2015
DOI: 10.1016/j.apm.2014.11.038
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Green’s function for uniform Euler–Bernoulli beams at resonant condition: Introduction of Fredholm Alternative Theorem

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Cited by 18 publications
(5 citation statements)
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“…They notice that for S near zero, it is the equivalent of 0 →  , in the absence of resonance L n S /    , the dynamic Green function reduced to the static Green function of a supported beam such explained in the paper (Hozhabrossadati SM et al, 2015).…”
Section: Introductionmentioning
confidence: 99%
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“…They notice that for S near zero, it is the equivalent of 0 →  , in the absence of resonance L n S /    , the dynamic Green function reduced to the static Green function of a supported beam such explained in the paper (Hozhabrossadati SM et al, 2015).…”
Section: Introductionmentioning
confidence: 99%
“…(1) With L being the length of the beam and the 8 coefficients from A to H being constant functions of u, these coefficients are calculated by evaluating the boundary and continuity conditions and shear force. The solution can be simplified, and solving the system with 8 equations, given this form, is developed in detail (Hozhabrossadati SM et al, 2015).…”
Section: Introductionmentioning
confidence: 99%
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“…The Green's functions were obtained by using the techniques of separation of variables and the Laplace transformation. Hozhabrossadati et al [24] analyzed the Bernoulli beams under the resonant condition and they developed a Green's function procedure by constructing the proper Green's function and adopting the pertinent boundary conditions. Mohammad et al [25] studied the thermoelastic static behaviors of a curved circular beam through Green's function technique.…”
Section: Introductionmentioning
confidence: 99%
“…In the past decades, there are many other works related to frequency analysis of interactive system consisting of a beam with several attachments. The analytical approaches used to solving this problem included assumed-modes method (Cha, 2005(Cha, , 2007, the Green's function method (Hozhabrossadati et al, 2015;Kukla, 1994;Kukla & Posiadala, 1994) x x x  , the beam is split into 1 n  segments, and the two boundaries are denoted as spring 0 and n. The first i -1 segments are between the spring j-1 to j ( 1, , 1 ji    ); the ji   segment is between the spring 1 i  to the sensor; the ji   segment is between the sensor and the spring i; and the rest segments are between the spring j-1 to j ( 1, ., j i n The compatibility conditions at each spring location can be written as For the sensor location, the compatibility conditions can be written as…”
Section: Analysis Of Quasi-static Moving Mass Problemmentioning
confidence: 99%