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Materials Science in Additive Manufacturing                             TPMS for perfect sound absorption



                                                               3.6. Sound absorption of graded TPMS structures

                                                               To enhance the sound absorption of the primitive structure,
                                                               a graded design method was applied to the primitive
                                                               acoustic metamaterials. The sound absorption coefficient
                                                               curves of GP-Ⅰ and GP-Ⅱ are displayed in Figure 16, and
                                                               the sound absorption characteristics are listed in Table 10.
                                                               As the thickness of GP-Ⅰ and GP-Ⅱ increases, the frequency
                                                               at the first peak f  shifts to a lower frequency. GP-30 mm-Ⅰ
                                                                            1
                                                               has the lowest resonance frequency (1660 Hz) compared
                                                               to the graded and uniform structures. Notably, the sound
                                                               absorption coefficients at the first peak of GP-Ⅰ are all
                                                               higher than those of GP-Ⅱ with the same thickness, and
                                                               the frequency at the first peak  f  of GP-Ⅰ are all lower
                                                                                          1
                                                               than that of GP-Ⅱ with the same thickness. The λ peak /T of
                                                               GP-24 mm-Ⅱ and GP-30 mm-Ⅱ is lower than 4, indicating
            Figure  14. Sound absorption curves of diamond and multicavity-  that the type Ⅱ primitive structure has poorer absorption
            diamond structures                                 capability than the theoretical periodic porous structures.
                                                               On the contrary, the λ peak /T of GP-18 mm-Ⅰ, GP-24 mm-Ⅰ,
                                                               and GP-30 mm-Ⅰ are higher than 6, suggesting the presence
            λ peak /T of the diamond structure also increases from 4.93   of a subwavelength absorption peak.
            to 5.82. The  α  of the diamond structure with different   There are two peaks in GP-18 mm-Ⅰ, GP-24 mm-Ⅰ, and
                        1
            thicknesses is the highest among the four kinds of uniform   GP-30 mm-Ⅰ. After a combination of four cavities with 12,
            TPMS structures, including gyroid, primitive, IWP, and   18, 24, and 30 mm thickness, five peaks are found in the
            diamond. It is demonstrated that the diamond structure   curves of multicavity-GP-Ⅰ; the resonance peaks include
            has the best sound absorption performance at high   1980, 2420, 3060, 3970, and 5940 Hz. The sound absorption
            frequency among these four TPMS structures.
                                                               coefficient at the second peak of multicavity-GP-Ⅰ is 0.998,
              There  are  five  peaks  on the  sound  absorption curve   reaching the perfect absorption. Six peaks are found in the
            of the multicavity-diamond structure at frequencies of   curves of multicavity-GP-Ⅱ; the resonance peaks include
            2070, 2530, 3320, 4660, and 5940 Hz. The first four peaks   1200, 2280, 2850, 3630, 5090, and 5940  Hz. Notably,
            of  the multicavity-diamond structure correspond to  the   the  α  of the first resonance peak of multicavity-GP-Ⅱ
                                                                   1
            resonance peaks of Diamond-12 mm, Diamond-18 mm,   is 0.618, and this absorption value is lower than that of
            Diamond-24 mm, and Diamond-30 mm; the fifth peak of   multicavity-GP-Ⅰ, but the frequency of multicavity-GP-Ⅱ is
            multicavity-diamond corresponds to the second resonance   lower than that of multicavity-GP-Ⅰ. The sound absorption
            peak of Diamond-30 mm. The appearance of five peaks is   coefficient at the third peak of multicavity-GP-Ⅱ is 0.988,
            related to the interaction between the sound absorption   which is close to perfect sound absorption. The λ peak /T of
            peaks of the porous structure of four cavities with different   multicavity-GP-Ⅱ is 9.65, which is the highest among all
            heights in the multicavity-diamond structure, with all five   the TPMS structures assessed in this study.
            resonance peaks above 0.83. Additionally, the second peak   The acoustic band structures of GP-Ⅰ and GP-Ⅱ with
            achieves perfect sound absorption (α = 1).
                                                               different thicknesses are displayed in  Figure  15. The
              The acoustic band structures of the diamond structure   upper limit frequencies of the bandgap of GP-18 mm-Ⅰ,
            with different thicknesses are displayed in Figure 17. The   GP-24 mm-Ⅰ, and GP-30 mm-Ⅰ are 4310, 3350, and 2890 Hz,
            acoustic bandwidth of the diamond structure decreases   respectively; the lower  limit  frequency  of  the  bandgap  of
            as the thickness increases from 18 to 30 mm. The upper   GP-18 mm-Ⅰ, GP-24 mm-Ⅰ, and GP-30 mm-Ⅰ are 3580, 2800,
            limit frequencies of the bandgap of Diamond-18  mm,   and 2350 Hz, respectively. The first bandgap of GP-18 mm-Ⅰ,
            Diamond-24 mm, and Diamond-30 mm are 3830, 2900,   GP-24 mm-Ⅰ, and GP-30 mm-Ⅰ are 730, 500, and 540 Hz,
            and 1860 Hz, respectively, and the lower limit frequency   respectively. A  second bandgap was identified in GP-24
            of bandgap of Diamond-18  mm, Diamond-24  mm,      mm-Ⅰ and GP-30 mm-Ⅰ at a higher frequency, suggesting
            and Diamond-30  mm are 2890, 2070, and 1500  Hz,   that the lower limit frequency of GP-Ⅰ shifts to the lower
            respectively. The resonance frequency of the first peaks   frequency as the thickness increases. The width of the
            of Diamond-18 mm and Diamond-24 mm are within the   bandgap of GP-18 mm-Ⅱ is 21.9% wider than that of GP-18
            above range.                                       mm-Ⅰ; the width of the bandgap of GP-24 mm-Ⅱ is 32%



            Volume 4 Issue 1 (2025)                         14                             doi: 10.36922/msam.5737
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