Submitted:
14 July 2023
Posted:
18 July 2023
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Abstract
Keywords:
1. Introduction
- Selection of the parameters to be estimated in the investigated problem, namely choice of the sought quantities to be identified, toward assessment and calibration of the specific behaviour and model.
- Design of the experiment, as the best suitable experimental procedure to collect response data as source of information for a subsequent identification phase.
- Test simulation, by computational modelling, to effectively reproduce the experimental phenomena, in a reliable manner, to evaluate numerical counterparts of experimental measurements.
- Definition of a feasible “search domain”, namely of a constrained space of the underlying system parameters, with limits possibly suggested by experts or guidelines, to be adopted within the identification procedure.
- Sensitivity analysis (see, e.g., [8]) of the investigated problem, with respect to the sought parameters, in order to efficiently understand the specific influence of the selected parameters (possibly, to be reduced) on the system behaviour and, specifically, on the observed quantities.
- Formulation of an appropriate “discrepancy function”, to be minimised, as a scalar norm between measured and computed quantities, therefore forming a function of the input sought parameters, possibly also accounting for sources of uncertainty.
- Selection and implementation of a minimisation algorithm, in order to handle, in a robust and efficient manner, the foreseen optimisation problem of inverse identification, selecting for instance among mathematical programming methods, evolutive methods or artificial intelligence methods.
- Validation and accuracy checks, developed to test and confirm the effectiveness of the specific devised approach, either on pseudo–experimental (necessary validation condition) or real experimental measurement data.
2. Parameter Identification Relying on Dynamic Measurements: Problem Setup
- The adoption of modal properties, as a unique source of measurement data, intrinsically brings in a “non–well posedness” condition, in terms of multiple “realisations”, in terms of ratios between stiffness and mass properties of a structural system, namely leading to the identification of the correlated parameters, as also shown by the “valley” of minima in the discrepancy function plot for a two–dimensional parameter space (see Figure 1).
- Uniqueness of the optimisation problem may be found, in a two–dimensional parameter space, fixing either one of the two constitutive parameters or their ratio. Therefore, in a practical application case study, additional evaluations or measurements shall be required, to possibly estimate specific mechanical parameters at the local scale (e.g., by material testing) or from global scale measurements devised by experimentally controlled static or dynamic testing of the structure.
- The enlargement of the parameter space size further exhibits a correlation between parameters, namely a possible balancing effects or multiple mathematically equivalent “realisations”. Such an observation is graphically depicted in Figure 2, where three–dimensional cross sections of the discrepancy function, analysed in a four–dimensional parameter space, reveal possible “valleys” of minima, also in terms of ratios between stiffness or mass density parameters (Figure 2a and Figure 2b, respectively).
- Therefore, a robust Inverse Analysis procedure shall require complemented measurement data, suitable to assess the behaviour of diverse structural components and capable to estimate, possibly in a sequential procedure, both stiffness and mass density properties, for instance also considering experimental static or dynamic loading tests on the structure.
3. Optimised Structural Modelling on the Case Study of a Historical Concrete Bridge
- Among the selected modelling parameters, for material and boundary condition standpoints, with reference to the selected measurements and discrepancy function, a major role is assumed by nine mechanical constitutive parameters, namely Young’s moduli () and mass densities () of the structural components, as pointed out by previous sensitivity analyses in [37].
- Global property measurement, such as for natural frequency, may suffer reduced sensitivity effects, causing significant difficulties in specific parameter identification. This particular condition can be observed from the numerical results in Table 2, third and fourth columns, where the global frequency variation is computed for a 30% range variation on parabolic arches elastic modulus () and mass density (), with variation gain on the results approximately reduced by one order of magnitude.
- According to the previous point, in order to ensure a robust and reliable parameter identification procedure, specific requirements are expected in the measuring stages, namely significantly reducing noise effects and providing complete structural observations, possibly complemented by local detailing measurements and estimations.
- As a complementary global source of measurement information, vibration modes can carry similar observations, as the above–mentioned for natural frequencies, both on sensitivity effects and complete measurement requirements. As an example, the results reported in Figure 7 graphically represent the numerical results for the second vibration mode of the bridge at the base configuration and for a 30% range variation of various specific parameters, without, however, structurally meaningful mode shape variations.
- The effect of boundary conditions on the mode shapes and natural frequencies appears to be less sensitive with respect to material parameters of bridge structural components (see, also, sensitivity analysis in [37]). However, the influence of mechanical parameters of elastic boundary conditions can rule a contribution approximately of one order of magnitude lower, though not negligible on a global scale structural behaviour (see, for an example, Table 2, fifth column). Therefore, particular attention is required in setting numerical model definition also regarding the boundary conditions, in order to produce a reliable numerical instrument, avoiding biased parameter fitting, in Inverse Analysis methodology for structural assessment and diagnosis.
4. Conclusions
Acknowledgments
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| Parameter | Lower | Upper | Reference |
|---|---|---|---|
| bound | bound | value | |
| Deck elastic modulus, [GPa] | 24.4 | 45.4 | 34.9 |
| Main longitudinal girders elastic modulus, [GPa] | 24.4 | 45.4 | 34.9 |
| Parabolic arches elastic modulus, [GPa] | 25.0 | 46.4 | 35.7 |
| Hangers elastic modulus, [GPa] | 25.0 | 46.4 | 35.7 |
| Upper transverse beams elastic modulus, [GPa] | 25.0 | 46.4 | 35.7 |
| Deck mass density, [kg/m3] | 1710 | 3170 | 2440 |
| Main longitudinal girders mass density, [kg/m3] | 1710 | 3170 | 2440 |
| Parabolic arches mass density, [kg/m3] | 1710 | 3170 | 2440 |
| Hangers mass density, [kg/m3] | 1710 | 3170 | 2440 |
| Upper transverse beams mass density, [kg/m3] | 1710 | 3170 | 2440 |
| I–support translational (x–axis) spring stiffness, [kN/m] | 10−7 | 10−3 | 10−5 |
| I–support translational (y–axis) spring stiffness, [kN/m] | 108 | 1012 | 1010 |
| I–support rotational spring stiffness, [kNm] | 10−7 | 10−3 | 10−5 |
| II–support rotational spring stiffness, [kNm] | 10−7 | 10−3 | 10−5 |
| Frequency [Hz] | Reference parameter values | +30% | +30% | +30% |
|---|---|---|---|---|
| 2.5312 | +1.28% | −4.22% | +0.07% | |
| 3.7908 | +3.53% | −2.91% | +0.01% | |
| 3.9781 | +4.41% | −5.30% | +0.06% | |
| 5.4889 | +1.52% | −1.42% | +0.08% | |
| 5.8677 | +3.72% | −1.77% | +0.30% | |
| 6.4903 | +1.63% | −4.26% | +0.00% | |
| 7.7809 | +4.66% | −6.00% | +0.18% | |
| 7.8392 | +4.08% | −2.36% | +0.15% | |
| 8.8131 | +2.41% | −2.80% | +0.16% | |
| 10.311 | +1.84% | −5.40% | +0.01% | |
| 10.325 | +4.03% | −2.99% | +0.10% | |
| 10.672 | +3.73% | −4.45% | +0.28% | |
| 10.888 | +4.45% | −5.72% | +0.23% | |
| 12.139 | +1.38% | −4.10% | +0.06% | |
| 12.160 | +4.05% | −1.55% | +0.01% | |
| 12.490 | +2.43% | −1.46% | +0.09% |
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