Eur. Phys. J. Appl. Phys.
Volume 79, Number 3, September 2017
|Number of page(s)||16|
|Section||Instrumentation and Metrology|
|Published online||04 August 2017|
The anisosphere as a new tool for interpreting Foucault pendulum experiments. Part I: harmonic oscillators
Université du Québec à Chicoutimi, 555 Boulevard de l'Université, Saguenay, QC G7H 2B1, Canada
a e-mail: email@example.com
Revised: 30 June 2017
Accepted: 30 June 2017
Published online: 4 August 2017
In an attempt to explain the tendency of Foucault pendula to develop elliptical orbits, Kamerlingh Onnes derived equations of motion that suggest the use of great circles on a spherical surface as a graphical illustration for an anisotropic bi-dimensional harmonic oscillator, although he did not himself exploit the idea any further. The concept of anisosphere is introduced in this work as a new means of interpreting pendulum motion. It can be generalized to the case of any two-dimensional (2-D) oscillating system, linear or nonlinear, including the case where coupling between the 2 degrees of freedom is present. Earlier pendulum experiments in the literature are revisited and reanalyzed as a test for the anisosphere approach. While that graphical method can be applied to strongly nonlinear cases with great simplicity, this part I is illustrated through a revisit of Kamerlingh Onnes’ dissertation, where a high performance pendulum skillfully emulates a 2-D harmonic oscillator. Anisotropy due to damping is also described. A novel experiment strategy based on the anisosphere approach is proposed. Finally, recent original results with a long pendulum using an electronic recording alidade are presented. A gain in precision over traditional methods by 2–3 orders of magnitude is achieved.
© The Author(s) 2017
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