• Title/Summary/Keyword: 반공진 진동수

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Vibration Test Fixture Design by Antiresonance Frequency Analysis (반공진 진동수 해석에 의한 진동시험 치구설계)

  • 김준엽;윤을재;장성조;김도영
    • Proceedings of the Korean Society of Propulsion Engineers Conference
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    • 1997.11a
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    • pp.33-34
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    • 1997
  • 장비나 부품이 비행 또는 수송 등 실제상황에서 겪게되는 진동환경에 얼마만큼 견디는지 여부를 확인하고, 예상되는 동적 하중에 의한 성능저하나 오 동작이 일어나지 알는지 확인하기 위해 환경진동시험(environmental vibration test)이 수행된다. 이러한 환경진동시험의 경우에는 대형(대용량)의 진동시험기(shaker 또는 exciter)가 이용되며 진동시험기로부터 에너지를 시험물에 기계적으로 전달시켜줄 수 있는 진동 시험치구(이하, "치구(fixture)")가 필요하게 된다. 따라서 치구의 설계문제가 대두되며, 환경진동시험의 성공여부를 좌우하는데 대단히 중요한 역할을 하게 된다. 치구의 설계시 가장 중요한 점은 시험규격에 정해진 기준스펙트럼(specified reference spectrum)이 치구 위에 설치될 여러 시험물부착점들에 그대로 전달될 수 있는 강체치구(rigid fixture)를 설계하는 것이 가장 이상적이지만 치구의 공진 및 반공진 특성으로 인해 시험물부착점들 마다 스펙트럼이 달라지게 된다. 따라서 시험물은 과대시험(overtest) 또는/그리고 과소시험(undertest)를 겪게된다.최근의 진동시험제어 기법으로서는 다채널시스템을 이용한 여러 시험부착점들에서의 진동레벨의 평균을 제어하는 평균제어기법(average control technique)이 이용되므로서 시험주파수 범위에서 공진진동수(resonance frequency)들은 기준스펙트럼과 동일하게 제어가 가능하나 반공진 진동수(antiresonance frequency)들에서는 반공진 진동수들이 갖는 물리적 특성으로 인해 기준스펙트럼과 동일하게 제어가 이루어지지 않으므로시험규격에 정해진 정확한 진동시험이 수행되지 못하게된다.본 연구에서는 치구의 설계단계에서 치구 위의 여러 시험물 부착점들- 평균제어점(average control points)- 에서의 반공진 진동수들을 고려하여 그 감도를 게산하고, 치구의 구조변경을 수행하여 시험물 부착점들에서의 반공진 진동수를 일치시키므로서 종래의 진동시험제어시 나타나는 반공진진동수에서의 문제점을 제거할 수 있고, 그 결과 시험물 부착점들에서의 스펙트럼이 시험규격에 정해진 스펙트럼대로 진동시험이 수행될 수 있게 하는데 있다.

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Structural Dynamic Modification of Fixture using Antiresonance Frequency Analysis (반공진 진동수 해석에 의한 치구 설계 변경)

  • 김준엽;윤을재
    • Journal of the Korean Society of Propulsion Engineers
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    • v.1 no.2
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    • pp.48-57
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    • 1997
  • The method of antiresonance frequency analysis of multi-input system is proposed. The structural dynamic modification using antiresonance frequency analysis is also applied to reduce the undertest at specimen attachment points on the fixture in environmental vibration test, which is resulted from the inconsistency of antiresonance frequencies. Several computer simulations show that the proposed method can remove the undertest problem which is not removed in conventional vibration test control. And the effectiveness of the method is verified with the impact hammer excitation of aluminium fixture model.

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Structural Dynamic Modification of Fixture by Antiresonance Frequency Analysis in Environmental Vibration Test Control (환경진동시험 제어에서 반공진 진동수해석에 의한 치구의 구조변경설계)

  • 김준엽;정의봉
    • Journal of KSNVE
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    • v.5 no.4
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    • pp.555-563
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    • 1995
  • This paper proposes the method of antiresonance frequency analysis of multi-input multi-output system. The structural dynamic modification techniques by antiresonance frequency analysis are also applied to reduce the undertest at specimen attachment points on the fixture in environmental vibration test, which is resulted from the inconsistency of antiresonance frequencies at any specified points. Several computer simulations show that the proposed method can remove the undertest problem which is not removed in conventional vibration test control. And the effectiveness of the method is verified with the impact hammer excitation of aluminium fixture model.

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Vibration characteristics of an ultrasonic waveguide for cooling (냉각용 초음파 웨이브가이드의 진동 특성)

  • Kim, Hyunse;Lim, Euisu
    • The Journal of the Acoustical Society of Korea
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    • v.39 no.6
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    • pp.568-575
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    • 2020
  • Ultrasound has been widely used in various industrial fields. One of challenging application areas is cooling microelectronics. Ultrasonic cooling systems can work with air, argon (Ar) and nitrogen (N2) instead of conventional refrigerant such as freon gas, which can cause global warming. Furthermore, ultrasonic systems do not have moving parts, thus high durability can be obtained. So it is necessary to develop ultrasonic cooling systems due to environmental issues and durability points. In this paper, the design and fabrication processes are explained. When designing the system, a feasibility test was performed with a prototype cooler. Based on the result, finite element analysis with ANSYS software was performed. The predicted anti-resonance frequency for a piezoelectric actuator was 34.8 kHz, which was in good agreement with the experimental result of 34.6 kHz with 0.6% error. In addition, the predicted anti-resonance frequency for the ultrasonic waveguide was 39.4 kHz, which also agreed well with the experimental value of 39.8 kHz with 1.0% error. Based on these results, the developed ultrasonic waveguide might be applicable in microchip cooling.

The Design of Broadband Ultrasonic Transducers for Fish Species Identification - Dual Resonance Design of a Ultrasonic Transducer Using a Single Acoustic Matching Layer - (어종식별을 위한 광대역 초음파 변환기의 설계 II - 단일음향정합층을 이용한 이중공진형 변환기의 설계 -)

  • 이대재
    • Journal of the Korean Society of Fisheries and Ocean Technology
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    • v.34 no.1
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    • pp.74-84
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    • 1998
  • A doubly resonant ultrasonic transducer has been designed as an attempt to increase the bandwidth of underwater transducers. The dual resonance conditions were accomplished by attaching a single acoustic matching layer on the front face of a Tonpilz transducer consisted of an aluminum head, a piezoelectric ring, a brass tail and a prestress bolt. A modified Mason's model was used for the performance analysis and the design of transducers, and the constructed transducers were tested experimentally and numerically by changing the impedances and thicknesses of the head, tail and matching layers in the water tank. Two distinct resonance peaks in the transmitting voltage response(TVR) of a developed transducer were observed at 34.3 and 40.4 kHz, respectively, with the difference frequency of 6.1kHz and the center frequency of 37.2kHz. The values of TVR at these frequencies were 136.5 dB re $1\;\muPa/V$ at 34.3 kHz and 136.8 dB re $1\;\muPa/V$ at 40.4 kHz, respectively. Reasonable agreement between the experimental results and the numerical results was achieved. From this result, it is expected that the generation of the distinct resonances at any two desired frequencies can be achieved through the proper choice of the matching layer to provide the impedance transformation between the transducer and the medium.

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