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https://doi.org/10.1002/nme.255
DC Field | Value | |
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dc.title | Convergence study of the truncated Karhunen-Loeve expansion for simulation of stochastic processes | |
dc.contributor.author | Huang, S.P. | |
dc.contributor.author | Quek, S.T. | |
dc.contributor.author | Phoon, K.K. | |
dc.date.accessioned | 2014-06-17T08:15:51Z | |
dc.date.available | 2014-06-17T08:15:51Z | |
dc.date.issued | 2001-11-30 | |
dc.identifier.citation | Huang, S.P., Quek, S.T., Phoon, K.K. (2001-11-30). Convergence study of the truncated Karhunen-Loeve expansion for simulation of stochastic processes. International Journal for Numerical Methods in Engineering 52 (9) : 1029-1043. ScholarBank@NUS Repository. https://doi.org/10.1002/nme.255 | |
dc.identifier.issn | 00295981 | |
dc.identifier.uri | http://scholarbank.nus.edu.sg/handle/10635/65354 | |
dc.description.abstract | A random process can be represented as a series expansion involving a complete set of deterministic functions with corresponding random coefficients. Karhunen-Loeve (K-L) series expansion is based on the eigen-decomposition of the covariance function. Its applicability as a simulation tool for both stationary and non-stationary Gaussian random processes is examined numerically in this paper. The study is based on five common covariance models. The convergence and accuracy of the K-L expansion are investigated by comparing the second-order statistics of the simulated random process with that of the target process. It is shown that the factors affecting convergence are: (a) ratio of the length of the process over correlation parameter, (b) form of the covariance function, and (c) method of solving for the eigen-solutions of the covariance function (namely, analytical or numerical). Comparison with the established and commonly used spectral representation method is made. K-L expansion has an edge over the spectral method for highly correlated processes. For long stationary processes, the spectral method is generally more efficient as the K-L expansion method requires substantial computational effort to solve the integral equation. The main advantage of the K-L expansion method is that it can be easily generalized to simulate non-stationary processes with little additional effort. Copyright © 2001 John Wiley & Sons, Ltd. | |
dc.description.uri | http://libproxy1.nus.edu.sg/login?url=http://dx.doi.org/10.1002/nme.255 | |
dc.source | Scopus | |
dc.subject | Covariance models | |
dc.subject | Karhunen-Loeve expansion | |
dc.subject | Non-stationary Gaussian process | |
dc.subject | Simulation | |
dc.subject | Stationary Gaussian process | |
dc.subject | Stochastic representation | |
dc.type | Article | |
dc.contributor.department | CIVIL ENGINEERING | |
dc.description.doi | 10.1002/nme.255 | |
dc.description.sourcetitle | International Journal for Numerical Methods in Engineering | |
dc.description.volume | 52 | |
dc.description.issue | 9 | |
dc.description.page | 1029-1043 | |
dc.description.coden | IJNMB | |
dc.identifier.isiut | 000171912600008 | |
Appears in Collections: | Staff Publications |
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