IMPACT2014 & SMASH Vibration propagation and damping tests V0A-V0C: Testing and simulation

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IMPACT2014 & SMASH Vibration propagation and damping tests V0A-V0C: Testing and simulation SAFIR2014 Final seminar, 20.3.2015 Kim Calonius, Seppo Aatola, Ilkka Hakola, Matti Halonen, Arja Saarenheimo, Ari Vepsä and Markku Tuomala (TUT) VTT Technical Research Centre of Finland Ltd.

2 Introduction IMPACT2014 project focused on impact testing of reinforced concrete structures with water-filled, soft and hard projectiles. The purpose of the project was to simulate the phenomena arising in an aircraft crash against concrete structures and to measure the response of the structure. SMASH project focused on numerical simulation of the same phenomena. This presentation concentrates on three similar soft impact tests, V0A-V0C, which were carried out with the same structure having a front wall, a floor and a rear wall. The purpose of the tests was to obtain data regarding the propagation and damping of vibration and how they change from one test into another when the structure gets damaged. This presentation covers both testing and simulation.

3 The target

4 The target

5 The target

6 Reinforcement 50 mm Floor: direction of the impact: 10 mm rebars with spacing of 50 mm transverse direction: 6 mm rebars with spacing of 50 mm Front and rear walls: 6 mm rebars with spacing of 50 mm, both faces and both directions Stirrups around the hit point Concrete cover: 15 mm on both faces

7 7 accelerometers 7 displacement sensors 10 strain gauges 4 support forces (1 on each horizontal support) 2 high shutter speed video cameras Instrumentation

8 The missile Soft stainless steel missile =254 mm, t=2mm Total mass Test A: 50.08 kg Test B: 49.92 kg Test C: 50.03 kg Impact velocities A: 111.2 m/s B: 113.6 m/s C: 116.8 m/s Shortening and the number of folds A:1011/1201 mm B:1001/1153 mm C:1101/1274 mm A:22 folds B:20 folds C:25 folds

9 High speed video (V0A-Front) vimp=111.2 m/s

10 The target after the tests Back Front

11 Modal analysis Measurement model 94 output points 3 degrees of freedom on each point Before Impact Tests After 1st Impact Test After 3rd Impact Test After 3rd Impact Test ref MP 101 ref MP 101 ref MP 101 ref MP 102 Frequency Damping Frequency Damping Frequency Damping Frequency Damping (Hz) (%) (Hz) (%) (Hz) (%) (Hz) (%) 16.0 0.7 15.1 3.5 13.1 0.9 32.6 1.7 35.8 1.9 36.5 1.8 45.4 0.6 43.6 1.1 41.3 1.7 41.3 1.8 56.2 1.4 54.4 1.9 52.8 2.0 70.8 0.8 68.4 1.2 65.6 1.5 66.0 1.2 134.2 1.1 116.2 1.3 96.4 3.4 94.4 3.3 151.5 0.7 136.7 2.2 121.0 3.7 225.9 0.7 215.1 1.4 199.2 2.1 267.6 0.6 265.5 0.6 254.6 1.0 255.8 0.3 The natural frequencies decreased slightly from test to the next with mode 2 making an exception. In general, the frequencies decreased 5 28 % from the first measurement set to the last one with the average value being 10 %. In general, the damping values increased with modes 1 and 2 making exceptions as their damping decreased from test 1 to test 3.

12 Time domain Displacements Frequency domain

13 Displacements The measured peak values increased somewhat from test to the next one 34 % on average between tests A and B 17 % on average between tests B and C Part of the increase can be credited to the increasing impact velocity from test A to test B and from test B to test C: The main frequencies at which the response occurred decreased slightly from test to the next one with the frequencies being slightly lower than the ones identified in the modal analyses.

14 Accelerations Time domain Frequency domain The impact duration

15 Accelerations The measured peak values decreased somewhat from test to the next one 49 % on average between tests A and B 19 % on average between tests B and C The main frequencies at which the response occurred decreased slightly from test to the next one with the frequencies being slightly lower than the ones identified in the modal analyses.

