• 제목/요약/키워드: magnetic field interference

검색결과 99건 처리시간 0.022초

FBG센서를 이용한 콘크리트 충진 FRP 스트럿 보강 PSC 교량의 스트럿 거동 분석 (Behavior of Strut in Concrete-filled FRP PSC Bridge using FBG Sensors)

  • 정원석;강동훈;안주옥
    • 한국방재학회 논문집
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    • 제9권6호
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    • pp.11-15
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    • 2009
  • 최근 국내에서는 PSC(Prestressed Concrete) 박스 거더 교량의 교폭을 늘리고 자중을 줄이기 위한 목적으로 박스의 수를 줄이는 대신 콘크리트 충진 FRP(Concrete Filled FRP, CFFRP) 스트럿을 상판 캔틸레버 부분에 설치하는 공법이 시공되고 있다. 이러한 CFFRP 스트럿은 사례가 많지 않은 교량 구조물로서 설계 및 시공에서의 불확실성을 제거하기 위해 교량 시스템에서의 스트럿 거동을 실험적으로 분석할 필요가 있다. 따라서 본 연구에서는 대상교량에 대해 현장시험을 실시하여 CFFRP 스트럿의 국부 거동을 분석하고자 한다. 특히 전자기파 간섭에 대해 면역이 우수한 광센서인 FBG(fiber Bragg grating) 센서를 기반으로 시험을 실시하여 잡음이 없는 우수한 응답을 성공적으로 획득하였다. 현장시험에서는 재하트럭의 속도와 횡방향 위치를 매개변수로 시험을 실시하였다. 그 결과 CFFRP 스트럿은 하중재하 위치와 속도에 관계없이 압축상태에 존재하고 있으며, 통과 차량의 횡방향 위치가 CFFRP 스트럿의 거동에 민감한 요소임을 확인하였다.

Shape memory alloy (SMA)-based head and neck immobilizer for radiotherapy

  • Lee, Hyun-Taek;Kim, Sung-In;Park, Jong Min;Kim, Ho-Jin;Song, Dae-Seob;Kim, Hyung-Il;Wu, Hong-Gyun;Ahn, Sung-Hoon
    • Journal of Computational Design and Engineering
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    • 제2권3호
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    • pp.176-182
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    • 2015
  • Head-and-neck cancer is often treated with intensive irradiation focused on the tumor, while delivering the minimum amount of irradiation to normal cells. Since a course of radiotherapy can take 5-6 weeks or more, the repeatability of the patient posture and the fastening method during treatment are important determinants of the success of radiotherapy. Many devices have been developed to minimize positional discrepancies, but all of the commercial devices used in clinical practice are operated manually and require customized fixtures for each patient. This is inefficient and the performance of the fixture device depends on the operator's skill. Therefore, this study developed an automated head-and-neck immobilizer that can be used during radiotherapy and evaluated the positioning reproducibility in a phantom experiment. To eliminate interference caused by the magnetic field from computed tomography hardware, Ni-Ti shape-memory alloy wires were used as the actuating elements of the fixtures. The resulting positional discrepancy was less than 5 mm for all positions, which is acceptable for radiotherapy.

Spin Wave Interference in Magnetic Nanostructures

  • Yang, Hyun-Soo;Kwon, Jae-Hyun;Mukherjee, Sankha Subhra;Jamali, Mahdi;Hayashi, Masamitsu
    • 한국자기학회:학술대회 개요집
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    • 한국자기학회 2011년도 자성 및 자성재료 국제학술대회
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    • pp.7-8
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    • 2011
  • Although yttrium iron garnet (YIG) has provided a great vehicle for the study of spin waves in the past, associated difficulties in film deposition and device fabrication using YIG had limited the applicability of spin waves to practical devices. However, microfabrication techniques have made it possible to characterize both the resonant as well as the travelling characteristics of spin waves in permalloy (Py). A variety of methods have been used for measuring spin waves, including Brillouin light scattering (BLS), magneto-optic Kerr effect (MOKE), vector network analyzer ferromagnetic resonance (VNA-FMR), and pulse inductive microwave magnetometry (PIMM). PIMM is one of the most preferred methodologies of measuring travelling spin waves. In this method, an electrical impulse is applied at one of two coplanar waveguides patterned on top of oxide-insulated Py, producing a local disturbance in the magnetization of the Py. The resulting disturbance travels down the Py in the form of waves, and is inductively picked up by the other coplanar waveguide. We investigate the effect of the pulse width of excitation pulses on the generated spin wave packets using both experimental results and micromagnetic simulations. We show that spin wave packets generated from electrical pulses are a superposition of two separate spin wave packets, one generated from the rising edge and the other from the falling edge, which interfere either constructively or destructively with one another, depending upon the magnitude and direction of the field bias conditions. A method of spin wave amplitude modulation is also presented by the linear superposition of spin waves. We use interfering spin waves resulting from two closely spaced voltage impulses for the modulation of the magnitude of the resultant spin wave packets.

