Articles

Flexural wave bandgap properties of phononic crystal beams with interval parameters

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  • 1. State Key Laboratory of Mechanics and Control of Mechanical Structures, Nanjing University of Aeronautics and Astronautics, Nanjing 210016, China;
    2. School of Naval Architecture & Ocean Engineering, Jiangsu University of Science and Technology, Zhenjiang 212100, Jiangsu Province, China;
    3. Department of Ophthalmology, University of Pittsburgh, Pittsburgh 15213, PA, U.S.A.

Received date: 2022-07-24

  Revised date: 2022-09-22

  Online published: 2023-02-04

Supported by

the National Natural Science Foundation of China (Nos. 12272172 and 11847009), the Natural Science Foundation of Jiangsu Higher Education Institutions of China (No. 22KJB580005), the Youth Talent Promotion Project from China Association for Science and Technology (No. 2022QNRC001), and the Priority Academic Program Development of Jiangsu Higher Education Institutions of China

Abstract

Uncertainties are unavoidable in practical engineering, and phononic crystals are no exception. In this paper, the uncertainties are treated as the interval parameters, and an interval phononic crystal beam model is established. A perturbation-based interval finite element method (P-IFEM) and an affine-based interval finite element method (A-IFEM) are proposed to study the dynamic response of this interval phononic crystal beam, based on which an interval vibration transmission analysis can be easily implemented and the safe bandgap can be defined. Finally, two numerical examples are investigated to demonstrate the effectiveness and accuracy of the P-IFEM and A-IFEM. Results show that the safe bandgap range may even decrease by 10% compared with the deterministic bandgap without considering the uncertainties.

Cite this article

Feiyang HE, Zhiyu SHI, Denghui QIAN, Y. K. LU, Yujia XIANG, Xuelei FENG . Flexural wave bandgap properties of phononic crystal beams with interval parameters[J]. Applied Mathematics and Mechanics, 2023 , 44(2) : 173 -188 . DOI: 10.1007/s10483-023-2947-8

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