• 제목/요약/키워드: gain coefficient

검색결과 400건 처리시간 0.022초

전력용 HEMT를 이용한 1740~1780MHz 대역의 MMIC 전력증폭기 설계 (Design of MMIC Power Amplifier using Power HEMT at 1740~1780MHz)

  • 윤관기;조희철이진구
    • 대한전자공학회:학술대회논문집
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    • 대한전자공학회 1998년도 추계종합학술대회 논문집
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    • pp.675-678
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    • 1998
  • In this paper, power amplifiers for PCS phone were designed with the GEC Marconi H40 HEMT libray. The 1st stage was carefully designed in order to obtain k〉1 using a parallel resistor, and its S21 gain of 18.3dB and input reflection coefficient of -4dB were obtained. And S21 gain of 18dB and input reflection coefficient of -7dB were obtained from the 2nd stage. Finally, total S21 gain of 38dB, input reflection coefficient of -16dB, power gain of 35.2dB, output power of 28.7dBm and PAE(power added efficiency) of 29% were obtained from the designed MMIC power amplifiers. The chip size is $1.729$\times$0.94\textrm{mm}^2.$

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XeCl 레이저 증폭기의 활성기체 압력에 따른 포화 에너지 밀도와 소신호 이득계수 측정 (Measurements of Saturation Energy Denity and Small Signal Gain Coefficient Dependent on the Active Gas Pressure in XeCl Laser Amplifier)

  • 김규옥;김용평
    • 한국광학회지
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    • 제5권4호
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    • pp.457-460
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    • 1994
  • XeCl 레이저 증폭기의 포화 에너지 밀도와 소신호 이득계수를 활성기체의 압력을 변화시키면서 측정하였다. Xe이 30mb, He이 2000mb일 때, HCl이 34, 52, 73, 92으로 압력이 높아짐에 따라 포화 에너지 밀도는 1.3, 1.45, 2.0, $2.3mJ/\textrm{cm}^2$로 거의 선형적으로 증가하였지만 소신호 이득계수는 6.5, 7.5, 7.0, 7.0%/cm로 거의 변화하지 않았다.

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Diffusion Coefficient of Iron in ZnSe Polycrystals from Metal Phase for mid-IR Gain Medium Application

  • Jeong, Junwoo;Myoung, NoSoung
    • Applied Science and Convergence Technology
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    • 제23권6호
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    • pp.371-375
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    • 2014
  • Diffusion coefficient of Fe in polycrystalline host ZnSe as a mid-IR gain medium has been measured in the annealing temperature ranges of 850 to $950^{\circ}C$. The synthesis of the samples was carried out in quartz ampoule in which the Fe thin film deposited by physical vapor evaporation method on the ZnSe. One can realize that the diffusion coefficient strongly depends on the surface active surfactants through the cleaning process and the substrate temperature during the thin film deposition leading to $2.04{\times}10^{-9}cm^2/s$ for $Fe^{2+}:ZnSe$. The Annealing temperature dependence of the Fe ions diffusion in ZnSe was used to evaluate the activation energy, $E_a$=1.39 eV for diffusion and the pre-exponential factor $D_0$ of $13.5cm^2/s$.

이득-반사계수 관계를 이용한 마이크로파 광대역 증폭기용 유손실 정합회로의 설계 (Design of Lossy Matching Network for Microwave Broadband Amplifier Using the Relationship Between Gain and Reflection Coefficients)

  • 구경헌;이충웅
    • 대한전자공학회논문지
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    • 제26권5호
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    • pp.10-17
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    • 1989
  • 마이크로와 광대역증폭기용 유손실 정합회로를 설계하기 위한 새로운 방법을 제시한다. 이 방법은 트랜지스터를 모델링 없이 측정된 산란계수를 이용하여 표시하며, 유손실 정합회로를 무손실 정합회로 사이에 유손실 직렬 임피던스 또는 병렬 어드미턴스가 삽입된 구조로 생각한다. 증폭기의 이득과 반사계수사이의 선형관계식을 유도하고 이를 이용하여 적절한 이득과 반사계수를 선택하는 법을 제시한다. 증폭기의 이득 및 반사계수와 유손실 정합 소자의 임피던스 사이에는 쌍 일차 변환의 관계가 있으며 일정 이득 원이나 일정 반사계수원을 임피던스 평면 또는 스미스 차트에 그려 적절한 정합 소지값을 선택 할 수 있다. 본 논문에서 제안된 방법이 유용함을 보이기 위하여 증폭기설계 예를 제시하였다.