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심자도에서 신경회로망을 이용한 허혈성 심장질환 분류 (A Classification of lschemic Heart Disease using Neural Network in Magnetocardiogram)

  • 엄상희
    • 한국정보통신학회논문지
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    • 제20권11호
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    • pp.2137-2142
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    • 2016
  • 심장에서 발생된 전류는 전위 뿐만 아니라 자기장을 생성한다. 본 논문에서는 61 채널 양자 간섭 장치 (SQUID) 시스템을 사용하여 심자도 (MCG)의 신호를 취득하고, 이것으로부터 임상적으로 유의하다고 생각되는 다양한 특징 파라미터를 계산한다. 이를 입력으로 신경회로망 알고리즘을 적용하여 허혈성 심장질환의 분류를 수행하였다. 심자도 신호는 전처리 과정을 통해 파라미터의 추출을 용이하게 하였다. 연구에 사용된 데이터는 정상인 10명과 안정형 협심 증세를 보이는 허혈성 심장질환 환자 10명분의 신호이다. 이들 신호로부터 임상적으로 유의한 특징점, 특징 간격 파라미터 및 진폭비를 추출하였다. 심자도 특징 파라미터를 신경회로망 입력으로 사용하여 허혈성 심장질환의 분류가 가능함을 보였다.

반자성으로 커플링된 NiFe/Ru/NiFe 박막에서의 자기이방성의 변화 (Magnetic Anisotropy Behavior in Antiparallely Coupled NiFe/Ru/NiFe Films)

  • 송오성;정영순;이기영
    • 한국자기학회지
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    • 제13권3호
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    • pp.97-102
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    • 2003
  • 고집적 TMR소자의 프리층에 적용될 수 있는 인위적페리층(synthetic ferrimagnetic layer : SyFL)인 NiFe/Ru/NiFe박막을 만들고, 결정에너지, 지만에너지, 교환에너지를 고려한 총에너지로부터 평형상태에서의 관계식에서 Ru두께에 따른 보자력( $H_{c}$)변화와, 스핀플로핑자계( $H_{sf}$ ), 포화자계( $H_{s}$)에 대해 알아보았다. Ta(50$\AA$)/NiFe(50$\AA$)Ru(4~20$\AA$)/NiFe(30$\AA$)/Ta(50$\AA$) 구조를 ICP (inductively coupled plasma)형 헬리콘스퍼터로 제작하고, 주어진 Ru두께에서의 시편을 SQUID로 $\pm$15kOe까지 분석하여 M-H루프를 측정하였다. 에너지를 고려한 평형상태 예측은 실험과 잘 일치하였으며, 이방성에너지 $K_{u}$= 1000erg/㎤, 교환에너지 $J_{ex}$= 0.7erg/$\textrm{cm}^2$까지 조절이 가능하였다. 상온에서 $H_{c}$를 10 Oe이하로 만드는 것이 가능하였고, 공업적으로 의미있는 $H_{s}$, $H_{sf}$ 의 범위를 Ru두께 4~10 $\AA$에서 선택이 가능하였다. 또한 50 $\AA$이하의 얇은 NiFe박막에서 자기탄성계수는 0이 아닌 (+)로 작용할 수 있다는 점과 NiFe/Ru 계면 조도를 간접적으로 예상하는 것이 가능하였다.

