• Title/Summary/Keyword: 분산파

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DISPERSION OF RAYLEIGH WAVES IN THE KOREAN PENINSULA (한반도의 레일리파 분산에 대한 연구)

  • Cho Kwang-hyun;Lee Kiehwa
    • 한국지구물리탐사학회:학술대회논문집
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    • 2005.05a
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    • pp.29-36
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    • 2005
  • The crustal structure of Korean Peninsula is investigated by analyzing phase velocity dispersion data of Rayleigh wave. Earthquakes recorded by three component seismographs during 1999 - 2004 in South Korea are used in this study. The fundamental mode signals of Rayleigh waves are obtained from vertical components of seismograms by multiple filter technique method and phase match filter method. Velocity dispersion curves of surface waves for 14 propagation paths on the great circle are computed from the fundamental mode signals on the great circle path by two-station method. Treating the shear velocity of each layer as an independent parameter, phase velocities of Rayleigh wave are inverted. The result models are regarded as average structure for surface wave propagation paths respectively. All the results can be explained by an earth model of the Korean Peninsula comprising crust of shear-wave velocity increasing from 2.8 to 3.25 km/sec from top to 33 km depth and uppermost mantle of shear-wave velocity between 4.55 and 4.67 km/sec.

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Inversion of spectral analysis of surface waves with analytic Jacobian (해석적 자코비안을 이용한 표면파 기법의 역산)

  • Ha, Hee-Sang
    • Journal of the Korean Geophysical Society
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    • v.5 no.3
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    • pp.233-245
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    • 2002
  • The spectral-analysis-of-surface-waves (SASW) method is a nondestructive testing method based upon generation and detection of elastic stress waves. SASW is widely used as one of the techniques to determine stiffness profile in engineering geophysics. The essential steps involved are construction of an experimental dispersion curve from data collected in situ, and inversion of the dispersion curve to determine the stiffness profile. The main object of this study is to derive an analytical Jacobian for the inversion. If we set the subsurface to N homogeneous layer, it could save 2N times Jacobian calculation compared to numerical jacobian calculation during inversion. To reconstruct a stiffness profile, constrained damped least square method was applied for the inversion. The algorithm was tested for the numerical data and for the real asphalt and tunnel data, which were able to verify the stiffness profile. The stiffness profile reconstructed by the algorithm showed the possibility to appraise the soundness of tunnel with applications SASW.

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Numerical Studies for the Application of the SASW Method in an Inclined Soil Layer (경사지반에서 SASW기법 적용시 수치해석을 이용한 영향요소 연구)

  • 김동수;윤종구;이병식;박형춘
    • Journal of the Korean Geotechnical Society
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    • v.17 no.1
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    • pp.77-84
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    • 2001
  • SASW 기법은 실험에서 얻은 실험분산곡선이 현장 지반 강성의 주상을 합리적으로 반영하므로 실험결과로부터 전단파 속도 주상도를 신속하게 결정할 수 있는 장점을 가지고 있다. 그러나, 실험결과를 해석하는 과정에서 현재까지는 지반의 층상구조를 수평으로 가정하는 근본적인 한계점을 지니고 있었다. 이는 지반이 수평층상구조가 아닐 경우 해석적인 해를 구하기 힘들기 때문이다. 본 논문에서는 유한요소 수치해석을 통하여 경사진 지반에서 SASW 기법을 수행했을 경우 지반경사를 고려한 지반 조건이 실험분산곡선에 미치는 영향을 규명하였다. 이를 위하여 지반의 기울기와 표면파 전파 방향이 실험분산곡선에 미치는 영향과 파의 전파형상에 미치는 영향을 규명하기 위한 해석을 수행하였다. 해석결과 경사지반에서 지반 조건이 변함에 따라 실험 분산곡선에 많은 변화가 나타났고, 경사진 지반에서 파의 전파현상은 수평 층에서의 파의 전파형상과는 전혀 다른 특성으로 나타남을 알 수 있었다.

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Optimal Power Factor Control of Inverter-based DG for Reduction in Capacity of Active Harmonic Filter (고조파 능동 필터의 용량 감소를 위한 인버터 기반 분산전원의 역률 제어 기법 제안)

  • Kim, Young-Jin;Hwang, Pyeong-Ik;Moon, Seung-Il
    • Proceedings of the KIEE Conference
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    • 2009.07a
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    • pp.197_198
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    • 2009
  • 신재생 에너지원과 같은 인버터 기반 분산전원의 계통 연계가 활발히 이루어지고 있는 요즘, 인버터로 인한 고조파 발생이 중요한 전기 품질 문제로 대두되고 있다. 본 논문에서는 PSCAD/EMTDC를 이용하여, 분산전원의 인버터 모델을 구현하여 고조파를 측정하였고, 이를 감소시키기 위한 수동 및 능동 필터를 모델링하였다. 또한 분산전원의 연계 기술기준 중 역률 및 고조파 제한규정을 만족하면서 동시에 능동 필터와 분산전원의 인버터 용량을 최소화 할 수 있는 역률 제어 기법을 제안하였으며, 이를 시뮬레이션을 통해 확인하였다.

