Theory¶
One particle, one medium, one mechanism — nature's forces as contact forces
The idea in one breath¶
Empty space isn't empty. It's filled with an unimaginably vast sea of tiny particles called neutrinos — each moving fast and spinning as it goes — and that sea is the medium earlier physicists called the aether. Everything — the pull of gravity, the glow of light, the force that binds an atom's core — comes from this sea pushing on matter. Where the sea is dense and calm it pushes hard; where it flows fast it pushes less. When the push is stronger on one side of an object than the other, the object is shoved toward the weaker side. That leftover push is what we call a force.
If you've ever watched two boats drift together when the water rushes between them, or felt a shower curtain pull inward when the water runs, you've already seen this effect. Neumekan says the universe's forces work the same way — through a real, physical medium, following ordinary Newtonian mechanics in absolute space and time.
What makes this more than a picture is how it is built. The theory starts from a short list of assumptions about a single neutrino particle, works out the principles a sea of them must obey, and then derives gravity, light, and electromagnetism as results. Those forces are outputs of the mechanics, not extra postulates — the guiding rule is that nothing is assumed which could instead be shown.
How to read this page
The main text needs no advanced mathematics. The boxed "For the technically inclined" sections add the equations, derivations, and peer-reviewed references for readers and reviewers who want the full rigor. The framework is developed as a dependency chain — definitions → assumptions → principles → mechanisms → equations → correspondence with known physics → predictions → validation → falsification — and this page follows that spine.
1. The starting point: a real, massive medium¶
For three centuries, physicists believed light traveled through an invisible medium called the aether. They pictured it as weightless and perfectly still. When the famous Michelson–Morley experiment (1887) failed to detect any "aether wind," science concluded the aether didn't exist — and rebuilt physics without it.
Neumekan argues this was the wrong conclusion. The mistake wasn't believing in a medium — it was assuming the medium was weightless and motionless. A medium with mass would be dragged along with the spinning Earth, just like the atmosphere. There would be no aether wind to detect at ground level — which is exactly what Michelson and Morley found.
So the aether was never disproved. Only the massless aether failed. And we now know a perfect candidate for a massive medium already exists: the neutrino — a real particle, with real (if tiny) mass, pouring through all of space.
For the technically inclined
Experiments confirm neutrinos carry small but nonzero mass and permeate space. Neumekan identifies the neutrino with the historical aether (the Ether). A massive medium co-rotates with the Earth, so the relative velocity at the surface is ≈ 0 and the Michelson–Morley fringe shift vanishes — the null result is consistent with a massive aether, not evidence against it. This is the framework's founding inversion: it does not reject the aether, it rejects Einstein's rejection of it.
The signal at altitude¶
There is a second, less famous chapter. Dayton Miller repeated the experiment on Mount Wilson (~1.7 km up) and reported a persistent signal of about 9–10 km/s — not zero. For a century this was dismissed as experimental error. Neumekan reads it differently: the aether wind grows with altitude, because the co-rotating sea slips more freely the farther you rise above the ground that drags it.
For the technically inclined
The entrainment boundary layer follows a slip profile \(f(h) = 1 - e^{-h/\delta}\): near the surface \(f(0)\approx 0\) (Michelson–Morley null), and at altitude \(f(h)>0\) (Miller's residual wind). Near the ground this linearizes to roughly ~6 (km/s) per km of altitude, giving ≈ 10 km/s at Mount Wilson's 1.7 km and ≈ 0 at sea level. The decisive test favoring Miller over Shankland's 1955 thermal rebuttal is that Miller's signal tracked sidereal time (23h 56m, fixed to the stars), not solar time (24h, fixed to the daily heating cycle) — thermal artifacts follow the Sun, a genuine cosmic-frame wind follows the stars.
