Page 2 of 2

Re: Atomic Displacements in the RS

Posted: Tue Apr 14, 2026 2:08 pm
by MWells
A useful clarification here is that a lot of the confusion comes from treating Larson’s notation as though it were the structure itself.

Larson uses more than one notational compression. In some forms the photon/reversal base is explicit, while in later atomic forms it is suppressed. So if one person is reasoning from a form that still includes the base and another is reasoning from the later compressed atomic notation, they can look “off by one” even when they are talking about the same structure. This is why hydrogen and the early rotational base can appear inconsistent if the notation systems are mixed.

Also, a-b-c should not be read too literally as ordinary geometric coordinates. They are displacement components of a rotating scalar-motion system:
  • a and b belong to the two-dimensional magnetic organization
  • c belongs to the one-dimensional electric organization
So the key issue is not “where is the missing third spatial coordinate?” but “what organization of scalar motion is being counted in each component?”

The electric/magnetic equivalences are also not best understood as naive Euclidean geometry. The atom is not built by taking a sphere or cube literally and then converting that geometry. The conversion rules are structural equivalences between magnetic and electric organization in the rotating scalar-motion system. That is why trying to interpret every step as ordinary area/volume geometry leads to confusion.

The safest way to reconstruct Larson is to keep four things separate from the beginning:
  1. primitive base / reversal
  2. magnetic organization
  3. electric organization
  4. notation compression
In practice, that means:
  • start with the least-compressed form, not the finished atomic shorthand
  • decide first whether the primitive/reversal base is still explicit or has already been suppressed
  • keep magnetic and electric organization distinct
  • do not mix particle notation, atomic notation, and early-base notation as though they were the same layer
  • if something seems off by one unit, first ask whether one form includes the base and the other does not
So the safest way to read Larson is:
  • do not assume one notation covers every context
  • do not treat a-b-c as ordinary coordinates
  • do not mix explicit-base and compressed atomic forms
  • do not interpret electric/magnetic conversion as simple schoolbook geometry
  • only compress to the later shorthand after the structure is already understood
That does not solve every problem, but it removes a large fraction of the unnecessary confusion.