TY - JOUR
T1 - Insights into acoustic properties of seven selected triply periodic minimal surfaces-based structures
T2 - A numerical study
AU - Lu, Jin You
AU - Silva, Tarcisio
AU - Alzaabi, Fatima
AU - Abu Al-Rub, Rashid K.
AU - Lee, Dong Wook
N1 - Publisher Copyright:
© The Author(s) 2023.
PY - 2024/3
Y1 - 2024/3
N2 - Poly(methyl methacrylate)-based triply periodic minimal surfaces (TPMS) structures promise great potential in phononic applications, but the complicated TPMS structure induces a design challenge for controlling their properties. Numerical acoustic simulations of seven major PMMA-based TPMS lattice structures are presented for low-frequency sound attenuation applications while varying their relative density. Except for the local resonances in primitive and Neovius-based lattice structures, the acoustic properties of other TPMS structures show a common Bragg bandgap with a central frequency of around 435 Hz and a bandwidth of around 286 Hz, which results from multiple scattering of periodic unit cells. In contrast, the acoustic bandgaps of primitive and Neovius-based lattices have much smaller and larger complete bandgaps, respectively, which are mainly attributed to the local resonances in their geometric cavities with different sizes. Thus, by taking the mechanism of generated bandgaps in the TPMS-based lattice structures into consideration, we can design suitable bandgaps for acoustic applications in the specific frequency range.
AB - Poly(methyl methacrylate)-based triply periodic minimal surfaces (TPMS) structures promise great potential in phononic applications, but the complicated TPMS structure induces a design challenge for controlling their properties. Numerical acoustic simulations of seven major PMMA-based TPMS lattice structures are presented for low-frequency sound attenuation applications while varying their relative density. Except for the local resonances in primitive and Neovius-based lattice structures, the acoustic properties of other TPMS structures show a common Bragg bandgap with a central frequency of around 435 Hz and a bandwidth of around 286 Hz, which results from multiple scattering of periodic unit cells. In contrast, the acoustic bandgaps of primitive and Neovius-based lattices have much smaller and larger complete bandgaps, respectively, which are mainly attributed to the local resonances in their geometric cavities with different sizes. Thus, by taking the mechanism of generated bandgaps in the TPMS-based lattice structures into consideration, we can design suitable bandgaps for acoustic applications in the specific frequency range.
KW - acoustic metamaterials
KW - finite element modeling
KW - phononic bandgap
KW - sound isolation
KW - Triply periodic minimal surfaces
UR - http://www.scopus.com/inward/record.url?scp=85170850173&partnerID=8YFLogxK
U2 - 10.1177/14613484231190986
DO - 10.1177/14613484231190986
M3 - Article
AN - SCOPUS:85170850173
SN - 1461-3484
VL - 43
SP - 208
EP - 219
JO - Journal of Low Frequency Noise Vibration and Active Control
JF - Journal of Low Frequency Noise Vibration and Active Control
IS - 1
ER -