Estimating the upper limit of prehistoric peak ground acceleration using an in situ, intact and vulnerable stalagmite from Plavecká priepast cave (Detrekői-zsomboly), Little Carpathians, Slovakia—first results
Abstract:Earthquakes hit urban centres in Europe infrequently, but occasionally with disastrous effects. Obtaining an unbiased view of seismic hazard (and risk) is therefore very important. In principle, the best way to test probabilistic seismic hazard assessments (PSHAs) is to compare them with observations that are entirely independent of the procedure used to produce PSHA models. Arguably, the most valuable information in this context should be information on long-term hazard, namely maximum intensities (or magnitu… Show more
“…where a 0 = 0.559; a 1 = 3.507; a 2 = 9.820; a 3 = 19.244; a 4 = 31.808; D is the average diameter, H is the height of stalagmite, q is the mass density of the stalagmite, E is the dynamic Young's modulus (see also Bednárik 2009;Gribovszki et al 2017). The latter values are given in Table 4, and they show indeed a rather good correspondence with the numerical values in the far right column of Table 3.…”
Abstract-Recently, it has been argued that natural, intact stalagmites in caves give important constraints on seismic hazard since they have survived all earthquakes over their (rather long) life span. This suggests that the pattern of oscillation should be fully understood, including the splitting of eigenfrequencies that has occurred in recent cave observations. In the present study, we simulate the oscillation of a given stalagmite by setting up four simplified models of the stalagmite. The dimensions of the intact stalagmite were measured in situ, and the geo-mechanical and elastic parameters of broken stalagmite samples, determined in geo-mechanical laboratory, have been taken into account. The eigenfrequencies of the stalagmite are then calculated numerically, by the finite element method, and compared with the measured in situ values. The latter have shown splitting of eigenfrequencies, which we were able to reproduce by the numerical model calculations taking into account the asymmetric shape of the stalagmite.
“…where a 0 = 0.559; a 1 = 3.507; a 2 = 9.820; a 3 = 19.244; a 4 = 31.808; D is the average diameter, H is the height of stalagmite, q is the mass density of the stalagmite, E is the dynamic Young's modulus (see also Bednárik 2009;Gribovszki et al 2017). The latter values are given in Table 4, and they show indeed a rather good correspondence with the numerical values in the far right column of Table 3.…”
Abstract-Recently, it has been argued that natural, intact stalagmites in caves give important constraints on seismic hazard since they have survived all earthquakes over their (rather long) life span. This suggests that the pattern of oscillation should be fully understood, including the splitting of eigenfrequencies that has occurred in recent cave observations. In the present study, we simulate the oscillation of a given stalagmite by setting up four simplified models of the stalagmite. The dimensions of the intact stalagmite were measured in situ, and the geo-mechanical and elastic parameters of broken stalagmite samples, determined in geo-mechanical laboratory, have been taken into account. The eigenfrequencies of the stalagmite are then calculated numerically, by the finite element method, and compared with the measured in situ values. The latter have shown splitting of eigenfrequencies, which we were able to reproduce by the numerical model calculations taking into account the asymmetric shape of the stalagmite.
“…In contrast, the presence of intact speleothems indicates that, considering their growth, no earthquake-driven ground motions were sufficiently large to break them. Hence, knowing the speleothem's characteristics allows estimating an upper limit on past horizontal ground motions that did not result in the failure of studied speleothems [12][13][14][15][16][17][18][19][20]. This information provides an important view in the past seismicity in the area where the cave is located.…”
Section: Introductionmentioning
confidence: 99%
“…The natural frequency and damping factor of the speleothems are fundamental parameters in the study of their response to seismic shaking. With an eigenfrequency in the range of moderate local (1)(2)(3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18)(19)(20) or larger remote earthquakes (0.1-10 Hz), earthquake ground motions can cause resonance of the speleothem. Their failure can occur at a lower acceleration than predicted by static methods.…”
Section: Introductionmentioning
confidence: 99%
“…Their failure can occur at a lower acceleration than predicted by static methods. The in situ study of the natural frequency of speleothems has been done with a laser interferometer [23,24] or with a geophone attached to the stalagmite [13][14][15][16][17]19]. In those experiments, the stalagmite was slightly excited using a finger or a rubber hammer.…”
Broken or deformed speleothems have been used as indicators of paleo-earthquakes since the 1990s; however, a causal link is difficult to prove except for some thin speleothems. In contrast, the presence of intact speleothems permits estimating an upper limit of the level of horizontal ground motions of past seismicity in the area. The natural frequencies of speleothems are fundamental parameters for their response to earthquakes. This study proposes a new method of in situ characterization of these natural frequencies. Tested in the Han-sur-Lesse cave (Belgian Ardennes), the method is based on recording the ambient seismic noise using three-component sensors on a stalagmite and a 3D laser scan of its shape. The ambient seismic noise records allow a precise determination of the eigenfrequencies of the stalagmite. In addition, numerical models based on the 3D scan show good consistency between measured and modeled data. The joint analysis of these two techniques concludes that the shape of the stalagmite (elliptical cross-section and shape irregularities) influence the eigenfrequencies and polarization of the modes while also causing a near-orthogonal split of natural frequencies. The motions recorded on the stalagmite show significant amplification compared to those recorded at the free surface outside the cave, which has a strong impact on seismic hazard assessment based on speleothems.
“…There are, however, cases when the lowest eigenfrequencies of the studied bodies close to collapse or breaking can be only several hertz or lower, falling thus into a typical seismic-frequency band and, therefore, resonances may occur. The examples are, e.g., natural rock columns in the Chiricahua Mountains, Arizona, where the heights of columns may be limited by a fundamental vibrational mode that matches the seismic shaking of large and moderate prehistoric earthquakes occurred nearby (Hall 1996), the Minaret of Jam in Afghanistan with fundamental period longer than one second (Menon et al 2004) or speleothems (Lacave et al 2004;Becker et al 2006), where eigenfrequencies can be measured in situ, calculated theoretically and modelled numerically by finite element method (Gribovszki et al 2017(Gribovszki et al , 2018. Precariously balanced rocks represent another class of bodies as they are not fixed to their bedrocks and thus their wobbling is possible.…”
Stability of precariously balanced rocks is employed in seismic hazard estimates. Standard toppling models of these rocks are based on a rigid body motion, i.e., this approximation assumes that their eigenfrequencies are infinite in any position of a rock. This assumption is, however, questionable in the case of rocking stones oscillating with lowest eigenfrequencies of only several hertz when resonance effects facilitating rolling/wobbling due to a seismic signal cannot be a priori excluded. An example demonstrating existence of such low frequencies is ''the Hus Pulpit'' rocking stone located in the Central Bohemian Pluton (49.568N,14.363E). The observed lowest frequencies recorded by a Guralp CMG-40T seismometer located on the top of this rocking stone are 3, 7 and 9 Hz with the quality factors of 60, 55 and 77, respectively. Using the COMSOL Multiphysics software package we model the oscillations of this rocking stone numerically and demonstrate that these observed low frequencies and their dampings can be explained by a force interaction between the stone base and the bedrock that can formally be interpreted as the damped elastic response of the bedrock to its surface deformation by the stone. We also numerically study stability of the stone under the presence of such an interaction and conclude that beginning of toppling requires very high horizontal PGV (PGA) for input seismic frequencies even at the resonance frequencies. However, different numerical models, where the seismic displacements are considered as the direct input at the rock base, can result in rock instabilities under a presence of an M ¼ 7 earthquake at a distance of about 150 km.
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