• Title/Summary/Keyword: oscillation frequency

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An Antenna-Integrated Oscillator Design Providing Convenient Control over the Operating Frequency and Output Power (동작주파수 및 출력파워 조절이 용이한 신호생성용 안테나 설계)

  • Lee, Dong-Ho;Lee, Jong-In;Kim, Mun-Il
    • Journal of Satellite, Information and Communications
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    • v.1 no.1
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    • pp.54-58
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    • 2006
  • A new design for easily controlling operating frequency of an antenna-integrated planar oscillator is introduced. The oscillator circuit of a broadband negative-resistance active part and a passive load including a patch antenna. The patch resonance is used for determining the oscillation frequency. This design reduces the possibility of mismatch between antenna radiation and oscillation frequencies. To achieve optimum output power, load-pull simulation for the negative-resistance circuit is used. The load-pull simulation shows the feed point and the delay of feed line can affect the oscillation power. Two negative-resistance circuits capable of supporting oscillation over full C-band and X-band are fabricated. The oscillation frequency, output power and phase noise for different patch antennas are measured.

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NUMERICAL FLOW VISUALIZATION ANALYSIS AROUND AN OSCILLATING SQUARE CYLINDER (정사각봉의 진동에 의한 유동해석)

  • Ju, M.K.;Ajith Kumar, R.;Sohn, C.H.;Gowda, R.H.L.
    • 한국전산유체공학회:학술대회논문집
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    • 2007.10a
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    • pp.115-119
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    • 2007
  • In this paper, a flow visualization analysis has been carried out on an oscillating square section cylinder, numerically, using a commercially available code CFD-ACE. In this study, the square cylinder is forced to oscillate at different frequencies of excitation, viz., fe/fo=0.5, 1.0 and 2.0 (where, fe is the excitation frequency provided to the cylinder and fo is the natural vortex shedding frequency from the stationary cylinder at a particular Reynolds number (=5200). In all the cases, the peak-to-peak amplitude of oscillation is kept at 32% of the side dimension of the square cylinder. These studies are conducted to understand the influence of frequency of oscillation on the flow field features around the cylinder, particularly the mode of vortex shedding. Results indicate that, the flow field around a square cylinder is very much influenced by the excitation frequency, in particular the vortex shedding mode. It is also found that, the vortex street parameters are significantly influence by the oscillation frequency. Comparison with earlier reported experimental studies has also been attempted in this paper. In appears that, such a numerical exercise (as performed in this paper) is first of its kind. It is believed that, these studies would enable one to understand the mechanisms underlying the flow-induced vibrations of a square section cylinder.

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Nonlinear Behaviors of a Gas-filled Bubble Oscillator with Large Amplitude of Excitation (큰 압력 진폭에 의해 구동되는 기포진동체의 비선형 거동 특성)

  • 김동혁
    • Journal of Advanced Marine Engineering and Technology
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    • v.26 no.1
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    • pp.116-124
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    • 2002
  • The bubble model by Keller and Prosperetti is adapted to solve the nonlinear oscillation of a gas bubble. This formulation leads to accurate results since it introduces the energy equation instead of the polytropic assumption for the bubble interior. The numerical method used in this study is stable enough to handle large amplitude of bubble oscillation. The numerical results show some interesting nonlinear phenomena fur the bubble oscillator. The excitation changes the natural frequency of the bubble and makes some harmonic resonances at $f/f_0=1/2, 1/3$ and so on. The natural frequency of a bubble oscillator decreases compared with the linear case result, which means that the nonlinear bubble oscillation system is a "softening"system. In addition, the frequency response curve jumps up or down at a certain frequency. It is also found that there exist multi-valued regions in the frequency response curve depending on the initial conditions of bubble. The dependency of the bubble motion on the initial condition can generate extremely large pressure and temperature which might be the cause of the acoustic cavitation and the sonoluminescence.inescence.

Characteristics of Flow p ast an Oscillating Sphere (진동하는 구를 지 나는 유동의 특성)

  • Lee, Dae-Sung;Yoon, Hyun-Sik;Ha, Man-Yeong
    • 한국전산유체공학회:학술대회논문집
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    • 2008.03b
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    • pp.284-287
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    • 2008
  • Flow over a sphere under forced oscillation at Re=300 is simulated for various frequency ratios which are defined as excitation frequency over natural frequency of stationary sphere. The results of oscillating sphere are compared with those of stationary sphere and an oscillating cylinder. Detailed vortical structures, hydrodynamic forces and frequencies of the wake are prescribed as a function of frequency ratio. For oscillating sphere, planar symmetry of the wake is kept and two nearly symmetric hair pin vortices are induced by oscillation for one period of oscillation when the frequency ratio is bigger than 0.5. Modulation phenomenon which can be found in an oscillating cylinder were not seen for an oscillating sphere.

