equation D.3 eq:E-kernel-condition

Rests on

No declared or derived dependency edges point away from this node yet.

Supports

• depends_on theorem D.2 Buckingham's $\Pi$ theorem ¶
  • depends_on definition 31.51 The other similarity groups ¶
    • depends_on definition A.760 The convecting layer ¶
      • depends_on proposition A.761 The Boussinesq equations ¶
        • depends_on definition A.763 Two-dimensional rolls ¶
        • depends_on proposition A.765 The roll equations ¶
    • depends_on phenomenon 31.78 Convective onset at a computed threshold ¶
      • depends_on proposition A.761 The Boussinesq equations ¶ ↺
      • depends_on remark 31.79 Bénard's own cells, and Taylor's cylinders ¶
      • depends_on remark 31.81 Where the threshold comes from, and what it costs ¶
      • depends_on theorem A.767 Marginal stability of the conducting state ¶
        • depends_on remark A.768 Two conventions for the wavenumber ¶
        • depends_on theorem A.769 The Lorenz system ¶
    • depends_on proposition A.766 Nondimensionalisation ¶
      • depends_on theorem A.767 Marginal stability of the conducting state ¶ ↺
      • depends_on theorem A.769 The Lorenz system ¶ ↺
    • depends_on remark 31.89 The Mach number and the regimes it separates ¶
      • depends_on phenomenon 31.93 The Mach cone ¶
  • depends_on phenomenon 31.84 The five-thirds spectrum ¶
    • depends_on proposition 31.85 The Kolmogorov scales ¶
    • depends_on remark 31.86 The one exact result, and the split attribution ¶
  • depends_on proposition 31.85 The Kolmogorov scales ¶ ↺