Numerical simulation study reveals gravitomagnetic field strength scales with momentum coherence across diverse topologies, indicating momentum organization amplifies frame-dragging effects.
Since the formulation of the gravitoelectromagnetic (GEM) decomposition of linearized General Relativity, the gravitomagnetic field of macroscopic bodies has been computed exclusively from their total angular momentum J, treating each body as a single rotating object. This approach is entirely adequate for rigid-body rotation, where all constituents co-rotate and the macroscopic formula B_g = GJ/(c²r³) correctly captures the collective field. However, a question that appears never to have been systematically posed is: what happens to the collective gravitomagnetic field when the microscopic momenta of the N constituents are not uniformly organized? The reason this question was never asked is straightforward: astrophysicists study objects that already rotate as wholes, particle physicists do not concern themselves with gravitational consequences at microscopic scales, and no engineering discipline has historically designed systems in which microscopic momentum organization is a controlled variable. The intersection of these domains — the deliberate architectural organization of momentum — did not exist until the development of Momentonics [5,6]. This work poses that question within standard linearized GR and answers it through over 7,000 independent numerical simulations using the Micro-Macro Momentum-Gravitomagnetic Model (MMGM). The principal result is the Momentonic Scaling Relation (MSR): |B_g| ∝ N^α(f), α(f) ≈ ½ + 0.31·f where f ∈ [0,1] is the fraction of coherently organized momentum. Three regimes emerge: the Statistical Regime (α ≈ ½, disordered momentum, ∝√N), the Momentonic Regime (½ < α < 1, partially organized), and the Constructive Regime (α = 1, perfectly organized, ∝N). A systematic study across eleven distinct spatial topologies establishes a second, independent result: ring-topology configurations universally achieve α = 1.000 regardless of orientation or eccentricity, while volumetric distributions are bounded by α ≈ 0.82. This admits a compact formulation: momentum organization determines the scaling regime; geometry determines how efficiently that organization becomes a collective gravitomagnetic field. The following table illustrates the gravitomagnetic contribution across physical and engineered systems, from ordinary matter to architectures operating within the Constructive Regime: System Regime α h_GM/h_GE GM contribution Ideal gas (300 K) Statistical 0.50 ~10⁻¹⁷ negligible Crystalline solid (300 K) Statistical 0.50 ~10⁻¹⁵ negligible Superconductor (Nb, 4 K) Momentonic ~0.75 ~10⁻⁷ detectable (SQUID) Earth (rotating) Constructive ~1.0 ~10⁻⁹ measured (GPB) ABÏON ring at 0.10c Constructive 1.00 ~0.07 7% of total ABÏON ring at 0.30c Constructive 1.00 ~0.60 60% of total Neutron star Constructive ~1.0 ~0.67 67% of total The table reveals a remarkable progression: the gravitomagnetic sector — negligible in ordinary matter — becomes the dominant component of the gravitational structure in systems with organized high-velocity momentum. The ABÏON counter-rotating ring architecture [5], operating within the Constructive Regime at relativistic peripheral velocities, achieves a gravitomagnetic contribution comparable to that of astrophysical objects — through engineered momentum organization rather than stellar-scale mass. No new physics is introduced. All results follow from the gravitational Biot-Savart law applied to individual constituents — the same equation available since the GEM formulation was established. The novelty lies entirely in asking a question that existing disciplinary boundaries made invisible: what is the collective gravitomagnetic consequence of microscopic momentum organization? The answer — that it varies by up to eleven orders of magnitude depending on organization and topology — establishes momentum organization as a gravitationally relevant physical variable that has been systematically overlooked for a century of General Relativity.
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Alvaro Fabian BRICIO ARZUBIDE (2026) studied this question.
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