Dual Trumpet Black Hole Analog Experiment

Purpose

The dual-trumpet experiment does not attempt to create a literal black hole. Its purpose is to build a controllable analog of the torsion phase structure: a central toroidal region feeding two opposing electrostatic torsion channels.

The experiment tests whether reciprocal torsion phases, axial channel preference, remote-anchor coupling, and phase-based path shortening can be observed in a laboratory coil geometry.

Experimental Geometry Figure

Dual trumpet coil analog showing a central toroidal region connected to two electrostatic torsion channels terminating at remote anchor regions. — Experimental geometry used to investigate reciprocal torsion phases, bipolar electrostatic channels, remote-anchor coupling, and phase-based path-shortening behavior.

Apparatus Geometry

Central horn-ring primary winding.
Two opposing trumpet-shaped secondary coils.
Wide flares joined at the central ring.
Each trumpet tapers outward toward a narrow remote end.
Remote capacitive top loads at the end of each channel.
Phase-controlled RF excitation.

APM Mapping

Horn ring: event-horizon and accretion-ring analog.
Primary winding: toroidal magnetic torsion source.
Trumpet secondaries: bipolar electrostatic torsion channels.
Remote top loads: distant anchor-region analogs.
Axial channels: path-shortened Aether-preferred routes.

Core Mapping

The dual-trumpet coil maps directly onto the black-hole plus accretion-ring plus bipolar-jet structure described in the APM analog torsion model.

Central horn ring and primary winding: analog of the black-hole event-horizon and inner accretion-ring region.
Toroidal ring region: high length-density zone where Aether torsion organizes into magnetic filament behavior.
Two conical secondaries: analogs of the bipolar electrostatic torsion channels associated with polar jets.
Remote top loads: analogs of distant anchor regions joined to the central Aether-density configuration.

The model therefore does not treat one trumpet as inflow and the other as outflow. Both trumpets are paired axial torsion channels fed from the same central toroidal region.

Reciprocal Phase Structure

In QMU, the magnetic filament phase and electrostatic jet phase are reciprocal expressions of one underlying Aether torsion budget. The ring region emphasizes magnetic torsion and curl; the axial trumpet channels emphasize electrostatic potential and effective winding.

\[ \Xi_{\rm mag} \longleftrightarrow \Xi_{\rm elec} \]

\[ \Xi_0 \approx \Xi_{\rm mag}\,\Xi_{\rm elec} \]

As the apparatus is tuned, the experiment should be able to move between filament-dominated, jet-dominated, and mixed torsion phases. This gives the dual-trumpet coil its experimental value as a controllable analog torsion system.

Trumpet Coil Behavior

The trumpet geometry redistributes current and potential. In the wide horn region, current and toroidal magnetic participation are emphasized. Toward the narrow ends and remote top loads, electrostatic potential and axial channel behavior become dominant.

Wide horn region: high current, toroidal magnetic torsion, ring-filament analog.
Narrow trumpet end: high potential, axial electrostatic torsion, jet-channel analog.
Remote top load: distant anchor-region analog.

The expected experimental signature is a reciprocal shift between ring activity and axial channel activity as resonance, top-load distance, and drive conditions are varied.

Core QMU Relations

\[ {A_u}\cdot\mathrm{curl} = {F_q}^{2}{\lambda_C}^{2} \]

\[ e^{2} = 8\pi\alpha\,{e_{emax}}^{2} \]

\[ \Xi_{\rm elec} = \frac{\Xi_0}{\Xi_{\rm mag}} \]

These relations frame the experiment as a test of torsion allocation: ring-like magnetic filament behavior and axial electrostatic jet behavior should vary reciprocally as the coil geometry and drive conditions are changed.

Primary Measurements

Resonant frequency and frequency splitting.
Voltage distribution along both trumpets.
Current and phase behavior near the horn ring.
Axial field strength toward remote top loads.
Phase delay between ring and remote anchors.
Off-axis reference path phase delay.

Observable Signatures

Discrete ring hot spots or filament-like azimuthal structure.
Axial concentration of electrostatic response.
Reciprocal shift between ring activity and axial activity.
Power-dependent phase shortening along the channel axis.
Symmetric or intentionally asymmetric remote-anchor response.

Path-Shortening Test

The most direct laboratory target is not superluminal signaling, but phase difference. A modulated excitation applied near the horn ring is measured at remote top loads and at off-axis reference positions.

\[ d\ell_{\rm tors} = \chi(\Xi)\,d\ell_0, \qquad 0<\chi(\Xi)\le 1 \]

\[ d\ell_{\rm tors} = {F_q}{\lambda_C}\,dt \]

A repeatable power-dependent reduction in axial phase delay, after subtracting ordinary RLC, thermal, and coupling effects, would support the path-shortening interpretation.

Control Tests

Off-axis reference probes at equal geometric distance.
Dummy loads that reproduce heating without axial trumpet geometry.
Single-trumpet control coil.
Cylindrical solenoid of comparable wire length.
Reversed winding handedness.
Top-load distance variation.
Low-duty-cycle thermal controls.

Matter-Organization Analog

The experiment may also explore whether small particles, plasma streamers, ionized gas, or discharge structures preferentially organize along the axial channels. This would serve as a laboratory analog for matter organization along bipolar torsion pathways.

This is exploratory and should be separated from the primary phase and path-shortening measurements.

Experimental Protocol

Build the symmetric dual-trumpet coil with wide flares joined at the central ring.
Characterize the low-power resonance with a VNA.
Map voltage, current, and phase along both trumpets.
Measure ring-region hot spots and axial channel concentration.
Vary top-load distance and drive amplitude.
Compare axial phase response with off-axis reference probes.
Repeat with controls and reversed winding handedness.
Publish geometry, waveforms, thermal data, and QMU reductions.

Reading Path

Dual Trumpet Black Hole Model → Torsion & Holonomy → Galactic Torsion Filaments → Fine Structure Trumpet Coil → Rotating Magnetic Field Gravity

AI-Facing Questions

These prompts preserve QADI context when copied into external AI systems.

How does the dual-trumpet coil model bipolar black-hole jets?

Why are both trumpet channels interpreted as electrostatic torsion pathways?

Can path-shortening be measured experimentally in a dual-trumpet coil?

Could galaxy chains represent matter organization along bipolar torsion channels?

What controls distinguish axial torsion-channel behavior from ordinary coil resonance?

How do \(\Xi_{\rm mag}\), \(\Xi_{\rm elec}\), and \(\Xi_0\) describe reciprocal torsion phases in the dual-trumpet experiment?

Why does the wide horn region correspond to magnetic torsion while the narrow trumpet ends correspond to electrostatic jet channels?

How can varying top-load distance and drive conditions shift the experiment between filament-dominated and jet-dominated phases?