• 제목/요약/키워드: Pulse Width

검색결과 1,788건 처리시간 0.029초

마이크로스트립 선로상 가우시안 펄스신호의 전파특성 해석 및 측정 (Propagation characteristic analysis and measurement of gaussian pulse signals on the microstrip line)

  • 이승엽;신호섭;김남;권원현
    • 한국통신학회논문지
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    • 제23권6호
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    • pp.1425-1432
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    • 1998
  • The propagation properties of Gaussian pulse signals on the microstrip line are investigated by the Kirschning & Jansen's approximated equation to meet the frequency range of a pulse, accuracy, and geometrical requiremtns of the microstrip line. The dispersion of pulse signals is analyzed regarding to the relative permittivity .epsilon.$_{r}$, substrate height h and strip width w of the microstrip line. To verify theoretical results, several samples of 50.OMEGA. microstrip lines are fabricated. And the characteristics of pulse propagation along these lines are simple measured using VNA(Vector Network Analyzer) with time-domain analysis function. A fairly good agreement has been found between the measured pulse waveforms and computer simulations.

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고전압 펄스트랜스의 설계에 관한 기초 연구 (A Basic Study about Design of High Voltage Pulse Transformer)

  • 정현주;정영환;이동훈;홍정환;김희제;조정수
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1999년도 하계학술대회 논문집 E
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    • pp.2198-2200
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    • 1999
  • In this study, it is the purpose to study about design and manufacture of a pulse transformer for using in pulse generator and a pulse laser system. In this experiment, a ferite core in transformer instead of air core is used. The performance of the transformer is demonstrated by a voltage pulse waveform according to inductance of primary and secondary in transformer. As a result, the voltage pulse width is increased as increasement of inductance in transformer. And the voltage rate between primary and secondary is almost same with rate of inductance between primary and secondary.

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펄스형성선로로 구성된 선형유도가속기용 양방향 펄스 전원 (Bidirectional pulse generator made from pulse forming lines for linear induction accelerator)

  • 박정호;김종해;고광철;강형부
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1997년도 하계학술대회 논문집 E
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    • pp.1681-1683
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    • 1997
  • Linear induction accelerator devised for high current beam accelerating is divided into two types. In the first type, a unidirectional pulse is injected to an accelerating gap and in the second type, a bidirectional pulse is injected. The purpose of this paper is design and manufacture of bidirectional pulse generator for linear induction accelerator, where the pulse width for acceleration is more than 50[nsee] and the designed maximum charging voltage is more than 200[kV].

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Ultrashort Pulsed Laser Machining for Biomolecule Trapping

  • Choi, Hae-Woon;Farson, Dave F.;Lee, L.James;Lee, Ho
    • Journal of the Optical Society of Korea
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    • 제13권3호
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    • pp.335-340
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    • 2009
  • Ultrashort pulse laser drilling of polycarbonate track-etched membrane (pTEM) material was used to fabricate a mouse embryo cell trapping device. Holes with a diameter of $2{\mu}m$ to $5{\mu}m$ were fabricated on a $10{\mu}m$ thick membrane using a femtosecond laser with a 150 fs pulse width and 775 nm wavelength and multiple-pulse irradiation. In cell trapping tests, the overall cell occupancy of the machined holes in the fabricated pTEM was found to be more than 80%. The results of a single pulse and multiple pulse irradiation were compared in terms of the surface quality. It was generally found that a single pulse with high energy was less desirable than irradiation with multiple pulses of lower energy.

Novel Compact Current Type Pulse Power Generator

  • Min, B.D.;Kim, J.H.;Pavlov, E.;Yoo, D.W.;Rim, G.H.
    • 전력전자학회:학술대회논문집
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    • 전력전자학회 2005년도 전력전자학술대회 논문집
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    • pp.529-531
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    • 2005
  • This paper proposes a compact pulse generator fur NOx removal application for diesel automotive. The rising time is important factor to increase NOx removal efficiency in pulsed corona discharge method. Manufacturing cost and compactness of the pulse power generator should be satisfied for automotive application. The proposed pulse power uses a low voltage thyristor, a pulse transformer with the function of saturated magnetic switch, and series connected general diodes as opening switch to satisfy that requirements. With 200 resistor load, the experiment results show that the output voltage is 21kV, the rising time is about 21ns, and the pulse width (FWHM) is about 42ns.

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부귀환펄스선형증폭기의 이득 안정도에 관한 연구 (A System on the Gain Stability of Negative Feedback Pulse Linear Amplifier)

  • 이병선
    • 대한전자공학회논문지
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    • 제10권5호
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    • pp.7-15
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    • 1973
  • 부귀환펄스선형증폭기에 단계전압과 방사능검출기에서 나오는 펄스와 같이 빠른 펄스를 인가하였을 경우의 이득 안정도에 관하여 해석하였고 실험하였다. 이들 빠른 입력전압이 부귀환증폭기에 인가되면 출력전압의 선형도와 안정도는 증폭기의 rise time의 수배가 경과하여야 부귀효과가 나타난다. 이 제한을 주리기 위하여는 부귀환증폭기의 rise time을 계측할려는 입력펄스의 폭보다 적도록 설계하여야 한다는 것을 표시하였다.

