Coupling of two mechanical oscillators
Are two identical simple pendulums oscillating in the same plan, with the same pulsation such as:
- (formula known as of the small oscillations)
Coupling of the two pendulums
To place a spring length at rest equal to the distance M1M2 = has, between the motionless pendulums. By doing this, the 2 oscillators are coupled and the two degrees of freedom x1 and x2 of the movement of each pendulum will be coupled by the spring of stiffness K .
Symmetry
The symmetry of the problem reveals two modes:
- one symmetrical: x1 = x2: the spring does not play any part and the pulsation remains unchanged.
- the other antisymmetric x1 = - x2: the point medium of the spring remains motionless. One finds with two not coupled oscillators with recall by a spring of stiffness 2k. The pulsation is such as:
It would thus be enough to have changed the coordinates of the problem into X1 =x 1+x2 and X2 = x1-x2 to involve decoupling: it is a general situation for linear oscillators. By choosing the coordinates known as " normales" , the coupling disappears. It is thus a concept relating to the selected point of view .
Double resonance
Arbitrarily let us call (one has just seen it) K = kl/mg, the constant of coupling . If one forces the movement of the first mass by a sinusoidal force F cos (t) then the movement x1 (T) will be a sinusoidal movement of amplitude complexes x1 (p) such as:
who is a reality in accordance with the Théorème of Foster-Tuttle, with resonance with the two own pulsations and a pulsation " bouchon" (x1 (T) =0), just at the moment when the mass m2 oscillates on this pulsation. This one is such as , x2 having a finished amplitude.
However, the phenomena described here are valid only for small oscillations.
See too
-
Constant of coupling
- Coupling of two oscillators
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