| 11. | At the equilibrium position, the net restoring force vanishes.
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| 12. | Its unstable equilibrium position is obtained by rotating the figure 180?about a horizontal axis.
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| 13. | Once put into motion the block will oscillate back and forth around the equilibrium position.
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| 14. | Here " g " represents the equilibrium position.
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| 15. | "' Acoustic phonons "'are coherent movements of atoms of the lattice out of their equilibrium positions.
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| 16. | Moreover, the ions are not in fact stationary, but continually undergo thermal vibrations about their equilibrium positions.
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| 17. | When the Arm is hanging down in the stable equilibrium position \ theta _ 2 = 0.
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| 18. | For example, let us assume the equilibrium position sit somewhere on the rising slope of the resonance.
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| 19. | Due to the consistent vibration induced through thermal energy, they are permanently deviating from their equilibrium position.
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| 20. | On each bounce, the system is " trying " to return to its equilibrium position, but overshoots it.
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