gem-lte-core

GEM-LTE and magnetohydrodynamics: a supplementary view

This directory is a supplementary view of the GEM-LTE model that applies its equivalence to magnetohydrodynamics (MHD). The core model (in src/ and experiments/) solves Laplace’s tidal equations with tidal forcing on a shared manifold. The documents here ask what that model looks like when read as a toroidal plasma device:

Three device types organize the picture: the tokamak (axisymmetric), the reversed-field pinch (axisymmetric, with a self-reversing toroidal field) and the stellarator (non-axisymmetric, longitude-selective).

Model equatorial wind column

The unified view (model_column.py): a model of the equatorial zonal wind from 1 to 200 hPa.

The structure is modelled, not fitted point by point; the drive timing, gating and ENSO response come from the fits described below.

Documents

Document What it covers
landreman_gfd_synthesis_framework.md The original framework note mapping Landreman’s analytic 3D MHD equilibria (arXiv:2609.26742) onto GEM-LTE. Kept unchanged for reference; its unsupported claims are corrected in the next document.
landreman_lte_synthesis.md The checked synthesis. The exact link: the LTE response is a harmonic oscillator in the manifold, so fitted windings act like field lines with a rotational transform. Empirical tests, and section 8: the MHD ↔ rotating-fluid factor table, poloidal versus toroidal forcing, and the ENSO evidence (pinned standing mode, ORAS5 thermocline).
qbo_tokamak.md The detailed QBO device. A reversing poloidal drive; the comb impulse and the lunar ecliptic-latitude modulation, giving the 2.370-yr beat; the saturating core and strobe-gated penetration that make the shoulders; the helical, high-winding ripple; and the QBO record read as an MHD “shot” (1 yr = 1 s).
qbo_switching_plasma.md The short version: the QBO as a switched toroidal plasma, with existing laboratory systems for each ingredient (AC tokamaks, reversed-field pinches, oscillating-field current drive, the Plumb–McEwan tank). Phase-locking, absolute-phase and SAO tests.
stellarator_emulation.md The stellarator layer. Within the Pacific basin ENSO acts as one standing mode. In the equatorial winds, wavenumber > 0 emerges below 70 hPa and follows the ENSO windings, while the zonal-mean flow above follows the QBO.

Selected figures

The QBO as a switched toroidal plasma

The short version as a schematic. A switch (the Sun) fires twice per cycle with alternating polarity. A modulator (the Moon’s ecliptic latitude) sets each pulse’s height. A ring plasma reverses its edge flow when the drive passes a threshold. The stroboscopic beat gives the QBO’s 2.37-yr period with nothing tuned.

SAO above, QBO below

ERA5 equatorial winds, 1–70 hPa.

Where wavenumber > 0 emerges

The split between layers, by zonal wavenumber.

Pinned standing mode along the equator

ENSO’s spatial structure. Each winding’s amplitude and phase along the equatorial Pacific: one phase east of a node near 160°E, with Darwin and Tahiti pressure locked in opposite phase. A standing wave, not a travelling one.

Code and data

These documents are exploratory. Where a result is negative or not yet decisive, the documents say so (for example, the post-2006 QBO phase step, and the lack of winding-selective modes within the Pacific basin).