• 한국정보통신학회논문지
• /
• 제7권3호
• /
• pp.437-447
• /
• 2003

Circulant Matrix Factorization (CMF)는 covariance 행렬의 spectral factorization된 결과를 얻을 수 있다. 우리는 얻어진 결과를 가지고 일반적으로 잘 알려진 방법인 Schur algorithm을 이용하여 finite impulse response(FIR)와 infinite impulse response (IIR) lattice 필터를 설계하는 방법을 제안하였다. CMF는 기존에 많이 사용되는 root finding을 사용하지 않고 covariance polynomial로부터 minimum phase 특성을 가지는 polynomial을 얻는데 유용한 방법이다. 그리고 Schur algorithm은 toeplitz matrix를 빠르게 Cholesky factorization하기 위한 방법으로 이 방법을 이용하면 FIR/IIR lattice 필터의 계수를 쉽게 찾아낼 수 있다. 본 논문에서는 이러한 방법들을 이용하여 FIR과 IIR lattice 필터의 설계의 계산적인 예제를 제시했으며, 제안된 방법과 다른 기존에 제시되었던 방법 (polynomial root finding과 cepstral deconvolution)들과 성능을 비교 평가하였다.

• 대한전기학회논문지
• /
• 제37권11호
• /
• pp.720-726
• /
• 1988

본 논문에서는 적응 알고리즘을 마이크로컴퓨터에 의하여 실현하고 그것을 열교환기에 응용하였으며 실험결과 검토하엿다. 실험을 위하여 제작된 열교환기는 비최소위상 시스템으로 판정되었으며 직접 수확적으로 모형화하는 데에는 많은 어려움이 있었다. 따라서 PID제어방법 등 다른 고전적인 제어 방법들을 사용하려면 실험을 통한 많은 시행착오를 거쳐 시스템의 파라미터 값들을 결정해야하고 시스템의 파라미터 값들이 변화할 경우 좋은 성능을 보장하지 못한다. 이런 어려움을 극복하고 제어기의 성능을 향상시키기 위해 비최소상위 시스템에 적용할 수 있는 두 가지 적응제어 방식을 선택하여 열교환기에 응용하여 보았다. 아울러 적응제어 방식의 성능을 종래의 PID제어기에 의한 결과와 비교하여 보았다.이러한 연구의 최종적인 목적은 산업플랜트에 손쉽게 적용될 수 있는 제어기를 마이크로프로세서를 사용하여 구성하는 것이다.

• 대한조선학회논문집
• /
• 제45권5호
• /
• pp.469-476
• /
• 2008

In this paper, it is shown that an input-output (I/O) feedback linearized controller can be designed rationally by utilizing the time-scale properties of heave and pitch for an underwater vehicle. It is assumed that the dynamics of the vehicle is restricted to the vertical plane. An output-feedback control is designed, which stabilizes steady cruising paths. It is shown that the vehicle dynamics with acceleration as output becomes minimum phase. The dynamics can be transformed into a reduced system through a kind of partial linearization and singular perturbation technique. The reduced system is not only minimum phase but also exactly I/O linearizable via feedback. The I/O dynamic characteristics of the heave and pitch modes can be made linear and decoupled. Furthermore it becomes independent of cruising condition such as vehicle velocity. This study may help for designing autopilot systems for underwater vehicles.

• 소성∙가공
• /
• 제18권6호
• /
• pp.500-507
• /
• 2009

Tensile deformation behavior with different strain rate was investigated. $Zr_{56.2}Ti_{13.8}Nb_{5.0}Cu_{6.9}Ni_{5.6}Be_{12.5}$(bulk metallic glass alloy possessed crystal phase which was called $\beta$-phase of dendrite shape, mean size of $20{\sim}30{\mu}m$ and occupied 25% of the total volume) was used in this study. Maximum tensile strength was obtained as 1.74GPa at strain rate $10^2s^{-1}$ and minimum strength was found to be 1.6GPa at $10^{-1}s^{-1}$. And then, maximum plastic deformation occurred at the strain rate of $5{\times}10^{-2}s^{-1}$ and represented 1.75%, though minimum plastic deformation showed 0%. In the specific range of strain rate, relatively higher plastic deformation and lower ultimate tensile strength were found with lots of shear bands. The fractographical observation after tensile test indicated that vein like pattern on the fracture surface was well developed especially in the above range of strain rate.

• 한국소성가공학회:학술대회논문집
• /
• 한국소성가공학회 2009년도 춘계학술대회 논문집
• /
• pp.353-354
• /
• 2009

Tensile deformation behavior with different strain rate was investigated. $Zr_{56.2}Ti_{13.8}Nb_{5.0}Cu_{6.9}Ni_{5.6}Be_{12.5}$ (bulk metallic glass alloy possessed crystal phase which was called $\beta$-phase of dendrite shape, mean size of $20{\sim}30{\mu}m$ and occupied 25% of the total volume) was used in this study. Maximum tensile strength was obtained as 1.74Gpa at strain rate of $10^2/s$ and minimum strength was found to be 1.6GPa at $10^{-1}/s$. And then, maximum plastic deformation occurred at the strain rate of $5{\times}10^{-2}/s$ and represented 1.75%, though minimum plastic deformation showed 0%. In the specific range of strain rate, relatively higher plastic deformation and lower ultimate tensile strength were found with lots of shear bands. The fractographical observation after tensile test indicated that vein like pattern on the fracture surface was well developed especially in the above range of strain rate.

