• Title/Summary/Keyword: 음향 재질 음속

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Studying Acoustical Properties of Micro-Speaker as a Function of Diaphragm Material (진동판의 재질에 따른 마이크로스피커의 음향특성연구)

  • Oh Sei-Jin
    • The Journal of the Acoustical Society of Korea
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    • v.25 no.5
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    • pp.222-228
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    • 2006
  • The acoustical property of micro-speaker had been investigated as a function of the diaphragm material in this study. Young's modulus and the density of material is deeply related to the determination of sound velocity and stiffness. As a result, it was appeared that the resonance frequency of micro-speaker was PEI < PPS < PET < PEN. This experimental result was in an excellent agreement with the theoretical one. The increasing ratio of sound pressure level to the frequency between 20Hz and the resonance frequency ($f_s$) and the high resonance frequency ($f_h$) were not affected by the diaphragm material.

Acoustic Characteristics of Sand Sediment with Circular Cylindrical Pores in Water (수중 원통형 다공성 모래퇴적물의 음향특성)

  • 윤석왕;이용주;노희설
    • The Journal of the Acoustical Society of Korea
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    • v.21 no.2
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    • pp.110-119
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    • 2002
  • Acoustic characteristics of water sediment were experimentally studied in laboratory. Water saturated sand sediment less than the grain size of 0.5 mm diameter is uniformly distributed in an acryl box (100 mm×100mm×42mm) with material thickness 1 mm. Pores in the acryl box are modeled as the structure of cylindrical pore tubes (diameter 3 mm and length 42 mm) filled with water. Cylindrical pore tubes have porosities 0%, 5%, 11%, 18% and 26 % controlled by the tube numbers. Transmitted acoustic waves through sand sediment specimen are analyzed as the functions of porosity and frequency from 0.3 MHz to 4 MHz. Transmitted acoustic waves are mixed with the first-kind wave from whole specimen and the second-kind wane from cylindrical pore tubes. For the center frequency 1 MHz, the first kind wave is dominant but for the center frequency 2.25 MHz, the second kind wave is dominant. In the case of the first-kind wave, as the porosity increases, the transmission coefficient decreases and the sound speed decreases to the sound speed of water. As the frequency increases, the transmission coefficient decreases but the sound speed is almost constant. In the case of the second-kind wave, as the porosity increases, the transmission coefficient increases but the sound speed is almost constant. The transmission coefficient and the sound speed are almost constant as a function of frequency.

A study on temperature dependent acoustic receiving characteristics of underwater acoustic sensors (수중음향센서 수온 변화에 따른 음향 수신 특성 변화 연구)

  • Je, Yub;Cho, Yohan;Kim, Kyungseop;Kim, Yong-Woon;Park, Saeyong;Lee, Jeong-Min
    • The Journal of the Acoustical Society of Korea
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    • v.38 no.2
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    • pp.214-221
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    • 2019
  • In this paper, a temperature dependent acoustic receiving characteristics of underwater acoustic sensor is studied by theoretical and experimental investigations. Two different types (low mid frequency sensor and high frequency sensor) of underwater acoustic sensors are designed with different configuration of baffle and conditioning plate. The temperature dependent characteristics of the acoustic sensors are investigated within the temperature range from $-2^{\circ}C$ to $35^{\circ}C$. The material properties of the piezoelectric ceramics, molding and baffle, which are the primary materials of the acoustic sensors, are measured with temperature change. The temperature dependent RVS (Receiving Voltage Sensitivity) characteristics of the acoustic sensors are simulated by using the measured material properties. The RVS changes of the acoustic sensors are measured by changing temperature in the watertank where the acoustic sensors are installed. The measured and the simulated data show that the temperature dependent characteristics of the acoustic sensors are mainly dependent for the sound speed changes of the molding material.