equation 29.66 eq:rigid-rotating-eom

Rests on

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

Supports

• assumes experiment Foucault: the pendulum at the Panthéon ¶
• depends_on example 29.52 Sizes of the three terms at the Earth's surface ¶
• depends_on phenomenon 29.53 Rotation is locally detectable, uniform motion is not ¶
  • depends_on phenomenon 20.12 Coriolis deflection ¶
  • depends_on remark 18.2 What is assumed here, and what is measured ¶
  • depends_on remark 29.54 What the bucket does and does not settle ¶
• depends_on phenomenon 29.58 Weather systems circulate, and the sense is set by the hemisphere ¶
  • depends_on remark 29.59 The bathtub, and the limits of the argument ¶
• depends_on phenomenon 29.56 Falling bodies are deflected eastward ¶
• depends_on phenomenon 29.61 The Foucault pendulum ¶
  • depends_on phenomenon 34.11 The swing plane precesses at the vertical component of the Earth's rotation ¶
  • depends_on remark 29.62 The same rate read as a holonomy ¶
  • tests experiment Foucault: the pendulum at the Panthéon ¶ ↺
• depends_on phenomenon 29.55 Effective gravity varies with latitude ¶
  • depends_on proposition 29.57 The Eötvös effect ¶
• depends_on proposition 29.57 The Eötvös effect ¶ ↺
• depends_on theorem 29.60 Planar central motion in a rotating frame ¶
  • depends_on phenomenon 29.61 The Foucault pendulum ¶ ↺