• 제목/요약/키워드: Pulsed power system

검색결과 211건 처리시간 0.03초

레이저 추적 시스템을 위한 레이더 시스템 개발 (Development of Radar System for Laser Tracking System)

  • 성기평;임형철;최만수;유성열
    • 우주기술과 응용
    • /
    • 제4권1호
    • /
    • pp.1-11
    • /
    • 2024
  • 한국천문연구원이 개발한 인공위성 레이저 추적 시스템(satellite laser ranging, SLR)은 지상에서 극초단파 펄스 레이저를 발진하여 우주물체를 추적하는 관측 영역에서 레이저에 의해 비행체가 피폭되지 않도록 사전에 이를 탐지하고, 레이저 발진을 중지시키는 것을 목적으로 비행체 감시 레이더 시스템을 거창 SLR 시스템에 개발하였다. 개발한 비행체 감시 레이더 시스템은 고주파대역(X-band) 레이더로 SLR 시스템이 지향하는 방향에 라디오 주파수(radio frequency, RF) 펄스 신호를 송신하고 수신하는 RHS(radar hardware subsystem)와 SLR 운영시스템과 인터페이스를 유지하면서 RHS로부터 획득한 RF 펄스 신호를 바탕으로 비행체 검출 여부 판단 및 레이저 발진을 중지시키는 MCS(main control subsystem)로 구성하였다. 본 논문에서는 비행체 감시 레이더 시스템을 구성하는 RHS와 MCS 설계 내용을 기술하고, SLR 운영시스템과의 인터페이스 및 운용 시나리오를 제시한다. 개발된 비행체 감시 레이더 시스템은 항공기를 이용한 실증 시험을 통해 비행체 검출 및 레이저 중지 신호를 발생하는 것을 확인하여 검증하였다.

$\alpha-Fe_2O_3$ 박막에서 스핀 재 정렬에 관한 연구 (The Spin Reorientations in $\alpha-Fe_2O_3$ Thin Film)

  • 서정철;이호선
    • 한국자기학회지
    • /
    • 제11권1호
    • /
    • pp.21-25
    • /
    • 2001
  • Si 기판 위에 $\alpha$-Fe$_2$O$_3$ 박막을 pulsed laser deposition system으로 제조하여 결정학적 및 자기적 성질을 X선 회절 및 Mossbauer 분광법을 사용하여 연구하였다. 박막의 제조조건은 laser의 출력 5.128 W/$cm^2$, 산소의 압력 0.1 torr, 기판의 온도 30$0^{\circ}C$에서 가장 이상적이었으며 이를 공기 중 80$0^{\circ}C$에서 1일간 열처리하였다. 입자는 크기는 길이 200~300nm, 폭 70-150 nm정도의 타원체로 기판에 비스듬히 누운 형태를 취하고 있으며 결정은 육방정계 형태의 corundum 구조로서 결정상수는 a = 5.03 0.05 $\AA$, c = 13.73$\pm$0.05 $\AA$로 측정되었다. 원자의 스핀 방향은 감마선 방향(기판에 수직 방향)에 대하여 평균적으로 Morin 변환 이하에서는 38$^{\circ}$, 그 이상에서는 48$^{\circ}$의 각을 이루며 특정한 방향을 선호하고있는 것으로 나타났다. Morin 변환은 200 K에서 실온가지 넓은 온도 범위에서 일어나며, c-축에 대한 원자의 스핀 방향은 48$^{\circ}$에서 80$^{\circ}$정도의 변화만이 관측되었다.

  • PDF

Study of The Anisotropy of Electron Energy Distribution of Optical-Field Ionized Oxygen Plasma by Using Polarization Spectroscopy

  • Kim, Dong-Eon;Kim, Jae-Hoon;Kawachi, Tetsuya;Hasegawa, Noboru;Sukegawa, Kouta;Iwamae, Atsushi;Fujimoto, Takashi
    • Journal of the Optical Society of Korea
    • /
    • 제7권3호
    • /
    • pp.145-149
    • /
    • 2003
  • The anisotropy of electron energy distribution in oxygen plasmas produced by a high intensity laser was investigated by using polarization spectroscopy. An ultra-short pulsed laser with a pulse duration of 66.5 fs and a power density of $1 {\times} 10^17/ W/$\textrm{cm}^2$$ was used. At this power density and pulse duration, the plasma was generated predominantly by optical field ionization. The degree of polarization of OVI 1s$^2$2p$^2$p2- 1s$^2$4d$^2$D$^{0}$ (J = 1/2-3/2 and 3/2-5/2) transition line at 129.92 $\AA$ was measured. O VI 1s$^2$2p$^2$P$^2$ -1s$^2$4s$^2$S$^2$ (J = 1/2-1/2 and 3/2-1/2) transition line at 132.26 $\AA$ was used to calibrate the sensitivity of the optical system. The dependencies of the degree of polarization on the initial gas density and on the laser polarization were investigated. When the laser polarization was changed from a linear to a circular polarization, the degree of polarization was decreased. When the initial gas density was increased, the degree of polarization was decreased.

