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Exact(5)
The condition for resonance is that the orbital periods of the moon and the ring particles be a ratio of whole numbers.
The condition for resonance is obtained.
The frequencies in vertical and horizontal directions are obtained and the condition for resonance is also revealed.
It is found that the existence of an eigenfrequency ω=ω0+iδ with a small imaginary part δ⪡ω0is not a sufficient condition for resonance under an external forcePexp (iω0t).
It can be understood from the condition for resonance in the presence of anisotropy field (HA): hf/μBg = Hcenter + H A, where h is the Plank's constant, g ≈ 2 for a free electron, f (8.984 GHz) is the fixed frequency of the applied microwave magnetic field, and μ B is the Bohr magnetron, respectively [31].
Similar(55)
It is shown that the presence of parametric terms gives rise to additional conditions for resonance in the support motion.
The theory successfully explains the acoustic and hydrodynamic conditions for resonance in experiments with a single side branch.
Conditions for resonance are obtained by applying He's variational iteration method, which should be avoided in the cushioning packaging design.
Conditions for resonance are obtained by applying the variational iteration method-II (VIM-II), which should be avoided in the cushioning packaging design.
The splitting of 2D band in the Raman spectra of SWCNTs was observed earlier [5, 10, 16] and was explained by the peculiarities of double electron-phonon resonance process providing different resonant conditions for resonances with different van Hove singularities (vHSs) of SWCNTs.
The condition for the resonance appearance is established when the frequency of light photons matches the frequency of surface electrons oscillating against the restoring force of the positive nuclei.
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