• 제목/요약/키워드: Pitch angle

검색결과 698건 처리시간 0.023초

Simulink에서 계통연계 풍력발전시스템의 전압변동 시뮬레이션 (Simulation for Voltage Variations of a Grid-connected Wind Turbine Generation System by Simulink)

  • 안덕근;노경수
    • 대한전기학회논문지:전력기술부문A
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    • 제53권11호
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    • pp.589-595
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    • 2004
  • This paper presents a modeling and simulation of a grid-connected wind turbine generation system with respect to wind variations, starting of large induction motor and three-phase fault in the system, and investigates voltage variations of the system for disturbances. It describes the modeling of the wind turbine system including the drive train model, induction generator model, and grid-interface model on MATLAB/Simulink. The simulation results show the variation of the generator torque, the generator rotor speed, the pitch angle, terminal voltage, system voltage, fault current, and real/reactive power output, etc. Case studies demonstrate that the pitch angle control is carried out to achieve maximum power extraction for wind speed variations, starting of a large induction motor causes a voltage sag due to a large starting current, and a fault on the system influences on the output of the wind turbine generator.

An Algorithm for Robust Noninteracting Control of Ship Propulsion System

  • Kim, Young-Bok
    • Journal of Mechanical Science and Technology
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    • 제14권4호
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    • pp.393-400
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    • 2000
  • In this paper, a new algorithm for noninteracting control system design is proposed and applied to ship propulsion system control. For example, if a ship diesel engine is operated by consolidated control with controllable pitch propeller (CPP), the minimum fuel consumption is achieved satisfying the demanded ship speed. For this, it is necessary that the ship is operated on the ideal operating line which satisfies the minimum fuel consumption, and the both pitch angle of CPP and throttle valve angle are controlled simultaneously. In this context of view, this paper gives a controller design method for a ship propulsion system with CPP based on noninteracting control theory. Where, linear matrix inequality (LMI) approach is introduced for the control system design to satisfy the given $H_{\infty}$, constraint in the presence of physical parameter perturbation and disturbance input. To the end, the validity and applicability of this approach are illustrated by the simulation in the all operating ranges.

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2차원 초음속 추력편향노즐을 이용한 쉴리렌 가시화 실험연구 (Schlieren Visualization of the Thrust Vector Flowfield in a Supersonic Two-Dimensional Nozzle)

  • 정한진;최성만;장현수
    • 한국가시화정보학회지
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    • 제9권3호
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    • pp.30-37
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    • 2011
  • The thrust vectoring concept has been used for use in new advanced supersonic aircraft. This study presents the performance characteristics of the thrust vectoring nozzle by visualizing the shock behaviors with Schlieren method. The scaled models were designed and manufactured to see the shock behaviors of the various airflow condition. Also we executed experimental tests to see the geometrical effects of the thrust vector nozzle by changing pitch angle and length of pitch flaps. From this study we could understand the supersonic flow characteristics of the thrust vector nozzle. The total thrust of thrust vector nozzle is diminished by increasing the flap angle. But there is an optimum flap length ratio for attaining the highest thrust level and proper pitch effect.

2-D 가변 추력편향 노즐 설계 및 유동해석 (Numerical Analysis and Design of the 2-D Variable Convergent-Divergent Thrust Vectoring Nozzle)

  • 김윤희;최성만;장현수
    • 한국추진공학회:학술대회논문집
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    • 한국추진공학회 2010년도 제35회 추계학술대회논문집
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    • pp.170-176
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    • 2010
  • 초음속 항공기에서 피치 편향이 가능한 추력편향 노즐에 대한 해석적 연구를 수행하였다. 초음속 항공기의 비행조건에서 터보팬 엔진의 기본성능을 도출하였으며, 이를 바탕으로 이차원형태의 피치 편향이 가능한 추력편향 노즐을 설계하였다. 상용 해석프로그램인 Fluent 를 이용하여 축소확대 노즐에 대한 기본 유동특성을 파악하고, 피치 추력편향시의 유동특성과 비교하였다.

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학생들이 사용한 세 종류 NiTi file systems의 screw-in effect 비교 (Comparison of screw-in effect of three NiTi file systems used by undergraduates)

