• 제목/요약/키워드: microwave absorption

검색결과 170건 처리시간 0.026초

전파흡수체의 전파흡수특성 측정기법에 관한 연구 (A Study on Measuring Technique of Electromagnetic Wave Absorbing Characteristics of Microwave Absorbers)

  • 김동일;안영섭;정세모
    • 한국전자파학회지:전자파기술
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    • 제4권1호
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    • pp.10-19
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    • 1993
  • 전파홉수체의 전파홉수능 측정방법은 기본적으로 다양한 마이크로파 측정법이 이용될 수 있지만, 레이다용전파홉수체의 경우, 전파의 주파수가높기 때문에 파장이 짧아서 측정오차가큰문제점이 있다. 따라서 본 연구에서는 전파홉수체의 전파홉수능을 실험적으로 간단히 측정할 수 있게 하기 위한 2 20rnrn¢동축관 생플흘더 및 Type-N connector로 부터 $20mm\phi$동축관으로의 변환Adaptor를 제작하여 전파홉수체의 설계 및 특성(전파홉수능) 평가에 사용할 수 있게 하였다. 또 구형도파관을 이용한 재료정수 측정법을 채용하여 시료의 형상동의 영향을 적게 받는 실측 방법에 관하여 검토하였다. 나아가서, 구형도파관을 이용한 재료정수 측정치를 반사감쇠량으로 환산한 전파홉수능파 동축관으로 측정한 전파흡수능의 주파수 특성을 구하여 거의 일치함을 밝히고 있다.

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평형스트립라인을 이용한 페라이트계 전파흡수체의 특성측정에 관한 연구 (A Study on the Measurement of Absorbption Characteristics for Ferrite Electromagnetic Wave Absorbers Using Parallel Stripline.)

  • 김동일
    • 한국항해학회지
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    • 제17권3호
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    • pp.77-83
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    • 1993
  • The goal of this research is to get a measuring system for absorption characteristics over the frequency band with 30MHz to 1, 000MHz concerning the ferrite electromagnetic wave absorbers, for example, grid-type and sintered flat type, etc. It is, however, very difficult to measure the absorption characteristics as in low frequency as in 30 MHz. In this research, therefore, we propose a standing wave method using parallel striplines, fabricate the measuring system, and measure the characteristic of ferrite microwave absorbers using the proposed mea-suring system.

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RF Characterizations of Patterned CoNbZr Magnetic Thin Film on Transmission Line

  • Kim, Ki-Hyeon
    • Journal of Magnetics
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    • 제11권3호
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    • pp.130-134
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    • 2006
  • The microwave power absorption for the patterned CoNbZr magnetic film has been investigated by coplanar waveguide method. The power absorption peaks of the patterned CoNbZr film (50 ${\mu}m$ ${\times}$ 2 mm ${\times}$ 2 ${\mu}m$), were observed at around 5.7 GHz. The observed resonance peak was in good agreement with calculated ferromagnetic resonance frequency including magnetic shape anisotropy effects. Compared with the coplanar waveguide without a magnetic film, the characteristic impedance of patterned film was shown to be increased. This resulted from the large increment of inductance up to 33 % without any significant changes of the capacitance.

Broadband metamaterial absorber using resistive layers

  • Kim, Y.J.;Yoo, Y.J.;Hwang, J.S.;Son, H.M.;Rhee, J.Y.;Kim, K.W.;Lee, Y. P.
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2016년도 제50회 동계 정기학술대회 초록집
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    • pp.359.1-359.1
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    • 2016
  • The electromagnetic (EM) properties of media, such as propagation, focusing and scattering, strongly rely on the electric permittivity and the magnetic permeability of media. Recently, artificially-created metamaterials (MMs) composed of periodically-arranged unit cells with tailored electric permittivity and magnetic permeability have drawn wide interest due to their capability of adjusting the EM response. MM absorbers using the conventional sandwich structures usually have very high absorption at a certain frequency, and the absorption properties of MMs can be adjusted simply by changing the geometrical parameters of unit cell. In this work, we suggested an incident-angle-independent broadband perfect absorber based on resistive layers. We analyze the absorption mechanism based on the impedance matching with the free space and the distribution of surface currents at specific frequencies. From the simulation, the absorption was expected to be higher than 96% in 1.4-6.0 GHz. The corresponding experimental absorption was found to be higher than 96% in 1.4-4.0 GHz, and the absorption turned out to be slightly lower than 96% in 4.0-6.0 GHz owing to the irregularity in the thickness of resistive layers.

