• Title/Summary/Keyword: 최대진폭

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The Structures and Dielectric Properties of Plasma Polymerized Polyethylene (플라즈마 중합 폴리에틸렌 구조와 유전특성)

  • 김두석
    • Journal of the Korean Institute of Illuminating and Electrical Installation Engineers
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    • v.14 no.3
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    • pp.38-42
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    • 2000
  • Plasma polymerized thin films were manufactured inter-electrode coupled plasma polymerization apparatus. The deposition rate reached its maximum between 40[W] and 100[W]. In the ESCA analysis, peaks revealing -CH2, -CH, -C- were present at 285.4 and 285.5[eV] respectively. The C=O peak at 532.8[eV] and the C-O peak at 533.8[eV], which were grouped with an unignorable amount of oxygen were conformed. In ESR analysis, the curve revealing strong amplification was in saturation, which was affected by weak power. This is considered as a -CH-Ch=Ch- structure containing the Allyl group. The relative permittivity of the plasma polymerized thin films was about 3.5 at a frequency of 100[Hz]∼200[kHz]. The dissipation factor showed allow value of 0.008.

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Design and performance of a CE-CPSK modulated digital delay locked tracking loop (CE-CPSK 변조된 디지털 지연동기루프의 설계 및 성능 분석)

  • 김성철;송인근
    • Journal of the Korea Institute of Information and Communication Engineering
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    • v.4 no.2
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    • pp.417-426
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    • 2000
  • In this paper, CE-CPSK(Constant Envelope Continuous Phase Shift Keying) modulated DS/SS(Direct Sequence Spread Spectrum) transceiver with 908 MHz carrier frequency and 1.5 MHz PN clock rate is proposed. To overcome the effect of nun-linear power amplifier, CE-CPSK modulation method which has the constant envelope and continuous phase characteristics is proposed. To analyze the DS/SS receiver performance with respect to code tracking loop, multipath fading channel is characterized as a two-ray Rayleigh fading channel. To compensate the demerit of analog delay locked loop, digital delay locked loop is employed for code tracking loop. Simulation and experimental examination has been carried out in AWGN(Additive White Gaussian Noise) and Rayleigh fading channel environment in order to prove validity of the proposed method.

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The Implementation of the Compensation Algorithm of Time Delay for Microwave Polar Transmitters (마이크로파 폴라 송신기의 시간지연 보상 알고리즘 구현)

  • Kim, Min-Soo;Lee, Kun-Joon;Rhee, Young-Chul
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
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    • v.26 no.9
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    • pp.790-797
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    • 2015
  • In this paper, We made the microwave polar transmitter based on the software to analyze the synchronization status between the phase signal and the amplitude signal of polar transmitter, and analyzed the result. In order to solve the time delay mismatch problem, we applied simplified compensation algorithm and compared the synchronization status between the two paths before and after compensation. Before compensation, the value of time delay mismatch was the maximum of 97 nsec at 9.3 GHz with the occupied bandwidth of 12 MHz, but after applying the compensation algorithm, the signals between the two paths were synchronized, and we identified the occupied bandwidth could recover to the previous 3.7 MHz.

A Design of a Diredt Digital Frequency Syntheszer with an Array Type CORDIC Pipeline (파이프라인형 CORDIC를 이용한 직접 디지털 주파수 합성기 설계)

  • 남현숙;김대용;유영갑
    • Journal of the Korean Institute of Telematics and Electronics D
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    • v.36D no.5
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    • pp.36-43
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    • 1999
  • A new design of a Direct Digital Frequency Synthesizer(DDFS) is presented, where a pipelined Coordinate Rotate Digital Computer(CORDIC) circuit is employed to calculate amplitude values of all the phase angles of sinusoidal waveforms produced. a near-optimal number of pipeline stages is determined based on an error analysis of calculated amplitude values in terms of the number of bits. The DDFS was implemented using a field programmable gate array, yielding a stable operating frequency of 11.75MHz. The measurement results show higher resolution, faster operating speed and simpler fabrication process, compared to ROM-based counterparts. The CORDIC-based DDFS yields 5 times higher resolution than conventional ROM-based versions.

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Numerical Analysis of Optical Soliton Transmission in Fibers with Periodically Compensated Loss (손실이 주기적으로 보상되는 광섬유에서의 솔리톤 전송에 대한 수치적 분석)

  • 이명우;김란숙;서동선
    • The Journal of Korean Institute of Communications and Information Sciences
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    • v.19 no.7
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    • pp.1191-1202
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    • 1994
  • We numerically investigate a stable propagation regime of soliton pulse trains in fibers with periodically copensated loss by lumped optical amplifiers. When amplification solition pulses is 1.2~1.5 and the minimum soliton separation normalized by the soliton width becomes about 6. In cases of L=50[km], the allowable range of A is 1.5~1.7 under =6. The maximum allowable variation of the loss compensation in each lumped amplifier becomes +-2% of the fiber loss when L=50[km], A=1.6, and =6. Generally, the allowable rages of the soliton amplitude A and amplifier gain are inversely proportional to the amplification period L.

