• 제목/요약/키워드: Number of Excitations

검색결과 86건 처리시간 0.02초

음향여기에 의한 2차원 후방계단과 공동 내의 유동 및 열전달 특성 변화 (Flow and Heat Transfer Characteristics in a Separated Flow over Backward-facing Step and Cavity Controlled by Acoustic Excitation)

  • 조형희;강승구;이동호
    • 대한기계학회논문집B
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    • 제25권9호
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    • pp.1253-1262
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    • 2001
  • Experimental study is conducted to investigate the heat/mass transfer and flow characteristics for the flow over backward-facing step and cavities. A naphthalene sublimation method has been employed to measure the mass transfer coefficients on the duct wall and LDV system has been used to obtain mean velocity profiles and turbulence intensities. Reynolds number based on the step height and free stream velocity is 20,000 and St numbers of acoustic excitations given to separated flow are 0.2 to 0.4. The spectra of streamwise velocity fluctuation show a sharp peak forcing frequency for an acoustically excited flow. The results reveal that the vortex pairing and overall turbulence level are enhanced by the acoustic excitation and a significant decrease in the reattachment length and the increased turbulence intensity are observed with the excitation. A certain acoustic excitation increases considerably the heat/mass transfer coefficient at the reattachment point and in the recirculation region. For the cavities, heat/mass transfer is enhanced by the acoustic excitation due to the elevated turbulence intensity. For the 10H cavity, the flow pattern is significantly changed with the acoustic excitation. However, for the 5H cavity, the acoustic excitation has little effect on the flow pattern in the cavity.

비정질 $Fe_{78}Si_{9}B_{13}$ 합금의 구조와 자성 연구 (Structural Analysis and Magnctic Propcrics of Amorphous $Fe_{78}Si_{9}B_{13}$ Alloy)

  • 이희복;송인명;유성초;임우영
    • 한국자기학회지
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    • 제3권3호
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    • pp.179-184
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    • 1993
  • 비정질 합금 $Fe_{78}Si_{9}B_{13}$의 구조를 X-선 회절상을 분석하여 구하였다. 계산된 동경분포함수(RDF)의 첫번째 peak는 최인접 원자의 분포를 나타내는 것으로 Gaussian 함수형태를 나타낸다. 구조분석에서 본 시료의 최인접 원자배위수는 13.5이고, 최인접 원자간 평균거리 $r_{0}$$2.595{\AA}$, 인접원자들의 분포를 나타내는 Gaussian 함수의 변수 ${\delta}r$$0.27{\AA}$이다. 저온에서의 포화자화의 온도 의존성은 spin 파로 설명할 수 있으며, 이 때에 계산된 spin파 stiffness 상수는 $117.8\;meV\;{\AA}^2$ 이다. 또한, 포화자화의 온도 의존성을 Handrich의 분자장 이론식과 맞추어 얻은 변수는 각각 S=1/2 일때 ${\Delta}=0.32$이고, S=1 일때 ${\Delta}=0.23$으로 이론식과 실험결과가 전체적으로 잘 일치한다. 구조분석 결과와 분자장 이론식에서 구한 변수를 활용하여 spin파 stiffness 상수를 계산할 수 있으며, 이로써 구한 값은 S=1/2일때 $149\;meV\;{\AA}^2$ 이고, S=1 일 때 $138\;meV\;{\AA}^2$ 이다. 또한, 평균 교환결합상수 J($r_{0}$)는 S=1/2일때 17.9 meV이고, S=1일때는 J($r_{0}$)는 6.7 meV 으로 추정된다.

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Semi-active storey isolation system employing MRE isolator with parameter identification based on NSGA-II with DCD

