Page 35 - MSAM-4-1
P. 35

Materials Science in Additive Manufacturing                             TPMS for perfect sound absorption



            30  mm (Figure  7). There are four main resonance   3.2. Sound absorption characteristics of gyroid and
            absorption peaks above 1500  Hz, namely 2670, 3310,   multicavity-gyroid structures
            4560,  and  6200  Hz.  The  ratio  of  the  first  absorption   The sound absorption coefficient curves of gyroid
            peak wavelength to structure thickness (λ peak /T) is 4.34.   structures with individual cavity and multicavity-gyroid
            This represents a subwavelength absorption peak, as   structures are displayed in  Figure  8. The first resonance
            the λpeak/T is >4, which exhibits a quarter wavelength   peak of the gyroid structure was identified. The analysis
            resonance frequency (QWRF) of 2891 Hz at 30 mm. The   of resonance peaks is listed in Table 6. As the thickness
            sound absorption coefficient of the first, second, third,   of the gyroid structure increases from 12 to 30 mm, the
            and fourth absorption peaks are 0.944, 0.944, 0.499, and   resonance peaks decrease from 5590 to 2000 Hz, indicating
            0.240, respectively. These four peaks correspond to the   that the resonance absorption peak of the gyroid structure
            acoustic resonance of four cavities with different depths.   shifts toward lower frequencies as the thickness increases.
            The resonance peak of the multicavity structure without   A  quarter-wavelength resonance has been found in
            porous structure filling is narrow, and the frequency   periodic porous structures with hard-backing,  and the
                                                                                                     8
            band of the first peak with sound absorption coefficients   QWRF is equal to c/4T, where c is the wave propagation
            exceeding 0.5 is only 210 Hz.                      speed in air and T is the thickness of porous structures.
                                                               The theoretical QWRF of periodic porous structures with
                                                               6, 12, 18, 24, and 30 mm is 14458, 7229, 4819, 3614, and
                                                               2891 Hz, respectively (i.e., f = c/4T; c = 347 m/s). The λ peak /T
                                                               of the gyroid structure is calculated and listed in Table 6.
                                                               The uniform gyroid structures present a subwavelength
                                                               absorption peak, as the λ peak /T is >4. The experimental first
                                                               absorption peak frequency of the Gyroid-24 mm structure
                                                               is 2590  Hz, which is 1024  Hz lower than the QWRF,
                                                               suggesting that the sheet-based gyroid structure has better
                                                               absorption capability than the theoretical periodic porous
                                                               structures.
                                                                 Five peaks are visible on the spectrum of the multicavity-
                                                               gyroid structure, the first four peaks (2160, 2670, 3600, and
                                                               4810 Hz) corresponding to the four individual absorption
                                                               peaks for each cavity with Gyroid-12 mm, Gyroid-18 mm,
            Figure 6. A two-microphone impedance tube          Gyroid-24 mm, and Gyroid-30 mm, respectively. The fifth

                         A                            B






















            Figure 7. Sound absorption coefficient curves of multicavity structures. (A) Multicavity model without TPMS. (B) Sound absorption curve of multicavity
            model
            Abbreviation: h: Height of cavity



            Volume 4 Issue 1 (2025)                         8                              doi: 10.36922/msam.5737
   30   31   32   33   34   35   36   37   38   39   40