• 제목/요약/키워드: Dispersive Wave

검색결과 132건 처리시간 0.029초

흐름의 영향을 받는 파랑 그룹의 비선형 집중 (Nonlinear Focusing Wave Group on Current)

  • 쥬리언 투보울;에핌 페리높스키;크리스티안 카리프
    • 한국해안해양공학회지
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    • 제19권3호
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    • pp.222-227
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    • 2007
  • 심해에서 생성된 최극해파가 파랑과 상호작용하는 현상에 대한 연구를 수행하였다. 이러한 파랑은 분산집중을 이용하여 산정하였다. 이러한 과정은 선형 및 비선형 방정식의 해를 구하여 얻을 수 있다. 상호작용에서 비선형성의 역할을 강조하였다.

연속웨이브렛 변환을 이용한 충격음 위치 규명 (CWT-Based Method for Identifying the Location of the Impact Source in Buried Pipes)

  • 김의열;김민수;이상권;고재필
    • 대한기계학회논문집A
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    • 제34권11호
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    • pp.1555-1565
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    • 2010
  • 본 연구에서는 지하에 매설된 가스 파이프에 가해진 충격의 위치를 탐지하기 위한 개선된 방법을 제시하고 있다. 가스 파이프에서 가스 누출은 건설 기계 장비에 의한 기계적 충격에 의해 발생하며, 가스 이송산업계에 치명적인 재해을 발생시킬 수 있다. 이와 같은 문제를 초기에 발견하고 조치를 취하기 위해 기존에는 충격 위치 탐지를 위해 상관 관계 기법이 사용되어 왔다. 하지만, 외부 충격에 의해 파이프 따라 전파되는 음향파의 분산 특성은 양쪽 센서에 측정되는 도착 시간을 사용하여 센서 사이에 도착 시간 지연을 예측하는데 상당한 에러를 발생 시킬 수 있다. 그래서 이 논문에서는 분산파 대신 직접파의 도착 시간 지연을 측정하기 위해 웨이블렛 기법을 사용하였다. 제안된 방법은 지하에 매설된 실제 가스 파이프에서 측정된 음향 신호에 적용하여 기존의 상관 관계 기법에 비해 외부 충격 위치를 추정하는데 보다 효과적임을 확인하였다.

DEVELOPMENT OF A NEW MODEL FOR NONLINEAR-DISPERSIVE WAVES OVER ARBITRARY DEPTHS

  • Nadaoka, Kazuo
    • 한국해안해양공학회:학술대회논문집
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    • 한국해안해양공학회 1998년도 정기학술강연회 발표논문 초록집 Annual Meeting of Korean Society of Coastal and Ocean Engineers
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    • pp.5-11
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    • 1998
  • Wave nonlinearity and dispersivity have mutually counteracting effects on the wave evolution process; i.e., the former makes the wave profile steeper, while the latter milder. Therefore to describe evolution of nonlinear water waves under general condition such as nonlinear random waves over arbitrary depths, both the wave nonlinearity and dispersivity must be properly taken into account in the wave modeling. (omitted)

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충격하중을 받는 보에서 압전 필름센서와 웨이브렛 변환을 이용한 문산파동의 해석 (Dispersive Wave Analysis of a Beam under Impact Load by Piezo-Electric Film Sensor and Wavelet Transform)

  • 권일범;최만용;정현조
    • 한국구조물진단유지관리공학회 논문집
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    • 제5권4호
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    • pp.215-225
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    • 2001
  • Stress waves monitored on the surface of structures under various loading conditions can provide useful information on the structural health status. In this paper, stress waves are measured by several sensors when a steel beam is impacted by a ball drop. The sensors used include the piezo-electric film Sensor, the electrical strain gage, and the ultrasonic transducer, and special attention is given to the pieza film sensor. The wavelet transform is used for the time-frequency analysis of dispersive waves propagating in the beam. The velocities of the wave produced in the team due to the lateral impact is found to be frequency-dependent and identified as the flexural wave velocity based on the comparisons with the Timoshenko beam theory. A linear impact site identification method is developed using the flexural wave, and the impact sites of the beam can be accurately estimated by the piezo film sensors. It is found that the piezo film sensor is appropriate for sensing stress waves due to impact and for locating impact sites in the beam.

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적층 Unidirectional CFRP 판의 이방성과 Lamb wave의 $S_0$ Mode 군속도의 관계 (The Relationship Between Group velocity of Lamb wave $S_0$ Mode and Anisotropy in Laminated Unidirectional CFRP Plates)

  • 이정기;김영환;이승석;김호철
    • 한국복합재료학회:학술대회논문집
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    • 한국복합재료학회 2004년도 추계학술발표대회 논문집
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    • pp.272-277
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    • 2004
  • The elastic waves in the plate are dispersive waves with the characteristics of Lamb waves. However, $S_0$ symmetric mode is less dispersive in the frequency region less than first cut-off frequency. And, in anisotropic plates such as CFRP plates, the propagation velocities vary with the direction. So, the wave vector direction to be the phase velocity direction is not accord with the energy flow direction to be the group velocity direction. In this work, the group velocities of the $S_0$ symmetric mode less than the first cut-off frequency was analyzed with the group velocity dispersion curves in unidirectional CFRP plate. And, the group velocity curve obtained by the group velocity dispersion curves are compared with the measured velocities as varied the propagation direction of the Lamb wave. The measured velocities are good agreement with the corrected group velocity curve except near the fiber direction which is called the cusp region. When the propagation direction is not accorded with the principal axis, the direction of the group velocities declines to the fiber direction in the unidirectional CFRP plates. This implies that the energy propagates preferentially toward fiber direction.

