Faraday Paradox Experiment (RTT‑Aware Protocol)
Overview#
This protocol reproduces the classical Faraday disk experiment and records results using the RTT‑Inside schema faraday_paradox_experiment.schema.json.
The goal is to measure EMF under three rotational configurations and annotate the results with triadic (Spin–Charge–Temperature) field conditions.
Objectives#
- Measure EMF generated by a rotating conducting disk in a magnetic field.
- Compare three configurations:
- Disk rotates, magnet fixed.
- Disk and magnet co‑rotate.
- Magnet rotates, disk fixed.
- Record triadic conditions (spin bias, charge gradient, temperature profile).
- Demonstrate RTT’s resolution of Faraday’s paradox via spin‑relative motion.
Equipment#
- Conducting disk (copper or aluminum), known radius.
- Permanent magnet (axial field, e.g., NdFeB).
- Motorized rotational drive with RPM control.
- Slip rings or brushes for center–rim EMF collection.
- Voltmeter or DAQ system.
- Tachometer (for RPM).
- Hall probe (for magnetic field measurement).
- Temperature sensor (optional).
- Non‑magnetic mounting hardware.
Schema Mapping#
This protocol populates the following fields:
| Schema Field | Source in Protocol |
|---|---|
experiment_id |
Assigned by operator |
disk_material |
Disk specification |
disk_radius_m |
Measured radius |
rotation_rate_rpm |
Motor RPM |
magnet_configuration |
Fixed / Co‑rotating / Rotating‑only |
magnet_rotation_rate_rpm |
RPM of magnet (if applicable) |
magnetic_field_tesla |
Hall probe measurement |
triadic_conditions.spin_bias |
Normalized rotational coupling |
triadic_conditions.charge_gradient |
Derived from EMF and geometry |
triadic_conditions.temperature_profile |
Temperature rise or estimate |
measured_emf_volts |
Voltmeter reading |
Procedure#
1. Baseline Setup#
- Mount the conducting disk on a non‑magnetic shaft.
- Position the magnet so its field is axial through the disk.
- Connect:
- Center of disk → slip ring → voltmeter.
- Rim of disk → brush → voltmeter.
- Ensure all components are stationary.
- Record baseline EMF.
2. Case A — Disk Rotates, Magnet Fixed#
- Fix the magnet rigidly to the lab frame.
- Spin the disk at several RPM values (e.g., 100, 500, 1000).
- For each RPM:
- Record
rotation_rate_rpm. - Measure EMF.
- Log triadic conditions:
- Spin bias ∝ RPM.
- Charge gradient ∝ EMF / radius.
- Temperature profile (optional).
- Record
Expected: EMF increases with RPM.
3. Case B — Disk + Magnet Co‑Rotate#
- Mechanically couple the magnet to the disk.
- Repeat the same RPM series.
- Record EMF and triadic conditions.
Expected: EMF remains similar to Case A.
4. Case C — Magnet Rotates, Disk Fixed#
- Fix the disk; allow only the magnet to rotate.
- Spin the magnet at the same RPM values.
- Record EMF and triadic conditions.
Expected: EMF ≈ 0 (within noise).
RTT Interpretation Notes#
- EMF arises from spin‑relative motion of charges through a substrate‑anchored field.
- Co‑rotation of magnet does not eliminate EMF because the field structure does not “move” with the magnet.
- Magnet‑only rotation produces no EMF because the conductor has no spin‑relative motion.
Data Recording#
All results should be stored as JSON instances of
faraday_paradox_experiment.schema.json.
See examples/faraday_paradox_example.json for a reference instance.
Safety Notes#
- Ensure all rotating components are shielded.
- Avoid contact with strong magnets.
- Use insulated leads and proper grounding.