Mobility of Plates with Identical Opposite Edges
1. INTRODUCTION
Acoustic absorber is used to absorb a certain frequency range of sound wave to reduce noise level and to improve the communication between the speaker and audiences. Traditionally, synthetic materials are used widely as acoustic absorber. These synthetic materials such as glass wool, stone wool and foam plastics not only cause pollution and global warming, but can also harmful to human life [1]. Thus, researchers have changed the focus towards natural materials as the alternative way to replace synthetic materials. Nor et al. [2] tested the effect of compression on the sound absorption properties of coir fiber. The compression work on coir fiber can enhance the sound absorption at low frequency. Putra et al. [3] employed the sugarcane wasted fibers as acoustic absorption material and the results show the increase of fiber density improves the sound absorption performance. Experimental work by Putra et al. [4] on paddy waste fibers also show good sound absorption coefficient and is comparable with synthetic glass wool at the same thickness. Traditionally, oil palm empty fruit bunch OPEFB fibers are used as burning fuel, fertilizers, mulching material and reinforcement materials in polymer composites [5]. This paper discusses the acoustic performance of OPEFB fibers which according to the author’s knowledge has not been investigated by other researchers.2. METHODOLOGY
The OPEFB fibers were weighted for 1, 2, 3, 4, 5, 6 and 7 grams and fitted into a 33 mm diameter aluminium mold for sample preparation. By using hot compression molding, the OPEFB fibers were compressed into samples with thickness of 10 mm and 20 mm as shown in Figure 1. Figure 1 OPEFB: a 5 gram of 20 mm thickness sample, b 5 gram of 10 mm thickness sample and c raw fiber The measurement of sound absorption coefficient was conducted using the impedance tube as shown in Figure 2 according to ISO 10534-2 [6]. The sample was fitted into the 33 mm diameter tube at one end while the other end was the location of a loudspeaker. White noise was generated from the computer through Audacity 1.3 Beta software and supplied into the tube through the loudspeaker. Two ½” pre-polarized free field microphones with ½” CCP pre-amplifier were located near the sample to record the built-up sound pressure. The two microphones were 22.5 mm apart. The loudspeaker was located 132.5 mm from the first microphone. The distance between the second microphone to the sample was 85 mm. The validity of the result was between frequency of 500 Hz to 4500 Hz due to the diameter of the tube. Range of the frequency was limited by the accuracy of the signal processing equipment and to avoid the occurrence of non-plane wave mode propagation [6]. Figure 2 Experimental setup for measurement of sound absorption coefficient Computer Noise generator, data acquisition system and display Loudspeaker Microphones Signal analyzer LDS Dactron Photon+ Removable cap Rigid Sample AmplifierParts
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» INTRODUCTION Proceeding Of Mechanical Engineering Research Day 2015 (MERD’15).
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