Predictor-corrector procedures for pseudo-dynamic tests
Purpose - To propose novel predictor-corrector time-integration algorithms for pseudo-dynamic testing.Design methodology approach - The novel predictor-corrector time-integration algorithms are based on both the implicit and the explicit version of the generalized-α method. In the non-linear unforce...
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| Published in | Engineering computations Vol. 22; no. 7; pp. 783 - 834 |
|---|---|
| Main Authors | , |
| Format | Journal Article |
| Language | English |
| Published |
Bradford
Emerald Group Publishing Limited
01.10.2005
Emerald |
| Subjects | |
| Online Access | Get full text |
| ISSN | 0264-4401 1758-7077 |
| DOI | 10.1108/02644400510619530 |
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| Abstract | Purpose - To propose novel predictor-corrector time-integration algorithms for pseudo-dynamic testing.Design methodology approach - The novel predictor-corrector time-integration algorithms are based on both the implicit and the explicit version of the generalized-α method. In the non-linear unforced case second-order accuracy, stability in energy, energy decay in the high-frequency range as well as asymptotic annihilation are distinctive properties of the generalized-α scheme; while in the non-linear forced case they are the limited error near the resonance in terms of frequency location and intensity of the resonant peak. The implicit generalized-α algorithm has been implemented in a predictor-one corrector form giving rise to the implicit IPC-ρ∞ method, able to avoid iterative corrections which are expensive from an experimental standpoint and load oscillations of numerical origin. Moreover, the scheme embodies a secant stiffness formula able to approximate closely the actual stiffness of a structure. Also an explicit algorithm has been implemented, the EPC-ρb method, endowed with user-controlled dissipation properties. The resulting schemes have been tested experimentally both on a two- and on a six-degrees-of-freedom system, exploiting substructuring techniques.Findings - The analytical findings and the tests have indicated that the proposed numerical strategies enhance the performance of the pseudo-dynamic test (PDT) method even in an environment characterized by considerable experimental errors. Moreover, the schemes have been tested numerically on strongly non-linear multiple-degrees-of-freedom systems reproduced with the Bouc-Wen hysteretic model, showing that the proposed algorithms reap the benefits of the parent generalized-α methods.Research limitations implications - Further developments envisaged for this study are the application of the IPC-ρ∞ method and of EPC-ρb scheme to partitioned procedures for high-speed pseudo-dynamic testing with substructuring.Practical implications - The implicit IPC-ρ∞ and the explicit EPC-ρb methods allow a user to have defined dissipation which reduces the effects of experimental error in the PDT without needing onerous iterations.Originality value - The paper proposes novel time-integration algorithms for pseudo-dynamic testing. Thanks to a predictor-corrector form of the generalized-α method, the proposed schemes maintain a high computational efficiency and accuracy. |
|---|---|
| AbstractList | Purpose - To propose novel predictor-corrector time-integration algorithms for pseudo-dynamic testing.Design methodology approach - The novel predictor-corrector time-integration algorithms are based on both the implicit and the explicit version of the generalized-α method. In the non-linear unforced case second-order accuracy, stability in energy, energy decay in the high-frequency range as well as asymptotic annihilation are distinctive properties of the generalized-α scheme; while in the non-linear forced case they are the limited error near the resonance in terms of frequency location and intensity of the resonant peak. The implicit generalized-α algorithm has been implemented in a predictor-one corrector form giving rise to the implicit IPC-ρ∞ method, able to avoid iterative corrections which are expensive from an experimental standpoint and load oscillations of numerical origin. Moreover, the scheme embodies a secant stiffness formula able to approximate closely the actual stiffness of a structure. Also an explicit algorithm has been implemented, the EPC-ρb method, endowed with user-controlled dissipation properties. The resulting schemes have been tested experimentally both on a two- and on a six-degrees-of-freedom system, exploiting substructuring techniques.Findings - The analytical findings and the tests have indicated that the proposed numerical strategies enhance the performance of the pseudo-dynamic test (PDT) method even in an environment characterized by considerable experimental errors. Moreover, the schemes have been tested numerically on strongly non-linear multiple-degrees-of-freedom systems reproduced with the Bouc-Wen hysteretic model, showing that the proposed algorithms reap the benefits of the parent generalized-α methods.Research limitations implications - Further developments envisaged for this study are the application of the IPC-ρ∞ method and of EPC-ρb scheme to partitioned procedures for high-speed pseudo-dynamic testing with substructuring.Practical implications - The implicit IPC-ρ∞ and the explicit EPC-ρb methods allow a user to have defined dissipation which reduces the effects of experimental error in the PDT without needing onerous iterations.Originality value - The paper proposes novel time-integration algorithms for pseudo-dynamic testing. Thanks