• 제목/요약/키워드: longitudinal magnetic field

검색결과 80건 처리시간 0.028초

Nonlinear Magnetosonic Wave Propagation in the Magnetosphere

  • Kim, Kyung-Im;Kim, Sungsoo S.;Lee, Dong-Hun;Kim, Kihong
    • 한국우주과학회:학술대회논문집(한국우주과학회보)
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    • 한국우주과학회 2004년도 한국우주과학회보 제13권1호
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    • pp.84-84
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    • 2004
  • Using a one-dimensional MHD code of Total Variation Diminishing (TVD) scheme, we perform simulations of propagation of nonlinear magnetosonic waves. A magnetosonic wave is a longitudinal wave propagating perpendicularly to the magnetic field lines, and involves compression and rarefaction of the magnetic field lines and the plasma. We first confirm the theoretical solution of Lee and Kim (2000) for the evolution of nonlinear magnetosonic waves in the homogeneous space. (omitted)

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FeCoGe/페놀 복합체의 정적 자기변형 측정 (Static measurement of magnetostriction of FeCoGe/phenol composites)

  • 박경일;나석민;신광호;임상호;사공건
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2003년도 하계학술대회 논문집 Vol.4 No.1
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    • pp.577-580
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    • 2003
  • The magnetostriction of FeCoGe/phenol composites, which is one of the magnetostrictive materials, measured at the external magnetic field. The measurement was carried out using the electrical-resistance strain gage, the wheaten's Bridge for eliminating the unnecessary voltage, and the lock-in-amp for signal amplification and noise filtering. When the external magnetic field was applied in the longitudinal the samples, the maximum strain of 120ppm was taken with regard to the 10wt.% phenol composite. This results indicate that the FeCoGe/phenol composites can be useful as an actuator because it has larger stain than the other solid state actuators such as piezo electric materials.

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FeCoGe/페놀 복합체의 영률 측정 (Young's Modulus Measurement of FeCoGe/phenol Composites)

  • 박경일;김홍근;신광호;사공건
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2003년도 제5회 영호남 학술대회 논문집
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    • pp.107-109
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    • 2003
  • The magnetostriction of FeCoGe/phenol composites is measured under the external magnetic field. A few Measurement are carried out by using the electrical-resistance strain gage, the Wheaton Bridge for eliminating the unnecessary voltage, the lock-in-amplifier for the signal amplification and noise filtering. When the external magnetic field is applied to the longitudinal direction against those samples which is the 10wt.% phenol in composites, the theoretical maximum strain of 120ppm is obtained. According to the larger strain than that of others solid state actuators and piezoelectric actuators. FeCoGe/phenol composites could be useful as an actuator.

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FeCoGeW/페놀 복합체의 자왜 및 영률 측정 (Magnetostriction and Young's Modulus Measurement of FeCoGeW/phenol Composites)

  • 박경일;김흥근;신광호;사공건
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2003년도 추계학술대회 논문집 Vol.16
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    • pp.325-328
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    • 2003
  • The magnetostriction of FeCoGeW/phenol composites is measured under the external magnetic field. A few Measurement are carried out by using the electrical-resistance strain gage, the Wheaton Bridge for eliminating the unnecessary voltage, the lock-in-amplifier for the signal amplification and noise filtering. When the external magnetic field is applied to the longitudinal direction against those samples which is the 10wt.% phenol in composites, the theoretical maximum strain of 120ppm is obtained. According to the larger strain than that of others solid state actuators and piezoelectric actuators. FeCoGeW/phenol composites could be useful as an actuator.

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Production of Hyperpolarized 129Xe Using Spin Exchange Optical Pumping

  • Kavtanyuk, Vladimir Vladimirovich;Kim, Wooyoung;Ando, Yu;Chebotaryov, Sergey;Seon, Yonggeun;Tan, Joshua Artem
    • Journal of the Korean Physical Society
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    • 제73권10호
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    • pp.1458-1465
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    • 2018
  • We present a constructed setup for polarizing $^{129}Xe$ noble gas. Hyperpolarized $^{129}Xe$ has been obtained via spin exchange with an optically pumped rubidium vapor. Optical pumping is based on polarizing the valence electron of rubidium by the resonant absorption of a circularly polarized laser light. The magnetic field of 30 G was used for obtaining $^{129}Xe$ polarization. The apparatus for detecting polarization is a nuclear magnetic resonance spectrometer. The highest $^{129}Xe$ polarization of 54% has been obtained using 60 W circularly polarized laser light with wavelength of 794.7 nm. The measured longitudinal relaxation time of the hyperpolarized $^{129}Xe$ was 72.3 minutes.

