• Title/Summary/Keyword: 위상 측정기

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Analysis of the Phase Change of a Laser Beam in a Laser Doppler Vibrometer Due To the Sound Field Radiated From Structures Vibrating Underwater (수중에서 진동하는 구조물로부터 방사되는 음에 기인한 레이저 도플러 진동측정기 광선의 위상변화에 대한 분석)

  • Kil, Hyun-Gwon;Jarzynski, Jacek
    • The Journal of the Acoustical Society of Korea
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    • v.27 no.4
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    • pp.178-182
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    • 2008
  • In measurements of the vibration of structures underwater with a laser Doppler vibrometer, the surface vibration is measured by means of detecting the phase change of the laser beam due to the structural vibration. The laser beam passes through the sound field radiated from the vibrating structures underwater. It experiences an additional phase change due to the change in refractive index in the radiated sound field. This phase change due to the sound field may cause the error in surface vibration measurements. In this paper, this phase change due to the radiated sound filed has been analyzed. The numerical simulation has been peformed to evaluate the phase change in sound field radiated from an infinite cylindrical structure vibrating underwater.

Temperature measurements using optical retarder (광 위상지연기를 이용한 온도측정)

  • 전상민;김용평
    • Korean Journal of Optics and Photonics
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    • v.13 no.3
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    • pp.240-244
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    • 2002
  • We proposed a novel temperature sensor based on the phenomena that the phase difference between principal polarization states in an optical retarder is a function of temperature. The polarization state of an optical beam is changed as it passes through the optical retarder, with the change dependent on the temperature. The temperature of the optical retarder is determined by comparison of the power difference between principal polarization states. A temperature sensor was successfully implemented using a polarization maintaining fiber of length 100 mm as the optical retarder. The change rate of phase difference on temperature was 0.236$^{\circ}C$$_{-1}$ and the measurement error was $\pm$0.038$^{\circ}C$ over the temperature region of -2.6$^{\circ}C$~3.4$^{\circ}C$.

Optical Fiber Wavemeter Using a Polarization Interferometer (광섬유 편광간섭계를 이용한 광파장 측정)

  • 이현우;이영주;김용평
    • Proceedings of the Optical Society of Korea Conference
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    • 2000.02a
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    • pp.86-87
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    • 2000
  • 지금까지 광파장 측정기로는 회절격자를 이용한 스펙트로미터$^{[1]}$ , 간섭계형 측정기$^{[2]}$ , 퓨리어변환 스펙트로미터$^{[3]}$ 등이 개발되어 왔다. 이러한 측정 방법들은 정밀도면에서 안정적이나 시스템의 부피가 크고, 복잡하며, 광학적 정렬의 어려움이 있다. 또한 WDM 파장영역인 1550nm 부근에서 회절격자를 이용한 스펙트로미터는 고가의 광검출기를 사용하여야 한다. 최근에는 기존의 광학적 정렬이나 기계적인 움직임이 없이 측정가능한 방법에 대한 연구가 활발하다. 본 논문에서는 위상지연기로 쓰인 Polarization Mantaining Fiber(PM-fiber)내에서 입사광의 파장에 따라 fast축과 slow축 방향 편광성분의 위상차가 파장의 함수인 것을 이용해 이 위상차에의한 서로 다른 편광성분의 Power의 차이를 측정함으로써 파장을 결정하는 저가의 휴대용 광파장 측정장비의 구현방법을 제시하였다. (중략)

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Measurements of optical wavelength using an optical fiber retarder (광섬유 위상지연기를 이용한 광파장 측정)

  • 이현우;김용평
    • Korean Journal of Optics and Photonics
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    • v.12 no.1
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    • pp.5-9
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    • 2001
  • A wavemeter was realized using the phenomena that the phase lag between principal polarization states in an optical retarder is a function of wavelength. The change in the polarization state of the optical beam as it passes through the optical retarder is dependent on wavelength. The wavelength of the optical beam is determined by comparing the power difference between principal polarization states. A prototype wavemeter was successfully implemented using a polarization maintaining fiber with birefringence $3\times10^{-4}$ and length 100 mm as the optical retarder. The measurement resolution was 0.08 nm over a wavelength region of 1554.38 nm-1557.l9 nm, which agreed well with theoretically calculated results. In addition, the dependence of operating characteristics on temperature was analyzed theoretically and experimentally.mentally.

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The Phase Difference Measurement Module Development for Amplitude Modulated Range Measurement System (진폭 변조 거리 측정 시스템을 위한 정밀 위상차 측정부 개발)

  • Noh, Hyoung-Woo;Park, Jeong-Ho;Kang, Il-Heung;Choi, Mun-Gak;Kim, Kang-Wook
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
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    • v.22 no.2
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    • pp.182-190
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    • 2011
  • A amplitude modulation(AM) range measuring system utilizes the phase difference of the modulated envelope of the reflected signal to measure the distance. It is known that the AM system has a problem in accuracy due to antenna leakage signals and spurious reflection signals, but an AM range measurement system using an active reflector, which shifts the frequency bands, has been proposed in order to minimize the measurement errors due to spurious signals. In this paper, a new phase measurement module for the AM range measurement system, which enables to measure long distance with good accuracy, is proposed. The modulation frequency is alternatively selected between 8 and 1 MHz, and the measured distance range with this module is up to 150 m within 2 cm accuracy. A JK flip-flop circuit is used for higher phase accuracy, and an XOR circuit is used to cover long distance.

