What, exactly, is gravity?
The standard answer is "attraction between masses." The EU answer is often "the electric force at large scales." Both of these describe a behaviour. Neither describes a mechanism. What is actually happening in the space between two bodies that results in the motion we call "falling"?
I will offer a mechanical model.
The Dielectric Medium as Pressure System
The Aether — call it the dielectric medium, the zero-point field, the vacuum — is not empty. It is a compressible medium with a variable density. Think of it as a fluid at pressure. Where nothing disturbs it, the pressure is uniform and nothing moves.
Matter disturbs it.
The nucleus of an atom is not a passive object sitting in the Aether. It is an active process — a standing wave that is continuously consuming the medium around it. The Aether flows inward and the standing wave is the result of that flow being captured into a resonant structure. In this model, Matter is a Drain — a local low-pressure sink in a high-pressure medium.
This is not metaphor. A pressure gradient in any compressible medium produces a net force toward the low-pressure region. That force is what we call gravity.
The consequence of this model is significant: Gravity is not a fixed property of mass. It is the flow rate of the Aetheric medium into the drain. And flow rate depends on the ambient pressure of the medium itself.
If the medium's background pressure changes — as it must, in a dynamic, electrically-active cosmos — then $G$ changes with it.
The Empirical Case: An Invitation to Look at Lageos Yourself
This is not idle speculation. The Lageos-I satellite has been in a near-circular orbit at ~5,900 km altitude since 1976. Its orbital evolution has been tracked to millimetre precision using Satellite Laser Ranging (SLR). Over 50 years that gives us 17,374 individual measurements of the semi-major axis — a near-continuous record of how the "gravitational constant" of the Earth has behaved for half a century.
The raw Two-Line Element (TLE) data is public. Space-Track.org carries the full archive. Anyone can download it.
I would encourage you to do one thing before we continue: download it, and run a simple statistical analysis. It will take twenty minutes. What you are looking for:
Three things to search for in the data:
- Point-to-point discontinuities. Compute Δa (the change in semi-major axis) between each consecutive measurement. You expect a smooth distribution around a small secular drift, with noise consistent with the known instrument precision (~10mm). Ask yourself: how many individual jumps larger than 10 metres appear in 50 years of data? Note the number down. Think about what a 10-metre jump means for an orbit that has moved less than 1 metre total in half a century.
- Rolling variance. Calculate the standard deviation of the semi-major axis in a rolling 100-point window across the full dataset. Look at the bottom 5th percentile — the "quietest" sections. Ask yourself whether those sections are uniformly distributed across the 50 years, or whether they form discrete bands in specific periods. A genuinely quiet orbit does not select decades.
- Time gaps. Look at the timestamp spacing. Satellite laser ranging is an active, continuous programme — there is no reason to stop. Ask yourself: how many gaps longer than 36 days appear in the record, and do they fall randomly, or do they cluster in any particular relationship to the discontinuities you found in step one?
What I will say is this: when I ran that analysis, the discontinuity count came to 865.
What the undoctored trend shows
Set that aside for a moment and look at the long-term signal. The orbital decay rate is not constant. The current rate (2015–2025) is approximately 230× the 50-year mean. At 5,900 km altitude, there is no atmosphere to cause drag. Tidal friction does not accelerate on a 10-year timescale.
The August 1996 data contains the clearest single event — a step-change of +1,456 metres in the semi-major axis, partially reversing within 48 hours. If we take the drain model seriously and ask what fractional change in the dielectric medium would produce that:
$$\frac{\delta\rho_A}{\rho_A}\bigg|_{1996} = \frac{\Delta a}{a} = \frac{1456}{12{,}271{,}000} \approx 1.19 \times 10^{-4}$$
A 0.012% impulse in the medium density, partially self-correcting in two days.
That is either the most extraordinary coincidence in the history of geodesy, or the medium through which the satellite travels briefly changed.
I leave the implications of 865 unexplained discontinuities in a public dataset — across 50 years of a satellite specifically designed to minimise noise — for the reader to sit with.
What this means for EU analysis
If $G$ is a flow rate rather than a constant, several things follow naturally:
- Orbital anomalies need no dark matter. Galaxies at different stages of their electrical history will sit in regions of different Aetheric density, and their rotational curves will reflect the local value of $G$ — not some invisible mass halo.
- The Pioneer anomaly is re-interpretable. An unexplained deceleration of ~8.74×10⁻¹⁰ m/s² toward the Sun is exactly what you would expect from a slowly increasing Aetheric density as the probe moves outward into a lower-pressure region — reducing the drain rate and therefore the effective $G$ experienced by the craft.
- Long-term geological instability has a non-tectonic driver. A rising Aetheric density increases the drain rate into the planetary nucleus, increasing internal dielectric stress in the crust. This is the mechanism behind cyclical geological catastrophism — and it is measurable.
These are not anomalies. They are data points on a curve. The curve has a peak.