• 전자공학회논문지SC
• /
• 제49권4호
• /
• pp.78-89
• /
• 2012

SR 모터의 발생토크는 비선형성이 심해서 토크리플을 최소화하는 기준전류명령을 결정하는 것이 매우 어렵다. 본 논문에서는 반복학습제어 방법을 이용하여 계산적으로 효율적인 SR 모터의 토크리플을 최소화하는 기준전류명령을 구하는 방법을 제안한다. 토크리플을 최소화하는 기준전류명령은 2차원 순람표(look-up table) 형태로 결정된다. 제안된 반복학습제어 방법은 토크모델을 이용하지 않기 때문에 모델오차에 대한 영향이 없고 정밀도가 높으며 계산적으로도 간단한다. 컴퓨터 시뮬레이션을 통해 제안된 방법이 효과적으로 동작됨을 입증한다.

• 한국해양공학회:학술대회논문집
• /
• 한국해양공학회 2002년도 추계학술대회 논문집
• /
• pp.68-72
• /
• 2002

Localization with array sensors has been applied for not only military but also non-military purposes. The identification of submarines and fish finding are those examples. Nowadays the demand for noise identification is increasing to characterize noise sources and improve acoustic performance of underwater acoustic equipment. For that reason KRISO/KORDI recently constructed an anechoic basin which bus reflection only at the free surface. This paper suggests a noise identification methods using MUSIC algorithm in such an acoustic field. For comparison phase delay sum and minimum valiance methods are also described. At first basic principles are described. A several numerical simulations are also performed. The results say that reflection effect many cause a new non-real source although good estimation is obtained under no reflection conditions.

• 한국조명전기설비학회지:조명전기설비
• /
• 제7권4호
• /
• pp.51-58
• /
• 1993

리니어 직류 모터의 고속, 고정도 위치제어에 대하여 포물선형 스위칭 함수에 최단시간 제어 방식을 제안하였다.제안한 방식은 간단한 구성으로 최단시간 제어를 실현한기 위하여 뱅-뱅 제어의 절환을 위상면에 설정한 포물선형 스위칭 함수상에서 행하는 것이다. 그러나 시스템의 모델링 오차등에 의하여 슬라이딩 모드를 발생시키므로 최단시간 제어를 위해 반복실험에 의하여 1회의 절환에 의한 뱅-뱅 제어를 실현하였다. 그 후 궤환 제어에 의하여 리니어 직류모터를 목표점에 정지시켰다.

• 대한전기학회:학술대회논문집
• /
• 대한전기학회 2005년도 추계학술대회 논문집 전기기기 및 에너지변환시스템부문
• /
• pp.26-28
• /
• 2005

Induction generator is the most common generator in wind energy systems because of its simplicity, ruggedness, little maintenance, price and etc. But the main drawbacks in induction generator is its need of reactive power means to build up the terminal voltage. This drawback is not an obstacle today where PWM inverters can accurately supplies the induction generator with its need from reactive power. For a insurance of three-phase induction generator requires capacitive reactance of the terminal. Most of previous work uses numerical iterative method to determine this minimum capacitor. But the numerical iteration takes long time and divergence may be occurs. In this paper is presented the design methods of the minimum self-excited capacitor required for induction generator operation. And a new formula from the equivalent circuit for stable generation operation of self-excited induction generator calculates the proper capacity to obtain the terminal voltage of the load stage. The validity of proposed design methods is confirmed by experimental and computed results.

• Journal of Mechanical Science and Technology
• /
• 제20권2호
• /
• pp.262-270
• /
• 2006

Direct numerical simulations (DNS) of turbulent channel flows up to $Re_{\tau}=1270$ are performed to investigate an elliptic feature and strain rate field on cross sections of coherent fine scale eddies (CFSEs) in wall turbulence. From DNS results, the CFSEs are educed and the strain rate field around the eddy is analyzed statistically. The principal strain rates (i.e. eigenvalues of the strain rate tensor) at the CFSE centers are scaled by the Kolmogorov length $\eta$ and velocity $U_k$. The most expected maximum (stretching) and minimum (compressing) eigenvalues at the CFSE centers are independent of the Reynolds number in each $y^+$ region (i. e. near-wall, logarithmic and wake regions). The elliptic feature of the CFSE is observed in the distribution of phase-averaged azimuthal velocity on a plane perpendicular to the rotating axis of the CFSE $(\omega_c)$. Except near the wall, phase-averaged maximum $(\gamma^{\ast}/\gamma_c^{\ast})$ and minimum $(\alpha^{\ast}/\alpha_c^{\ast})$ an eigenvalues show maxima on the major axis around the CFSE and minima on the minor axis near the CFSE center. This results in high energy dissipation rate around the CFSE.