Random Vibration in Mechanical Systems 1963
DOI: 10.1016/b978-1-4832-3259-1.50006-x
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Transmission of Random Vibration

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Cited by 38 publications
(49 citation statements)
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“…The classical TMD technology (Brock, 1946; Crandall and Mark, 1963; Den Hartog, 1956; Ormondroye and Den Hartog, 1928; Thomson and Dahleh, 1988), which dissipates vibratory energy through a set of damper and spring connecting a small mass (secondary system) to the main (primary) structure, has been illustrated in Figure 1(a). The natural frequency of the attached secondary system which is a TMD needs to be very close to the dominant mode of the primary structure, and thus a large reduction in the dynamic responses of the primary structure around the natural frequency of this dominant mode can be achieved.…”
Section: Tmds and Their Modificationsmentioning
confidence: 99%
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“…The classical TMD technology (Brock, 1946; Crandall and Mark, 1963; Den Hartog, 1956; Ormondroye and Den Hartog, 1928; Thomson and Dahleh, 1988), which dissipates vibratory energy through a set of damper and spring connecting a small mass (secondary system) to the main (primary) structure, has been illustrated in Figure 1(a). The natural frequency of the attached secondary system which is a TMD needs to be very close to the dominant mode of the primary structure, and thus a large reduction in the dynamic responses of the primary structure around the natural frequency of this dominant mode can be achieved.…”
Section: Tmds and Their Modificationsmentioning
confidence: 99%
“…Because Den Hartog (1956) first proposed an optimal design approach of TMD for an undamped single-degree-of-freedom (SDOF) structure, many optimal design methods of TMD system have been developed to suppress the structural vibration induced by various types of excitation sources. Crandall and Mark (1963) adopted the random vibration theory to analyze a SDOF structure attached with a single TMD system under white noise base excitation.…”
Section: Optimally Designed Tmd Systemmentioning
confidence: 99%
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