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A Study on the AE Characteristics of the Carbon Fiber Composite Material (탄소섬유 복합재료의 AE 특성에 관한 연구)

  • 옹장우;이영신;심봉식;지용관;주영상
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.13 no.1
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    • pp.105-114
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    • 1989
  • This study was carried out to measure the mechanical properties and the acoustic emission (AE) characteristics of the carbon fiber reinforced composites of several types of the stacking sequence. AE signals were detected during the tensile tests. The number of ringdown counts, total ringdown counts were plotted together with the load-displacement curves. The tensile load-displacement behavior of specimen is compared and discussed based on the measured AE properties in relation to the failure mechanism. With the increase of load, AE signals increased. This showed that failure had being propagated by matrix deformation and cracking, delamination, fiber debonding and breakage. Felicity ratio has been obtained by observation of ;the Kaiser effect according to the variation of load ratio. The reloading tests showed that the felicity ratio decreased obviously when the load ratio or damage increased. These AE characteristics are hopeful to be employed as the criteria to evaluate the failure processes of composites.

DYNAMIC PROPERTIES OF WASTE FILL SUBJECTED TO DYNAMIC COMPACTION (쓰레기 매립지반에서의 진동 동다짐 특성)

  • 송정락
    • Proceedings of the Korean Geotechical Society Conference
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    • 1993.06a
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    • pp.83-116
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    • 1993
  • This article analyzed the dynamic compaction incuced vibration of man made waste landfill. General dynamic properties and compaction-condition-related dynamic properties were analyzed. from the results, it was turned out that the shear modulus G=17496-58320 t/m2, dannpln ratio D=14~58%, dominant frequency f=6-14Hz. Also, it was turned out that the propagation velocitis of low amplitude shear wave and compressive wave were increased as the number of impact increased, the relation between peak particle velocity, and impact distance was wpp=5.08.[D/r E]-1.4, the peak particle velocity was high at the lower part of the waste fill layer and the range of dynamically improved area was about 6-10m.

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A study of Fatigue Crack Growth Behavior and Crack Closure in 5083-O Aluminum Alloy (5083-0 알루미늄合金의 疲勞균열進展 擧動과 균열닫힘에 관한 硏究)

  • 박영조;김정규;김일현
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.10 no.2
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    • pp.208-214
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    • 1986
  • To establish the evaluation of the fatigue crack growth behavior in 5083-O aluminum alloy, constant load-amplitude fatigue crack growth tests were carried out under the small scale yielding conditions. Crack length and closure of this material were measured by the compliance method using a clip-on gage. The main results obtained as follows: The fatigue crack growth rate against stress intensity factor range .DELTA.K exhibits the trilinear form with two transitions at the growth rate 5.5*10$^{-6}$ and 5.5*10$^{-5}$ mm/cycle, in the so-caled Region II. The trilinear form appears still in the plot of growth rate versus effective stress intensity factor range .DELTA. $K_{eff}$. Stress ratio R affects the relationship of crack growth rates versus .DELTA.K but does not affect the reation of crack growth rate versus .DELTA. $K_{eff}$. The experimental results indicate that the effective stress intensity range ratio U depends on the maximum stress intensity factor $K_{max}$, but not on the stress ratio R.o R.R.

Failure detection of composite structures using a fiber Bragg grating sensor (광섬유 브래그 격자 센서를 이용한 복합재 구조물의 파손 검출)

  • 고종인;김천곤;홍창선
    • Composites Research
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    • v.17 no.2
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    • pp.28-33
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    • 2004
  • Failure detection in a cross-ply laminated composite beam under tensile loading were performed using a fiber Bragg grating (FBG) sensor. A Passive Mach-Zehnder interferometric demodulator was proposed to enhance sensitivity and bandwidth. The proposed FBG sensor system without active device such as a phase modulator is very simple in configuration, easy to implement and enables the measurement of high-frequency vibration with low strain amplitude such as impact or failure signal. Failure signals detected by a FBG sensor had offset value corresponding to the strain shift with vibration at a maximum frequency of several hundreds of kilohertz. at the instant of transverse crack propagation in the 90 degree layer of composite beam.

A Study on Fluid Surface Movement Phenomena of Magnetic Fluids in a Container Subjected to a Horizontal Oscillation (수평진동이 있는 용기내 자성유체 액면 동요 현상에 관한 연구)

  • Kim, Dae-Wan;Park, Joung-Woo;Seo, Lee-Soo
    • Journal of the Korean Magnetics Society
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    • v.22 no.5
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    • pp.183-187
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    • 2012
  • In this paper, fluid movement of magnetic fluid which has free surface is investigated in a container subjected to a horizontal oscillation. Here, the vertical magnetic field is applied from the bottom of this container. The experiment is performed on the magnetic fluid in a rectangular and a cylindrical container and the effects of magnetic force exerted on the magnetic fluid are investigated on the resonance frequency and liquid surface displacement. The increase of magnetic field affects on the maximum resonance point and the liquid surface displacement. In result, it changes the amplitude of the surface wave and the period of sloshing fluid movement.