1985
DOI: 10.1016/0022-460x(85)90443-2
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Free vibrations of a mono-coupled periodic system

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Cited by 106 publications
(49 citation statements)
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“…It allows to define the vector of generalized displacements and generalized forces at the end of a periodic cell in terms of the same vector at the beginning of the cell. Examples for mono-coupled elastic periodic structures can be found in [20,[25][26][27]. In the present case, the structure is a bicoupled system, because there are 2 degrees of freedom, i.e.…”
Section: (B) Dispersion In the Asymptotic Reduced Modelmentioning
confidence: 93%
“…It allows to define the vector of generalized displacements and generalized forces at the end of a periodic cell in terms of the same vector at the beginning of the cell. Examples for mono-coupled elastic periodic structures can be found in [20,[25][26][27]. In the present case, the structure is a bicoupled system, because there are 2 degrees of freedom, i.e.…”
Section: (B) Dispersion In the Asymptotic Reduced Modelmentioning
confidence: 93%
“…We also assume that each cylinder has the same mass M" @ ah. Using the method of Faulkner & Hong (1985), we obtain eigenfrequencies and eigenmodes (normal modes) of the dry system as…”
Section: Resonant Modes For An Elastically Connected Cylinder Arraymentioning
confidence: 99%
“…If W ¼ 0 or p; only one of the two coincident eigenvalues must be taken. As usually done in the literature, previous findings can be restated in terms of the propagation constants m i ; instead of the eigenvalues l i ; by defining l i ¼ e To solve (2) it is convenient to rewrite it in terms of the propagation constant m: By letting l ¼ e m and multiplying by e 2m ; equation (2) reads…”
Section: Propagation Regions On the Invariants' Planementioning
confidence: 99%