  • 오승희;박정길;허복;김현철
    • Restorative Dentistry and Endodontics
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    • 제31권6호
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    • pp.477-484
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    • 2006
  • 학생들이 사용한 세 가지 NiTi file systems (ProFile$^{(R)}$, Hero Shaper$^{(R)}$, K3$^{TM}$)을 사용하여 성형한 모형 근관의 apical terminus width를 비교하여 flute angle 및 pitch 혹은 radial land가 screw-in effect에 미치는 효과를 알아보고자 하였다. NiTi file의 사용 경험이 없는 부산대학교 치과대학 4학년 학생 50명이 세 종류의 NiTi file systems- Pro File$^{(R)}$ (Dentsply Maillefer, Ballaigues, Switzerland), K3$^{TM}$ (SybronEndo, Glendora, France), Hero Shaper$^{\circledR}$(Micromega, Besancon, France)-을 사용하여 각 system으로 하나의 근관씩, 모두 150 개의 레진 블락 근관모형 (Endo Training Bloc; Dentsply Maillefer, Ballaigues, Switzerland)을 16 : 1 감속 handpiece를 장착한 electric motor (Tecnika ATR, Pistola, Italy)를 사용하여 300 rpm의 속도에서 torque는 30 (Tecnikamotor setting value)으로 성형하였다. 스캐너로 근관 성형 전 후 이미지를 채득하여 중첩한 후 근단부의 최종 폭경을 측정하였다. 통계분석은 one-way ANOVA와 95% 신뢰도의 Scheffe's multiple range test로 사후 검증하였다. ProFile$^{(R)}$의 근관 성형 후 근단부의 폭이 Hero Shaper$^{(R)}$ and K3$^{TM}$에 비해 통계학적으로 유의하게 작았다. 본 연구의 결과에서 근단부의 과도한 확대가 variable pitch와 helical angle를 가진active file에 비해 con-stant pitch와 helical angle을 가짐에도 불구하고 radial land를 가진passive file에서 적게 나타났다. 이 결과로 추정해 볼 때, variable pitch와 helical angle보다는 근본적으로 radial land가 screw-in effect의 예방에 더 큰 역할을 하는 것으로 추정될 수 있다 따라서 NiTi file의 사용 경험이 없는 초심자의 경우 근단부 폭경의 유지능력이 좋은 ProFile$^{(R)}$의 사용이 추천된다.

500W 급 다리우스형 풍력발전기의 최적설계를 위한 수치적 연구 (Numerical study to Determine Optimal Design of 500W Darrieus-type Vertical Axis Wind Turbine)

  • 이영태;임희창
    • 대한기계학회논문집B
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    • 제39권8호
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    • pp.693-702
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    • 2015
  • 본 논문은 NACA 익형의 블레이드를 가지는 다리우스 수직축 풍력발전기(VAWT)의 성능특성에 대한 연구이다. 다양한 설계변수를 이용한 다리우스 VAWT 의 최적 형상을 예측하기 위해서 블레이드 근처에서 나타나는 공력특성 및 박리유동, 유동과 블레이드 간의 상호작용, 이로 인해 유도되는 토크 및 출력특성 등을 분석하였다. 블레이드의 최적 형상 설계 및 주변 유동과의 상호작용 특성을 보기 위하여 다양한 인자들 (즉, 코드길이, 로터직경, 피치각, 블레이드의 두께비 및 비틀림각 등)을 고려하였다. 본 연구에서 연구결과로는 TSR 가 낮은 영역에서는 솔리디티가 큰 로터가 높은 출력계수를 가지는 반면, TSR 이 높은 영역에서는 솔리디티가 작은 로터가 높은 출력계수를 가진다. 블레이드의 익형이 안쪽으로 향하는 피치각은 $-2^{\circ}$와 비틀림각이 $0^{\circ}$ 일 때, 다리우스형 VAWT 가 최대 출력을 발생하였다.

막냉각 홀의 측면 방향 분사각, 확장각 및 주기가 막냉각 효율에 미치는 영향 (Effects of Compound Angle, Diffuser Angle, and Hole Pitch on Film-cooling Effectiveness)

  • 김선민;이기돈;김광용
    • 대한기계학회논문집B
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    • 제35권9호
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    • pp.903-913
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    • 2011
  • 본 연구에서는 가스터빈 블레이드의 냉각을 위해 사용되는 막냉각 홀을 대상으로 다양한 형상변수들이 막냉각 효율에 미치는 영향을 평가하기 위한 수치적 연구를 수행하였다. 삼차원 압축성 Reynolds-averaged Navier-Stokes 해석을 수행하였으며, 난류모델로는 shear stress transport 모델이 사용되었다. 해석을 통해 홀의 형상, 측면 방향 분사각, 홀의 주기 및 분사율이 막냉각 효율에 미치는 영향이 평가되었다. 해석결과, 원통형홀의 경우 측면 방향 분사각이 존재할 때 월등히 향상된 막냉각 효율을 보여주었으며, 홴형상 홀의 경우 측면 방향 분사각이 $20^{\circ}{\sim}30^{\circ}$일 때 가장 높은 막냉각 효율을 보여주었다. 또한 홀의 주기의 변화에 따른 성능평가 결과 높은 분사율일 때가 낮은 분사율의 경우보다 홀의 주기에 의존하는 경향을 보였다.

