Abstract

Locally resonant phononic crystals (LRPCs) beam is characterized by the band gaps; some frequency ranges within which flexural waves cannot propagate freely. So, the LRPCs beam can be used for noise or vibration isolation. In this paper, a LRPCs beam with distributed oscillators is proposed, and the general formula of band gaps and transmission spectrum are derived by the transfer matrix method (TMM) and spectrum element method (SEM). Subsequently, the parameter effects on band gaps are investigated in detail. Finally, a rubber concrete beam is designed to demonstrate the application of distributed LRPCs beam in civil engineering. Results reveal that the distributed LRPCs beam has multifrequency band gaps and the number of the band gaps is equal to that of the oscillators. Compared with others, the distributed LRPCs beam can reduce the stress concentration when subjected to vibration. The oscillator interval has no effect on the band gaps, which makes it more convenient to design structures. Individual changes of oscillator mass or stiffness affect the band gap location and width. When the resonance frequency of oscillator is fixed, the starting frequency of the band gap remains constant, and increasing oscillator mass of high-frequency band gap widens the high-frequency band gap, while increasing oscillator mass of low-frequency gap widens both high-frequency and low-frequency band gaps. External loads, such as the common uniform spring force provided by foundation in civil engineering, are conducive to the band gap, and when the spring force increases, all the band gaps are widened. Taken together, a configuration of LRPCs rubber concrete beam is designed, and it shows good isolation on the vibration induced by the railway. By the presented design flow chart, the research can serve as a reference for vibration isolation of LRPCs beams in civil engineering.

Highlights

  • Resonant phononic crystals (LRPCs) beam is characterized by the band gaps; some frequency ranges within which flexural waves cannot propagate freely

  • The distributed Locally resonant phononic crystals (LRPCs) beam can reduce the stress concentration when subjected to vibration. e oscillator interval has no effect on the band gaps, which makes it more convenient to design structures

  • There are two kinds of interpretations for the band gap mechanism of PCs, including Bragg scattering mechanism [14] and locally resonant (LR) mechanism [15]. e Bragg scatting band gaps are caused by multiple scatterings of the periodic inclusions, and they usually exist in high-frequency ranges, whereas the LR band gaps are caused by the locally resonant vibration of the inclusions, and the frequency range is almost two orders of magnitude lower than that of the Bragg scattering ones with similar structural size. at is, with LR mechanism, low-frequency band gaps can be obtained with PCs in a smaller structural size, while the Bragg scattering mechanism needs a larger structural size [16]. erefore, the LRPCs are of excellent low-frequency vibration/acoustic isolation characteristics

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Summary

Theoretical Model and Mechanism

It indicates that there are two frequency attenuation band gaps (ranges in shadows), and the theoretical derivation is verified. Ough the locally resonant band gaps are of low frequencies, the local resonance of oscillators may cause vibration stress concentration at attachment point of the beam In this case, this paper chooses the parameters in reference [31] and calculates the vibration stress of the parallel LRPCs beam and distributed LRPCs beam, respectively. It indicates that the LRPCs beams with distributed multioscillators are of advantage in reducing vibration stress concentration in beam body

Effects of Interval between Distributed Oscillators on Band
Resonance frequency
10 Resonance frequency of oscillator 2
Vibration Attention of LRPCs Rubber Concrete Beam
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