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Shell-model experiment: 8-shell run

Overview

The system is a cubic shell ODE: independent velocity-shell variables \(u_k\) and vorticity-shell variables \(\omega_k\) at integer wavenumbers \(k\), coupled by hand-built cubic transfer terms, a stretching coupling \(\lambda\) and a feedback coupling \(\sigma\), with linear damping \(\nu k^2\). It is not a Galerkin truncation of Navier–Stokes; \(u_k\) and \(\omega_k\) are separate state variables and the coupling structure is chosen by hand. Every threshold reported on this page — the amplitude \(A^*\), times to threshold crossing and classification scores — is a finite-window excursion threshold: \(A^*\) is the smallest initial amplitude for which the shell enstrophy \(\sum_k \omega_k^2\) exceeds a fixed excursion level within the integration window, and its value depends on the window length, the excursion level and the solver.

Question

Does the H/H'/H'' diagnostic hierarchy developed on the 6-shell ODE apply unchanged to the 8-shell ODE (4 velocity + 4 vorticity variables, wavenumbers \(k=1,2,3\) with forward transfer)? Quantities recorded: the diagnostic loop, the fitted power law between amplitude and peak shell enstrophy, the doubling-time criterion and the threshold amplitude \(A^*\).

Method

  1. Implement the 8-shell ODE with coupled velocity and vorticity variables and forward transfer between wavenumbers.
  2. Run the full 26-level hierarchy with the doubling-time criterion \(P\) as the primary discriminator.
  3. Sweep amplitudes to find \(A^*(\text{truth})\) by direct integration and \(A^*(P)\) from the criterion. Evaluate classification across 16 test amplitudes.
  4. Check for the diagnostic loop \(L_1 \to L_4 \to L_2 \to L_1\) at every checkpoint. Fit the power-law exponent of peak shell enstrophy against amplitude.
  5. Vary the window from \(T=30{,}000\) to \(T=80{,}000\) and record the \(P/\text{truth}\) ratio.

Results

Threshold amplitude

QuantityValueNote
\(A^*(\text{truth})\)0.2901.136 in the 6-shell ODE; the two systems have different coupling structures
\(A^*(P)\)0.277Doubling-time criterion estimate
\(P/\text{truth}\)95.5%86.1% in the 6-shell run

Classification

MetricResult
Score16/16 amplitudes classified
Diagnostic loop\(L_1 \to L_4 \to L_2 \to L_1\) present at every checkpoint
Fitted power-law exponent2.0

Window dependence

Window\(P/\text{truth}\)
\(T = 30{,}000\)93%
\(T = 50{,}000\)94%
\(T = 80{,}000\)95%

The ratio moves from 93% to 95% as the window lengthens from 30,000 to 80,000 steps.

Observation. The 8-shell ODE has sharper dynamics than the 6-shell ODE: trajectories that cross the excursion threshold do so more decisively, and those that stay below it are cleaner, so the doubling-time criterion sits closer to the direct-integration value (95.5% against 86.1%). The lower \(A^*\) (0.290 against 1.136) reflects the different coupling structure of the 8-shell system.

Analysis

  • Classification. All 16 test amplitudes are placed on the correct side of the direct-integration threshold within the window.
  • Criterion ratio. \(P/\text{truth} = 95.5\%\) for the 8-shell ODE against 86.1% for the 6-shell ODE.
  • Diagnostics carried over. The diagnostic loop, the fitted power-law exponent (2.0) and a positive \(A^*\) are all present in the 8-shell run.
  • Window dependence. The ratio rises from 93% to 95% as the window grows from \(T=30{,}000\) to \(T=80{,}000\).

Summary of the run

The diagnostic hierarchy runs unchanged on the 8-shell cubic ODE. The doubling-time criterion places 16/16 test amplitudes on the correct side of the direct-integration threshold, with \(P/\text{truth} = 95.5\%\), and the fitted power-law exponent is 2.0. These are finite-window excursion quantities of this ODE.

Reproducibility

../simplex/build/sxc exp_ns_8mode_solve.sx -o build/exp_ns_8mode_solve.ll

OPENSSL_PREFIX=$(brew --prefix openssl)
clang -O2 build/exp_ns_8mode_solve.ll \
  ../simplex/runtime/standalone_runtime.c \
  -o build/exp_ns_8mode_solve \
  -lm -lssl -lcrypto -L${OPENSSL_PREFIX}/lib

./build/exp_ns_8mode_solve

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