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A Numerical Study on the Effect of Near Surface Inhomogeneity on Rayleigh Wave Propagation and Dispersion (천부 불균질대에 의한 레일리파 전파 및 분산특성 고찰)

  • Lee, Sang-Min;Park, Kwon-Gyu;Byun, Joong-Moo
    • Geophysics and Geophysical Exploration
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    • v.9 no.2
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    • pp.148-154
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    • 2006
  • The effect of small-scale near surface inhomogeneity on Rayleigh wave propagation and dispersion has been investigated in this study using two-dimensional FEM elastic modeling. Various inhomogeneity models with a variety of geometrical shape and embedment depth which exist in homogeneous half-space and two-layered media are considered. Results show that any near surface inhomogeneity greater than one wavelength in terms of minimum wavelength of Rayleigh wave shows dispersion characteristics. Such dispersion effect become stronger as the dimensions of the inhomogeneity increase. The effect of horizontal dimension is more dominant factor governing the dispersion characteristics than vertical dimension. However, the dispersion effect can not be identifiable in seismogram if the horizontal dimension is not wide enough. Nonetheless, even in this case, the existence of inhomogeneity can be inferred by the reflection or transmission event of Rayleigh wave. The results can be expected to provide insights on the behavior of Rayleigh wave which may be helpful for designating field work or new processing scheme to detect near surface inhomogeneity by surface wave method.

Interpretation of Ground Wave Using Ray Method in Pekeris Waveguide (Pekeris 도파관에서 음선 접근법을 이용한 지면파 해석)

  • Choi, Jee-Woong
    • The Journal of the Acoustical Society of Korea
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    • v.28 no.3
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    • pp.208-212
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    • 2009
  • Ground wave is an acoustic wave propagating at a sediment sound speed in the case that sediment sound speed is constant with depth, which is explained by modal dispersion effects. In this paper, the ground wave in time domain is simulated using the ray-based approach, which is possible because the modal dispersion can be explained by the guiding of energy caused by reflection and refraction in the waveguide geometry. For a Pekeris waveguide, the ground wave can be interpreted as a sequence of head waves, called a head wave sequence [Choi and Dahl, J. Acoust. Soc. Am. 119, 3660-3668 (2006)]. The ground wave is simulated by convolution of the source signal with a channel impulse response of the head wave sequence, which is compared with simulated signals obtained via a Fourier synthesis of a complex parabolic equation (PE) field.

Thickness Measurement of Ni Thin Film Using Dispersion Characteristics of a Surface Acoustic Wave (표면파의 분산 특성을 이용한 Ni 박막의 두께 측정)

  • Park, Tae-Sung;Kwak, Dong-Ryul;Park, Ik-Keun;Kim, Miso;Lee, Seung-Seok
    • Journal of the Korean Society for Nondestructive Testing
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    • v.34 no.2
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    • pp.171-175
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    • 2014
  • In this study, we suggest a method to measure the thickness of thin films nondestructively using the dispersion characteristics of a surface acoustic wave propagating along the thin film surface. To measure the thickness of thin films, we deposited thin films with different thicknesses on a Si (100) wafer substrate by controlling the deposit time using the E-beam evaporation method. The thickness of the thin films was measured using a scanning electron microscope. Subsequently, the surface wave velocity of the thin films with different thicknesses was measured using the V(z) curve method of scanning acoustic microscopy. The correlation between the measured thickness and surface acoustic wave velocity was verified. The wave velocity of the film decreased as the film thickness increased. Therefore, thin film thickness can be determined by measuring the dispersion characteristics of the surface acoustic wave velocity.