16 Strains on the reinforcement

17 Strains on the reinforcement Only the strains measured at the hit area exceeded the static yield limit of the rebars. The strains at the junction between the front wall and the floor were roughly one decade lower and the strains at the junction between the floor and the rear wall two decades lower than those at the hit area. No clear tendency could be identified for the change of behaviour of the stresses between the consecutive tests. The additional permanent strains tended to decrease from test to the next. The elastic the strain variation happened mainly at two frequencies which tended to be slightly lower than the natural frequencies of vibration identified in the modal tests. These frequencies also tended to decrease 6-9 % from a test to the next.

18 Conclusions of the testing The damage caused for the structure by the tests was relatively mild and limited mainly to the front wall. The measured peak displacements increased slightly from a test to the next one. The measured peak accelerations decreased in a similar manner. Clear behaviour could be identified for the reinforcement strains. For each response type, the main frequencies at which the response occurred decreased slightly from a test to the next one with the frequencies being slightly lower than the ones identified in the modal analyses. All in all, the test series was a successful start for testing of vibration propagation and damping properties of three-dimensional reinforced concrete structures under soft projectile impact. wealth of valuable data for validation of predictive models valuable experience that can be used in future when designing similar tests.

19 Introduction to simulation The main aim of this first study was to carry out sensitivity analyses on the test set-up used in Test V0 in order to find out the essential phenomena to be considered in the future numerical studies of similar cases Two types of codes with also some differences in the applied methodology are used: Commercial Abaqus FE code In-house FE code using Reissner-Mindlin (RM) elements. Effect of the test frame Effect of the way how the loading is applied loading function calculated with the Riera method coupled approach where also the missile is modelled Abaqus/Explicit version 6.14-1 Mainly shell elements Beam elements for the bolts, spring elements for some supports Material properties based on material tests

20 Abaqus finite element model

21 Simulation cases with Abaqus case load frame gravity rate dep. damping line colour line type Riera no yes no no green square dot, double Riera no yes yes no green solid, double Riera yes no yes no orange solid Riera yes yes no no red square dot Riera yes yes yes no red solid Riera yes yes yes yes dark red dash dot missile yes no no no blue square dot missile yes no yes no blue solid

22 Loading in Abaqus model Impact force as function of time calculated with Riera method (Riera) and FEM (Missile contact). Deformed missile after test V0A and in the corresponding simulation of an impact to a rigid plate

23 Abaqus case M-F

24 Abaqus case M-F Equivalent plastic strain distribution in back surface rebars at 0.5 s with scale from 0 to 1 %.

25 Abaqus case R-F-G

26 Model with Reissner-Mindlin (RM) elements Moment curvature relationship with 6 mm and 10 mm bars. Finite element mesh of impact wall

27 RM model results Load function of the folding viscoplastic model. Final shape of the folding viscoplastic model

28 RM model results Floor response spectrum of acceleration history at top of rear wall with damping ratio of 0.05 and structural Rayleigh damping: d1: d2: d3: 0.05 at 45 and 5000 Hz 0.03 at 30 and 200 Hz 0.1 at 45 and 5000 Hz Floor response spectrum of acceleration history at top of rear wall showing effect of loading function: 2-a6: 2-a6-fold: average model folding model with damping ratio of 0.05 and structural Rayleigh damping: d1: 0.05 at 45 and 5000 Hz

29 Three consequtive impacts (RM model) Reissner-Mindlin elements No frame Rayleigh damping No folding

30 Simulation results RM model

31 Simulation results code load frame gravity Riera no yes Riera no yes Riera yes no Riera yes yes Riera yes yes Riera yes yes missile yes no missile yes no Floor response spectra of back slab top accelerations in the test and in several simulation cases with Abaqus model

32 Simulation results C frame C A A A frame Floor response spectra of back slab top accelerations in the test and in several simulation cases with RM model

33 Conclusions of the simulations Assumed nonlinear material properties of concrete strongly affect the bending behaviour of the wall. Most of the additional characteristics bring the dynamic model behaviour closer to the real behaviour of the test structure. Abaqus: Floor response spectra results obtained either using the loading function or by applying the missile model are rather similar below a frequency of 100 Hz. Correct Rayleigh damping would bring FRS closer to reality Reissner-Mindlin elements: Application of load was done in two alternative methods: Average visco-plastic folding mechanism was adopted in the Riera formulation Actual forming of folds was followed Only a small effect on the acceleration response spectra Behaviour of the front wall can already be predicted reliably Prediction of vibrations and deformation of the whole structure requires more study