2011
DOI: 10.1002/eqe.1147
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On the performance of lumped parameter models with gyro‐mass elements for the impedance function of a pile‐group supporting a single‐degree‐of‐freedom system

Abstract: SUMMARYLumped parameter models with a so called "gyro-mass" element (GLPMs) have been proposed recently in response to a strong demand for efficiently and accurately representing frequency-dependent impedance functions of soil-foundation systems. Although GLPMs are considered to be powerful tools for practical applications in earthquake engineering, some problems remain. For instance, although GLPMs show fairly close agreement with the target impedance functions, the accuracy of the transfer functions and the … Show more

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Cited by 26 publications
(25 citation statements)
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“…The configurations and properties of springs, dampers and masses need to be calibrated so that the overall dynamic response of the system is similar to the frequency response of the actual soil–foundation system. Different models have been proposed in literature such as , among many others.…”
Section: Review Of Time‐domain Analysis Methods With a Frequency‐depementioning
confidence: 99%
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“…The configurations and properties of springs, dampers and masses need to be calibrated so that the overall dynamic response of the system is similar to the frequency response of the actual soil–foundation system. Different models have been proposed in literature such as , among many others.…”
Section: Review Of Time‐domain Analysis Methods With a Frequency‐depementioning
confidence: 99%
“…This exponential in front of the summation term is the displacement definition introduced in Eq. (11) and can be divided out to formulate the expression for the impedance function in the frequency domain as presented in Eq. (13).…”
Section: Inverse Fourier Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…PROPOSED MODEL ASSEMBLYBecause the inelastic dynamic behavior of the condensed soil foundation segment can now be extracted in the form of a preselected number of (reduced) complex matrix pairs RF and S reduced , it is possible to develop a modified LP model assembly capable of emulating such behavior. The predefined type 3 LP design, proposed by Saitoh, is selected as the basis of the newly developed inelastic LP model. The resulting LP model for the scenario of a single interface DOF is illustrated in Figure .…”
Section: Inelastic Ssi System Order Reductionmentioning
confidence: 99%
“…where C i are the Fourier amplitude coefficients, f i are the discrete fast Fourier transform frequencies between 0.25 Hz ≤ f i ≤ 20 Hz, and Δf ≤ 0.05 Hz is the frequency interval used in the fast Fourier transform. It is noted herein that the mean frequency of excitation f m is used for the parameterization of the frequency-independent K-V model as opposed to the fundamental frequency f SSI of or the pseudonatural frequency (f pSSI ) of the coupled system, the latter defined as the frequency where the ratio of the horizontal displacement of the superstructure us is maximized with respect to the foundation motion up [42] for three main reasons: (i) being a key parameter of the dynamic stiffness of the system, (ii) it has been parametrically found as the most efficient alternative in defining frequencyindependent K-V models [21], and (iii) given that the site response analysis of the five soil profiles studied is equivalent linear, the fundamental frequency f SSI or f pSSI of each coupled system is effectively intensity-dependent, thus calibrating that the K-V model to the frequency of the system would hinder the identification of clear trends. In regard to the LP dynamic spring formulation, the three-core LP model illustrated in Figure 10(d) is selected for the particular study because of the accurate representation and computational efficiency that it has to offer.…”
Section: Extracted Dynamic Stiffness Integration Into the Bridge Fem mentioning
confidence: 99%