Black Hole Simulation

A black hole in GCD is the Γ(ω->1) pole -- the point where drift cost diverges and return becomes impossible. The event horizon is not imported from general relativity; it is derived independently as the structural boundary where τ_R = inf_rec.

Collapsus generativus est; solum quod redit, reale est. -- At the horizon, nothing returns.

Launch Immersive Space Simulator ->

GR <-> GCD Translation

GR Concept GCD Analog Formula
Event Horizonω -> 1 poleΓ(ω) = ω^3/(1-ω+ε) -> inf
Gravitational FielddΓ/dωGradient of drift cost
Mass|κ| well depthAccumulated log-integrity
Tidal Forced^2Γ/dω^2Cost curvature (spaghettification)
Gravitational LensingΔ = F - ICHeterogeneity gap deflects trajectories
Time DilationAscent/descent asymmetryCost(ascent) / Cost(descent) -> inf near horizon
Hawking TemperatureT_H = 1/(8pi|κ|)Inverse well depth -- shallow wells radiate hotter
Gravitational Redshiftz = Γ/(1+Γ)Photon energy loss escaping the well
ISCOω ~= 0.50Innermost stable circular orbit -- tidal destabilization
Photon Sphereω ~= 0.65Unstable circular photon orbits
Frame-Draggingω_drag(ω, a*)Lense-Thirring: ω*a**(1-ω^2)^-1.5
Ergosphereω > ω_ergoRegion where frame-dragging exceeds orbit speed
Penrose Processη_P(a*)Energy extraction: 1 - sqrt(1 - (a*/2)^2)
BH EntropyS_BH = κ^2/(4pi)Bekenstein analog from log-integrity squared
Orbital Precessionδφ(ω)6piω^2/(1-ω)^2 -- perihelion advance near well
GW Strainh(ω,C,d)4ω^2C/(d+ε) -- quadrupole radiation
Time Dilationdτ/dtsqrt(1 - ω) -- proper time slowdown near horizon
Radiative Efficiencyη_rad(a*)1 - sqrt(1 - 2/(3r_ISCO)) -- accretion luminosity

3D Gravity Well

The budget surface Γ(ω) rendered as a 3D funnel. The event horizon (ω -> 1) plunges to the center -- where cost diverges and τ_R = inf_rec. The bright band is the accretion disk. Orbiting particles spiral inward following Kepler-like trajectories. Drag to rotate * Scroll to zoom * Double-click to reset

* Stable   * Watch   * Collapse
WebGL * 64*96 mesh * 180 particles * 300 stars

Gravitational Infall

Drag ω toward 1.0 to "fall into" the black hole. Watch cost, tidal force, and escape ratio diverge at the event horizon. The three regime boundaries are marked.

Safe (ω=0) Stable Watch Collapse Horizon (ω=1)
0.100
STABLE

Budget Surface

The full cost landscape over (ω, C). Height = Γ(ω) + alpha*C. Entity positions are marked -- objects deeper in the potential well have higher ω. The dark ridge at ω -> 1 is the event horizon.

Entity Positions

Color Scale

Low cost High cost (horizon)

Entity Kernel Comparison

Each spacetime entity through the GCD kernel. The trace vector becomes six invariants; the invariants determine the regime. The heterogeneity gap Δ = F - IC is the lensing diagnostic.

Arrow of Time

Descent cost vs ascent cost as a function of depth. Near the horizon, escape cost diverges relative to infall cost -- this IS time dilation in GCD. The asymmetry ratio grows without bound as ω -> 1.

Tidal Force (d^2Γ/dω^2)

The second derivative of Γ(ω) measures the rate of change of the gravitational field -- the "spaghettification" diagnostic. Tidal force is small far from the horizon and catastrophic near it.

Gravitational Lensing

The heterogeneity gap Δ = F - IC determines lensing morphology. Small Δ -> Einstein ring. Large Δ -> weak distortion. The deflection angle theta = 4|κ|/(Δ+ε) mirrors Einstein's formula.

Frame-Dragging (Lense-Thirring)

A spinning black hole drags spacetime around it. In GCD, frame-dragging ω_drag = ω*a**(1-ω^2)^-1.5 diverges as ω -> 1 -- the ergosphere where dragging exceeds orbital velocity. At a* = 0 (Schwarzschild), there is no dragging; at a* -> 1 (extremal Kerr), the ergosphere fills the space.

Penrose Process -- Energy Extraction

The Penrose process extracts rotational energy from a spinning black hole. In GCD, efficiency η_P = 1 - sqrt(1 - (a*/2)^2). Maximum extraction at a* = 1 gives η_P ~= 13.4%. Also shown: radiative efficiency η_rad from accretion onto the ISCO, which reaches ~42% for extremal spin.

Proper Time Dilation (dτ/dt)

The ratio of proper time to coordinate time: dτ/dt = sqrt(1-ω). As ω -> 1, clocks freeze and time dilation becomes infinite. This is the GCD analog of gravitational time dilation at the Schwarzschild radius. Also shown: BH entropy S_BH = κ^2/(4pi), the Bekenstein analog.

Orbital Precession & Gravitational Waves

Orbital precession δφ = 6piω^2/(1-ω)^2 grows super-linearly near the horizon -- the GCD analog of Mercury's perihelion advance. Gravitational wave strain h = 4ω^2C/(d+ε) from the inspiral radiates the curvature channel as quadrupole waves.