Simon F
- 15
- 2
- TL;DR
- Could the Foucault pendulum be a Flückiger et al (2020) effect on a 2Ω⋅sin(φ) forcing?
The standard explanation of the Foucault pendulum is purely kinematic: the plane of oscillation stays fixed in inertial space while the planet rotates beneath it. But Norman Phillips (2000, 2001) showed that real forces — the horizontal component of Newtonian gravitation and centrifugal imbalance — drive a free particle into circular motion at frequency 2Ω⋅sin(φ), exactly twice the Foucault precession rate. This inertial circle is not a fictitious artifact: it is a genuine dynamical mode of the rotating planet.
Flückiger et al. (2020) independently showed that a spherical isotropic oscillator on a frame rotating at ζ precesses at ζ/2 — a purely geometric result.
Could the Foucault precession rate be a Flückiger effect on the inertial circle 2Ω⋅sin(φ) forcing?
Flückiger et al. (2020) independently showed that a spherical isotropic oscillator on a frame rotating at ζ precesses at ζ/2 — a purely geometric result.
Could the Foucault precession rate be a Flückiger effect on the inertial circle 2Ω⋅sin(φ) forcing?