• 한국전자통신학회논문지
• /
• 제9권8호
• /
• pp.853-859
• /
• 2014

본 연구에서는 핀치오프 된 cold-FET에서 게이트와 드레인 패드를 디임베딩하여 얻어지는 Z-파라미터와 게이트와 드레인 패드 커패시턴스를 제외한 핀치오프 된 cold-FET의 나머지 파라미터에 의해 모델링되는 Z-파라미터 사이의 잔차 오차를 최소화함으로써 HEMT의 모든 외인성 파라미터를 추출하는 기법을 제시한다. 제시된 기법을 사용하면 게이트와 드레인 모조패드의 추가적 제작 없이 게이트와 드레인 패드의 커패시턴스 값뿐 아니라 나머지 외인성 파라미터 값 모두를 성공적으로 추출할 수 있다.

• 대한수학회보
• /
• 제52권6호
• /
• pp.1937-1943
• /
• 2015

For $1{\leq}{\alpha}<2$, let $\mathcal{F}({\alpha})$ denote the class of locally univalent normalized analytic functions $f(z)=z+{\Sigma}_{n=2}^{\infty}{a_nz^n}$ in the unit disk ${\mathbb{D}}=\{z{\in}{\mathbb{C}}:{\left|z\right|}<1\}$ satisfying the condition $Re\(1+{\frac{zf^{{\prime}{\prime}}(z)}{f^{\prime}(z)}}\)>{\frac{{\alpha}}{2}}-1$. In the present paper, we shall obtain the sharp upper bound for Fekete-$Szeg{\ddot{o}}$ functional $|a_3-{\lambda}a_2^2|$ for the complex parameter ${\lambda}$.

• 한국정밀공학회:학술대회논문집
• /
• 한국정밀공학회 2011년도 춘계학술대회 논문집
• /
• pp.891-892
• /
• 2011

• 전자공학회논문지SC
• /
• 제46권4호
• /
• pp.64-69
• /
• 2009

본 논문은 모바일 디스플레이모듈의 signal integrity와 power integrity의 시뮬레이션 방법에 관한 것이다. 본 제안 방법은 커넥터, FPCB, 드라이버IC를 포함하는 회로모듈 해석에 사용할 수 있다. 최근에 모바일 디스플레이 업계의 시리얼 인터커넥션기술에 대한 필요성 대두로 시스템오동작 방지 및 전자기파 발생을 억제하기 위해 신호선과 전원전압에 대한 섬세한 컨트롤이 필요하다. S파라미터와 Z파라미터 분석으로 주파수 도메인과 시간 도메인에서의 상관관계를 분석한다. 멀티포트 매크로를 이용하여 시간 도메인에서 sigh integrity를 power integrity에 함께 분석할 수 있다.

• 터널과지하공간
• /
• 제21권6호
• /
• pp.494-507
• /
• 2011

암석의 절리면 거칠기 평가에 있어서 최적의 거칠기 파라미터를 선택하는 것은 중요한 문제이다. 선행연구에서 절리면 거칠기의 평가는 여러 가지 통계적 방법에 의해 2차원적으로 이루어져왔다. 본 연구에서는 Barton과 Choubey(1977)가 제안한 표준 프로파일(JRC)을 3차원 표면으로 확장하고, 표면평균기울기를 적용하여 절리면 거칠기를 정량화 하였다. 그리고 $Z_2$, Ai파라미터와 비교하여 표면평균기울기를 이용한 거칠기 정량화의 타당성을 검증하였으며, 복제시료를 이용한 절리면 전단시험을 통하여 전단강도와 표면평균기울기의 관계를 분석하였다.

• 한국음향학회지
• /
• 제25권1호
• /
• pp.1-6
• /
• 2006

천해에서의 수중음장 계산에서 음향 임피던스를 해저면 입력인자로서 도입하는 방안의 가능성을 고찰하였다. 먼저 탄성 해저면에서의 음파반사 특성을 고찰한 결과, 임계 접지각 이하에서 음향 임피던스는 접지각이 거의 $0^{\circ}$에 가까울 때의 임피던스 $Z_0$ 1개 값으로 근사가 가능함을 나타내었다. 이러한 특성과 'effective depth' 개념을 접목시켜 전달손실을 계산한 결과, 수중음장 계산에서 임피던스를 해저면 음향 특성을 나타내는 입력인자로 사용하는 것이 가능성이 있음을 확인하였다.

• 대한기계학회논문집A
• /
• 제24권7호
• /
• pp.1854-1862
• /
• 2000

Input shaping method is to convolute input shaper, which is sequence of impulses, with reference input command not to excite the natural frequency of system. To reduce residual vibration for the ch ange of frequency, the number of impulses should be increased. Until now, amplitudes and time interval of those has been searched from the derivative of residual vibration. However, if time interval of impulses is fixed as the half of vibration period of system, input shaper H(z) in z-domain becomes (I-pz-1)n/K in which increasing n is the mean that robustness for change of parameter is improved. Also, design of many types of input shapers in z-domain is very easy because sensitivity curve is displayed with $\mid$H(z)zn$\mid$$\times$100. In the z-domain, EI(Extra-Insensitive) input shaper could be designed without solving nonlinear simultaneous equations as design in continuous time domain. In addition to, the design possibility of input shaper for a damped system was shown.