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연속발진 도파형 이산화탄소 레이저의 이득계수 및 포화출력 측정 (Measurement of Gain Coefficient and Saturation Power of CW Waveguide CO_2$$ Laser)

  • 이승걸;김현태;박대윤
    • 한국광학회지
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    • 제1권2호
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    • pp.162-168
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    • 1990
  • 내경이 2.1mm인 Pyrex 모세관을 사용하여 길이가 150mm인 도파형 이산화탄소 레이저를 제작하였으며, 공진기내에 임의의 손실을 가할 수 있는 ZnSe 손실판을 설치하여 공진기의 내부손실에 따른 출력변화를 여러 방전조건에 대해 측정하였다. 본 실험에 Rigrod 이론을 적용하여 내부손실에 따른 출력변화를 예측했으며 실험치로부터 포화출력 및 불포화 이득계수를 구할 수 있었다. 방전전류와 혼합기체의 유입률이 증가함에 따라 포화출력은 증가하며, 불포화 이득계수는 감소하는 경향을 볼 수 있었다.

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Optimum thickness of GaAs top layer in AlGaAs-based 850 nm VCSELs for 56 Gb/s PAM-4 applications

  • Yu, Shin-Wook;Kim, Sang-Bae
    • ETRI Journal
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    • 제43권5호
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    • pp.923-931
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    • 2021
  • We studied the influence of GaAs top-layer thickness on the small-signal modulation response and 56 Gb/s four-level pulse-amplitude modulation eye quality of 850 nm vertical-cavity surface-emitting lasers (VCSELs). We considered the proportionality of the gain-saturation coefficient to the photon lifetime. The simulation results that employed the transfer-matrix method and laser rate equations led to the conclusion that the proportionality should be considered for proper explanation of the experimental results. From the obtained optical eyes, we could determine an optimum thickness of the GaAs top layer that rendered the best eye quality of VCSEL. We also compared two results: one result with a fixed gain-saturation coefficient and the other that considered the proportionality. The former result with the constant gain-saturation coefficient demonstrated a better eye quality and a wider optimum range of the GaAs top-layer thickness because the resultant higher damping reduced the relaxation oscillation.

지중매설관 열교환장치의 성능분석(I) -연속운전실험에서의 온도특성 및 열교환성능- (Performance Analysis of an Earth Tube Heat Exchanger(I) -Temperature Variation Characteristics and Heat Exchange Performance on the Mode of Continuous Operation)

  • 김영복;백이
    • Journal of Biosystems Engineering
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    • 제21권4호
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    • pp.436-448
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    • 1996
  • An earth tube soil air heat exchange system was designed, installed and operated as a single pass heat exchanger to utilize the geothermal energy as an natural energy source. This study was undertaken to investigate the potential of the heating and cooling, energy gain, heat exchange efficiency and coefficient of performance of the system. The system consisted of 30m in length and 30cm in diameter polyethylene pipes buried 2m deep in soil. Maximum heating and cooling performance were 2.51㎾ and 1.26㎾ at the air mass rate of 21cmm. Energy gain and coefficient of performance were the function of temperature difference between outside air and soil temperature. They were expressed as Q=0.33$ imes$$Delta T_{max}$+0.134(㎾) for energy gain and COP=0.44$ imes$$Delta T_{max}$+0.178 for coefficient of performance with correlation factor of 0.95. The mean of heat exchange efficiencies was 85.6%.

