Difference between revisions of "Forest UCM Osc 2-DOsc"
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The equations of motion are separable two equations, one for each direction | The equations of motion are separable two equations, one for each direction | ||
− | : <math>\ddot x = - \omega^2x</math> | + | : <math>\ddot x = - \omega^2x \Rightarrow x = A_x \cos(\omega t - \delta_x)</math> |
− | : <math>\ddot y = - \omega^2 y</math> | + | : <math>\ddot y = - \omega^2 y \Rightarrow y = A_y \cos(\omega t - \delta_y)</math> |
[[Forest_UCM_Osc#2-D_Oscillators]] | [[Forest_UCM_Osc#2-D_Oscillators]] |
Revision as of 14:46, 4 October 2014
Two Dimensional Oscillators
Isotropic Oscillator
The simplest 2-D oscillator that is composed of identical springs (same spring constant).
The equations of motion are separable two equations, one for each direction