to a predictor-corrector form of the generalized-α method, the proposed schemes maintain a high computational efficiency and accuracy. Purpose To propose novel predictor-corrector time-integration algorithms for pseudo-dynamic testing. Design/methodology/approach The novel predictor-corrector time-integration algorithms are based on both the implicit and the explicit version of the generalized-a method. In the non-linear unforced case second-order accuracy, stability in energy, energy decay in the high-frequency range as well as asymptotic annihilation are distinctive properties of the generalized-a scheme; while in the non-linear forced case they are the limited error near the resonance in terms of frequency location and intensity of the resonant peak. The implicit generalized-a algorithm has been implemented in a predictor-one corrector form giving rise to the implicit IPC-p, method, able to avoid iterative corrections which are expensive from an experimental standpoint and load oscillations of numerical origin. Moreover, the scheme embodies a secant stiffness formula able to approximate closely the actual stiffness of a structure. Also an explicit algorithm has been implemented, the EPC-pb method, endowed with user-controlled dissipation properties. The resulting schemes have been tested experimentally both on a two- and on a six-degrees-of-freedom system, exploiting substructuring techniques. Findings The analytical findings and the tests have indicated that the proposed numerical strategies enhance the performance of the pseudo-dynamic test (PDT) method even in an environment characterized by considerable experimental errors. Moreover, the schemes have been tested numerically on strongly non-linear multiple-degrees-of-freedom systems reproduced with the Bouc-Wen hysteretic model, showing that the proposed algorithms reap the benefits of the parent generalized-a methods. Research limitations/implications Further developments envisaged for this study are the application of the IPC-p, method and of EPC-pb scheme to partitioned procedures for high-speed pseudo-dynamic testing with substructuring. Practical implications The implicit IPC-p. and the explicit EPC-pb methods allow a user to have defined dissipation which reduces the effects of experimental error in the PDT without needing onerous iterations. Originality/value The paper proposes novel time-integration algorithms for pseudo-dynamic testing. Thanks to a predictor-corrector form of the generalized-a method, the proposed schemes maintain a high computational efficiency and accuracy. The purpose of the study is to propose novel predictor-corrector time-integration algorithms for pseudo-dynamic testing. The novel predictor-corrector time-integration algorithms are based on both the implicit and the explicit version of the generalized-a method. In the non-linear unforced case second-order accuracy, stability in energy, energy decay in the high-frequency range as well as asymptotic annihilation are distinctive properties of the generalized-a scheme; while in the non-linear forced case they are the limited error near the resonance in terms of frequency location and intensity of the resonant peak. The analytical findings and the tests have indicated that the proposed numerical strategies enhance the performance of the pseudo-dynamic test method even in an environment characterized by considerable experimental errors. Moreover, the schemes have been tested numerically on strongly non-linear multiple-degrees-of-freedom systems reproduced with the Bouc-Wen hysteretic model, showing that the proposed algorithms reap the benefits of the parent generalized-a methods. |
| Author | Bonelli, Alessio Bursi, Oreste S. |
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| Cites_doi | 10.1108/02644400110387262 10.1002/nme.1620151011 10.1007/s00466-001-0273-z 10.1002/1096-9845(200101)30:1<59::AID-EQE996>3.0.CO;2-X 10.1006/jsvi.2000.3104 10.1016/S0267-7261(97)00017-1 10.1080/002071799220263 10.1016/0029-5493(80)90147-8 10.1002/eqe.4290200605 10.1006/jsvi.2001.3690 10.1002/eqe.4290150402 10.1007/BF00913408 10.1061/(ASCE)0733-9399(1993)119:12(2496) 10.1002/eqe.18 10.1002/cnm.640 10.1002/nme.1620381605 10.1002/eqe.4290230705 10.1002/nme.135 10.1002/(SICI)1096-9845(199604)25:4<333::AID-EQE548>3.0.CO;2-M 10.1002/(SICI)1096-9845(199904)28:4<393::AID-EQE823>3.0.CO;2-C 10.1016/0045-7825(79)90086-0 10.1002/(SICI)1096-9845(199807)27:7<711::AID-EQE753>3.0.CO;2-6 10.1193/1.1585867 10.1002/eqe.44 10.1061/(ASCE)0733-9399(1999)125:2(216) 10.1016/S0045-7825(00)00262-0 10.1016/0143-974X(94)90059-0 10.1002/eqe.4290200208 10.1002/eqe.176 10.1061/(ASCE)0733-9399(1990)116:7(1638) 10.1002/eqe.4290100506 10.1115/1.2900803 10.1006/jsvi.2002.5017 10.1061/(ASCE)0733-9399(1999)125:10(1133) 10.1002/eqe.188 10.1002/eqe.4290050306 10.1016/S0045-7825(96)01036-5 10.1061/(ASCE)0733-9399(1990)116:7(1618) |
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| Keywords | Tests and testing Structures Numerical analysis Programming and algorithm theory Predictor-corrector methods Dynamic testing High precision Substructure Dynamic method System with n degrees of freedom Annihilation Resonance frequency High speed Mode component synthesis Modelling Localization Iterative methods Programming theory Numerical integration Experimental study Algorithm theory Time domain method High efficiency Asymptotic approximation Non linear effect High frequency |
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| Title | Predictor-corrector procedures for pseudo-dynamic tests |
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