  • Gu, Xiaoyu;Yu, Yang;Li, Jianchun;Li, Yancheng;Alamdari, Mehrisadat Makki
    • Earthquakes and Structures
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    • 제11권6호
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    • pp.1101-1121
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    • 2016
  • Base isolation, one of the popular seismic protection approaches proven to be effective in practical applications, has been widely applied worldwide during the past few decades. As the techniques mature, it has been recognised that, the biggest issue faced in base isolation technique is the challenge of great base displacement demand, which leads to the potential of overturning of the structure, instability and permanent damage of the isolators. Meanwhile, drain, ventilation and regular maintenance at the base isolation level are quite difficult and rather time- and fund- consuming, especially in the highly populated areas. To address these challenges, a number of efforts have been dedicated to propose new isolation systems, including segmental building, additional storey isolation (ASI) and mid-storey isolation system, etc. However, such techniques have their own flaws, among which whipping effect is the most obvious one. Moreover, due to their inherent passive nature, all these techniques, including traditional base isolation system, show incapability to cope with the unpredictable and diverse nature of earthquakes. The solution for the aforementioned challenge is to develop an innovative vibration isolation system to realise variable structural stiffness to maximise the adaptability and controllability of the system. Recently, advances on the development of an adaptive magneto-rheological elastomer (MRE) vibration isolator has enlightened the development of adaptive base isolation systems due to its ability to alter stiffness by changing applied electrical current. In this study, an innovative semi-active storey isolation system inserting such novel MRE isolators between each floor is proposed. The stiffness of each level in the proposed isolation system can thus be changed according to characteristics of the MRE isolators. Non-dominated sorting genetic algorithm type II (NSGA-II) with dynamic crowding distance (DCD) is utilised for the optimisation of the parameters at isolation level in the system. Extensive comparative simulation studies have been conducted using 5-storey benchmark model to evaluate the performance of the proposed isolation system under different earthquake excitations. Simulation results compare the seismic responses of bare building, building with passive controlled MRE base isolation system, building with passive-controlled MRE storey isolation system and building with optimised storey isolation system.

Analysis of Image Distortion on Magnetic Resonance Diffusion Weighted Imaging

  • Cho, Ah Rang;Lee, Hae Kag;Yoo, Heung Joon;Park, Cheol-Soo
    • Journal of Magnetics
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    • 제20권4호
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    • pp.381-386
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    • 2015
  • The purpose of this study is to improve diagnostic efficiency of clinical study by setting up guidelines for more precise examination with a comparative analysis of signal intensity and image distortion depending on the location of X axial of object when performing magnetic resonance diffusion weighted imaging (MR DWI) examination. We arranged the self-produced phantom with a 45 mm of interval from the core of 44 regent bottles that have a 16 mm of external diameter and 55 mm of height, and were placed in 4 rows and 11 columns in an acrylic box. We also filled up water and margarine to portrait the fat. We used 3T Skyra and 18 Channel Body array coil. We also obtained the coronal image with the direction of RL (right to left) by using scan slice thinkness 3 mm, slice gap: 0mm, field of view (FOV): $450{\times}450mm^2$, repetition time (TR): 5000 ms, echo time (TE): 73/118 ms, Matrix: $126{\times}126$, slice number: 15, scan time: 9 min 45sec, number of excitations (NEX): 3, phase encoding as a diffusion-weighted imaging parameter. In order to scan, we set b-value to $0s/mm^2$, $400s/mm^2$, and $1,400s/mm^2$, and obtained T2 fat saturation image. Then we did a comparative analysis on the differences between image distortion and signal intensity depending on the location of X axial based on iso-center of patient's table. We used "Image J" as a comparative analysis programme, and used SPSS v18.0 as a statistic programme. There was not much difference between image distortion and signal intensity on fat and water from T2 fat saturation image. But, the average value depends on the location of X axial was statistically significant (p < 0.05). From DWI image, when b-value was 0 and 400, there was no significant difference up to $2^{nd}$ columns right to left from the core of patient's table, however, there was a decline in signal intensity and image distortion from the $3^{rd}$ columns and they started to decrease rapidly at the $4^{th}$ columns. When b-value was 1,400, there was not much difference between the $1^{st}$ row right to left from the core of patient's table, however, image distortion started to appear from the $2^{nd}$ columns with no change in signal intensity, the signal was getting decreased from the $3^{rd}$ columns, and both signal intensity and image distortion started to get decreased rapidly. At this moment, the reagent bottles from outside out of 11 reagent bottles were not verified from the image, and only 9 reagent bottles were verified. However, it was not possible to verify anything from the $5^{th}$ columns. But, the average value depends on the location of X axial was statistically significant. On T2 FS image, there was a significant decline in image distortion and signal intensity over 180mm from the core of patient's table. On diffusion-weighted image, there was a significant decline in image distortion and signal intensity over 90 mm, and they became unverifiable over 180 mm. Therefore, we should make an image that has a diagnostic value from examinations that are hard to locate patient's position.

