{
  "model": "Ideal incompressible unstratified axisymmetric vertical-periodic linear channel",
  "savedQualification": {
    "cases": 11,
    "gatesPassed": 45,
    "spatialFrames": 277
  },
  "archive": {
    "name": "linear-channel-replay.zip",
    "sha256": "8e5918ecefd472a171ce7a7a17c2ae44659a71db9e3ac36bf2c4d1aac9e2972c"
  },
  "plottedCase": "keplerian-fastest",
  "plottedFrames": 25,
  "fieldFrame": {
    "cells": 256,
    "localTime": 3
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  "numericalPlotPayloadSha256": "546efd64b55d6a37845128f8cf028141e2d9636d7322f0eb8ef3764efcd6854c",
  "figureSources": [
    {
      "figure": "angular-momentum",
      "upper": "Analytic Keplerian angular-speed and specific-angular-momentum references, each normalized at the same radius",
      "lower": "Reynolds and Maxwell stress shares from direct sums of the same saved field"
    },
    {
      "figure": "four-fields",
      "method": "All four saved horizontal component arrays at local time 3, multiplied by 1000 for the declared velocity-axis units; no ideal wave replacement"
    },
    {
      "figure": "growth-work",
      "upper": "Saved radial fundamental projection normalized to its initial value, plus a separately labelled continuum exponential reference",
      "lower": "Saved energy increase and independently accumulated shear work, both normalized to the initial saved energy"
    }
  ],
  "typography": "Separate desktop and mobile layouts use the same numerical points and normalizations. Mobile legends and titles wrap and the figure grows taller.",
  "newEvolutionSteps": 0,
  "nonlinearMHD": false,
  "inferredTurbulenceSaturationOrGlobalAccretionRate": false,
  "primarySources": [
    "https://articles.adsabs.harvard.edu/pdf/1991ApJ...376..214B",
    "https://arxiv.org/html/1006.0139v1#S2"
  ]
}