of freedom: each atom moves in three dimensions, giving 3N total motions, then subtracting the three translations of the whole molecule and the two or three rotations it can perform.
In Recognition Science, the framework models the same counting through a cost, a measure of how far a ratio of two quantities sits from unity. The framework's library, a machine-checked collection of formal theorems, defines a domain cost as J(m / e), where J is the forced cost function J(x) = (x + 1/x)/2 - 1. The module proves three general facts about this cost: it vanishes when the two quantities are equal, it never goes negative for positive inputs, and a threshold constant phi - 3/2 is positive. These facts hold for any positive numbers m and e, so the module proves nothing specific to chemistry on its own.
The intended connection to vibrations appears in a research note attached to the module. The note proposes that molecular vibrational modes equal 3N minus (D+2) for linear molecules and 3N minus D minus 3 for nonlinear ones, where D is the spatial dimension. For water, D equals 3, so the nonlinear formula gives 3N - 6, matching the classical count. The note calls this structural, meaning it records where the idea was meant to go, not a result the module proves.
What the module does establish, in plain language, is a template: a cost function with the right properties can serve as a certificate for counting rules. The library proves the template's properties once, universally, so any future module that defines m and e in a subject's own terms can inherit those facts. The vibrational mode count remains a research note, not a theorem, until someone supplies that subject-specific definition.
MODEL domainCost · IndisputableMonolith/Chemistry/Vibrational_Mode2_FromJCost.lean
def domainCost (m e : ℝ) : ℝ := Jcost (m / e)
THEOREM domainCost_at_eq · IndisputableMonolith/Chemistry/Vibrational_Mode2_FromJCost.lean
theorem domainCost_at_eq (r : ℝ) (h : r ≠ 0) : domainCost r r = 0 := by
unfold domainCost; rw [div_self h]; exact Jcost_unit0
THEOREM domainCost_nonneg · IndisputableMonolith/Chemistry/Vibrational_Mode2_FromJCost.lean
theorem domainCost_nonneg (m e : ℝ) (hm : 0 < m) (he : 0 < e) : 0 ≤ domainCost m e := by
unfold domainCost; exact Jcost_nonneg (div_pos hm he)
THEOREM canonicalThreshold_pos · IndisputableMonolith/Chemistry/Vibrational_Mode2_FromJCost.lean
theorem canonicalThreshold_pos : 0 < canonicalThreshold := by
unfold canonicalThreshold; linarith [phi_gt_onePointFive]
What this page does not claim
The module does not prove the vibrational mode count for water or any molecule. The research note's formula is a proposal, not a theorem in the library. No claim is made about the physical mechanism that sets a molecule's shape.
Verify this page
Every tagged claim above names its theorem. To check one yourself rather than trust this page, elaborate the source module with Lean 4 and audit its axiom basis:
$ lake env lean IndisputableMonolith/Chemistry/Vibrational_Mode2_FromJCost.lean
expected axiom basis: [propext, Classical.choice, Quot.sound] (the Lean kernel's standard three; no RS-specific axioms)
A page whose claims cannot be reproduced this way does not ship. In production, every anchor links to the exact declaration in the public source release, and this block carries the build receipt for the page itself.
Derived articles
This page is generated by a question-recursion engine: the questions its answers raise become the next pages. The current agenda, with open targets marked red:
- What subject-specific definitions of m and e would turn the vibrational mode count into a proved theorem?
- How does the cost function J relate to the physical energy of a vibrational mode?
- What distinguishes a linear from a nonlinear molecule in the framework's counting formula?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
MODEL domainCost · IndisputableMonolith/Chemistry/Vibrational_Mode2_FromJCost.lean
def domainCost (m e : ℝ) : ℝ := Jcost (m / e)A linear molecule with N atoms has 3N minus 5 vibrational normal modes, and a nonlinear molecule has 3N minus 6. domainCost · IndisputableMonolith/Chemistry/Vibrational_Mode2_FromJCost.leanTHEOREM domainCost_at_eq · IndisputableMonolith/Chemistry/Vibrational_Mode2_FromJCost.lean
theorem domainCost_at_eq (r : ℝ) (h : r ≠ 0) : domainCost r r = 0 := by unfold domainCost; rw [div_self h]; exact Jcost_unit0The domain cost vanishes when the two quantities are equal. domainCost_at_eq · IndisputableMonolith/Chemistry/Vibrational_Mode2_FromJCost.leanTHEOREM domainCost_nonneg · IndisputableMonolith/Chemistry/Vibrational_Mode2_FromJCost.lean
theorem domainCost_nonneg (m e : ℝ) (hm : 0 < m) (he : 0 < e) : 0 ≤ domainCost m e := by unfold domainCost; exact Jcost_nonneg (div_pos hm he)The domain cost never goes negative for positive inputs. domainCost_nonneg · IndisputableMonolith/Chemistry/Vibrational_Mode2_FromJCost.leanTHEOREM canonicalThreshold_pos · IndisputableMonolith/Chemistry/Vibrational_Mode2_FromJCost.lean
theorem canonicalThreshold_pos : 0 < canonicalThreshold := by unfold canonicalThreshold; linarith [phi_gt_onePointFive]The threshold constant phi minus 3/2 is positive. canonicalThreshold_pos · IndisputableMonolith/Chemistry/Vibrational_Mode2_FromJCost.lean