• 제목/요약/키워드: wave splitting

검색결과 76건 처리시간 0.024초

비정질 $Fe_{83}B_9Nb_7Cu_1$의 M$\ (Distributions of Hyperfine Parameters in Amorphous $Fe_{83}B_9Nb_7Cu_1$ Alloys)

  • 윤성현;김성백;김철성
    • 한국자기학회지
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    • 제9권6호
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    • pp.271-277
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    • 1999
  • M ssbauer 분광법을 이용하여 비정질합금 Fe83B9Nb7Cu1의 자기적 성질을 연구하였다. 개선된 Vincze의 방법을 적용하여 각 온도에서 초미세자기장, 이성질체 이동치, 그리고 quadrupole line broadening의 분포함수들을 얻었고 큐리온도는 393K, Hhf(0)는 231kOe로 산출되었다. 환산된 평균 초미세 자기장(reduced average hyperfine field)의 온도 변화는 S=1 자기화 곡선에 비해 급히 감소하는 양상을 보였고 이를 설명하기 위해 Handrich의 분자장 이론에서 교환 상호 작용의 척도인 에 =0.75-0.64(T/Tc)+0.47(T/Tc)2의 온도 의존성을 도입하였다. 평균 초미세 자기장(Hhf(T))은 저온에서 스핀파 여기에 의한 공식 Hhf(T)=Hhf(0)[1-0.44(T/Tc)3/2-0.28(T/Tc)5/2- ]으로 분석하였고, 큐리온도 부근에서는 1.00[1-T/Tc]0.39의 관계를 갖는 것으로 나타났다. 초미세 자기장 분포곡선의 선폭은 13K에서 102kOe (3.29 mm/s)였으며, 오도가 증가함에 따라 감소했다. 큐리온도 이상에서 평균 quadrupole splitting값은 0.43 mm/s였으며 quadrupole 이동치 분포에 의한 선폭 증가는 13K에서 0.1 mm/s, 320K에서는 0.072 mm/s 정도로 초미세 자기장 분포나 quadrupole line broadening에 의한 선폭 증가보다 작았다. 이성질체 이동치의 온도 변화에 Debye 모형을 적용하여 Debye 온도를 D=424K로 산출하였다.

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FDS-HCIB법을 이용한 고립파에 의한 물체 운동 모사 (Simulation of Body Motion Caused by a Solitary Wave using the FDS-HCIB Method)

  • 신상묵;김인철;김용직
    • 대한조선학회논문집
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    • 제51권4호
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    • pp.265-273
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    • 2014
  • Wave-body interaction is simulated using a developed code based on the flux-difference splitting scheme for immiscible and incompressible fluids and the hybrid Cartesian/immersed boundary method. A free surface is captured as a moving contact discontinuity within a fluid domain and an approximated Riemann solver is used to estimate the inviscid flux across the discontinuity. Immersed boundary nodes are identified inside an instantaneous fluid domain near a moving body, then dependent variables are reconstructed at those immersed boundary nodes based on interpolation along local normal lines to the boundary. Free surface flows around an oscillating cylinder are simulated and the computed wave elevations are compared with other reported results. The generation of a solitary wave by a moving wave-maker is simulated and the time histories of wave elevations at two different points are compared with other results. The developed code is applied to simulate body motion of an elastically mounted circular cylinder as a solitary wave passes the body. The force acting on an elastically mounted cylinder is compared with the force acting on a fixed cylinder. Grid independency of the computed body motion is established based on a comparison of results using three different-size grids.

Determination of Incident Angle and Position of Optimal Mode Ultrasonic Beam for Flaw Detection in Anisotropic and Inhomogeneous Weldments by Ray Tracing

  • Zhao, Xinyu;Song, Sung-Jin;Kim, Hak-Joon;Gang, Tie;Kang, Suk-Chull;Choi, Yong-Hwan;Kim, Kyung-Cho;Kang, Sung-Sik
    • 비파괴검사학회지
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    • 제27권3호
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    • pp.231-238
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    • 2007
  • Ultrasonic inspection of austenitic steel weldments is a truly difficult task due to complicated wave propagation phenomena such as beam skewing, splitting and distortion. In order to understand these phenomena and design proper inspection procedures, simulation is increasingly paid more attention to. This article addresses a ray tracing based approach to determine incident angle and position of optimal wave mode ultrasonic beam for flaw detection in anisotropic and inhomogeneous austenitic steel weldments. Specially, the optimal mode of ultrasonic wave wave is selected by ray tracing simulation, and an optimization approach based on ray tracing and bi-section search is proposed in order to find the ray path connecting two given points in weldments. With help of this approach, the optimal incident angle and position of ultrasonic beam can be determined for a given flaw position.

A Preconditioning Method for Two-Phase Flows with Cavitation

  • Shin B.R.;Yamamoto S.
    • 한국전산유체공학회:학술대회논문집
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    • 한국전산유체공학회 2003년도 The Fifth Asian Computational Fluid Dynamics Conference
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    • pp.181-182
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    • 2003
  • A preconditioned numerical method for gas-liquid to-phase flow is applied to solve cavitating flow. The present method employs a density based finite-difference method of dual time-stepping integration procedure and Roe's flux difference splitting approximation with MUSCL-TVD scheme. A homogeneous equilibrium cavitation model is used. The method permits simple treatment of the whole gas-liquid two-phase flow field including wave propagation, large density changes and incompressible flow characteristics at low Mach number. By this method, two-dimensional internal flows through a venturi tuve and decelerating cascades are computed and discussed.

