2002
DOI: 10.1006/jsvi.2001.3964
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Specifying Nodes at Multiple Locations for Any Normal Mode of a Linear Elastic Structure

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Cited by 18 publications
(4 citation statements)
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“…The desired nodes can either coincide with the 301 Downloaded by [Selcuk Universitesi] at 23:24 04 February 2015 location of the oscillator chain or it can be located elsewhere. Using the same method, Cha [12] analyzed a freely vibrating structure with a series of sprung masses attached aiming to impose multiple nodes for any normal mode. Alsaif and Foda [13] presented an exact, direct, and elegant method based on the dynamic Green's function to determine the optimum values of masses and/or springs and their locations on a beam in order to confine the vibration at an arbitrary location.…”
Section: Introductionmentioning
confidence: 99%
“…The desired nodes can either coincide with the 301 Downloaded by [Selcuk Universitesi] at 23:24 04 February 2015 location of the oscillator chain or it can be located elsewhere. Using the same method, Cha [12] analyzed a freely vibrating structure with a series of sprung masses attached aiming to impose multiple nodes for any normal mode. Alsaif and Foda [13] presented an exact, direct, and elegant method based on the dynamic Green's function to determine the optimum values of masses and/or springs and their locations on a beam in order to confine the vibration at an arbitrary location.…”
Section: Introductionmentioning
confidence: 99%
“…However, the inverse problem of estimating a design parameter, such as a stiffness or a mass, so that the combined system meets certain requirements has received less attention. A few notable inverse problems investigated include the imposition of nodes at certain locations on a continuous structure by attaching resonators, [18][19][20] constructing a physically realizable system from a beam's eigen solutions 21 and generating by design certain natural frequencies in a beam with an added mass. 22 Table 1.…”
Section: Introductionmentioning
confidence: 99%
“…Cha and Pierre [8] proposed a method to impose a single node using the normal modes of a supported linear structure by mounting a chain of absorbers. Cha [8,9] used a set of parallel sprung masses to impose multiple nodes for any normal mode of an elastic structure. Cha [10] also induced a single or normal node on an elastic structure subjected to harmonic excitation by using a set of elastically mounted masses.…”
Section: Introductionmentioning
confidence: 99%