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Frequency Response Compensation Technique for Capacitive Microresonator (용량형 마이크로 공진기의 주파수 응답 보상 기법)

  • Seo, Jin-Deok;Lim, Kyo-Muk;Ko, Hyoung-Ho
    • Journal of Sensor Science and Technology
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    • v.21 no.3
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    • pp.235-239
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    • 2012
  • This paper presents frequency response compensation technique, and a self-oscillation circuit for capacitive microresonator with the compensation technique using programmable capacitor array, to compensate for the frequency response distorted by parasitic capacitances, and to obtain stable oscillation condition. The parasitic capacitances between the actuation input port and capacitive output port distort the frequency response of the microresonator. The distorted non-ideal frequency response can be compensated using two programmable capacitor arrays, which are connected between anti-phased actuation input port and capacitive output port. The simulation model includes the whole microresonator system, which consists of mechanical structure, transimpedance amplifier with automatic gain control, actuation driver and compensation circuit. The compensation operation and oscillation output of the system is verified with the simulation results.

Numerical Simulations for Combustion and NOx Emission Characteristics in Oscillating Combustion Burner (수치해석을 이용한 맥동연소과정 및 NOx 배출특성 해석)

  • Kim, Hoo-Joong;Cho, Han-Chang
    • Journal of the Korean Society of Combustion
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    • v.14 no.3
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    • pp.37-44
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    • 2009
  • An experimental study was conducted to reduce NOx emission in RT(radiant tube)burner by using oscillating combustion processes in RIST. A solenoid valve gives the various oscillating conditions, such as oscillation frequency, duty ratio of fuel flow. In this study, we used commercial software, CFD-ACE+ to predict combustion and NOx emission characteristics for various experimental oscillation conditions. The effect of oscillation frequency and duty ratio on NOx emission will be discussed in terms of flow field, temperature and equivalence ratio distributions in detail.

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A Study of High Power Microwave Output by K-band Waveguide (K-band 도파관을 이용한 대전력 마이크로파 출력장치 연구)

  • Kim, Won-Sop
    • The Transactions of the Korean Institute of Electrical Engineers P
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    • v.58 no.4
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    • pp.588-591
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    • 2009
  • We had experimental studies of microwave output generator. We experimented with a corrugate-shped K-band slow wave guide in the backward wave oscillator. It generated output 표 interaction between electron beam's generation and magnetic field. We estimated oscillation frequency at 24GHz by changing propagation velocity and group velocity. We identified movement by second harmonic of Cherencov interaction and slow cyclotron mode. In our study we achieved oscillation stabilization, generation of long pulse, improvement of oscillation efficiency and output.

Development and Application High Power Electron Beam (대 전력 전자빔의 개발과 응용)

  • Kim, Won-Sop;Kim, Jeong-Man
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2007.11a
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    • pp.480-480
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    • 2007
  • A large diameter plasma filled backward wave oscillator is investigated experimentally. The parameters of slow wave structure are chosen so that the oscillation frequency is high beam energy. Plasma is produced by the beam and it has favorable effects on beam propagation and Cerenkov oscillation.

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Characterization of Combustion Oscillation and Reduction of Abnormal Oscillation in a Power Generation Gas Turbine (발전용 가스터빈에서 발생하는 연소진동 특성 및 이상연소진동의 저감)

  • Seo, Seok-Bin;Ahn, Dal-Hong;Chung, Jae-Hwa
    • Proceedings of the KSME Conference
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    • 2004.11a
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    • pp.1682-1685
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    • 2004
  • Gas Turbine combustors for power plant can be reduced NOx emissions using lean premixed combustion technology. But the combustors are likely to occur combustion oscillations which damage operation reliability and mechanical life of the gas turbines. In this paper, characterizations of oscillation in a gas turbine combustor for power plant are presented. Combustion dynamics occur $1{\sim}1.5$ psi in amplitude with low frequency less than 140Hz during normal operation. An abnormal high level dynamics, 2.0 psi amplitude occur at 125 Hz frequency. Abnormal combustion oscillation is reduced by modulation of fuel supply valve control schedule.

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Characteristics of thermoacoustic oscillation in ducted flame burner (관형 연소기의 열 음향학적 특성에 관한 실험적 연구)

  • 조상연;이수갑
    • Journal of KSNVE
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    • v.7 no.6
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    • pp.985-991
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    • 1997
  • Combustion instability is a common phenomenon in a ducted flame burner and is known as accompanying low frequency oscillation. This is due to the interaction between unsteady heat release rate and sound pressure field, that is, thermoacoustic feedback. In Rayleigh criterion, combustion instability is triggered when the heat addition is in phase with acoustic oscillation. A Rijke type burner with a pre-mixed flame is built for investigating the effect of Reynolds number and equivalence ratio on thermoacoustic oscillation. The results suggest that the frequency of max, oscillation is dependent on Reynolds number and equivalence ratio whereas its magnitude is not a strong function of these two parameters.

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