GPS/IMU/OBD 융합기반 ACF/IMMKF를 이용한 차량 Pitch 추정 알고리즘 (Vehicular Pitch Estimation Algorithm with ACF/IMMKF Based on GPS/IMU/OBD Data Fusion)

  • 김주원;이명수;이상선
    • 한국통신학회논문지
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    • 제40권9호
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    • pp.1837-1845
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    • 2015
  • 도심지환경에서 정확한 차량 위치를 추정하기 위해서는 종방향 속도가 필요하다. 이러한 종방향 속도는 노면경사, 즉 차량의 피치각(Pitch) 산출을 통해서 가능하다. 하지만 단일 센서와 알고리즘을 이용한 피치각 추정에는 정확한 값을 기대할 수 없다. 본 논문에서는 정확한 피치각 추정을 위해 AKF(Adaptive Kalman Filter)와 CF(Complementary Filter)로 구성된 ACF(Adaptive Complementary Filter)를 이용하여 IMU(Inertial Measurement Unit)의 프로세스 노이즈와 측정에러를 주행환경에 맞게 조절하고, 이에 GPS(Global Positioning System)와 OBD(Onboard Equipment) 데이터를 융합한다. 그리고 노면 경사 모델에 따른 필터에 시스템 모델 최적화를 위해 IMMKF(Interactive Multiple Model Kalman Filter)를 사용하여 주행환경에 적합한 최종 피치각을 추정한다.

Computational Study on Unsteady Mechanism of Spinning Detonations

  • Matsuo, Akiko;Sugiyama, Yuta
    • 한국전산유체공학회:학술대회논문집
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    • 한국전산유체공학회 2008년도 학술대회
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    • pp.367-373
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    • 2008
  • Spinning detonations propagating in a circular tube were numerically investigated with a one-step irreversible reaction model governed by Arrhenius kinetics. Activation energy is used as parameter as 10, 20, 27 and 35, and the specific heat ratio and the heat release are fixed as 1.2 and 50. The time evolution of the simulation results was utilized to reveal the propagation mechanism of single-headed spinning detonation. The track angle of soot record on the tube wall was numerically reproduced with various levels of activation energy, and the simulated unique angle was the same as that of the previous reports. The maximum pressure histories of the shock front on the tube wall showed stable pitch at Ea=10, periodical unstable pitch at Ea=20 and 27 and unstable pitch consisting of stable, periodical unstable and weak modes at Ea=35, respectively. In the weak mode, there is no Mach leg on the shock front, where the pressure level is much lower than the other modes. The shock front shapes and the pressure profiles on the tube wall clarified the mechanisms of these stable and unstable modes. In the stable pitch at Ea=10, the maximum pressure history on the tube wall remained nearly constant, and the steady single Mach leg on the shock front rotated at a constant speed. The high and low frequency pressure oscillations appeared in the periodical unstable pitch at Ea=20 and 27 of the maximum pressure history. The high frequency was one cycle of a self-induced oscillation by generation and decay in complex Mach interaction due to the variation in intensity of the transverse wave behind the shock front. Eventually, sequential high frequency oscillations formed the low frequency behavior because the frequency behavior was not always the same for each cycle. In unstable pitch at Ea=35, there are stable, periodical unstable and weak modes in one cycle of the low frequency oscillation in the maximum pressure history, and the pressure amplitude of low frequency was much larger than the others. The pressure peak appeared after weak mode, and the stable, periodical unstable and weak modes were sequentially observed with pressure decay. A series of simulations of spinning detonations clarified that the unsteady mechanism behind the shock front depending on the activation energy.

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Computational Study on Unsteady Mechanism of Spinning Detonations

  • Matsuo, Akiko;Sugiyama, Yuta
    • 한국전산유체공학회:학술대회논문집
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    • 한국전산유체공학회 2008년 추계학술대회논문집
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    • pp.367-373
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    • 2008
  • Spinning detonations propagating in a circular tube were numerically investigated with a one-step irreversible reaction model governed by Arrhenius kinetics. Activation energy is used as parameter as 10, 20, 27 and 35, and the specific heat ratio and the heat release are fixed as 1.2 and 50. The time evolution of the simulation results was utilized to reveal the propagation mechanism of single-headed spinning detonation. The track angle of soot record on the tube wall was numerically reproduced with various levels of activation energy, and the simulated unique angle was the same as that of the previous reports. The maximum pressure histories of the shock front on the tube wall showed stable pitch at Ea=10, periodical unstable pitch at Ea=20 and 27 and unstable pitch consisting of stable, periodical unstable and weak modes at Ea=35, respectively. In the weak mode, there is no Mach leg on the shock front, where the pressure level is much lower than the other modes. The shock front shapes and the pressure profiles on the tube wall clarified the mechanisms of these stable and unstable modes. In the stable pitch at Ea=10, the maximum pressure history on the tube wall remained nearly constant, and the steady single Mach leg on the shock front rotated at a constant speed. The high and low frequency pressure oscillations appeared in the periodical unstable pitch at Ea=20 and 27 of the maximum pressure history. The high frequency was one cycle of a self-induced oscillation by generation and decay in complex Mach interaction due to the variation in intensity of the transverse wave behind the shock front. Eventually, sequential high frequency oscillations formed the low frequency behavior because the frequency behavior was not always the same for each cycle. In unstable pitch at Ea=35, there are stable, periodical unstable and weak modes in one cycle of the low frequency oscillation in the maximum pressure history, and the pressure amplitude of low frequency was much larger than the others. The pressure peak appeared after weak mode, and the stable, periodical unstable and weak modes were sequentially observed with pressure decay. A series of simulations of spinning detonations clarified that the unsteady mechanism behind the shock front depending on the activation energy.

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