Stated honestly
Modern shielded, cryogenic optical-resonator experiments find no aether wind. Neumekan's obligation is to show that the altitude/shielding geometry and the slip profile together explain both these nulls and Miller's signal, without inventing free parameters. This reconciliation is argued, not yet closed.
2. The building blocks¶
The whole theory is built from one object — a single neutrino particle — given a short list of simple, falsifiable properties:
| Property | What it means |
|---|---|
| Equal mass | every particle carries the same tiny rest mass |
| Equal size | every particle has the same tiny diameter |
| Variable volume | particles can crowd together or spread out, so the sea's density varies from place to place |
| Collision only | they fly faster than light and interact only by bouncing — no long-range forces between them |
| Spin | each one rotates, like a thrown ball |
| Rough, elastic surface | their surfaces have friction, so a collision can turn a push into a twist, passing spin from particle to particle |
Two more assumptions fix the stage: the particles obey ordinary Newtonian mechanics at all speeds (no relativity of the particles themselves), and the sea defines a single absolute rest frame. From here on, everything is worked out, not posited.
From these properties, three behaviors emerge that do all the work of physics:
| Behavior | What it means | What it produces |
|---|---|---|
| Pressure | crowded, fast particles push outward | the "stiffness" of space |
| Flow | the sea drifts from crowded regions toward emptier ones | gravity |
| Spin | rough, rotating particles carry a sideways twist | light and electromagnetism |
For the technically inclined
Neutrino particles are rigid elastic spheres of equal mass \(m_a\) and diameter \(D_a\) but variable occupied volume \(V_a\), so density \(\rho = m_a/V_a\) varies in space. Collision pressure follows kinetic theory and depends on translational motion only: $\(p = \tfrac{1}{3}\rho\, v_{ca}^2 \qquad\text{(EQ-001)}\)$ A particle's kinetic energy splits into translation \(E_t\) and spin \(E_r\); the ratio \(\alpha=(E_t+E_r)/E_t\) (with \(\alpha=1\) for no spin) sets the medium's heat-capacity ratio \(\gamma=(3\alpha+2)/(3\alpha)\) (EQ-002). Because a sphere's moment of inertia scales as \(m_a D_a^2\) and \(D_a\) is minuscule, collisions impart an enormous spin — the seed of all magnetic effects, and the reason the neutrino's \(\gamma\) is predicted to sit near 1. Collision and spin speeds follow the Maxwell–Boltzmann distribution, which the framework derives mechanically from Newton's laws — with no mass-ratio limit — rather than assuming it (Lin & Lin, 2019, 2021; extended H-theorem, 2025).
3. How a force arises¶
Picture the sea of neutrinos as a fluid, and use the same physics that lifts an airplane wing or drifts two boats together:
- Pressure is just crowding and speed. More neutrinos, moving faster, push harder.
- The sea flows from crowded regions toward emptier ones.
- Fast flow pushes less sideways. Where the sea speeds up, its sideways push drops — the same trade-off that lifts a wing.
When the push is uneven across an object, the object is driven toward the weaker-push side. Every force in this theory is a version of that one idea.
For the technically inclined
Pressure and energy density are locked together, \(p = \tfrac{2}{3}E\) with \(E = \tfrac12\rho v^2\) (EQ-008, EQ-009), so at steady state pressure, energy, and density all satisfy Laplace's equation \(\nabla^2 p = \nabla^2 E = \nabla^2\rho = 0\) (EQ-020). A single source then gives an inverse-distance field \(E(r)=E_s\,r_s/r\). The "fast flow pushes less" step is the compressible Bernoulli relation \(\beta\,p/\rho + v_f^2/2 = \text{const}\) with \(\beta = 2.5\) (EQ-010). Crucially, the Laplace pressure alone integrates to zero net force over a closed surface — the force appears only when the Bernoulli flow correction is added.
