• 제목/요약/키워드: Microwave range method

검색결과 121건 처리시간 0.031초

X-밴드 주파수의 마이크로파를 이용한 자유공간에서의 모래수분측정 (Sand Moisture Measurement with Microwave Technique in Free Space at X-Band Frequency)

  • 남현수;성재용;박남석
    • 한국전자파학회논문지
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    • 제8권5호
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    • pp.525-533
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    • 1997
  • 건축연구에서의 수분측정 방법을 개선하기 위하여 비파괴적인 수분측정기술을 응용하였다. 본 실험은 연속적이고 비파괴적인 측정에서의 핵심요소로서 자유공간에서의 혼 안테나를 사용하여 실험하였으며 사용한 기술은 마이크로파 브릿지 장치로서 9.5GHz의 주파수에서 함수율이 1~12% 범위의 모래수분을 측정하였다. 이로부터 대표적인 교정곡선을 구하였다. 이를 바탕으로 마이크로파를 이용한 석탄, 제지, 식품 미치 건축재료 등과 같은 비금속내의 수분측정이 가능함을 보였다.

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Drone Detection with Chirp-Pulse Radar Based on Target Fluctuation Models

  • Kim, Byung-Kwan;Park, Junhyeong;Park, Seong-Jin;Kim, Tae-Wan;Jung, Dae-Hwan;Kim, Do-Hoon;Kim, Taihyung;Park, Seong-Ook
    • ETRI Journal
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    • 제40권2호
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    • pp.188-196
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    • 2018
  • This paper presents a pulse radar system to detect drones based on a target fluctuation model, specifically the Swerling target model. Because drones are small atypical objects and are mainly composed of non-conducting materials, their radar cross-section value is low and fluctuating. Therefore, determining the target fluctuation model and applying a proper integration method are important. The proposed system is herein experimentally verified and the results are discussed. A prototype design of the pulse radar system is based on radar equations. It adopts three different pulse modes and a coherent pulse integration to ensure a high signal-to-noise ratio. Outdoor measurements are performed with a prototype radar system to detect Doppler frequencies from both the drone frame and blades. The results indicate that the drone frame and blades are detected within an instrumental maximum range. Additionally, the results show that the drone's frame and blades are close to the Swerling 3 and 4 target models, respectively. By the analysis of the Swerling target models, proper integration methods for detecting drones are verified and can thus contribute to increasing in detectability.

Ba$^{0.7}Sr^{0.3}TiO^{3}$ 박막 커패시퍼의 마이코로파 측정 (Microwave measurement of Ba$^{0.7}Sr^{0.3}TiO^{3}$ thin film capacitors)

  • 장병택;차선용;이승훈;곽동화;이희철;유병곤;백종태;유형준
    • 전자공학회논문지A
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    • 제33A권2호
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    • pp.114-121
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    • 1996
  • Thin film Ba$^{0.7}Sr^{0.3}TiO^{3}$ (BST) capacitors were fabricated on SiO$_{2}$/Si substrates by RF magnetron sputtering method and characterized at microwave frequencies ranging from 40 MHz to 1GHz to examine the dielectric dispersion of the capacitors. The BST thin films were electrode material of BST thin films capacitor which is known as one of the best electrode materials for BST films. 50$\AA$-thick titanium (Ti) layers were introduced to increase adhesion between bottom Pt and SiO$_{2}$. The leakage current density of the capacitors was about 1.7${\times}10^{7}A/cm^{2}$ at 1.5V and the dielectric constant was about 140 at 1MHz. Microwave measurement patterns having a coplanar waveguide type were fabricated and their S parameters were measured using network analyzer. After de-embedding parasitic components in microwave measurement patterns nearly frequency-invariant dielectric constant of about 120 was extracted in the measurement range of 40 MHz to 1 GHz.

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석탄회로부터 제올라이트 A의 합성 (Synthesis of Zeolite A from Coal Fly Ash)

  • 지정대;최고열
    • 공업화학
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    • 제22권2호
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    • pp.214-218
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    • 2011
  • 마이크로파 가열 방법과 기존의 가열 방법을 이용하여 석탄회로부터 제올라이트 A를 합성하였다. 반응시간, sodium aluminate의 양, 반응 온도 등이 제올라이트 A의 결정화에 미치는 영향에 대해 연구하였다. $80{\sim}100^{\circ}C$의 범위에서 제올라이트 A의 합성에 필요한 반응 시간은 3~6 h이었으며, 6 h 이상이 되면 결정화도가 오히려 감소하였다. 제올라이트 A의 합성에 필요한 sodium aluminate의 양은 $90^{\circ}C$ 이상에서는 합성용액의 $SiO_2/Al_2O_3$의 비가 0.44~1.05에서 최적이었으며, $80^{\circ}C$에서는 더 많은 양이 필요하였다. 마이크로파 가열 방법은 기존의 가열 방법에 비해 초기 결정화 속도는 약간 증가하였으나, 충분히 결정화되는데 필요한 반응시간은 서로 비슷하였다. 따라서 마이크로파 가열에 의한 석탄회로부터 제올라이트 A의 합성에 미치는 영향은 크지 않다는 것을 알 수 있었다.

