Encyclopedia Nuclear Nuclear Fission Energy From Jcost
ARTICLE 4 claims 4 theorems
Nuclear Fission Energy From Jcost
The standard 200 MeV of a uranium-235 fission event appears in Recognition Science as a ratio of masses run through a single cost function.
The fission energy relation
Nuclear fission releases energy when a heavy nucleus splits. For uranium-235, one event typically releases about 200 MeV (million electron volts), a figure measured in laboratories and used across reactor physics. The energy comes from the difference in binding energy between the original nucleus and its fragments, a fact established in the 1930s by Lise Meitner and Otto Frisch.
In Recognition Science, the framework models this same release through a ledger, a discrete record of recognition events, and a forced cost, the price the ledger pays for each recognition. The central cost function is J(x) = (x + 1/x)/2 - 1. It vanishes when its input equals 1, is nonnegative for positive inputs, and has a minimum at x = 1. The framework writes fission energy as E_fission = phi^rung_U * J(phi) * E_coh, where phi is the golden ratio (about 1.618), rung_U is a step index on a phi-power ladder, and E_coh is a coherence energy scale.
With rung_U near 30 and E_coh = 0.121 MeV, the expression gives phi^rung * 0.121 MeV, which lands near 200 MeV when phi^rung is about 1653, close to phi^21 (about 10946). This is a structural identification, not a derivation: the module does not define what m and e are for uranium specifically.
The machine-checked library of formal theorems proves three general facts about the cost function applied to a ratio m/e. First, domainCost r r = 0: the cost vanishes when the two quantities are equal. Second, domainCost m e is nonnegative for positive m and e. Third, the threshold phi - 3/2 is positive. These hold for any positive real inputs, because domainCost is defined as J(m/e) with no reference to a specific physical system.
The module itself establishes only these universal facts. It proves nothing specific to nuclear fission, because the definition of m and e in fission terms is absent. The 200 MeV agreement is a research note recording where the idea was meant to go, not a theorem. What the module does show is that the cost function has the right basic shape: zero at equality, nonnegative elsewhere, and a positive threshold tied to the golden ratio.
THEOREM domainCost_at_eq · IndisputableMonolith/Nuclear/FissionEnergyFromJCost.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/Nuclear/FissionEnergyFromJCost.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/Nuclear/FissionEnergyFromJCost.lean
theorem canonicalThreshold_pos : 0 < canonicalThreshold := by
unfold canonicalThreshold; linarith [phi_gt_onePointFive]
THEOREM domainCost · IndisputableMonolith/Nuclear/FissionEnergyFromJCost.lean
def domainCost (m e : ℝ) : ℝ := Jcost (m / e)
What this page does not claim
The 200 MeV agreement is a derived theorem; it is a structural note recording an intended direction. The module defines what m and e mean for uranium-235; it does not. The framework derives the fission energy from first principles; it only proves universal properties of the cost function.
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/Nuclear/FissionEnergyFromJCost.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 definition of m and e in uranium-235 terms would make the fission energy claim a theorem?
- How does the phi-power ladder assign rung values to specific nuclides?
- What is the coherence energy E_coh physically, and how is it measured or derived?
- Does the 200 MeV figure hold for all fission events or only the most probable split?
- How does the cost function's threshold phi - 3/2 relate to a fission barrier?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM domainCost_at_eq · IndisputableMonolith/Nuclear/FissionEnergyFromJCost.lean
theorem domainCost_at_eq (r : ℝ) (h : r ≠ 0) : domainCost r r = 0 := by unfold domainCost; rw [div_self h]; exact Jcost_unit0The cost vanishes when the two quantities are equal. domainCost_at_eq · IndisputableMonolith/Nuclear/FissionEnergyFromJCost.leanTHEOREM domainCost_nonneg · IndisputableMonolith/Nuclear/FissionEnergyFromJCost.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 cost is nonnegative for positive m and e. domainCost_nonneg · IndisputableMonolith/Nuclear/FissionEnergyFromJCost.leanTHEOREM canonicalThreshold_pos · IndisputableMonolith/Nuclear/FissionEnergyFromJCost.lean
theorem canonicalThreshold_pos : 0 < canonicalThreshold := by unfold canonicalThreshold; linarith [phi_gt_onePointFive]The threshold phi - 3/2 is positive. canonicalThreshold_pos · IndisputableMonolith/Nuclear/FissionEnergyFromJCost.leanTHEOREM domainCost · IndisputableMonolith/Nuclear/FissionEnergyFromJCost.lean
def domainCost (m e : ℝ) : ℝ := Jcost (m / e)The module proves nothing specific to nuclear fission, because domainCost is defined as J(m/e) with no reference to one. domainCost · IndisputableMonolith/Nuclear/FissionEnergyFromJCost.lean