Application of time-of-flight near infrared spectroscopy to Satsuma mandarin

  • Tsuchikawa, Satoru;Ito, Satomi;Inoue, Kinuyo;Miyamoto, Kumi
    • 한국근적외분광분석학회:학술대회논문집
    • /
    • 한국근적외분광분석학회 2001년도 NIR-2001
    • /
    • pp.1627-1627
    • /
    • 2001
  • In this study, a newly constructed optical measurement system, whose main components were a parametric tunable laser and a near infrared photoelectric multiplier, was applied to detection of the information for the inside of Satsuma mandarin using time-of-flight near infrared spectroscopy (TOF-NIRS). The combined effects on the time resolved profile of sample diameter, sugar content, the wavelength of the laser beam, and the detection position of transmitted light were investigated in detail. The samples used were Satsuma mandarin (Citrus unshu $M^{ARC}$.) (location: Wakayama, Japan) having the diameters of 50-84 mm. The sugar content measured by a refractometer varied from 9.9 to 16.3 Brix%. Equator of sample was irradiated vertically with the pulsed laser, and transmitted output power was measured on the restricted position of the equator using the optical fiber cable. The sampling time and the number of averaging the output power were 100 ns and 100 times, respectively. The variation of the attenuance of peak maxima At, the time delay of peak maxima t and the variation of full width at half maximum w were strongly dependent on the detection position and the wavelength of the laser beam. At, t and w increased gradually as the sample diameter increased to be much absorbed and vigorously scattered. On the other hand, each optical parameter had a tendency to increase as the sugar content increased. Such behavior was remarkable when the transmitted light was detected at the side face of a sample. When we apply TOF-NIRS to detection of the information for the inside of fruit with high moisture content like Satsuma mandarin, it is very important to give attention to the difference in the scattered light within tissues and the semi-straightly propagated light. Furthermore, we tried to express the resulting phenomena by using a model samples composed of water, sucrose, and milk. The variation of the time resolved profile is strongly governed by the combination of the light absorption component, scattering medium, and refractive index.

  • PDF

Application of time-of-flight near infrared spectroscopy to Satsuma mandarin

  • Tsuchikawa, Satoru;Ito, Satomi;Inoue, Kinuyo;Miyamoto, Kumi
    • 한국근적외분광분석학회:학술대회논문집
    • /
    • 한국근적외분광분석학회 2001년도 NIR-2001
    • /
    • pp.1626-1626
    • /
    • 2001
  • In this study, a newly constructed optical measurement system, whose main components were a parametric tunable laser and a near infrared photoelectric multiplier, was applied to detection of the information for the inside of Satsuma mandarin using time-of-flight near infrared spectroscopy (TOF-NIRS). The combined effects on the time resolved profile of sample diameter, sugar content, the wavelength of the laser beam, and the detection position of transmitted light were investigated in detail. The samples used were Satsuma mandarin (Citrus unshu $M_{ARC}$.) (location: Wakayama, Japan) having the diameters of 50-84 mm. The sugar content measured by a refractometer varied from 9.9 to 16.3 Brix%. Equator of sample was irradiated vertically with the pulsed laser, and transmitted output power was measured on the restricted position of the equator using the optical fiber cable. The sampling time and the number of averaging the output power were 100 ns and 100 times, respectively. The variation of the attenuance of peak maxima At, the time delay of peak maxima $\Delta$t and the variation of full width at half maximum Δw were strongly dependent on the detection position and the wavelength of the laser beam. At, $\Delta$t and $\Delta$w increased gradually as the sample diameter increased to be much absorbed and vigorously scattered. On the other hand, each optical parameter had a tendency to increase as the sugar content increased. Such behavior was remarkable when the transmitted light was detected at the side face of a sample. When we apply TOF-NIRS to detection of the information for the inside of fruit with high moisture content like Satsuma mandarin, it is very important to give attention to the difference in the scattered light within tissues and the semi-straightly propagated light. Furthermore, we tried to express the resulting phenomena by using a model samples composed of water, sucrose, and milk. The variation of the time resolved profile is strongly governed by the combination of the light absorption component, scattering medium, and refractive index.

