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Table 2. Valuesofabsorptioncoecientforselectedfrequenciesofsoundandunder-
pressurelevels(POLandABS)
Frequency [ Hz ]
500 1000 2000 4000 6400
Material
Underpressure [ MPa ]
Poly(methyl
methacrylate)
0
0,4570,5740,5810,571 0,58
(POL)
0,01
0,031 0,030,0340,043 0,05
0,02
0,0290,0280,0260,0380,047
0,03
0,0290,0280,0260,0380,048
0,04
0,0290,0270,025 0,040,047
0,05
0,0290,0280,0230,0380,046
0,06
0,0290,0270,0220,0380,046
0,07
0,0290,0270,022 0,040,046
0,08
0,0290,0270,0210,0420,046
0,09
0,0290,0270,022 0,040,046
0
0,2670,4480,4290,5470,464
0,01
0,0310,0340,0470,0580,088
0,02
0,0250,0280,0250,0420,042
0,03
0,0250,0270,0250,0450,038
0,04
0,0240,0260,0250,0440,039
0,05
0,0260,0270,0240,0480,038
0,06
0,0250,0270,0230,0470,045
Acrylonitrile/
0,07
0,0250,0270,0230,0450,046
Butadiene/
0,08
0,0250,0260,0220,0430,037
Styrene (ABS)
0,09
0,0250,0280,0220,0470,037
4.2 Comparisonof Acoustic Characteristics of Different Materials
The characteristics of the different granular materials under research show a
similarresponseinthefrequencydomain.Infig.7thereareplotsofabsorption
coecient for four different types of granular media with no underpressure in
sample. Additionally, in table 3 there are numerical values. It is easy to ob-
servethattherearesomenoticeabledisagreementsintheshapeoftheiracoustic
absorption characteristicswhen inside the structure there is only atmospheric
pressure. From about 500 to 1000Hz there is a rapid increase in value of ab-
sorptioncoecientforalltestedstructures.Next,fromabout1500to2000Hzit
stabilizesatacertainlevelthatismaintaineduntillabout6000Hz.Abovethat
levelthereisanotherincreaseofabsorptioncoecient.FormaterialsPOL,PS,
andPPthe valueofthetested coecientina broadrangeoffrequenciesfixes
atabout 0,6. A slightly different performance is observedfor ABS (fig. 6). At
thisstageofresearchitisdiculttofindatrustworthyansweraboutthecause
ofsuchbehavior.Onepossibleexplanationfor thiscouldbesomevariancesin
thegrainmix(sizeor/andshape).
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