4. The four forces, one mechanism¶
Gravity¶
A massive body sets the surrounding sea flowing toward it. By the wing-lift trade-off, the side where the sea flows faster pushes less, so the net push drives bodies together. Worked out properly, this leftover push comes out as an attractive force that falls off as \(1/r^2\) — Newton's law of gravity, but now with a physical cause instead of unexplained "action at a distance."
For the technically inclined
Integrating the Bernoulli-corrected pressure (the \(\cos^2\theta\) flow cross-term) over a sphere gives $\(\text{Force} = \frac{8\pi}{3}\,\frac{C_1 C_2}{r^2} \;\propto\; \frac{1}{r^2}\qquad\text{(EQ-011)}\)$ where each source strength \(C_i = k_E\,E_{si}\,r_{si}\) is set by its surface energy density and radius, and the factor \(8\pi/3\) comes from \(\int_0^\pi\cos^2\theta\sin\theta\,d\theta = \tfrac23\). This shares the exact algebraic form of Newton's gravity and Coulomb's law. Full derivation: Lin & Lin (2014), Substantial Aether Theory — Universal Gravity Force, J. Mechanics 30(3). The same result also follows from Lagally's theorem for two flow monopoles (EQ-026). Still open: recovering the numerical value of \(G\) from the aether parameters.
Light and electromagnetism¶
A gas normally carries only push–pull (sound-like) waves — not the sideways waves that light requires. That was the classic objection to any aether. Neumekan's answer is mechanical: because neutrinos are tiny and their surfaces are rough, a collision passes on a twist, and a medium that transmits twist can carry a transverse wave. Decouple the sea's equations of motion and that transverse wave falls out on its own, travelling at a fixed speed and matching Maxwell's source-free equations term for term. Light is not assumed to be a wave in the medium; it is derived as one.
The subtle part is why it comes out as light rather than an ordinary elastic vibration. In a normal solid a particle's spin is locked to the local swirl of the material, and the coupling is elastic — it acts on the spin angle, like a spring, which would give light a mass and a forbidden cutoff frequency. Neumekan's medium is different: the spin is independent of the flow's swirl, and the coupling acts on the spin rate (angular velocity), not the angle. That single change — a rate-type coupling in place of an elastic one — is exactly what removes the mass and leaves the clean, massless photon.
For the technically inclined
The medium is a micropolar (Cosserat–Eringen) continuum — the modern form of the rotational aether of MacCullagh (1839), FitzGerald and Larmor. Its constitutive law extends Navier's elastic-solid law with independent self-spin \(\Omega\) and volume-rotation \(\omega\), $\(\sigma_{ij} = \lambda\,\delta_{ij}\varepsilon_{kk} + 2\mu\,\varepsilon_{ij} + 2\mu\,e_{ijk}(\Omega_k-\omega_k)\qquad\text{(EQ-012)}\)$ Taking the curl of the equation of motion removes the longitudinal (sound) mode and leaves a pure transverse system carrying a shear wave at $\(c = \sqrt{\mu/\rho}\qquad\text{(EQ-013)}\)$ Solved as a free field, its eigenvalues and polarization are identical to the source-free Maxwell equations, with the electric field corresponding to averaged flow and the magnetic field to averaged spin — an output of the derivation, never an input. The one requirement is that the rotational coupling be rate-type (\(\propto\dot{\vec\theta}\)), not elastic (\(\propto\vec\theta\)): an elastic coupling opens a frequency gap \(\omega_0^2=2\kappa/\rho j\) (a photon mass), while a rate coupling closes it. Full derivation: Lin & Lin (2014), Substantial Aether Theory — Electromagnetic Wave, J. Mechanics 30(4); the elastic-vs-rate distinction and its variational (Lagrangian + Rayleigh-dissipation) derivation are set out in the group's companion micropolar papers.