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적분 슬라이딩 모드 제어기를 이용한 출력 궤환 안정화 (Output Feedback Stabilization using Integral Sliding Mode Control)

  • 오승록
    • 대한전기학회논문지:시스템및제어부문D
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    • 제52권3호
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    • pp.142-147
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    • 2003
  • We consider a single-input-single-output nonlinear system which can be represented in a normal form. The nonlinear system has a modeling uncertainties including the input coefficient uncertainty. A high-gain observer is used to estimate the states variables to reject a modeling uncertainty. A globally bounded output feedback integral sliding mode control is proposed to stabilize the closed loop system. The proposed integral sliding mode control can asymptotically stabilize the closed loop system in the presence of input coefficient uncertainty.

창호에 SHGC를 반영한 공동주택의 방위각별 에너지 효율성 평가를 통한 합리적인 창호 계획 방안 연구 (A Study on the optimized Performance Designing of the Window of the Apartment based on the Annual Energy Demand Analysis according to the Azimuth Angle applying the Solar Heat Gain Coefficient of the Window)

  • 이장범
    • 대한건축학회논문집:계획계
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    • 제35권11호
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    • pp.25-34
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    • 2019
  • It is important to design windows in a reasonable way considering the performance characteristics of the elements of the window rather than just to increase the thermal energy performance of the window. In this study, the Heat-transfer Coefficient as insulation performance of the windows and together with the grade of the glass's SHGC (Solar Heat Gain Coefficient) were analyzed to relate to the energy efficiency performance of the building by azimuth angle. Based on this basic study, the Heat-transfer Coefficient of windows and the SHGC rating of glass were applied to the unit plan of apartment building, and the Heating and Cooling Demand were analyzed by azimuth angle. Apartment plan types were divided into 2 types of Non-extension and extension of balcony. The designPH analysis data derived from the variant of the Heat-transfer Coefficient and SHGC, were put into PHPP(Passive House Planning Package) to analyze precisely the energy efficiency(Heating and Cooling Demands) of the building by azimuth angle. In addition, assuming the 'ㅁ' shape layout, energy efficiency performance and potential of PV Panel installation also were analyzed by floors and azimuth angle, reflecting the shading effects by surrounding buildings. As the results of the study, the effect of Heat Gain by SHGC was greater than Heat Loss due to the Heat-transfer Coefficient. So it is more effective to increase SHGC to satisfy the same Heating Demand, and increasing SHGC made possible to design windows with low Heat-transfer Coefficient. It was also revealed that the difference in annual Heating and Cooling Demands between the low, mid and high floor households is significantly high. In addition to it, the installation of PV Panel in the form of a shading canopy over the window reduces the Cooling Load while at the same time producing electricity, and also confirmed that absolute thermal energy efficiency could not be maximized without controlling the thermal bridge and ventilation problems as important heat loss factors.

Performances of Erbium-Doped Fiber Amplifier Using 1530nm-Band Pump for Long Wavelength Multichannel Amplification

  • Choi, Bo-Hun;Chu, Moo-Jung;Park, Hyo-Hoon;Lee, Jong-Hyun
    • ETRI Journal
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    • 제23권1호
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    • pp.1-8
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    • 2001
  • The performance of a long wavelength-band erbium-doped fiber amplifier (L-band EDFA) using 1530nm-band pumping has been studied. A 1530nm-band pump source is built using a tunable light source and two C-band EDFAs in cascaded configuration, which is able to deliver a maximum output power of 23dBm. Gain coefficient and noise figure (NF) of the L-band EDFA are measured for pump wavelengths between 1530nm and 1560nm. The gain coefficient with a 1545nm pump is more than twice as large as with a 1480nm pump. It indicates that the L-band EDFA consumes low power. The noise figure of 1530nm pump is 6.36dB at worst, which is 0.75dB higher than that of 1480nm pumped EDFA. The optimum pump wavelength range to obtain high gain and low NF in the 1530nm band appears to be between 1530nm and 1540nm. Gain spectra as a function of a pump wavelength have bandwidth of more than 10nm so that a broadband pump source can be used as 1530nm-band pump. The L-band EDFA is also tested for WDM signals. Flat Gain bandwidth is 32nm from 1571.5 to 1603.5nm within 1dB excursion at input signal of -10dBm/ch. These results demonstrate that 1530nm-band pump can be used as a new efficient pump source for L-band EDFAs.

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