Chromite 물질의 자기상호작용에 관한 뫼스바우어 분광연구 (Mössbauer Studies of Changed Interaction on Cr Ions in Chromite)

  • 최강룡;김철성
    • 한국자기학회지
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    • 제17권1호
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    • pp.47-50
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    • 2007
  • 최근 geometrical frustration 현상 및 멀티페로익 효과가 Cr 이온의 나선 스핀 구조에 기인하는 것으로 해석되고 있다. 이에 본 연구에서는 Cr 이온 자리에 Fe을 치환하여 $CoCrFeO_4$를 제조하였고, $M\"{o}ssbauer$ 분광법에 의해 자기적 미세 구조의 상관관계를 연구하였다. 졸겔법을 이용하여 Fd3m의 cubic 스피넬 구조를 갖는 $CoCr_2O_4,\;CoCrFeO_4$ 단일상을 합성하였고, Rietveld 법에 의한 분석결과 격자상수는 $a_0=8.340$에서 $8.377{\AA}$로 증가 하였으며, Cr, Fe 이온은 모두 팔면체 구조에 위치하는 것으로 분석되었다. 자기 상전이 온도는 $T_N=97K$에서 320 K로 증가하였으며, 상호작용의 변화에 따라서 field cooled 온도에 따른 자화 곡선의 변화를 관측하였다. $M\"{o}ssbauer$ 스펙트럼 분석결과 4.2 K에서 공명흡수선에 대한 초미세자기장($H_{hf}$) 값은 각각 507, 492 kOe 정도로 나타났으며, 이성질체 이동치($\delta$)는 0.33, 0.34 mm/s 정도로 Fe 이온상태가 둘 다 +3 가의 이온상태임을 알 수 있었다.

심자도용 접선성분자장 측정방식 스퀴드 센서열 설계 (Design of a SQUID Sensor Array Measuring the Tangential Field Components in Magnetocardiogram)

  • 김기웅;이용호;권혁찬;김진목;김인선;박용기;이규원
    • Progress in Superconductivity
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    • 제6권1호
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    • pp.56-63
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    • 2004
  • We consider design factors for a SQUID sensor array to construct a 52-channel magnetocardiogram (MCG) system that can be used to measure tangential components of the cardiac magnetic fields. Nowadays, full-size multichannel MCG systems, which cover the whole signal area of a heart, are developed to improve the clinical analysis with high accuracy and to provide patients with comfort in the course of measurement. To design the full-size MCG system, we have to make a compromise between cost and performance. The cost is involved with the number of sensors, the number of the electronics, the size of a cooling dewar, the consumption of refrigerants for maintenance, and etc. The performance is the capability of covering the whole heart volume at once and of localizing current sources with a small error. In this study, we design the cost-effective arrangement of sensors for MCG by considering an adequate sensor interval and the confidence region of a tolerable localization error, which covers the heart. In order to fit the detector array on the cylindrical dewar economically, we removed the detectors that were located at the corners of the array square. Through simulations using the confidence region method, we verified that our design of the detector array was good enough to obtain whole information from the heart at a time. A result of the simulation also suggested that tangential-component MCG measurement could localize deeper current dipoles than normal-component MCG measurement with the same confidence volume; therefore, we conclude that measurement of the tangential component is more suitable to an MCG system than measurement of the normal component.

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스퀴드 심자도 장치를 이용한 심방성 부정맥의 측정 (Detection of Rapid Atrial Arrhythmias in SQUID Magnetocardiography)