What "charge" and "current" really are¶
In this picture there is no charge substance. Neutrinos are electrically neutral. What we label "charge" is just the role a spot plays in the flow: a source that pumps the sea outward, or a sink that draws it in. A proton is a sink, an electron the opposite-sense flow, and their attraction is simply the sea flowing into the proton — no charge required. An electric current is likewise not a stream of charged particles but a directed flow of neutral neutrinos, pushed from high pressure toward low, which is why a current-carrying wire shows no net charge to the outside world.
Stated honestly — the sign problem
There is a real, unresolved difficulty here, and we flag it rather than paper over it. Naive steady-flow hydrodynamics gives the wrong sign for like charges: two identical flow monopoles come out attracting, whereas two like charges must repel. Getting the observed repulsion out of the flow picture is the single biggest open problem in Neumekan's electromagnetism. Candidate fixes — the unsteady/Bjerknes term, the source/sink energy assignment, or the flow sense — are under investigation. Until one is shown to work, the attraction/repulsion rule is asserted, not derived.
For the technically inclined
Charge is modelled as a monopole of the neutral flow field; two flow monopoles interact as \(F\propto C_1C_2/r^2\), the same algebraic form as gravity, with the source/sink role standing in for the charge sign. A steady current is a neutral drift \(\vec J \propto \rho_\nu\vec v_{\text{flow}}\) down the pressure gradient, and the magnetic field is the vorticity of that drift, \(\vec B \propto \tfrac12\nabla\times\vec v\). Two open items: (1) the sign of the like-charge force (above), and (2) the dimensioned source law — recovering Coulomb's constant and the coulomb itself from the neutrino parameters.
The strong and weak nuclear forces¶
Now put two neutrons side by side. Each drains the sea around it, so the gap between them flows faster than their outer sides. Faster flow in the middle means less push from the middle — so the outside push wins and the two neutrons are squeezed together. That squeeze is the strong nuclear force that binds the nucleus. Nuclear decay, in turn, is the sea's pressure occasionally pushing a neutron back out.
Honest status
Gravity and electromagnetism are derived in full in peer-reviewed papers. The strong and weak forces are so far explained qualitatively — a compelling mechanical picture, but not yet a complete, quantitative derivation. This is the active frontier of the work. The two-neutron field is set up as a superposition of low-order solid-harmonic modes \((l,m)\) centered on each neutron (EQ-024), with the force given by the surface integral of the resulting Bernoulli pressure.
5. A number the theory actually predicts¶
A good theory makes numbers, not just stories. Treating neutrinos as a gas that shares space with ordinary air molecules, kinetic theory lets us calculate the neutrino's mass from known gas properties:
This lands below the experimental upper limit set by neutrino detectors — so it is consistent with measurement, and it is falsifiable.
For the technically inclined
For two species that collide and thermalize, the RMS relation \(m_1 v_1^2 = m_2 v_2^2\) holds with no mass-ratio limit (proven mechanically in Lin & Lin, 2019–2021; EQ-007). With equal particle counts (Avogadro) this gives \(m_\nu = m_O\,(u_O/u_\nu)^2\). The collision speed follows from the wave speed via \(u = c\sqrt{3/\gamma}\) (EQ-017), using oxygen as the reference species, yielding the range above. Source: Lin & Lin (2023), Neutrino Mass Estimation by Kinetic Theory; consistent with the KamLAND-Zen upper limit.
Stated honestly
The same calculation implies a neutrino collision speed faster than light (\(u_\nu \approx 4\)–\(5\times10^8\) m/s, i.e. \(u=c\sqrt{3/\gamma}\)). Neumekan treats this as a real, local collision velocity in the neutrino frame — allowed because the particles obey Newtonian, not relativistic, mechanics — and flags it openly as a falsifiable exposure. The neutrino's spin behaviour (its heat-capacity ratio \(\gamma_\nu\)) is predicted to sit near 1, because spin holds most of its energy, but is only bounded (\(1<\gamma<5/3\)) at present — which is why the mass is a range rather than a single value.