Establishment of nanometer length standardization using the monolithic x-ray interferometer (일체식 엑스선 간섭계를 이용한 나노미터 표준확립)

  • 김원경;정용환;박진원;김재완;엄천일;권대갑
    • Proceedings of the Korea Crystallographic Association Conference
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    • 2002.11a
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    • pp.35-35
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    • 2002
  • 나노미터 표준을 확립하기 위하여 일체식 엑스선 간섭계에 광간섭계를 결합시킨 복합간섭계를 구성하였다. 복합간섭계는 광간섭계의 Zero crossing 지점부터 표준시편이 올려진 미소이동대의 이동거리를 변화된 위상값으로 읽고 그 변화량을 고분해능 변위 측정기인 엑스선 간섭계로 읽어들이는 구조로 구성된다. 본 연구에서는 미소이동대의 위치 변화와 관련된 광간섭계의 위상 안정도, 엑스선 간섭계 및 미소이동대의 위치 안정도 등이 나노미터 영역의 길이 측정에 매우 중요한 요인이 되므로, 미소이동대의 위치 변화시 정지상태에서의 위상 잠김 (phase locking) 안정도를 측정하였다. 마이켈슨 레이저간섭계의 한쪽 팔을 고정시키고 다른 한 팔은 미소이동대 위에 반사거울을 설치하여 미소이동대의 움직임을 측정하였다. 보다 안정된 위상잠김 상태를 확보하기 위하여 PID feedback loop controller를 사용하였다. 측정 결과 위상 변동폭이 0.022 degree 이하의 높은 위상잠김 안정도를 확보하였으며, 이를 길이단위로 환산하면 정지상태에서 약 0.02 nm 이하의 위치 안정도를 나타낸다.

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Construction of Ultrasound Pulsed Doppler Velocimeter (펄스 초음파 도플러 속도계의 제작에 관한 연구)

  • 현석봉;김수용;이재수
    • Progress in Medical Physics
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    • v.5 no.1
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    • pp.25-39
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    • 1994
  • To measure the velocity of heart wall and local flow transctaneously in blood vessels, we have developed a single channel 3.1 MHz pulsed ultrasonic Doppler velocity meter. Ultrasound pluse width and repetition frequency (PRF) used in the velocity meter is 1 ${\mu}$sec 6kHz reapectively, and the Doppler shift of the backscattered echo signal is sensed in a phase detector by coherent demodulation method. From the output of the phase detector, the Doppler signal corresponding to the mean velocity of acoustic wave scatterers over a small region is obtained by using a range gate, sample holder and band-pass filter. Mean frequency of Doppler signal is estimated by zero-crossing counter and the instantaneous velocity of scatters is displayed as a function of time. It is possible to estimate velocity profile, volume flow and flow acceleration of vessels in man if the number of channels and range resolution in increased.

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Compact and Wideband Correlator with Metamaterial Hybrid Rat-Race Coupler (Metamaterial 하이브리드 Rat-Race Coupler를 이용한 소형화된 광대역 코릴레이터)

  • Kim, Yang-Hyun;Seo, Chul-Hun
    • Journal of the Institute of Electronics Engineers of Korea TC
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    • v.46 no.2
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    • pp.147-151
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    • 2009
  • A wideband correlator, with 45% relative bandwidth is proposed at the frequency range of 3.1-5.1GHz. The structures of the correlator components such as the delay line and the Wilkinson power divider are designed to be realized in transmission line form using the Agilent's Advanced Design System (ADS). The correlator made by using three unique wideband 3-dB couplers, rat-race coupler and one 3-dB wilkinson power divider to reach the required bandwidth. The insertion loss, amplitude imbalance and phase imbalance between ports are presented. The proposed correlator makes compact size better than correlator of conventional structure.

Software Implementation of GSM Signal Measurements (GSM 신호 측정기의 소프트웨어 구현)

  • Hong, Dae-Ki;Kang, Sung-Jin
    • Journal of the Korea Academia-Industrial cooperation Society
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    • v.10 no.9
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    • pp.2369-2378
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    • 2009
  • In this paper, we implement measurement functionality for performance measurement of the GSM (Global System for Mobile Communication) terminal by using software. Generally speaking, the receiving algorithms in normal modems cannot be used directly to the measurement system due to the lack of the algorithm accuracy. In this paper, we propose the new receiver algorithm for precise GSM signal measurements. In the receiving algorithm, 2-stage (coarse stage, fine stage) parameters estimation (symbol-timing, frequency offset, carrier phase) scheme is used. To improve the estimation accuracy, we increase the number of the received signal samples by interpolation. The proposed GSM signal measurement algorithm can be used for verifying the hardware measurement system. In addition, the proposed algorithm can be used for the commercial system through code execution speed optimization.

High-speed, High-resolution Phase Measuring Technique for Heterodyne Displacement Measuring Interferometers. (헤테로다인 변위 측정 간섭계의 고속, 고분해능 위상 측정)

  • 김승우;김민석
    • Proceedings of the Korean Society of Precision Engineering Conference
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    • 2002.05a
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    • pp.203-206
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    • 2002
  • One of the ever-increasing demands on the performances of heterodyne interferometers is to improve the measurement resolution, of which current state-of-the-art reaches the region of sub-nanometers. We propose a new scheme of phase-measuring electronics that reduces the measurement resolution without further increase in clock speed. Our scheme adopts a super-heterodyne technique that lowers the original beat frequency to a level of 1 MHz by mixing it with electrically generated reference signal. The technique enables us to measure the phase of Doppler shift with a resolution of 1.58 nanometer at a sampling rate of 1 MHz. To avoid the undesirable decrease in the maximum measurable speed caused by the lowered beat frequency, a special from of frequency up-down counting technique is combined with the super-heterodyning. This alloys performing required phase unwrapping simply by using programmable digital gates without 2$\pi$ ambiguities up to the maximum velocity of 2.35 m/s.

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