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제모용 Long-Pulse Alexandrite Laser의 출력 특성 연구 (A study on the output characteristics of Long-pulse Alexandrite laser for hair removal)

  • 최진영;김상길;김태균;박종웅;송건주;정용호;홍정환;김희제
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2003년도 하계학술대회 논문집 C
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    • pp.1729-1731
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    • 2003
  • Recently many solid-state laser systems were widely used in the medical applications. So it is necessary to study various optimal laser parameters for adopting new medical treatments. Alexandrite laser using switching mode power supply has designed and experimented to adjust a pulse repetition rate by PIC one-chip microprocessor. The fundamental results have been obtained during the first financial year in 2002. We will be able to find out the optimal hair removal characteristics by the repetitive experiments of Alexandrite laser as the parameters such as pulse repetition rate, pulse width, and pulse energy etc.

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실리콘 비선형 Fabry-Perot 간섭계를 이용한 광펄스 변조와 축약 (Pulse Compression by the Nonlinear Silicon Fabry-Perot Interferometer)

  • 김달현;이재형;장준성
    • 한국광학회지
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    • 제1권1호
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    • pp.40-45
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    • 1990
  • 반도체 실리콘은 띠간격 근처의 에너지를 갖는 광자를 흡수하여 생성된 전자-정공쌍에 의해 굴절률이 비선형적으로 변하며 이에 따라 입사한 광펄스를 변조시킨다. Finesse가 큰 실리콘 Fabry-Perot 간섭계를 형성할 때, 이를 투과하는 광펄스가 실리콘의 굴절률을 변화시켜 스스로 간섭계의 보강간섭조건을 만족시킴으로써 반치폭이 1/5까지 축약되는 현상을 관측하였다. 그리고 관측된 결과는 수치해석으로 구한 결과와 잘 일치하였다.

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고출력 마그네트론 구동용 3.6 MW, $4\;{\mu}s$, 200 pps 펄스 모듈레이터 개발 (Development of a 3.6 MW, $4\;{\mu}s$, 200 pps Pulse Modulator for a High Power Magnetron)

  • 장성덕;권세진;배영순;오종석;조무현;남궁원;손윤규
    • 대한전기학회논문지:전기물성ㆍ응용부문C
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    • 제54권3호
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    • pp.120-126
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    • 2005
  • The Korean Superconducting Tokamak Advanced Research (KSTAR) tokamak device is being constructed to perform long-pulse, high-beta, advanced tokamak fusion physics experiments. The long-pulse operation requires the non-inductive current drive system such as the Lower-Hybrid Current Drive (LHCD) system. The LHCD system drives the non-inductive plasma current by means of C-band RF with 2-MW CW power and 5-GHz frequency. For the LHCD test experiments, an RF test system is developed. It is composed of a 5-GHz, 1.5-MW pulsed magnetron and a compact pulse modulator with $4\;{\mu}s$ of pulse width. The pulse modulator provides the maximum output voltage of 45 kV and the maximum current of 90 A. It is composed of 7 stages of Pulse Forming Network (PFN), a thyratron tube (E2V, CX1191D), and a pulse transformer with 1:4 step-up ratio. In this paper, the detailed design and the performance test of the pulse modulator are presented.

광용적맥파 신호를 이용한 수면 중 호흡 추정 (Estimation of Respiration Using Photoplethysmograph During Sleep)

  • 박종욱;이전;이효기;김호중;이경중
    • 대한의용생체공학회:의공학회지
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    • 제34권3호
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    • pp.105-110
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    • 2013
  • Respiratory signal is one of the important physiological information indicating the status and function of the body. Recent studies have provided the possibility of being able to estimate the respiratory signal by using a change of PWV(pulse width variability), PRV(pulse rate variability) and PAV(pulse amplitude variability) in the PPG (photoplethysmography) signal during daily life. But, it is not clear whether the respiratory monitoring is possible even during sleep. Therefore, in this paper, we estimated the respiration from PWV, PRV and PAV of PPG signals during sleep. In addition, respiration rates of the estimated respiration signal were calculated through a time-frequency analysis, and errors between respiration rates calculated from each parameter and from reference signal were evaluated in terms of 1 sec, 10 sec and 1 min. As a result, it showed the errors in PWV(1s: $36.38{\pm}37.69$ mHz, 10s: $36.53{\pm}38.16$ mHz, 60s: $30.35{\pm}38.72$ mHz), in PRV(1s: $1.45{\pm}1.38$ mHz, 10s: $1.44{\pm}1.37$ mHz, 60s: $0.45{\pm}0.56$ mHz), and in PAV(1s: $1.05{\pm}0.81$ mHz, 10s: $1.05{\pm}0.79$ mHz, 60s: $0.56{\pm}0.93$ mHz). The errors in PRV and PAV are lower than that of PWV. Finally, we concluded that PRV and PAV are more effective than PWV in monitoring the respiration in daily life as well as during sleep.