자장 세기와 스캔 방향이 다른 자기공명영상에서 측정된 해마 체적의 재현성 연구 (A study on the reproducibility of hippocampal volumes measured using magnetic resonance images of different magnetic field strengths and slice orientations)

  • 최유용;이동희;이상웅;이건호;권구락
    • 스마트미디어저널
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    • 제5권1호
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    • pp.44-48
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    • 2016
  • 장기추적 뇌영상 연구에서 자기공명영상장치의 노후 또는 기술 발전에 따른 업그레이드로 인해 연구기간 내 동일한 촬영 조건을 유지하기 어렵다. 특히, 자장 세기가 1.5T에서 3T로 증가한 경우가 많아, 기존 1.5T 영상을 새로운 3T 영상과 통합해서 분석에 사용하는 것이 가능한지 확인할 필요가 있다. 본 논문에서는 자장 세기와 스캔 방향이 다른 자기공명영상에서 측정한 해마 체적의 재현성을 연구 분석하였다. 실험참가자 296명의 3차원 T1 영상을 1.5와 3T 자기공명영상장치 각각에서 스캔 방향을 달리하여 획득하고 뇌영상 연구에 널리 사용되는 Freesurfer를 이용하여 실험참가자의 해마 체적을 측정하였다. 해마 체적의 영상종류 간 차이를 확인하기 위해 대응표본t-검정을 수행한 결과, 자기공명영상장치의 자장 세기와 스캔 방향에 따라 해마체적이 유의하게 차이가 있음을 확인하였다. 이런 결과는 촬영조건에 따라 측정된 해마체적이 달라질 수 있음을 의미하므로, 촬영 조건이 다른 영상을 통합 분석할 수 있는 기법의 개발이 필요하다고 판단된다.

Damping and vibration analysis of viscoelastic curved microbeam reinforced with FG-CNTs resting on viscoelastic medium using strain gradient theory and DQM

  • Allahkarami, Farshid;Nikkhah-Bahrami, Mansour;Saryazdi, Maryam Ghassabzadeh
    • Steel and Composite Structures
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    • 제25권2호
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    • pp.141-155
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    • 2017
  • This paper presents an investigation into the magneto-thermo-mechanical vibration and damping of a viscoelastic functionally graded-carbon nanotubes (FG-CNTs)-reinforced curved microbeam based on Timoshenko beam and strain gradient theories. The structure is surrounded by a viscoelastic medium which is simulated with spring, damper and shear elements. The effective temperature-dependent material properties of the CNTs-reinforced composite beam are obtained using the extended rule of mixture. The structure is assumed to be subjected to a longitudinal magnetic field. The governing equations of motion are derived using Hamilton's principle and solved by employing differential quadrature method (DQM). The effect of various parameter like volume percent and distribution type of CNTs, temperature change, magnetic field, boundary conditions, material length scale parameter, central angle, viscoelastic medium and structural damping on the vibration and damping behaviors of the nanocomposite curved microbeam is examined. The results show that with increasing volume percent of CNTs and considering magnetic field, material length scale parameter and viscoelastic medium, the frequency of the system increases and critically damped situation occurs at higher values of damper constant. In addition, the structure with FGX distribution type of CNTs has the highest stiffness. It is also observed that increasing temperature, structural damping and central angle of curved microbeam decreases the frequency of the system.