3T 능동차페형 전신 자기공명영상 장비로부터 얻어진 고해상도 자기공명영상 (High Resolution MR Images from 3T Active-Shield Whole-Body MRI System)

  • Bo-Young Choe;Sei-Kwon Kang;Myoung-Ja Chu;Hyun-Man Baik;Euy-Neyng Kim
    • Investigative Magnetic Resonance Imaging
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    • 제5권2호
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    • pp.138-148
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    • 2001
  • 목적 : 임상적용 가능시간 내에 세계 최초의 3T 능동차폐형 자석을 장착한 전신용 자기공명영상장비를 이용하여 고해상도의 자기공영영상을 획득하였다. 대상 및 방법: 128 MHz의 공명주파수를 갖는 RF코일을 사용하여 정상인으로부터 스핀에코와 고속 스핀에코 펄스 시퀀스를 적용한 두뇌, 무릎, 발 및 손목영상 등을 획득하였다. 전형적인 펄스시퀀스의 매개변수는 $512{\times}512$ matrix, 20 cm FOV, 3 mm 절편두께, 1 NEX를 사용하였다. 특히 T1 강조영상을 위하여 TR=500 ms, TE=10 혹은 17.4 ms을 사용하였으며, T2 강도영상을 위하여 TR=4000 ms, TE=108 ms을 사용하였다. 결과: 3T의 신호대잡음비는 기존 병원에 설치된 1.57에 비하여 2.7배 정도 향상되었다. 3T자기공명영상은 매우 미세한 혈관 구조물을 표출하는데 도움을 주며, 또한 백질과 회질의 상당한 대조도를 제공하여 주었다. 결론: 본 연구결과에서 37로부터 얻은 자기공명영상은 기존 1.57 영상에서 얻은 영상에 비하여 더 높은 해상도와 민감도를 제공하여 주었다 3T 고자장 자기공명영상에 나타난 증가된 신호대잡음비는 생체 조직단위의 영상을 획득하는데 유용하였다. 이러한 고해상도의 자기공명영상은 비침습적인 방법으로서 미세조직의 이상유무를 진단하는데 있어서 향후 더욱 임상에 도움을 주리라 예상한다.

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3T 능동차폐형 자기공명영상 장비로부터 얻어진 개의 자기공명영상 (Canine MR Images from 3T Active-Shield MRI System)

  • Choe, Bo-Young;Park, Chi-Bong;Kang, Sei-Kwon;Chu, Myoung-Ja;Kim, Euy-Neyng;Lee, Hyoung-Koo;Suh, Tae-Suk
    • 한국의학물리학회지:의학물리
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    • 제12권2호
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    • pp.113-124
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    • 2001
  • 목적: 수의 영상진단을 위하여 3T 능동차폐형 자석을 장착한 전신용 자기공명영상장비를 이용하여 고해상도의 개 두뇌, 척추, 복부 및 골반 자기공명영상을 획득하였다. 대상 및 방법: 128 MHz의 공명주파수를 갖는 RF코일을 사용하여 정상 개 및 환축으로부터 스핀에코와 고속 스핀에코 펄스시퀀스를 적용하였다. 전형적인 펄스시퀀스의 매개변수는 512$\times$512 matrix, 20 cm FOV, 3 mm 절편두께, 1 NEX를 사용하였다. 특히 T1 강조영상을 위하여 TR=500 ms, TE=10 혹은 17.4 ms을 사용하였으며, T2 강도영상을 위하여 TR=4000 ms, TE=108 ms을 사용하였다. 결과: 3T의 신호대잡음비는 기존 1.5T에 비하여 2.7배 정도 향상되었다. 본 연구에서 획득한 고해상도의 자기공명영상은 기존의 20cm FOV, 5m의 절편두께와 256$\times$256 해상도의 영상에 비하여 4배이상 증가하였다 3T 자기공명영상은 매우 미세한 혈관 구조물을 표출하는데 도움을 주며, 또한 백질과 회질의 상당한 대조도를 제공하여 주었다. 결론: 본 연구결과에서 3T로부터 얻은 자기공명영상은 기존 1.5T 영상에서 얻은 영상에 비하여 더 높은 해상도와 민감도를 제공하여 주었다. 3T 고자장 자기공명영상에 나타난 증가된 신호대잡음비는 생체 조직단위의 영상을 획득하는데 유용하였다. 이러한 고해상도의 자기공명영상은 비침습적인 방법으로서 미세조직의 이상유무를 진단하는데 있어서 향후 더욱 임상에 도움을 주리라 예상한다. 향후 자기공명영상은 수의 진단방사선분야에 새로운 장을 열어줄 수 있으리라 기대한다.

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