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Real-time Modeling and Rendering of Tidal in Qiantang Estuary

  • Wang, Chang-Bo
    • International Journal of CAD/CAM
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    • 제9권1호
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    • pp.79-83
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    • 2010
  • Tidal bore is a peculiar nature phenomenon which is caused by the lunar and solar gravitation. Based on the physical characters of tidal bores, in this paper we propose a novel method to model and render this phenomenon, especially the tidal waves in Qiantang estuary. According to Boltzmann equation for tidal waves, we solve it with the novel triangle mesh of Kinectic Flux Vector Splitting (KFVS) mode. Then a method combining a curve forecasting wave and particles model is proposed to render the dynamic scenes of overturning tidal waves. Finally, with some rendering technologies, various realistic tidal waves under diversified conditions is rendered in real time.

잠수물체에 의하여 발생되는 비선형파의 수치 시뮬레이션 (Numerical Simulations of Nonlinear Waves Generated by Submerged Bodies)

  • 강국진
    • 한국전산유체공학회지
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    • 제2권1호
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    • pp.13-20
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    • 1997
  • A fundamental study for the numerical scheme to simulate unsteady nonlinear waves by solving Euler equations is presented. First a conservation form and a non-conservation form of the Euler equations with a free surface fitted coordinate system are compared. Next, a time splitting fractional step method and an alternating direction implicit(ADI) method for the time integration are compared. For the comparative study, flow calculations around a bottom bump in a channel and a NACA 0012 hydrofoil in a flume are performed. The results show that the ADI method with a third order upwind differencing scheme is very efficient in reducing the computing time with keeping the accuracy, And, there is no distinct difference between two expression forms except that the non-conservative form shows faster wave propagating velocity than the conservation form. Some results are compared with experiments and show good agreement.

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How Shock Wave Interacts with a Vortex ?

  • Chang Keun-Shik;Chang Se-Myong
    • 한국가시화정보학회:학술대회논문집
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    • 한국가시화정보학회 2004년도 춘계학술대회 논문집
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    • pp.1-7
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    • 2004
  • When a vortex diffracts upon encountering a vortex, many strong and weak waves are produced in the course of interaction. They are the cause of shock wave attenuation and noise production. This phenomenon is fundamental to understanding the more complex supersonic turbulent Jet noise. In this paper we have reviewed the research on shock-vortex interaction we have carried on last seven years. We have computationally investigated the parameter effect. When a shock is strong, shock diffraction pattern becomes complex since the slip lines from the triple points on Mach stem curl into the vortex, causing an entropy layer. When the vortex is unstable, vortexlets are brought about each of which make shock diffraction of a reduced intensity. Strong vortex produces quadrupole noise as it impinges into a vortex. Elementary interaction models such as shock splitting, shock reflection, and shock penetration are presented based on shock tube experiment. These models are also verified by computational approach. They easily explain production and propagation of the aforementioned quadrupole noise, Diverging acoustics are explained in terms of shock-vortexlet interactions for which a computational model Is constructed.

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포물형 근사식에 의한 천해파 산정모델 (Wave Transformation Model in the Parabolic Approximation)

  • 서승남
    • 한국해안해양공학회지
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    • 제2권3호
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    • pp.134-142
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    • 1990
  • 천해파랑의 변형을 추정하기 위한 광각 포물형 근사식이 제시되었다. 완경사 파랑식으로부터 분리행별법을 사용하여 유도된 포물형 근사식은 기존에 비해 일반화된 형태를 취하고 있다. 유한차분법에 의한 수치모델을 제시한 후 모델의 검증을 위해 원형천퇴 및 타원형천퇴의 수리모형 실험결과와 비교하였다. 수치결과는 거의 모든 점에서 실측치에 잘 부합되었고, 특히 회절현상이 뚜렷이 나타나는 천퇴 뒤편의 파랑특성을 잘 재현해 주었다.

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Michelson 간섭계에 의한 고체의 선팽창계수 측정방법 (Measurement Method of Linear Expansion Coefficient for Solid Matter using Michelson Interferometer)

  • 김홍균;김영선
    • 공학교육연구
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    • 제16권2호
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    • pp.24-30
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    • 2013
  • This paper deals with the measurement theory and technique of linear expansion coefficient for solid material using Michelson interferometer. The Michelson interferometer produces interference fringes by splitting a beam of monochromatic light so that one beam strikes a fixed mirror and the other a movable mirror. When the reflected beams are brought back together, an interference pattern results. Precise distance measurements until a quarter of wave length can be made with the Michelson interferometer by moving the mirror and counting the interference fringes which move by a photo diode. This paper represents the application of Michelson interferometer for measuring infinitesimal length system and shows the measurement method of linear expansion coefficients for various materials like copper, aluminum and iron. the results are good agreement with theoretical value within margin of error for each materials.

TEMPERATURE DEPENDENCE OF SPIN WAVE RESONANCE IN AMORPHOUS FILMS

  • Kim, Y.Y.;Baek, J.S.;Lee, S.J.;Lee, T.G.;Lim, W.Y.;Yu, S.C.;Lee, S.H.;Jang, P.W.
    • 한국자기학회지
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    • 제5권5호
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    • pp.524-527
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    • 1995
  • The temperature dependence of spin wave mode separation in amorphous $Co_{89.5}Zr_{10.5}$ thin film has been investigated at temperatures between 100 K and 300 K. The magnetization and the spectroscopic splitting factor were obtained for the main resonance mode in parallel and perpendicular magnetic field. ${\Delta}H_{2-3}$, the difference between resonance field of mode 2 and the resonance field of mode 3, increases with decreasing temperature. The linewidth increases for all the modes with decreasing temperature. Especially in mode 3 it increases rapidly below 200 K. This phenomenon could be caused by the increase of exchange stiffness constant or the decrease of surface magnetic anisotropy constant with decreasing temperature.

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