  • PDF

DIAGNOSTICS OF PLASMA INDUCED IN Nd:YAG LASER WELDING OF ALUMINUM ALLOY

  • Kim, Jong-Do;Lee, Myeong-Hoon;Kim, Young-Sik;Seiji Katayama;Akira Matsunawa
    • 대한용접접합학회:학술대회논문집
    • /
    • 대한용접접합학회 2002년도 Proceedings of the International Welding/Joining Conference-Korea
    • /
    • pp.612-619
    • /
    • 2002
  • The dynamic behavior of Al-Mg alloys plasma was very unstable and this instability was closely related to the unstable motion of keyhole during laser irradiation. The keyhole fluctuated both in size and shape and its fluctuation period was about 440 ${\mu}{\textrm}{m}$. This instability has been estimated to be caused by the evaporation phenomena of metals with different boiling point and latent heats of vaporization. Therefore, the authors have conducted the spectroscopic diagnostics of plasma induced in the pulsed YAG laser welding of Al-Mg alloys in air and argon atmospheres. In the air environment, the identified spectra were atomic lines of Al, Mg, Cr, Mn, Cu, Fe and Zn, and singly ionized Mg line, as well as strong molecular spectrum of AlO, MgO and AIH. It was confirmed that the resonant lines of Al and Mg were strongly self-absorbed, in particular in the vicinity of pool surface. The self-absorption of atomic Mg line was more eminent in alloys containing higher Mg. These facts showed that the laser-induced plasma was relatively a low temperature and high density metallic vapor. The intensities of molecular spectra of AlO and MgO were different each other depending on the power density of laser beam. Under the low power density irradiation condition, the MgO band spectra were predominant in intensity, while the AlO spectra became much stronger in higher power density. In argon atmosphere the band spectra of MgO and AlO completely vanished, but AlH molecular spectra was detected clearly. The hydrogen source was presumably the hydrogen solved in the base Metal, absorbed water on the surface oxide layer or H$_2$ and $H_2O$ in the shielding gas. The temporal change in spectral line intensities was quite similar to the fluctuation of keyhole. The time average plasma temperature at 1 mm high above the surface of A5083 alloy was determined by the Boltzmann plot method of atomic Cr lines of different excitation energy. The obtained electron temperature was 3, 280$\pm$150 K which was about 500 K higher than the boiling point of pure aluminum. The electron number density was determined by measuring the relative intensities of the spectra1lines of atomic and singly ionized Magnesium, and the obtained value was 1.85 x 1019 1/㎥.

  • PDF

Breakdown Properties in Physiological Saline by High Voltage Pulse Generator

  • Byeon, Yong-Seong;Song, Ki-Baek;Uhm, Han-Sup;Shin, Hee-M.;Choi, Eun-Ha
    • 한국진공학회:학술대회논문집
    • /
    • 한국진공학회 2011년도 제41회 하계 정기 학술대회 초록집
    • /
    • pp.333-333
    • /
    • 2011
  • We have investigated the breakdown properties in liquids by high voltage pulse system. High voltage pulse power system is consisted of the Marx-generator with two capacitors (0.5 ${\mu}F$, withstanding voltage is 40 kV), to which the charging voltage can be applied to maximum 30 kV DC, spark gap switch and charging resistor of 20 $M{\Omega}$. We have made use of tungsten pin electrodes of anode-cathode (A-K), which are immersed into the liquids. The breakdown voltage and current signals are measured by high voltage probe (Tektronix P6015A) and current monitor (IPC CM-1.S). Especially the high speed breakdown or plasma propagation characteristics in the pulsed A-K gap have been investigated by using the high speed ICCD camera. We have measured the electron temperature through the Boltzmann plot method from the breakdown spectrums. Here the A-K gap has been changed by 1 mm, 2 mm, and 3 mm. The used liquids are distilled water and solution of salt (0.9 %). The output voltage and current signals at breakdown in distilled water are shown to be bigger than those in saline solution. The breakdown voltage and current characteristics in liquids will be discussed in accordance with A-K gap distances. It is also found that the electron temperatures and plasma densities in liquids are decreased in conformity with A-K gap.

  • PDF

UV 감지기로서 CCD어레이를 사용한 소형 디지털 광 오존모니터 (A New Small Size Digital Optical Ozone Monitor Using CCD Array as a UV Detector)

  • 정완영;이승철
    • 한국정보통신학회논문지
    • /
    • 제12권1호
    • /
    • pp.158-163
    • /
    • 2008
  • UV기술에 기반한 오존모니터는 신호의 안정성 때문에 널리 활용되어오고 있다. 먼저 오존 발생기에서 나오는 오존농도를 실시간, 고정 밀로 측정하기 위해서 저압 수은램프를 UV광원으로 하고, 광증배관을 UV 감지기로 하는 시스템을 구성하였다. 이 구조는 저 비용의 고농도 오존의 계측에 유용한 시스템으로서 단순한 구조와 비교적 우수한 계측성 능을 얻을 수 있었다. 제조된 시스템은 $0.05{\sim}2w1.%$의 측정 농도영역에서 좋은 선형성을 나타내었다. ppm정도의 보다 정밀한 농도계측을 위해서는 UV광원으로서 고출력 펄스 크세논램프를 사용하고, CCD어레이를 광스펙트로메터로 사용하도록 시스템을 설계하였다. CCD출력으로부터의 광신호는 우수한 반응성과 띄어난 광해상도를 가지고 디지털신호로 변환되고, 이 디지털신호는 PC의 스크린에 디스플레이 되도록 설계되었다. 제작된 시스템은 $10{\sim}10,000ppm$ 영역에서 선형적이고 우수한 감도를 보였으며 저 농도의 오존을 측정하는 시스템으로서의 가능성을 보여주었다.