  • 김기웅;권혁찬;김기담;이용호;김진목;김인선;임현균;박용기;김두상;임승평
    • Progress in Superconductivity
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    • 제7권1호
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    • pp.28-35
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    • 2005
  • We propose a method to measure atrial arrhythmias (AA) such as atrial fibrillation (Afb) and atrial flutter (Afl) with a SQUID magnetocardiograph (MCG) system. To detect AA is one of challenging topics in MCG. As the AA generally have irregular rhythm and atrio-ventricular conduction, the MCG signal cannot be improved by QRS averaging; therefore a SQUID MCG system having a high SNR is required to measure informative atrial excitation with a single scan. In the case of Afb, diminished f waves are much smaller than normal P waves because the sources are usually located on the posterior wall of the heart. In this study, we utilize an MCG system measuring tangential field components, which is known to be more sensitive to a deeper current source. The average noise spectral density of the whole system in a magnetic shielded room was $10\;fT/{\surd}Hz(a)\;1\;Hz\;and\;5\;fT/{\surd}Hz\;(a)\;100\;Hz$. We measured the MCG signals of patients with chronic Afb and Afl. Before the AA measurement, the comparison between the measurements in supine and prone positions for P waves has been conducted and the experiment gave a result that the supine position is more suitable to measure the atrial excitation. Therefore, the AA was measured in subject's supine position. Clinical potential of AA measurement in MCG is to find an aspect of a reentry circuit and to localize the abnormal stimulation noninvasively. To give useful information about the abnormal excitation, we have developed a method, separative synthetic aperture magnetometry (sSAM). The basic idea of sSAM is to visualize current source distribution corresponding to the atrial excitation, which are separated from the ventricular excitation and the Gaussian sensor noises. By using sSAM, we localized the source of an Afl successfully.

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Formation and Characteristics of the Fluorocarbonated SiOF Film by $O_2$/FTES-Helicon Plasma CVD Method

  • Kyoung-Suk Oh;Min-Sung Kang;Chi-Kyu Choi;Seok-Min Yun
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 1998년도 제14회 학술발표회 논문개요집
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    • pp.77-77
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    • 1998
  • Present silicon dioxide (SiOz) 떠m as intennetal dielectridIMD) layers will result in high parasitic c capacitance and crosstalk interference in 비gh density devices. Low dielectric materials such as f f1uorina뼈 silicon oxide(SiOF) and f1uoropolymer IMD layers have been tried to s이ve this problem. I In the SiOF ftlm, as fluorine concentration increases the dielectric constant of t뼈 film decreases but i it becomes unstable and wa않r absorptivity increases. The dielectric constant above 3.0 is obtain어 i in these ftlms. Fluoropolymers such as polyte$\sigma$따luoroethylene(PTFE) are known as low dielectric c constant (>2.0) materials. However, their $\alpha$)Or thermal stability and low adhesive fa$\pi$e have h hindered 야1리ru뚱 as IMD ma따"ials. 1 The concept of a plasma processing a찌Jaratus with 비gh density plasma at low pressure has r received much attention for deposition because films made in these plasma reactors have many a advantages such as go여 film quality and gap filling profile. High ion flux with low ion energy in m the high density plasma make the low contamination and go어 $\sigma$'Oss피lked ftlm. Especially the h helicon plasma reactor have attractive features for ftlm deposition 야~au똥 of i앙 high density plasma p production compared with other conventional type plasma soun:es. I In this pa야Jr, we present the results on the low dielectric constant fluorocarbonated-SiOF film d밑JOsited on p-Si(loo) 5 inch silicon substrates with 00% of 0dFTES gas mixture and 20% of Ar g gas in a helicon plasma reactor. High density 띠asma is generated in the conventional helicon p plasma soun:e with Nagoya type ill antenna, 5-15 MHz and 1 kW RF power, 700 Gauss of m magnetic field, and 1.5 mTorr of pressure. The electron density and temperature of the 0dFTES d discharge are measUI벼 by Langmuir probe. The relative density of radicals are measured by optic허 e emission spe따'Oscopy(OES). Chemical bonding structure 3I피 atomic concentration 따'C characterized u using fourier transform infrared(FTIR) s야3띠"Oscopy and X -ray photonelectron spl:’따'Oscopy (XPS). D Dielectric constant is measured using a metal insulator semiconductor (MIS;AVO.4 $\mu$ m thick f fIlmlp-SD s$\sigma$ucture. A chemical stoichiome$\sigma$y of 야Ie fluorocarbina$textsc{k}$영-SiOF film 따~si야영 at room temperature, which t the flow rate of Oz and FTES gas is Isccm and 6sccm, res야~tvely, is form려 야Ie SiouFo.36Co.14. A d dielec$\sigma$ic constant of this fIlm is 2.8, but the s$\alpha$'!Cimen at annealed 5OOt: is obtain려 3.24, and the s stepcoverage in the 0.4 $\mu$ m and 0.5 $\mu$ m pattern 킹'C above 92% and 91% without void, res야~tively. res야~tively.

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