Numerical Verification of HWAW Method in the Near Field (근거리장에서 HWAW 기법의 수치해석적 검증)

  • Bang, Eun-Seok;Park, Hyung-Choon;Kim, Dong-Soo
    • Journal of the Korean Geotechnical Society
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    • v.23 no.2
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    • pp.5-17
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    • 2007
  • Various field setup and filtering criteria have been suggested to avoid the near field effects in surface wave methods. Unlike other surface wave methods HWAW method uses the near field component positively. It is possible by using maximum energy point based on time-frequency map and inversion method to consider receiver locations from the source point and body wave component. To verify the HWAW method in the near field numerical study was performed and the wave propagation in the stratified soil media was simulated due to a surface point load. All of five representative soil models were used. The experimental dispersion curves, determined by HWAW method at the various receiver distances in the region of near field, all coincided well with the theoretical dispersion curves determined by 3D forward modeling (Kausel's method). Consequently, it was considered that the HWAW method can provide reliable $V_s$ profiles effectively in the near field.

Pochhammer 방정식의 분산곡선구성에서 본 비혼합해의 활용 방안

  • 김윤영
    • Journal of the KSME
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    • v.31 no.4
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    • pp.332-340
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    • 1991
  • 본 글에서는 속이 찬 실린더(solid cylinder)에서의 비대칭 탄성파전파 문제를 풀기 위한 해석적 방법의 일부를 소개하고자 한다. 속이찬 실린더에 있어서는 측면벽의 경계조건에 상관없이 평 판에서의 Fourier 시리즈와 유사한 단순해가 존재하지 않는다고 밝혀져 왔다(1). 그러나 최근 발표된 본인의 논문(2)에서 지적된 것처럼, 매우 특별한 측면 경계조건을 갖는 경우에만 정해가 존재한다. 특히 탄성파전파에 관한 한, 이러한 정해는 물리적으로 볼 때 팽창파(dilatational wave)와 전단파(shear wave)가 서로 얽히지 않는 상태에 해당되기 때문에, 소위 "비혼합 해(uncoupled solution)"라 불린다. 이 "비혼합해(uncoupled solution)"의 실제 사용 예를 들면, 상술된 바와 같이 일반적인 측면 경계조건을 갖는 속이 찬 실린더 문제를 풀기 위한 시도함 수(trial function)로 사용될 수 있을 것이다. 주지하는 바와 같이 자유측면벽(traction-free cylindrical wall)을 갖는 속이 찬 실린더는 공학적으로 매우 중요한 구조요소이다. 이 경우에는 측면벽의 경계조건으로 말미암아, 해가 정해의 형태로 존재하지 않는다. 특히 이 구조물에서의 탄성파전파 문제를 다루고자 할 때, 먼저 분산관계식(dispersion relation)을 구한 다음, 이를 이 용해 경계문제를 푸는 것이 상용적으로 사용되는 방법이다. 이 분산 관계식은 파장과 주파수 와의 관계를 나타내는 것으로, 그 복잡성으로 말미암아 이 식을 사용되는 수치해법으로 정확하게 구하는 것은 거의 불가능하다. 따라서, 본 글에서는 특별한 측면벽을 갖는 속이 찬 실린더의 비혼합해를 활용하여 자유측면벽을 갖는 속이 찬 실린더의 분산관계식(pochhammer의 분산관 계식이라 불린다)을 구하는 법을 설명하고자 한다. 이를 위해 비혼합해가 존재하는 측면경계조 건에 대해 먼저 살펴보고자 한다.조 건에 대해 먼저 살펴보고자 한다.

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Comparison of Shear-wave Velocity Sections from Inverting SH-wave Traveltimes of First Arrivals and Surface Wave Dispersion Curves (SH파 초동주시 역산과 표면파 분산곡선 역산으로부터 구한 횡파속도 단면 비교)

  • Lee, Chang-Min;Kim, Ki-Young
    • Journal of the Korean Geophysical Society
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    • v.8 no.2
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    • pp.67-74
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    • 2005
  • Two-dimensional S-wave velocity sections from SH-wave refraction tomography and surface wave dispersions were obtained by inverting traveltimes of first arrivals and surface wave dispersions, respectively. For the purpose of comparison, a P-wave velocity tomogram was also obtained from a P-wave refraction profiling. P and Rayleigh waves generated by vertical blows on a plate with a sledgehammer were received by 100- and 4.5-Hz geophones, respectively. SH-waves generated by horizontal blows on both sides of a 50 kg timber were received by 8 Hz horizontal geophones. The shear-wave signals were enhanced subtracting data of left-side blows from ones of the right-side blows. Shear-wave velocities from tomography inversion of first-arrival times were compared with ones from inverting dispersion curves of Rayleigh waves. Although the two velocity sections look similar to each other in general, the one from the surface waves tends to have lower velocities. First arrival picking of SH waves is troublesome since P and PS-converted waves arrive earlier than SH waves. Application of the surface wave method, on the other hand, is limited where lateral variation of subsurface tructures is not mild.

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