실시간 경계를 위한 라이다 데이터 처리의 가속화 방법 (An Acceleration Method for Processing LiDAR Data for Real-time Perimeter Facilities)

  • 이윤임;이은석;노희전;이성현;김영철
    • 한국정보통신학회:학술대회논문집
    • /
    • 한국정보통신학회 2022년도 춘계학술대회
    • /
    • pp.101-103
    • /
    • 2022
  • 중요시설 실시간 감지 시스템으로는 주로 CCTV를 사용하고 있다. CCTV의 경우 감지에 대한 정확성은 높지만 시야각이 좁기 때문에 레이다(RADAR)와 같은 센서와 함께 혼용되어 사용되고 있다. 라이다(LiDAR)는 고출력의 펄스 레이저를 이용하여 물체에 반사되어 돌아오는 시간을 감지하여 거리정보를 획득하는 기술이다. 라이다의 경우 데이터 처리량으로 인해 서버의 동시 처리 센서 개수의 제약으로 인해 비용적으로나 기술적으로나 활용도가 높지 않은 문제점이 있다. 광망 센서에 의한 감지 방식 또한 강풍과 혹한에 취약하고 동물 훼손에 따른 유지보수의 문제도 있다. 본 논문에서는 기존의 라이다 센서에서 사용하는 905nm 파장대가 아닌 1550nm 파장대를 사용함으로써 기상 환경에 대한 영향은 강하고, 다수의 센서를 통합하여 관제할 수 있는 시스템 개발을 제안하고자 한다.

  • PDF

Optical Diagnostics of Nanopowder Processed in Liquid Plasmas

  • Bratescu, M.A.;Saito, N.;Takai, O.
    • 한국진공학회:학술대회논문집
    • /
    • 한국진공학회 2011년도 제40회 동계학술대회 초록집
    • /
    • pp.17-18
    • /
    • 2011
  • Plasma in liquid phase has attracted great attention in the last few years by the wide domain of applications in material processing, decomposition of organic and inorganic chemical compounds and sterilization of water. The plasma in liquid is characterized by three main regions which interact each - other during the plasma operation: the liquid phase, which supply the plasma gas phase with various chemical compounds and ions, the plasma in the gas phase at atmospheric pressure and the interface between these two regions. The most complex region, but extremely interesting from the fundamental, chemical and physical processes which occur here, is the boundary between the liquid phase and the plasma gas phase. In our laboratory, plasma in liquid which behaves as a glow discharge type, is generated by using a bipolar pulsed power supply, with variable pulse width, in the range of 0.5~10 ${\mu}s$ and 10 to 30 kHz repetition rate. Plasma in water and other different solutions was characterized by electrical and optical measurements. Strong emissions of OH and H radicals dominate the optical spectra. Generally water with 500 ${\mu}S/cm$ conductivity has a breakdown voltage around 2 kV, depending on the pulse width and the repetition rate of the power supply. The characteristics of the plasma initiated in ultrapure water between pairs of different materials used for electrodes (W and Ta) were investigated by the time-resolved optical emission and the broad-band absorption spectroscopy. The deexcitation processes of the reactive species formed in the water plasma depend on the electrode material, but have been independent on the polarity of the applied voltage pulses. Recently, Coherent anti-Stokes Raman Spectroscopy method was employed to investigate the chemistry in the liquid phase and at the interface between the gas and the liquid phases of the solution plasma system. The use of the solution plasma allows rapid fabrication of the metal nanoparticles without being necessary the addition of different reducing agents, because plasma in the liquid phase provides a reaction field with a highly excited energy radicals. We successfully synthesized gold nanoparticles using a glow discharge in aqueous solution. Nanoparticles with an average size of less than 10 nm were obtained using chlorauric acid solutions as the metal source. Carbon/Pt hybrid nanostructures have been obtained by treating carbon balls, synthesized in a CVD chamber, with hexachloro- platinum acid in a solution plasma system. The solution plasma was successfully used to remove the template remained after the mesoporous silica synthesis. Surface functionalization of the carbon structures and the silica surface with different chemical groups and nanoparticles, was also performed by processing these materials in the liquid plasma.

  • PDF