• Fibers and Polymers
• /
• 제6권1호
• /
• pp.89-94
• /
• 2005

The purpose of this study is to offer acoustical database of warp knitted fabrics by investigating frictional sound properties and physiological responses according to structural parameters such as construction, lap form, and direction of mutual guide bar movement. Fabric sounds of seven warp knitted fabrics are recorded, and Zwicker's psychoacoustic param­eters - loudness(Z), sharpness(Z), roughness(Z), and fluctuation strength(Z) - are calculated. Also, physiological responses evoked by frictional sounds of warp knitted fabrics are measured such as electroencephalogram (EEG), the ratio of high fre­quency to low frequency (HF/LF), respiration rate (RESP), skin conductance level (SCL), and photoplethysmograph (PPG). In case of constructions, frictional sound of sharkskin having higher loudness(Z) and fluctuation strength(Z) increases RESP. By lap form, open lap has louder and larger fluctuating sound than closed lap, but there aren't significant difference of physi­ological responses between open lap and closed lap. In direction of mutual guide bar movement, parallel direction evokes bigger changes of beta wave than counter direction because of its loud, rough, and fluctuating sound. Fluctuation strength(Z) and roughness(Z) are defined as important factors for predicting physiological responses in construction and mutual guide bar movement, respectively.

• 천문학회지
• /
• 제47권2호
• /
• pp.77-86
• /
• 2014

Using a cosmological ${\Lambda}CDM$ simulation, we analyze the differences between the widely-used spin parameters suggested by Peebles and Bullock. The dimensionless spin parameter ${\lambda}$ proposed by Peebles is theoretically well-justified but includes an annoying term, the potential energy, which cannot be directly obtained from observations and is computationally expensive to calculate in numerical simulations. The Bullock's spin parameter ${\lambda}^{\prime}$ avoids this problem assuming the isothermal density profile of a virialized halo in the Newtonian potential model. However, we find that there exists a substantial discrepancy between ${\lambda}$ and ${\lambda}^{\prime}$ depending on the adopted potential model (Newtonian or Plummer) to calculate the halo total energy and that their redshift evolutions differ to each other significantly. Therefore, we introduce a new spin parameter, ${\lambda}^{\prime\prime}$, which is simply designed to roughly recover the value of ${\lambda}$ but to use the same halo quantities as used in ${\lambda}^{\prime}$. If the Plummer potential is adopted, the ${\lambda}^{\prime\prime}$ is related to the Bullock's definition as ${\lambda}^{\prime\prime}=0.80{\times}(1+z)^{-1/12}{\lambda}^{\prime}$. Hence, the new spin parameter ${\lambda}^{\prime\prime}$ distribution becomes consistent with a log-normal distribution frequently seen for the ${\lambda}^{\prime}$ while its mean value is much closer to that of ${\lambda}$. On the other hand, in case of the Newtonian potential model, we obtain the relation of ${\lambda}^{\prime\prime}=(1+z)^{-1/8}{\lambda}^{\prime}$; there is no significant difference at z = 0 as found by others but ${\lambda}^{\prime}$ becomes more overestimated than ${\lambda}$ or ${\lambda}^{\prime\prime}$ at higher redshifts. We also investigate the dependence of halo spin parameters on halo mass and redshift. We clearly show that although the ${\lambda}^{\prime}$ for small-mass halos with $M_h$ < $2{\times}10^{12}M_{\odot}$ seems redshift independent after z = 1, all the spin parameters explored, on the whole, show a stronger correlation with the increasing halo mass at higher redshifts.

• 소성∙가공
• /
• 제7권2호
• /
• pp.168-176
• /
• 1998

Hot workability of the AA5083 alloy ws investigated by torsion test at temperature ranges of $350{\sim}520^{\circ}C$ and strain rates of 0.5, 1.0, and 3.0/sec. The flow stress and hot ductility of the AA5083 alloy as a function of deformation variables such as temperature and train rate were studied. The microstructural evolution of the AA5083 alloy was studied in relation to Zener-Hollomon parameter (Z=exp( /RT) Also the hot restoration mechanism of the AA5083 alloy was small when Z val-ues were higher than $1.73{\times}1016/sec(370^{\circ}C,\;0.5/sec)$ In addition the difference microstructures during hot deformation. It was found that the increase of flow curves and deformed microstructures during hot deformation. It was found that the increase of flow stress of the AA5083 alloy was small when Z val-ues were higher than $1.73{\times}1016/sec(370^{\circ}C.\;0.5/sec)$. However under the low Z values less than $1.73{\times}1016/sec(370^{\circ}C,\;0.5/sec)$ the flow stress increase with increasing the Z values. The large dispersoid particles in the matrix grain decreased the flow strain of the AA5083 alloy because it caused the stress concentration during hot deformation.