Encyclopedia Physics Physics Combustion From Jcost
ARTICLE 3 claims 3 theorems
Physics Combustion From Jcost
Combustion is rapid oxidation releasing heat and light; in Recognition Science its efficiency balance becomes a proved cost equation.
Combustion as recognition cost
Combustion is the rapid oxidation of a fuel that releases heat and light. In an engine or flame, the key quantity is the fuel-air equivalence ratio φ, the actual fuel-to-air ratio divided by the stoichiometric ratio. A flame burns stoichiometrically when φ equals 1, meaning exactly enough air is present to burn all the fuel. Rich mixtures (φ greater than 1) have excess fuel; lean mixtures (φ less than 1) have excess air. The adiabatic flame temperature, the hottest temperature a flame can reach with no heat lost, peaks at or near stoichiometric conditions.
The framework of Recognition Science models this balance with a cost function, a number that measures how far a system sits from equilibrium. The framework's central proved result is that any cost function satisfying five plain conditions must equal J(x) = (x + 1/x)/2 - 1. At x = 1, this cost is zero, which the framework identifies with stoichiometric combustion. Off-stoichiometric mixtures, whether rich or lean, carry a positive cost. The framework's machine-checked library of formal theorems proves both facts: J(1) = 0 and J(r) greater than 0 for any positive r not equal to 1.
In Recognition Science, the module also counts five canonical combustion regimes: lean deflagration, stoichiometric, rich deflagration, detonation, and distributed reaction zone. The framework proves this count equals 5 by a direct computation. The five regimes form a certificate structure that packages the count and the two cost facts into one object. The plain-language meaning is that the framework derives combustion's basic efficiency balance from its cost equation, rather than treating it as an independent assumption.
What this establishes in practice is a bridge from a purely mathematical cost function to a physical phenomenon. The stoichiometric point, where combustion is most efficient, is the same point where the recognition cost is zero. Rich and lean mixtures are exactly the states where the cost turns positive. This is a derivation, not a measurement: the framework shows that if the cost equation holds, combustion's central balance follows. It does not predict flame temperatures or reaction rates, and it does not replace the chemistry of oxidation.
THEOREM stoichiometric_equilibrium · IndisputableMonolith/Physics/CombustionFromJCost.lean
/-- Stoichiometric combustion = recognition equilibrium (J = 0). -/
theorem stoichiometric_equilibrium : Jcost 1 = 0 := Jcost_unit0
THEOREM off_stoichiometric_cost · IndisputableMonolith/Physics/CombustionFromJCost.lean
/-- Off-stoichiometric combustion has positive J-cost. -/
theorem off_stoichiometric_cost {r : ℝ} (hr : 0 < r) (hne : r ≠ 1) :
0 < Jcost r := Jcost_pos_of_ne_one r hr hne
THEOREM combustionRegimeCount · IndisputableMonolith/Physics/CombustionFromJCost.lean
theorem combustionRegimeCount : Fintype.card CombustionRegime = 5 := by decide
What this page does not claim
This module does not derive flame temperatures or reaction kinetics. The identification of stoichiometric with J = 0 is a framework modeling choice, not a measured law. The five regimes are enumerated, not derived from the cost equation.
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/Physics/CombustionFromJCost.lean
expected axiom basis: [propext, Classical.choice, Quot.sound] (the Lean kernel's standard three; no RS-specific axioms)
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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 physical conditions select each of the five combustion regimes?
- How does the adiabatic flame temperature vary with the equivalence ratio?
- Does the cost function extend to predict ignition energy or flame speed?
- What distinguishes a detonation from a deflagration in this framework?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM stoichiometric_equilibrium · IndisputableMonolith/Physics/CombustionFromJCost.lean
/-- Stoichiometric combustion = recognition equilibrium (J = 0). -/ theorem stoichiometric_equilibrium : Jcost 1 = 0 := Jcost_unit0The framework proves J(1) = 0, identifying stoichiometric combustion with zero recognition cost. stoichiometric_equilibrium · IndisputableMonolith/Physics/CombustionFromJCost.leanTHEOREM off_stoichiometric_cost · IndisputableMonolith/Physics/CombustionFromJCost.lean
/-- Off-stoichiometric combustion has positive J-cost. -/ theorem off_stoichiometric_cost {r : ℝ} (hr : 0 < r) (hne : r ≠ 1) : 0 < Jcost r := Jcost_pos_of_ne_one r hr hneThe framework proves J(r) is positive for any positive r not equal to 1, covering rich and lean mixtures. off_stoichiometric_cost · IndisputableMonolith/Physics/CombustionFromJCost.leanTHEOREM combustionRegimeCount · IndisputableMonolith/Physics/CombustionFromJCost.lean
theorem combustionRegimeCount : Fintype.card CombustionRegime = 5 := by decideThe framework proves the number of combustion regimes equals 5. combustionRegimeCount · IndisputableMonolith/Physics/CombustionFromJCost.lean