산소결핍 페롭스카이트 La1/3Sr2/3FeO2.96의 외부 자기장 하에서의 Mössbauer분광학적 연구 ([Mössbauer] Spectroscopic Study of La1/3Sr2/3FeO2.96 under the External Magnetic Field)

  • 윤성현;정종용
    • 한국자기학회지
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    • 제15권2호
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    • pp.81-84
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    • 2005
  • 다결정성 $La_{1/3}Sr_{2/3}FeO_{2.96}$에서의 전하불균형(charge disproportionation, CD) 전이의 근원에 대해 x선 회절법과 외부장 $M\ddot{o}ssbauer$ 분광법을 이용하여 알아보았다. 전이온도 이상에서 외부 자기장에 의한 효과를 알아보기 위해 시료의 온도를 225K로 유지한 상태에서 6 T이하의 외부 자기장을 감마선의 진행방향에 대해 각각 수직과 수평으로 걸어주었다. 외부장이 없을 경우 평균원자가 $Fe^{3.6+}$에 기인하는 상자성 단일 흡수선이 나타났다. 자기장이 감마선의 방향과 평행할 경우, 면적비가 3:0:1:1:0:3인 자기적 Zeeman 스펙트럼이 중앙의 단일선(singlet)에 중첩되어 나타났다. 하지만 자기장이 감마선의 방향에 수직일 경우엔 중앙의 단일선은 사라지고 면적비 3:4:1:1:4:3인 6-선 스펙트럼만 나타나서 큰 이방성을 보였다. 외부장 하에서 단일 흡수선의 존재는 Fe 이온간의 전자의 재빠른 도약 현상으로 설명하였다. 외부장 하에서도 단일흡수선이 존재해, 자기장이 전자의 도약에 의한 전도메커니즘에 큰 영향을 주지 못하는 것으로 나타났다.

Observation of the Domain Structures in Soft Magnetic (Fe97A13)85N15/Al2O3 Multilayers

  • Stobiecki, T.;Zoladz, M.
    • Journal of Magnetics
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    • 제8권1호
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    • pp.13-17
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    • 2003
  • The longitudinal magnetooptical Kerr effect was used to analyse magnetic domains in soft magnetic ${(Fe_{97}A1_3)}_{85}N_{15}$/$Al_{2}O_{3}$ multilayers in order to get microscopic understanding of interlayer exchange coupling. The measuring system consists of a Kerr microscope, a CCIR camera (with an 8-bit framegrabber), 16 bit digital camera and computer system for real-time image processing and to control external magnetic field and cameras. The strength of ferromagnetic (EM) coupling as a function of the spacer thickness of $Al_2O_3$ was investigated. It was found that strong FM-coupling, strong uniaxial anisotropy and coherent rotation of the magnetization have been observed for the spacer thickness in the range of 0.2 nm $\leq$ t $\leq$ 1 m, however, weak FM-coupling, patch domains and $360^{\circ}$-walls occur for the spacer thickness of t = 2.5 nm. At a spacer thickness of t $\geq$ 5 nm transition takes place from weak FM-coupling to the decoupled state where complex interlayer interactions and different types of the domain walls were observed.

[ $^{11}B$ ] Nuclear Magnetic Resonance Study of Spin Structures in Terbium Tetraboride

  • Mean, B.J.;Kang, K.H.;Kim, J.H.;Hyun, I.N.;Lee, Moo-Hee;Cho, B.K.
    • 한국자기공명학회논문지
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    • 제10권2호
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    • pp.197-202
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    • 2006
  • [ $^{11}B$ ] nuclear magnetic resonance (NMR) measurements were performed on the single crystals of $TbB_4$ to investigate local electronic structure and 4f spin dynamics. $^{11}B$ NMR spectrum, Knight shift, spin-lattice and spin-spin relaxation rates were measured down to 4K at 8T. $^{11}B$ NMR shift and linewidth are huge and strongly temperature dependent due to the 4f moments. In addition, both are proportional to magnetic susceptibility, indicating that the hyperfine field at the boron site originates from the 4f spins of Tb. Below $T_N$, the single broad resonance peak of $^{11}B$ NMR splits into several peaks reflecting the local magnetic fields due to antiferromagnetic spin arrangements. The longitudinal and the transverse relaxation rates, $1/T_1\;and\;1/T_2$, independent of temperature above $T_N$, decreases tremendously confirming huge suppression of spin fluctuation below $T_N$.

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