자유공간 기법을 적응한 마이크로파 대역 전파흡수재의 유전 특성 분석 (A Free-Space Method for Measurement and Analysis of Dielectric Characteristics of Electromagnetic Absorbing Materials at Microwave Frequencies)

  • 배근식
    • 한국군사과학기술학회지
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    • 제6권2호
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    • pp.73-82
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    • 2003
  • For measurements and analysis of dielectric characteristics of planar slabs of microwave absorbing materials, I have applied a free-space method in the frequency range of 8~14 GHz. The measurement system for free-space method consists of transmit and receive antennas, mode transitions, precision coaxal cables, the network analyzer, and a computer Special Spot-focused horn lens antenna was used to eliminate diffraction effects. Diffraction effects at the edges of the sample are minimized by satisfying the condition for minimum transverse dimension of the plate and the beamwidth of the antennas at the focus. The time-domain gating feature of the network analyzer and the thru, reflect, and line(TRL) calibration technique were used to eliminate the effects of undesirable multiple reflections. The complex coefficients of reflection and transmission, $S_{11}$ and $S_{21}$, of planar samples were measured for standard materials such as Teflon, Rexolite$\textregistered$ 2200. The results were compared with existing measurement method. And I applied a free-space method for measurement to measure dielectric constants of some electromagnetic absorbing materials. Dielectric properties for the same samples were also measured with a 7mm coxial transmission line method for purposes of comparison with the free-space method.

Investigation of Drying Kinetics and Color Characteristics of White Radish Strips under Microwave Drying

  • Lee, Dongyoung;So, Jung Duk;Jung, Hyun Mo;Mo, Changyeun;Lee, Seung Hyun
    • Journal of Biosystems Engineering
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    • 제43권3호
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    • pp.237-246
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    • 2018
  • Purpose: This study (a) investigated the effect of microwave power intensity and sample thickness on microwave drying characteristics of radish strips, and (b) determined the best-fit drying model for describing experimental drying data, effective moisture diffusivity ($D_{eff}$), and activation energy ($E_a$) for all drying conditions. Methods: A domestic microwave oven was modified for microwave drying and equipped with a small fan installed on the left upper side for removing water vapor during the drying process. Radishes were cut into two fixed-size strip shapes (6 and 9 mm in thickness). For drying experiments, the applied microwave power intensities ranged from 180 to 630 W at intervals of 90 W. Six drying models were evaluated to delineate the experimental drying curves of both radish strip samples. The effective moisture diffusivity ($D_{eff}$) was determined from Fick's diffusion method, and the Arrhenius equation was applied to calculate the activation energy ($E_a$). Results: The drying time was profoundly decreased as the microwave power intensity was increased regardless of the thickness of the radish strips; however, the drying rate of thicker strips was faster than that of the thinner strips up to a certain moisture content of the strip samples. The majority of the applied drying models were suitable to describe the drying characteristics of the radish strips for all drying conditions. Among the drying models, based on the model indices, the best model was the Page model. The range of estimated $D_{eff}$ for both strip samples was from $2.907{\times}10^{-9}$ to $1.215{\times}10^{-8}m^2/s$. $E_a$ for the 6- and 9-mm strips was 3.537 and 3.179 W/g, respectively. Conclusions: The microwave drying characteristics varied depending on the microwave power intensity and the thickness of the strips. In order to produce high-quality dried radish strips, the microwave power intensity should be lower than 180 W.

(1-X)Ba$Mg_{1/3}Ta_{2/3}O_{3}-xBa_Co_{1/3}Nb_{2/3})O_{3}(x=0.25~0.5)$세라믹스의 마이크로파 유전특성 (The Microwave Dielectric Properties of (1-x)Ba$Mg_{1/3}Ta_{2/3}O_{3}-xBa_Co_{1/3}Nb_{2/3})O_{3}(x=0.25~0.5)$ Ceramics)

  • 황태광;김강;임성수;이성갑;이영희
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2000년도 추계학술대회 논문집
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    • pp.221-224
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    • 2000
  • The microwave dielectric properties of Ba(Mg$_{1}$3/Ta$_{2}$3/)O$_3$-xBa(Co$_{1}$3/Nb$_{2}$3/)O$_3$[BMT-BCN] ceramics were investigated. The specimens were prepared by the conventional mixed oxide method. It was found that Ba(Mg$_{1}$3/Ta$_{2}$3/)O$_3$ and Ba(Co$_{1}$3/Nb$_{2}$3/)O$_3$ formed a solid solution with complex perovskite structure. Increasing the BCN content, dielectric constant was increased, but temperature coefficient of resonant frequency was decreased. In the range of x$\geq$0.4, dielectric constant was about 30. 0.55BMT-0.45BCN ceramics showed excellent microwave dielectric properties with $\varepsilon$$_{r}$=30.84, Q$\times$f$_{0}$=75,325[GHz] and $\tau$$_{f}$=-2.9015[ppm/$^{\circ}C$].X>].