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골중납 측정의 시료 전처리 (산분해법과 마이크로웨이브 분해법)와 측정 방법 (유도결합 플라즈마 질량분석법과 흑연로 원자 흡수 분광 광도법)의 비교 (Comparisons of sample preparation (acid digestion and microwave digestion) and measurement (inductively coupled plasma mass spectrometry and graphite furnace atomic absorption spectrometry) in the determination of bone lead)

  • 윤충식;최인자;박성균;김록호
    • 분석과학
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    • 제16권2호
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    • pp.152-158
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    • 2003
  • 본 연구는 인체의 골중 납 농도를 측정하는데 필요한 시료 전처리법과 기기 분석법을 평가하기 위하여 수행되었다. 절단한 인간 사체 다리의 뼈를 상온에서의 산 분해법과 마이크로웨이브 분해법 (microwave oven method)을이용하여 납을 추출하였으며, 유도결합 플라즈마 질량분석법 (ICP-MS)과 흑연로 원자 흡수 분광 광도법 (GF-AAS)으로 납 농도를 측정하였다. 표준시료를 이용하여 회수율을 조사한 결과, 산분해 후 ICP-MS로 측정한 경우 높은 회수율을 보였으나, 산분해 후 GF-AAS로 측정한 것은 표준 농도보다 낮은 값을 보였으며, 마이크로웨이브 분해한 경우는 두 측정기기 모두 표준 농도보다 높은 값을 보였다. 뼈 시료의 경우, 산분해 후 ICP-MS로 측정한 납 농도는 GF-AAS의 값과 높은 상관성을 보였으나 (상관계수 = 0.983), GF-AAS가 ICP-MS보다 계통적으로 높은 값을 측정하였다. 마이크로웨이브 분해 역시 두 분석방법이 높은 상관성을 보였으나 (상관계수 = 0.950), 대체로 산분해에 의한 값보다 높은 농도를 보였다. 결론적으로, 상온에서 질산으로 분해 후 ICP-MS를 이용하여 측정한 것이 골중 납 농도를 결정하는데 편이성과 정확성 면에서 가장 효율적인 방법으로 보인다.

방전에 의한 프라즈마에서의 마이크로파 전파특성 (The Properties of Microwave Propagation in Discharging Plasma)

  • 양인응;노방현;김봉열
    • 대한전자공학회논문지
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    • 제5권3호
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    • pp.31-39
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    • 1968
  • 외부자계가 가해진 냉프라즈마에서의 마이크로파 전파 특성을 측정하였다. 직류방전프라즈마는 두 전극판을 구형도파관에 삽입한것과, 또한 유리시설관을 구형도파관에 삽입한 것에서 이루어졌다. 마이크로파 전파방향, 방전관축, 외부자계는 각각 수직이고, 자속밀도, 방전유기, 기체압등이 증가할때 프라즈마를 전파하는 마이크로파의 감쇠 및 흡수는 증가함을 보았다.

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Study of Non-uniform Plasma Layer Variation with Optically-Controlled Microwave Pulses

  • Wang, Xue;Yun, Ji-Hun;Kim, Yong-K.
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2009년도 하계학술대회 논문집
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    • pp.90-91
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    • 2009
  • We study of the variation on non-uniform plasma in different layer of the semiconductor. The transient response in different plasma layer has been evaluated theoretically. The reflection function of dielectric microstrip lines resulting from the presence of plasma are evaluated by the transmission line model. The diffusion length is small compared to the absorption depth. The variation of characteristic response in plasma layer with microwave pulses which has in localized has been evaluated.

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Design of Thin RC Absorbers Using a Silver Nanowire Resistive Screen

  • Lee, Junho;Lee, Bomson
    • Journal of electromagnetic engineering and science
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    • 제16권2호
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    • pp.106-111
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    • 2016
  • A resistive and capacitive (RC) microwave absorber with a layer thickness less than a quarter of a wavelength is investigated based on closed-form design equations, which are derived from the equivalent circuit of the RC absorber. The RC absorber is shown to have a theoretical 90% absorption bandwidth of 93% when the electrical layer thickness is $57^{\circ}$ (about ${\lambda}_0/6$). The trade-offs between the layer thickness and the absorption bandwidth are also elucidated. The presented formulation is validated by a design example at 3 GHz. The RC absorber is realized using a silver nanowire resistive rectangular structure with surrounding gaps. The measured 90% absorption bandwidth with a layer thickness of ${\lambda}_0/8$ is 76% from 2.3 GHz to 5.1 GHz in accordance with the theory and EM simulations. The presented design methodology is scalable to other frequencies.

A Study of the Properties of Optically Induced Layers in Semiconductors Aided by the Reflection of Optically Controlled Microwave Pulses

  • Wang, Xue;Choi, Yue-Soon;Park, Jong-Goo;Kim, Yong-K.
    • Transactions on Electrical and Electronic Materials
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    • 제10권4호
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    • pp.111-115
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    • 2009
  • We present a study on the reflection of optically controlled microwave pulses from non uniform plasma layers in semiconductors. The transient response of the microwave pulses in different plasma layers has been evaluated by means of the reflection function of dielectric microstrip lines. The lines were used with an open-ended termination containing an optically induced plasma region, which was illuminated by a light source. The reflection characteristics impedance resulting from the presence of plasma is evaluated by means of the equivalent transmission line model. We have analyzed the variation of the transient response in a 0.01 cm layer with a surface frequency in the region of 128 GHz. In the reflection the variation of the diffusion length $L_D$ is large compared with the absorption depth $1/{\alpha}_l$. The variation of the characteristic response of the plasma layer with differentially localized pulses has been evaluated analytically. The change of the reflection amplitude has been observed at depths of 0.1 cm, 0.01 cm and $0.1{\times}10^{-5}$ cm respectively.