Skip to content
Structural Selection
Part VIChapter3 min read·509 words

3.1 State Variables and Fields

Reading widthWidth
Text sizeText

3. Mathematical Framework

3.1 State Variables and Fields

The framework is defined on a continuous spatial domain with explicit time dependence. The fundamental state of the system is specified by three fields:

  • The scalar density field
ρ(x,t),\rho(\mathbf{x},t),

interpreted as an informational or mass-like density.

  • The velocity field
v(x,t),\mathbf{v}(\mathbf{x},t),

which carries inertial degrees of freedom and enables momentum storage and transport.

  • The emergent potential
Φ(x,t),\Phi(\mathbf{x},t),

which is not postulated as a gravitational potential a priori, but is generated dynamically from the density field.

No additional force fields, metrics, or geometric structures are assumed. All subsequent dynamics arise solely from the interaction of these variables.

3.2 Dynamical Equations of the Inertial Emergent Gravity Model

The evolution of the system is governed by three coupled equations. These equations constitute the complete dynamical content of the model.

Continuity Equation

Conservation of density is enforced through the standard transport equation:

tρ(x,t)+(ρ(x,t)v(x,t))=0\boxed{ \partial_t \rho(\mathbf{x},t) + \nabla \cdot \big( \rho(\mathbf{x},t)\,\mathbf{v}(\mathbf{x},t) \big) = 0 }

This equation ensures that the density field evolves solely through advection by the velocity field.

Equation of Motion with Damping

The velocity field evolves according to an inertial equation with linear damping:

tv(x,t)=Φ(x,t)γv(x,t)\boxed{ \partial_t \mathbf{v}(\mathbf{x},t) = -\nabla \Phi(\mathbf{x},t) - \gamma\,\mathbf{v}(\mathbf{x},t) }

Here, γ\gamma is a damping coefficient controlling the transition between overdamped and inertial regimes. The presence of the time derivative tv\partial_t \mathbf{v} is essential: without it, orbital and cyclic dynamics are strictly forbidden.

Screened Poisson Equation

The emergent potential is determined instantaneously from the density field via a screened Poisson equation:

(2μ2)Φ(x,t)=ρ(x,t)ρ\boxed{ \left(\nabla^2 - \mu^2\right)\Phi(\mathbf{x},t) = \rho(\mathbf{x},t) - \langle \rho \rangle }

The subtraction of the spatial mean ρ\langle \rho \rangle enforces global neutrality, while the screening scale μ1\mu^{-1} controls the effective range of interaction. This equation introduces no force law; it merely defines how Φ\Phi responds to density fluctuations.

3.3 Extracted Observables (Non-Assumed Quantities)

All diagnostic quantities used to classify gravitational behavior are extracted from the evolving fields. None are imposed at the level of the equations.

Centers of Mass

For each localized density component ρi(x,t)\rho_i(\mathbf{x},t), the center of mass is defined as

ri(t)=xρi(x,t)dxρi(x,t)dx\boxed{ \mathbf{r}_i(t) = \frac{\int \mathbf{x}\,\rho_i(\mathbf{x},t)\,d\mathbf{x}} {\int \rho_i(\mathbf{x},t)\,d\mathbf{x}} }

Binary Separation

The instantaneous separation between two density concentrations is

d(t)=r1(t)r2(t)\boxed{ d(t) = \left\| \mathbf{r}_1(t) - \mathbf{r}_2(t) \right\| }

Radial Velocity

The radial velocity is obtained by temporal differentiation:

d˙(t)=ddtd(t)\boxed{ \dot d(t) = \frac{d}{dt} d(t) }

Zero crossings of d˙(t)\dot d(t) serve as indicators of turning points in the relative motion.

Angular Momentum Proxy

An effective angular momentum diagnostic is defined by

L(t)=(r1(t)r2(t))×veff(t)\boxed{ L(t) = \big(\mathbf{r}_1(t) - \mathbf{r}_2(t)\big) \times \mathbf{v}_{\mathrm{eff}}(t) }

where veff(t)\mathbf{v}_{\mathrm{eff}}(t) is the spatially averaged velocity within a localized density region. This quantity is not conserved a priori, but its persistence or decay provides a direct measure of inertial structure.

The time-averaged magnitude,

L=1T0TL(t)dt,\boxed{ \langle |L| \rangle = \frac{1}{T}\int_0^T |L(t)|\,dt, }

plays a central role in classifying dynamical phases in later sections.

Source: Gravity as a Temporally Closed Dynamical Phase/03_Mathematical Framework.tex in the verified v2 revision. Found an issue with this section? Submit a criticism.
Cite this section

Plain text

Hassan, A. (2026). 3.1 State Variables and Fields. In Gravity as a Temporally Closed Dynamical Phase, The Complete Structural Selection Corpus. Nuronova Genix Corp. https://structuralselection.org/book/chapter/3-1-state-variables-and-fields

BibTeX

@incollection{hassan202631statevariablesandf,
  author    = {Hassan, Akram},
  title     = {3.1 State Variables and Fields},
  booktitle = {The Complete Structural Selection Corpus},
  publisher = {Nuronova Genix Corp},
  year      = {2026},
  url       = {https://structuralselection.org/book/chapter/3-1-state-variables-and-fields}
}

RIS

TY  - CHAP
AU  - Hassan, Akram
TI  - 3.1 State Variables and Fields
T2  - The Complete Structural Selection Corpus
PB  - Nuronova Genix Corp
PY  - 2026
UR  - https://structuralselection.org/book/chapter/3-1-state-variables-and-fields
ER  -