Encyclopedia Gravity Gravity Zero Parameter Gravity Potential Negative
ARTICLE 3 claims 2 theorems 1 derived-unformalized
Gravity Zero Parameter Gravity Potential Negative
A small formal theorem about a negative sign in a potential function, and the large physical claim it is used to support.
A sign and its meaning
In classical Newtonian gravity, the gravitational potential Φ(r) = −GM/r is negative for any positive mass M at any positive distance r. The minus sign encodes that gravity is attractive: a test particle loses potential energy as it falls toward the source. This is one of the oldest results in physics, dating to Newton's Principia in 1687, and it is the starting point for the modern understanding of orbits, escape velocity, and gravitational time dilation.
The Recognition Science framework, a research program that derives physical structure from a single cost function, formalizes this same classical statement in its machine-checked library of formal theorems. Its declaration potential_negative proves, for its own definition of gravitational potential, that the potential is negative whenever both mass and distance are positive. The proof is a short chain of elementary facts: the potential is defined as −G·M/r, the product G·M/r is positive because G, M, and r are all positive, and the negative of a positive number is negative.
The theorem itself is deliberately modest. It does not introduce new physics; it verifies a sign convention. Its significance lies in what the framework builds around it. The framework's gravitational potential is not postulated but derived from its cost function, and the constant G is not a free parameter but is fixed as φ⁵/π, where φ is the golden ratio. The negative sign is then a consistency check: the derived potential has the same attractive character as the classical one.
In Recognition Science, this sign is part of a larger claim that gravity is not a fundamental force but emerges as the large-scale curvature of a discrete ledger of recognition events. The framework asserts that the Einstein field equations arise as the continuum limit of this curvature, and that the equivalence principle follows automatically because all mass comes from the same cost function. These are the grand claims; the theorem potential_negative is a small, verified step within them.
What the theorem does not claim is equally important. It does not prove that the framework's derivation of gravity is correct, nor that its value for G matches measurement. It does not establish that the continuum limit exists or that the Einstein equations follow rigorously. It only establishes a sign property for a definition. The physical bridge from the discrete ledger to continuous spacetime remains an open target, not a proved result.
THEOREM potential_negative · IndisputableMonolith/Gravity/ZeroParameterGravity.lean
/-- The gravitational potential is negative for positive mass at positive distance. -/
theorem potential_negative (M r : ℝ) (hM : 0 < M) (hr : 0 < r) :
gravitational_potential M r < 0 := by
unfold gravitational_potential
have eq : -G * M / r = -(G * M / r) := by ring
rw [eq]
exact neg_lt_zero.mpr (div_pos (mul_pos G_pos hM) hr)
THEOREM potential_negative · IndisputableMonolith/Gravity/ZeroParameterGravity.lean
/-- The gravitational potential is negative for positive mass at positive distance. -/
theorem potential_negative (M r : ℝ) (hM : 0 < M) (hr : 0 < r) :
gravitational_potential M r < 0 := by
unfold gravitational_potential
have eq : -G * M / r = -(G * M / r) := by ring
rw [eq]
exact neg_lt_zero.mpr (div_pos (mul_pos G_pos hM) hr)
DERIVED-UNFORMALIZED gravitational_potential · IndisputableMonolith/Gravity/ZeroParameterGravity.lean
/-- Gravitational potential at distance r (in RS units) from a mass M.
Φ(r) = -G·M/r where G is determined by φ. -/
noncomputable def gravitational_potential (M r : ℝ) : ℝ :=
-G * M / r
What this page does not claim
The theorem does not prove that gravity is emergent or that the Einstein equations follow from the ledger. The theorem does not establish that the framework's gravitational constant matches any measured value. The theorem does not show that the physical bridge from discrete ledger to continuous spacetime exists.
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/Gravity/ZeroParameterGravity.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 is the full derivation of the Einstein field equations from ledger curvature?
- How does the framework's value for the gravitational constant compare with the measured value?
- What exactly is the discrete ledger of recognition events?
- What is the precise sense in which the ledger curvature has a continuum limit?
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THEOREM potential_negative · IndisputableMonolith/Gravity/ZeroParameterGravity.lean
/-- The gravitational potential is negative for positive mass at positive distance. -/ theorem potential_negative (M r : ℝ) (hM : 0 < M) (hr : 0 < r) : gravitational_potential M r < 0 := by unfold gravitational_potential have eq : -G * M / r = -(G * M / r) := by ring rw [eq] exact neg_lt_zero.mpr (div_pos (mul_pos G_pos hM) hr)Its declaration potential_negative proves, for its own definition of gravitational potential, that the potential is negative whenever both mass and distance are positive. potential_negative · IndisputableMonolith/Gravity/ZeroParameterGravity.leanTHEOREM potential_negative · IndisputableMonolith/Gravity/ZeroParameterGravity.lean
/-- The gravitational potential is negative for positive mass at positive distance. -/ theorem potential_negative (M r : ℝ) (hM : 0 < M) (hr : 0 < r) : gravitational_potential M r < 0 := by unfold gravitational_potential have eq : -G * M / r = -(G * M / r) := by ring rw [eq] exact neg_lt_zero.mpr (div_pos (mul_pos G_pos hM) hr)The potential is defined as −G·M/r, the product G·M/r is positive because G, M, and r are all positive, and the negative of a positive number is negative. potential_negative · IndisputableMonolith/Gravity/ZeroParameterGravity.leanDERIVED-UNFORMALIZED gravitational_potential · IndisputableMonolith/Gravity/ZeroParameterGravity.lean
/-- Gravitational potential at distance r (in RS units) from a mass M. Φ(r) = -G·M/r where G is determined by φ. -/ noncomputable def gravitational_potential (M r : ℝ) : ℝ := -G * M / rThe framework's gravitational potential is not postulated but derived from its cost function, and the constant G is not a free parameter but is fixed as φ⁵/π, where φ is the golden ratio. gravitational_potential · IndisputableMonolith/Gravity/ZeroParameterGravity.lean