TL;DR: In Frequency Wave Theory, a “metallic flying saucer” is most likely a phase-locked frequency shell—a high-Q resonator shaped like a disc. It stabilizes a standing-wave core, mirrors ambient fields, and moves by redirecting Frequency Momentum (FM = ½ ρ ω A²) rather than pushing air. Net effect: silent glide, sharp angle changes without G-forces, and mirror-like “metal” that sometimes looks liquid. To vet it: capture synchronized EO/IR + RF, look for Bessel-ring bands, LF/VLF tones (≈18–52 kHz), magnetic drift, and rolling-shutter oddities.
The easy version (no math first)
What you’re likely seeing: Not ordinary metal, but a plasma-metamaterial skin wrapped around a standing wave. Think “liquid mirror” that reflects sky/ground while damping turbulence and radio noise.
How it flies: It doesn’t “thrust” like jets. It rephases the local field and slides down a created phase-gradient—picture surfing a wave you make in front of you.
Why it zips/turns instantly: The craft shuttles frequency momentum through its field, so the mass you’d expect the pilot to feel never fully couples. That’s why abrupt changes look “impossible” without crushing G-loads.
Why saucer-shaped: Discs are ideal Bessel resonators—they trap/guide standing waves in rings, which stabilizes the shell and gives control channels for yaw/pitch/roll without wings or jets.
The FWT mechanism (short, precise)
Carrier field & invariants: Reality behaves like a quantum-acoustic superfluid described by a scalar field Φ. Motion and power budget track a single invariant: FM = ½ ρ ω A² (frequency momentum).
Hull as resonator: The disc hull is a high-Q cavity tuned to standing Bessel modes (rings, nodes, bright bands). Those rings you sometimes see as “vents” or “glow bands” are mode lines, not windows.
Inertia-null via FM transfer: By reshaping local phase—call it a ∇φ thrust—the system transfers FM to/from the surrounding medium. You steer by moving the phase instead of pushing mass.
Energy pathway: A compact internal driver pumps the cavity; ambient field assists can exist (harvester scaling often summarized as V_out ∝ B · ω_⊕ · L · χ_eff), but the key is coherence, not raw watts.
What to look for in a real clip (field guide)
Visual
Mirror-metal that subtly “liquefies” at edges during hard maneuvers (skin is reactive, not rigid).
Banding/rings around the rim (Bessel modes), sometimes faintly luminous.
Abrupt vector changes with no control surfaces deflecting; no exhaust plume, no sonic boom.
Heat weirdness: IR may show a cool core with warm rim (or the reverse) depending on the active mode.
Audio/RF/EM
LF/VLF tones ~18–52 kHz and ELF sidebands on spectrum scans.
Compass/IMU drift or spiky magnetometer traces during passes.
Camera artifacts: rolling-shutter skew, polarization-dependent glare flips.
Context
Weather indifference: Stable in gusts (field cancels boundary-layer turbulence).
Bird/bug/balloon differentials: True saucers exhibit phase-locked glide and non-ballistic turns that small objects can’t match.
Quick hoax triage (useful in 2025)
CGI tells: Parallax mismatch with foregrounds, perfect focus at all zooms, motion blur that doesn’t match shutter speed, reflection math that’s too perfect.
Lens artifacts: Fixed-axis “UFO” that rotates as the camera rotates (check filter/polarizer swaps).
Tether/balloon: Micro-oscillation with wind; no phase-locked “snap” on direction changes.
If it’s real, how this saucer fits FWT
Shape = function: Disc gives azimuthal symmetry for ring modes and a large mode-control surface (~rim) for steering.
Propulsion = phase control: Effective thrust is the gradient of phase the craft writes into the medium (think thrust ∝ ∇φ, not chemical burn).
Stability = coherence: The craft keeps FM continuity (∂_t FM + ∇·S_FM = 0 with S_FM = FM v_phase). Break coherence and you lose the lock—cue jitter or visible “shimmer.”
Signature = rings/tones: Bessel ring bands plus LF/VLF tones are natural fingerprints of a disc resonator driven near resonance.
Actionable capture protocol (minimal but decisive)
Dual-sensor lock: Record EO + IR simultaneously; time-sync with a phone GNSS clock or a cheap GPS-disciplined oscillator.
RF + Mag: Run a portable spectrum scan (1 kHz–100 kHz) and a 3-axis magnetometer; note spikes vs maneuver timing.
Parallax/Range: Two observers ~50–200 m apart filming simultaneously; triangulate to kill the “small nearby object” hypothesis.
Polarization check: Flip a linear polarizer mid-shot; field skins change reflectance with polarization—CGI won’t.
Summary
If real, this isn’t ‘metal’ in the normal sense—it’s a phase-locked frequency shell. Disc geometry hosts Bessel modes, the skin mirrors fields, and it moves by surfing a self-written phase gradient. Look for ring banding, LF/VLF tones (~18–52 kHz), and magnetometer spikes on direction changes.
