Abstract
The regularity of earthquakes, their destructive power, and the nuisance of ground vibration in urban environments, all motivate designs of defence structures to lessen the impact of seismic and ground vibration waves on buildings. Low frequency waves, in the range 1–10 Hz for earthquakes and up to a few tens of Hz for vibrations generated by human activities, cause a large amount of damage, or inconvenience; depending on the geological conditions they can travel considerable distances and may match the resonant fundamental frequency of buildings. The ultimate aim of any seismic metamaterial, or any other seismic shield, is to protect over this entire range of frequencies; the long wavelengths involved, and low frequency, have meant this has been unachievable to date. Notably this is scalable and the effects also hold for smaller devices in ultrasonics. There are three approaches to obtaining shielding effects: bragg scattering, locally resonant sub-wavelength inclusions and zero-frequency stop-band media. The former two have been explored, but the latter has not and is examined here. Elastic flexural waves, applicable in the mechanical vibrations of thin elastic plates, can be designed to have a broad zero-frequency stop-band using a periodic array of very small clamped circles. Inspired by this experimental and theoretical observation, all be it in a situation far removed from seismic waves, we demonstrate that it is possible to achieve elastic surface (Rayleigh) wave reflectors at very large wavelengths in structured soils modelled as a fully elastic layer periodically clamped to bedrock. We identify zero frequency stop-bands that only exist in the limit of columns of concrete clamped at their base to the bedrock. In a realistic configuration of a sedimentary basin 15 m deep we observe a zero frequency stop-band covering a broad frequency range of 0–30 Hz.
Highlights
The desire to deflect, absorb or redirect waves is ubiquitous across many fields: electromagnetics, optics, hydrodynamics, acoustics and elasticity
[53] Bloch’s theorem means that, for an infinite array, one need only consider the wavenumbers in the irreducible Brillouin zone (IBZ) which, for a square lattice, are those in the triangle GXM (G = (0, 0), X = (p a, 0), M = (p a, p a)) shown as the inset to figure 1(a) and for clarity we show the frequency dependence versus wavenumbers going around the edges of the IBZ
We explore the potential of seismic metamaterial devices shown in figure 2; the side view shows a structure atop a soil layer of finite thickness that overlays the bedrock; columns clamped to the bedrock puncture the soil layer and reach to the surface, or close to the surface, a top view shows the array of columns encircling the building to be protected
Summary
The desire to deflect, absorb or redirect waves is ubiquitous across many fields: electromagnetics, optics, hydrodynamics, acoustics and elasticity. Ground vibrations, caused by even minor earthquakes, have an impact upon the structural integrity of buildings and intrusive ground vibrations from urban train systems, subways, machinery such as piledrivers and roads often affect property values or land usage. These vibrations are not a nuisance, but small magnitude vibration due to machinery, or nearby railway lines, can cause significant damage to buildings, especially over time [2]. These long, low frequency, waves that are the hardest to develop protection measures against and it is an open problem to develop such devices
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