6. Bold, falsifiable predictions¶
A theory is only as good as the risks it takes. Neumekan makes distinctive predictions that depart sharply from mainstream physics:
- A repulsive force between two stars (two sources of the sea), and likewise between two black holes (two sinks).
- Black holes are super-heavy nuclei — concentrations of nuclear matter far heavier than any natural atom, not the event-horizon objects of General Relativity.
- A black hole can explode into a new star under the pressure of a nearby star — and a dead star can collapse into a black hole.
- Radioactive waste decays faster near the Sun, where the neutrino pressure is higher.
- A faster-than-light "longitudinal" wave. Because the sea is compressible, it carries a second, push–pull wave in addition to light — one that travels faster than light itself, decoupled from electromagnetism, and a candidate carrier for near-instant gravitational signalling.
- The neutrino's heat-capacity ratio is close to 1 — a direct, testable consequence of its spin holding most of its energy.
If these fail, the theory is wrong — and that is exactly what makes them worth testing.
For the technically inclined
The compressible medium carries both a transverse wave (light, at the shear speed \(c_T=\sqrt{\mu/\rho}\)) and a longitudinal wave (at \(c_L=\sqrt{(\lambda+2\mu)/\rho}\)). Their ratio is fixed by the moduli alone, \(c_L/c_T=\sqrt{2+\lambda/\mu}>1\) for any mechanically stable medium — so the longitudinal mode is genuinely superluminal. Nineteenth-century workers (MacCullagh, Larmor) deliberately dropped this mode to avoid it; Neumekan keeps it as a real, falsifiable channel (Theory-Chain Prediction 9).
The hardest challenges, stated plainly
Two of these predictions face serious observational tension today: stellar binaries are gravitationally bound (not repelling), and LIGO/Virgo have recorded black-hole mergers inspiraling (not repelling). Neumekan must either identify the mechanism that overturns its own repulsion prediction, or accept falsification on these points. We record the tension rather than bury it.
7. From force to atoms and molecules¶
The same calculation that gives the force between two neutrons can be pushed further:
- Hold the background pressure constant (ignore gravity) and the neutron-pair calculation reproduces patterns that look like the electron clouds quantum mechanics draws around a nucleus — but here they fall straight out of a mechanical fluid, with no Schrödinger equation.
- Scale up to many nuclei and the method, in principle, builds toward molecular structure — far more complex, but the same physics throughout.
For the technically inclined
Neumekan argues that quantum mechanics describes what happens without a mechanical why, and offers the aether flow field as the missing mechanism. This is a deliberately strong, still-unsettled claim.
8. What's still open¶
We are honest about the gaps. To finish the force calculation, three quantities still need to be pinned down — by experiment or further theory:
- How strongly the sea "grabs" a neutron as it flows past (a friction figure).
- How dense the sea is right at a neutron's surface.
- How dense the background sea is across the cosmos.
These aren't hidden problems — they are the clear next questions, and naming them is how the theory moves forward. The bigger open items are just as plainly stated: getting the right sign for the force between like charges (today the steady-flow picture gives the wrong one); connecting the derived inverse-square law to the measured value of \(G\); recovering the dimensioned laws of electric charge and current; confronting the superluminal-wave and altitude entrainment-slip predictions with modern optical-resonator tests; and reconciling the repulsion predictions with bound binaries and black-hole mergers.
For the technically inclined
The two-neutron problem is solved as a superposition of low-order solid-harmonic modes \((l,m)\) centered on each neutron, with boundary conditions on the neutron surfaces; the force is the surface integral of the resulting non-uniform Bernoulli pressure. The three undetermined boundary parameters are the neutrino–neutron friction coefficient, the surface neutrino density, and the cosmological background density. A numerical two-neutron example is implemented in the NeuMekan simulation code.
Where to go next¶
- Publications — the peer-reviewed papers behind every derivation above
- About — the people and the decades of work
- Contact — questions, review, or collaboration welcome