%% SCRAP: architecture/03-architecture/physics-engine/ssm-equations %% SOURCE: docs/working/architecture/03-architecture/physics-engine/ssm-equations.md %% STATUS: WORKING %% FITS: dev-guide/ch-physics %% EDITORIAL: lifted — prose rewritten to press voice \section{Mathematical Models of the Steady-State Machine} %% PATENT: This scrap covers patent-adjacent empirical relationships (the capacity %% law and its candidate claim language). Claim wording in the source is summarized %% as description only; no claim language is drafted here. Flag for Bob before any %% promotion that touches the claims. This section presents performance models derived empirically from the Steady-State Machine (SSM) experimental record: 51{,}840 runs of the StarForth VM across 128 feedback-loop configurations. Five relationships were extracted from the data with measurable precision. The headline result is a capacity law, $\Lambda(\mathrm{DoF}) = 4096 / (\mathrm{DoF}+1)$, which holds with a 0.00\% coefficient of variation across all stable configurations. These models are exploratory. Several borrow functional forms and names from physics --- the Lorentz factor, the Friedmann equation, the Schwarzschild radius --- purely because the data happens to fit those forms. The physics vocabulary is a modeling convenience for describing adaptive-system behavior; it is not a claim that the runtime obeys relativity or cosmology. Throughout, \textit{degrees of freedom} (DoF) denotes the number of enabled feedback loops, ranging from 0 to 7. \subsection{Equation 1 --- Performance Scaling with Load} Execution time scales with the number of enabled loops according to a Lorentz-like factor: \begin{equation} \tau(\mathrm{DoF}) = \tau_0 \cdot \gamma(\mathrm{DoF}), \qquad \gamma = \frac{1}{\sqrt{1 - \beta^2}}, \qquad \beta^2(\mathrm{DoF}) = 0.0736\,\mathrm{DoF} + 0.1464, \end{equation} with $\tau_0 = 31.67$\,ms/word the rest-state performance. The empirical fit is $R^2 = 0.938$. The $\beta^2$ term grows linearly with DoF, so each additional loop carries increasing marginal overhead. The structural similarity to relativistic time dilation is offered as a predictive model, not a physical claim. \subsection{Equation 2 --- Window Capacity Law $\Lambda$} The central empirical finding is an inverse capacity law: \begin{equation} \Lambda(\mathrm{DoF}) = \frac{W_0}{\mathrm{DoF} + 1}, \qquad W_0 = 4096. \end{equation} Equivalently, the product $\Lambda \times (\mathrm{DoF}+1) = W_0$ is conserved across all stable configurations. \begin{table}[ht] \centering \small \begin{tabular}{rrrr} \toprule DoF & Ideal $\Lambda$ & $\Lambda \times (\mathrm{DoF}+1)$ & Stability (CV) \\ \midrule 0 & 4096.0 & 4096.0 & 17.34\% \\ 1 & 2048.0 & 4096.0 & 16.70\% \\ 2 & 1365.3 & 4096.0 & 15.31\% \\ 3 & 1024.0 & 4096.0 & 13.91\% \\ 4 & 819.2 & 4096.0 & 13.77\% \\ 5 & 682.7 & 4096.0 & 13.96\% \\ 6 & 585.1 & 4096.0 & 14.33\% \\ 7 & 512.0 & 4096.0 & 22.06\% \\ \bottomrule \end{tabular} \caption{Window capacity verification. The conserved product holds at $4096.0 \pm 0.0$, a 0.00\% coefficient of variation.} \end{table} The symbol $\Lambda$ is borrowed from cosmology for convenience: it denotes the effective window capacity per degree of freedom, with $W_0 = 4096$ bytes an empirically determined constant. As loops are added, proportional window capacity must fall to preserve stability, and the conserved product behaves as a stability invariant. Notably, $W_0 = 4096 = 2^{12}$ was not designed --- it emerged from experimental optimization, and may reflect memory page-size alignment, cache-line constraints, or buffer-size effects. \subsection{Equation 3 --- Expansion Dynamics (Friedmann Form)} The growth in execution time as loops activate fits a Friedmann-like form: \begin{equation} H^2(\mathrm{DoF}) \approx c_1\,\rho(\mathrm{DoF}) + c_2\,\Lambda(\mathrm{DoF}) + c_3, \end{equation} with the fitted relation \begin{equation} H^2 = -2.24\times10^{12}\,\mathrm{DoF} \;-\; 4.51\times10^{9}\,\Lambda \;+\; 2.11\times10^{13}. \end{equation} Here $H$ stands in for the performance growth rate, $\rho$ for the degrees of freedom, and $\Lambda$ for window-capacity pressure. The negative coefficients indicate that both DoF and $\Lambda$ contribute to deceleration --- the system resists unbounded growth through feedback regulation. \subsection{Equation 4 --- Instability Threshold (Schwarzschild Form)} A Schwarzschild-like radius models the onset of instability: \begin{equation} r_s(\mathrm{DoF}) = \frac{\mathrm{DoF}}{W_{\mathrm{norm}}}, \qquad W_{\mathrm{norm}} = \frac{\text{window}}{4096}. \end{equation} In this analogy $r_s$ is the instability threshold, DoF the computational load, and $W_{\mathrm{norm}}$ the available space. The configurations with the highest coefficient of variation sit near this threshold. \begin{table}[ht] \centering \small \begin{tabular}{rrrrr} \toprule Config & DoF & $r_s$ & CV & Performance \\ \midrule 1 & 1 & 1.00 & 26.90\% & 32.43\,ms \\ 84 & 3 & 3.00 & 26.36\% & 34.94\,ms \\ 46 & 4 & 4.00 & 25.70\% & 50.27\,ms \\ 59 & 5 & 5.00 & 25.31\% & 50.43\,ms \\ \bottomrule \end{tabular} \caption{Configurations nearest the instability threshold. Where $r_s \ge \mathrm{DoF}$, the system tends toward instability.} \end{table} \subsection{Equation 5 --- Energy--Momentum Form} Total execution time fits an energy--momentum relation: \begin{equation} E^2 = E_0^2 + p^2, \qquad E = \tau(\mathrm{DoF}), \qquad E_0 = \tau_0 = 31.67\,\mathrm{ms}, \qquad p(\mathrm{DoF}) = 5.20\,\mathrm{DoF} + 6.55. \end{equation} Here $E_0$ is the all-loops-off baseline, $p$ the additional time cost from loops, and $E$ total execution time. Momentum scales linearly with DoF ($R = 0.425$, $p < 10^{-6}$). \begin{table}[ht] \centering \small \begin{tabular}{rrrrr} \toprule Config & DoF & $E_{\text{total}}$ & $E_{\text{rest}}$ & $p$ \\ \midrule 0 & 0 & 31.67 & 31.67 & 0.00 \\ 35 & 3 & 31.59 & 31.67 & 0.00 \\ 55 & 5 & 31.91 & 31.67 & 3.88 \\ 124 & 5 & 59.48 & 31.67 & 50.35 \\ \bottomrule \end{tabular} \caption{Energy--momentum decomposition for selected configurations.} \end{table} Two configurations are notable. Config~\#35 carries three enabled loops yet sits at near-zero momentum, suggesting an optimal arrangement where loop interactions cancel. Config~\#124, the worst performer, carries the same DoF as Config~\#55 but enormous momentum (50.35) --- a destructive combination of loops. \subsection{Interpretation and Open Experiments} The recurring observation is that these adaptive-runtime relationships fit functional forms also found in general relativity, thermodynamics, and quantum mechanics. The strongest of them, the capacity law, is exact to within measurement. Whether this reflects a deep property of feedback-driven systems or an emergent coincidence remains open; the SSM data is presented as evidence that the functional forms are useful predictive models. Several follow-on experiments are proposed: \begin{itemize} \item \textbf{Window-size scaling.} Vary the window across 1024, 2048, 4096, 8192, and 16384 bytes and test whether $\Lambda(\mathrm{DoF}) = W/(\mathrm{DoF}+1)$ holds, i.e.\ whether the 4096 constant scales linearly with window size. \item \textbf{Critical window capacity.} Reduce the window in steps and locate a $W_{\text{crit}}$ below which the selector collapses to the all-off configuration. \item \textbf{Maximum degrees of freedom.} Extend beyond seven loops and test whether the capacity law holds up to a $\mathrm{DoF}_{\max}$, with the candidate $\mathrm{DoF}_{\max} \approx \log_2(W_0) = 12$. \end{itemize} %% PATENT: The source proposes patent claims based on the capacity law, the %% Lorentz-like scaling, and the Schwarzschild-like threshold, and outlines %% publication and funding strategy. That material is intentionally omitted here %% pending Bob's instruction; do not draft claim language in this scrap. %% TODO(bob): confirm which empirical relationships may appear in citable form.