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Chapter 30: Collapse-Driven Planetary Decay

The Slow Death of Worlds

Planets seem eternal, but they age and die through processes deeper than erosion or cooling. Ψhē Cosmology reveals that planetary decay follows collapse dynamics—worlds slowly unravel as their binding collapse fields weaken, leak, and reorganize. Every planet carries within it the seeds of its own dissolution.

30.1 Decay Through Collapse Leakage

Definition 30.1 (Collapse Evaporation): A planet loses binding when: dψdt=Γψ2\frac{d\psi}{dt} = -\Gamma \psi^2

where Γ is the evaporation coefficient. Collapse slowly bleeds into space.

30.2 The Unraveling Process

Theorem 30.1 (Exponential Decay): Planetary mass decreases as: M(t)=M0exp(tτψ)M(t) = M_0 \exp\left(-\frac{t}{\tau_\psi}\right)

where τ_ψ = 1/(Γψ₀) is collapse lifetime.

Proof: Mass couples to integrated collapse density. As ψ decreases through evaporation, the total mass bound by collapse diminishes exponentially. The timescale depends on initial collapse strength. ∎

30.3 Atmospheric Stripping

Atmospheres escape first:

Definition 30.2 (Jeans Escape): Atmospheric loss rate: Φ=n(h)vthexp(vesc2vth2)\Phi = n(h) v_{th} \exp\left(-\frac{v_{esc}^2}{v_{th}^2}\right)

Modified by collapse: v_esc = √(2ψ). Weakening collapse accelerates atmospheric loss.

30.4 Core Cooling Dynamics

Interior heat dissipates:

Theorem 30.2 (Thermal Death): Core temperature follows: Tcore(t)=T0(ψ(t)ψ0)2/3T_{core}(t) = T_0\left(\frac{\psi(t)}{\psi_0}\right)^{2/3}

Collapse decay reduces gravitational heating, accelerating cooling.

30.5 Magnetic Field Collapse

Dynamos fail as worlds age:

Definition 30.3 (Magnetic Decay): Field strength diminishes: B(t)=B0exp(tτB)B(t) = B_0 \exp\left(-\frac{t}{\tau_B}\right)

where τ_B = τ_ψ/3. Magnetic protection fails before complete dissolution.

30.6 Tidal Disruption

Close encounters accelerate decay:

Theorem 30.3 (Roche Dissolution): A planet disrupts when: d<2.46R(ρplanetρstar)1/3d < 2.46 R \left(\frac{\rho_{planet}}{\rho_{star}}\right)^{1/3}

Modified by ψ-weakening, reducing effective density.

30.7 Radioactive Depletion

Internal heat sources exhaust:

Definition 30.4 (Nuclear Decay): Heating rate decreases: H(t)=iH0,iexp(λit)H(t) = \sum_i H_{0,i} \exp(-\lambda_i t)

Combined with collapse decay, planets freeze from within.

30.8 Crustal Relaxation

Mountains flatten, valleys fill:

Theorem 30.4 (Topographic Decay): Surface relief diminishes: hmax(t)=h0exp(tτrelax)h_{max}(t) = h_0 \exp\left(-\frac{t}{\tau_{relax}}\right)

where τ_relax ∝ η/ψ². Weaker collapse allows faster erosion.

30.9 Orbital Expansion

Dying worlds drift outward:

Definition 30.5 (Decay-Driven Migration): Semi-major axis increases: dadt=2aψdψdt\frac{da}{dt} = \frac{2a}{\psi}\frac{d\psi}{dt}

As binding weakens, orbits expand toward escape.

30.10 Phase Transition Death

Final collapse reorganization:

Theorem 30.5 (Catastrophic Transition): When ψ < ψ_critical: 2Fψ2=0\frac{\partial^2 F}{\partial \psi^2} = 0

The planet undergoes phase transition—solid to dust, atmosphere to void.

30.11 Observable Predictions

Planetary decay leaves traces:

  1. Mars' Lost Atmosphere: Collapse decay stripped gases
  2. Mercury's Large Core: Mantle evaporated with collapse
  3. Asteroid Belt: Failed planet from insufficient collapse
  4. Cometary Breakup: Collapse failure during perihelion
  5. Hot Neptune Desert: Collapse evaporation zone

Each reveals decay in action.

30.12 The Mortality of Worlds

Planets die not through drama but through quiet dissolution—collapse fields slowly unwinding, releasing matter back to space. The process takes billions of years, but inevitability remains. Every world contains a clock, ticking down through collapse decay toward eventual dispersal.

In the end, all planets return to dust—their collapse exhausted, their time complete.


Next: Chapter 31: ψ-Ring Genesis from Orbital Collapse Haloes