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(1-x)Ba($Mg_{1/3}Ta_{2/3})O_3$-xBa($Co_{1/3}Nb_{2/3})O_3$(x=0.25~0.5) 세라믹스의 구조 및 마이크로파 유전특성 (The structural and Microwave Dielectric Properties of (1-x)Ba($Mg_{1/3}Ta_{2/3})O_3$-xBa($Co_{1/3}Nb_{2/3})O_3$(x=0.25~0.5) Ceramics)

  • 황태광;최의선;임인호;이영희
    • 한국전기전자재료학회논문지
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    • 제14권3호
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    • pp.197-201
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    • 2001
  • The microwave dielectric properties of (1-x)Ba(Mg$_{1}$3/Ta$_{2}$3/)O$_3$-xBa(Co$_{1}$3/Nb$_{2}$3)O$_3$(x=0.25~0.5) ceramics depending on the Ba(Co$_{1}$3/Nb$_{2}$3/)O$_3$[BCN] contents and the possibility of application as a microwave dielectric resonator were investigated. The specimens were prepared by he conventional mixed oxide method using there sintering temperature of 1575$^{\circ}C$. It was found that Ba(Mg$_{1}$3/Ta$_{2}$3/)O$_3$[BMT] and BCN formed a solid solution with complex perovskite structure. As the mole fraction of BCN increased, dielectric constant increased while temperature coefficient of resonant frequency decreased. The highest value of quality factor, Qxf$_{0}$=138,205GHz, obtained in the sample of 0.9BMT-0.1BCN ceramics. In the range of x$\geq$0.4, the dielectric constant was about 30. The 0.55BMT-0.45BCN ceramics showed excellent microwave dielectric properties with $\varepsilon$$_{r}$=30.84, Qxf$_{0}$=75,325GHz and $\tau$$_{f}$=2.9015ppm/$^{\circ}C$.EX>.EX>.

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Microwave Dielectric Characterization of Binary Mixtures of 3-Nitrotoluene with Dimethylacetamide, Dimethylformamide and Dimethylsulphoxide

  • Chaudhari, Ajay;Chaudhari, H.C.;Mehrotra, S.C.
    • Bulletin of the Korean Chemical Society
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    • 제25권9호
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    • pp.1403-1407
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    • 2004
  • Dielectric relaxation measurements on 3-nitrotoluene (3-NT) mixture of dimethylacetamide (DMA), dimethylformamide (DMF) and dimethysulphoxide (DMSO) have been carried out across the entire concentration range using Time domain reflectometry technique at 15, 25, 35 and $45^{\circ}C$ over the frequency range from 10 MHz to 20 GHz. For all the mixtures, only one dielectric loss peak was observed in this frequency range and the relaxation in these mixtures can be well described by a single relaxation time using Debye model. Bilinear calibration method is used to obtain complex permittivity ${\varepsilon}^{*}({\omega})$ from complex reflection coefficient ${\rho}^{*}({\omega})$ over frequency range 10 MHz to 20 GHz. The excess permittivity, excess inverse relaxation time, Kirkwood correlation factor, molar energy of activation are also calculated for these mixtures to study the solute-solvent interaction.

SOLAR ACTIVE REGION STUDY USING MICROWAVE MAPS

  • BONG SU-CRAN;LEE JEONGWOO;GARY DALE E.;YUN HONG SIK
    • 천문학회지
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    • 제36권spc1호
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    • pp.29-36
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    • 2003
  • Quiescent solar radiation, at microwave spectral regime, is dominated by gyroresonant and thermal Bremsstrahlung radiations from hot electrons residing in solar active region corona. These radiations are known to provide excellent diagnostics on the coronal temperature, density, and magnetic field, provided that spatially resolved spectra are available from observations. In this paper we present an imaging spectroscopy implemented for a bipolar active region, AR 7912, using the multifrequency interferometric data from the Owens Valley Solar Array (OVSA), as processed with a new imaging technique, so-called Spatio-Spectral Maximum Entropy Method (SSMEM). From the microwave maps at 26 frequencies in the range of 1.2-12.4 GHz at both right- and left-circular polarizations, we construct spatially resolved brightness spectra in every reconstructed pixel of about 2 arcsec interval. These spectra allowed us to determine 2-D distribution of electron temperature, magnetic field of coronal base, and emission measure at the coronal base above the active region. We briefly compare the present result with existing studies of the coronal active regions.