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분산성 램파의 전파에서 입력 파형의 복원을 위한 신호처리 (Signal Processing Techniques for Recovering Input Waveforms in Dispersive Lamb Wave Propagation)

  • 정현조;조성종
    • 한국소음진동공학회:학술대회논문집
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    • 한국소음진동공학회 2013년도 춘계학술대회 논문집
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    • pp.694-695
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    • 2013
  • An experimental study has been made with the use of time reversal concepts to recover the input waveform in a long range propagation of dispersive Lamb waves. Three techniques have been tested: Regular TR, 1 bit TR and Inverse filter (IF). The IF approach was found to completely recover the original input signal. Moreover, the IF technique significantly increases the contrast, i.e., the ratio of the recovered signal and the sideband signal.

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Analysis on the Calculation of Plasma Medium with Parallel SO-FDTD Method

  • Duan, Xule;Yang, Hong Wei;Kong, Xiangkun;Liu, Han
    • ETRI Journal
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    • 제31권4호
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    • pp.387-392
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    • 2009
  • This paper introduces a novel parallel shift operator finite-difference time-domain (SO-FDTD) method for plasma in the dispersive media. We calculate the interaction between the electromagnetic wave of various frequencies and non-magnetized plasma by using the parallel SO-FDTD method. Then, we compare the results,which are calculated with serial and parallel SO-FDTD executions to obtain the speedup ratio and validate the parallel execution. We conclude that the parallel SO method has almost the same precision as the serial SO method, while the parallel approach expands the scope of memory and reduces the CPU time.

ARTICLES : MULTICHANNEL ANALYSIS OF SURFACE WAVES (MASW) - AN OVERVIEW

  • ChoonB.Park
    • 지구물리
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    • 제6권2호
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    • pp.99-105
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    • 2003
  • Rayleigh waves which has more than 70% of the total seismic energy is the principal component of ground roll. Frequency component of a surface wave has a different propagation velocity, that is, phase velocity, which results in a different wavelength called dispersion. Rayleigh wave is one of the most common ways to use the dispersive properties of surface waves. MASW is a seismic method to evaluate shear-wave velocity information of the ground.

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일방향 적층 복합재료 판에서 한 음원에서 발생된 램파의 군속도 (The Group Velocity of Lamb Wave Generated by the one Source in Unidirectional Laminated Composite Plates)

  • 이정기;이상호
    • 한국음향학회지
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    • 제25권3호
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    • pp.107-112
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    • 2006
  • 판재를 따라 전파하는 Lamb wave (램파)는 주파수에 따라 속도가 변하는 분산특성을 갖는다. 일반적으로 등방성 재료에서는 파수 벡터 방향과 에너지 흐름 방향은 같아, 파면이 원형을 유지하면서 전파하지만, 복합재료와 같이 이방성재료에서는 파수 벡터와 에너지 흐름 방향이 서로 다르다. 따라서 이방성 재료에서 하나의 속도에서 다른 속도로 전환하려면 방향을 교정해야 하고 이에 따라 크기도 달라지게 된다. 본 연구에서는 복합재료 판재에서 전파하는 램파 분산방정식을 이용하여 대칭, 비대칭 모드의 분산선도를 작성하였고, 각도에 따라구한 위상속도 분산선도에서 얻어진 위상속도 값으로 slowness surface를 구한 후, 이로부터 군속도의 크기와 방향을 교정하였고, 이를 실험적으로 측정한 속도값과 비교하여 서로 일치함을 확인하였다.

Nonlinear Displacement Discontinuity Model for Generalized Rayleigh Wave in Contact Interface

  • Kim, No-Hyu;Yang, Seung-Yong
    • 비파괴검사학회지
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    • 제27권6호
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    • pp.582-590
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    • 2007
  • Imperfectly jointed interface serves as mechanical waveguide for elastic waves and gives rise to two distinct kinds of guided wave propagating along the interface. Contact acoustic nonlinearity (CAN) is known to plays major role in the generation of these interface waves called generalized Rayleigh waves in non-welded interface. Closed crack is modeled as non-welded interface that has nonlinear discontinuity condition in displacement across its boundary. Mathematical analysis of boundary conditions and wave equation is conducted to investigate the dispersive characteristics of the interface waves. Existence of the generalized Rayleigh wave(interface wave) in nonlinear contact interface is verified in theory where the dispersion equation for the interface wave is formulated and analyzed. It reveals that the interface waves have two distinct modes and that the phase velocity of anti-symmetric wave mode is highly dependent on contact conditions represented by linear and nonlinear dimensionless specific stiffness.