Spiral Model

Motivation

Standard field theory describes particles as excitations of fields, often in an abstract, high-dimensional space. In my work I start from a more geometric and topological picture: a spiral structure built around a dipole, with a special role played by a zero point (node) where phase and direction can change.

This is not meant to replace the Standard Model. It is an attempt to provide a geometric, phase-based description of how stable matter and persistent fields could emerge from repeated, structured cycles.

Core Picture

The basic ingredients of the spiral model are:

– a dipole: two opposing “monopole” channels, conventionally labelled N and S,

– a spiral trajectory: not just a circle, but a helical / spiral path that needs a 720° cycle to return to its original state (spinor-like behaviour),

– a zero point (node): a narrow region where the field effectively passes through zero and where the phase can flip or re-route between channels.

Experimentally, I probe this using a magnetometer and a rotating setup. When I rotate a magnet through full cycles and record the field every 10 degrees, I consistently see:

– smooth “pulling” of the field within 10° sectors,

– sharp changes near certain angles,

– and two stable angular regions where the field crosses zero and the effective energy in that sector drops to a minimum.

These regions I interpret as manifestations of the node – the zero point in the spiral trajectory of the field.

Spinor-like 720° Behaviour

In the model, a full informational cycle requires 720°, not 360°. After 360° the state returns geometrically but with a flipped sign (similar to a spin-½ spinor). Only after 720° does it return to the original state.

Formally I encode this as a function s(θ) with:

s(θ + 360°) = −s(θ)

s(θ + 720°) = s(θ)

This double-cycle structure is at the heart of the spiral model and later becomes important when I talk about electrons and discrete pairs.

Electron as a Finite Spiral Structure

In this framework, I model the electron not as a point, but as a finite spiral structure composed of a fixed number of phase–coupled pairs (for now: 18 pairs in 36 domains). Each pair corresponds to a segment of the spiral that passes through the node and returns in the opposite channel.

The exact number is a working postulate, not yet a theorem. What matters at this stage is the idea:

– the electron has an internal phase structure,

– this structure is tied to a dipole and a node,

– and its stability comes from completing closed 720° cycles in a finite, repeatable pattern.

Relation to Measurements

The spiral model is constrained by real data:

– repeated magnetometer measurements as a function of angle,

– stable positions of nodes (angles where the field consistently crosses zero),

– asymmetry between “N” and “S” halves of the cycle.

The model must reproduce these features. Wherever it does not, it must be revised. This is a work in progress, not a finished doctrine.