• IEIE Transactions on Smart Processing and Computing
• /
• 제1권3호
• /
• pp.152-160
• /
• 2012

This paper proposes a frame-level rate control algorithm for low delay video applications to reduce the fluctuations in the bitrate. The proposed algorithm minimizes the bitrate fluctuations in two ways with minimal coding loss. First, the proposed rate control applies R-Q model to all frames including the first frame of every group of pictures (GOP) except for the first one of a sequence. Conventional rate control algorithms do not use any R-Q models for the first frame of each GOP and do not estimate the generated-bit. An unexpected output rate result from the first frame affects the remainder of the pictures in the rate control. Second, a rate-distortion (R-D) cost is calculated regardless of the hierarchical coding structure for low bitrate fluctuations because the hierarchical coding structure controls the output bitrate in rate distortion optimization (RDO) process. The experimental results show that the average variance of per-frame bits with the proposed algorithm can reduce by approximately 33.8% with a delta peak signal-to-noise ratio (PSNR) degradation of 1.4dB for a "low-delay B" coding structure and by approximately 35.7% with a delta-PSNR degradation of 1.3dB for a "low-delay P" coding structure, compared to HM 8.0 rate control.

• 대한전기학회:학술대회논문집
• /
• 대한전기학회 1991년도 추계학술대회 논문집 학회본부
• /
• pp.237-240
• /
• 1991

In this paper, silicon oxynitride(SiON) films were chemically deposited by 193 nm Excimer laser irradiated parallel to the substrate. the laser pulse energy was 80 mJ, repetetion rate was 80 Hz and the laser average power was 6.4 watt, the gas ratio of $N_2O/NH_3$ was 0.75, the substrate temperature was $300^{\circ}C$, and the chamber pressure was 2 torr. And then, the interface state density($N_{ss}$) was characterized by DLTS(Deep Level Transient Spectroscopy). In addition, the capture cross section($\sigma$) and activation energy(${\Delta}E$) was also obtained. The resulting Nss values were $5.5{\times}10^{10}-3.2{\times}10^{11}(eV^{-1}cm^{-2})$, $\sigma$ was $6.64{\times}10^{-20}-2.114{\times}10^{-17}(cm^2)$, the ${\Delta}E$ of two peaks were $8.93{\times}10^{-2}$(eV), 0.375(eV).

• 한국전산유체공학회지
• /
• 제13권1호
• /
• pp.21-27
• /
• 2008

A numerical study for laminar flow in the entrance region of helical tubes for uniform inlet velocity conditions is carried out by means of the finite volume method to investigate the effects of Reynolds number, pitch and curvature ratio on the flow development. This results cover a curvature ratio range of 1/10$\sim$1/320, a pitch range of 0.0$\sim$3.2, and a Reynolds number range of 125$\sim$2000. It has been found that the curvature ratio does significantly effect on the angle of flow development, but the pitch and Reynolds number do not. The characteristic angle $\phi_c(=\phi/\sqrt{\delta})$, or the non-dimensional length $\overline{l}(=l\sqrt{\delta}cos(atan\lambda)/d)$ can be used to represent the flow development for uniform inlet velocity conditions. In uniform inlet velocity conditions, the growth of boundary layer delays the flow development attributed to centrifugal force, and in which conditions the amplitude of flow oscillations is smaller than that in parabolic inlet velocity conditions. If the pitch increases or if the curvature ratio or Reynolds number decreases, the minimum friction factor and the fully developed average friction factor normalized with the friction factor of a straight tube and the flow oscillations decrease.

• 정보처리학회논문지A
• /
• 제12A권1호
• /
• pp.23-30
• /
• 2005

인과순서 메시지 전달 알고리즘은 모든 전송되는 메시지가 인과순서로 전달되도록 한다. 인과순서를 유지하기 위해서는 전송되는 모든 메시지가 제어정보를 가지고 다녀야 하고, 제어정보의 크기는 관련된 프로세스의 수에 비례하여 커지게 되므로 제어정보의 크기를 줄이는 것은 분산시스템의 주요한 관심사가 되어 왔다. 본 논문에서는 실시간 성질을 가지는 멀티미디어 자료를 위한 효율적인 ${\Delta}$-인과순서 알고리즘을 제안하고 평가하였다. 제안된 알고리즘은 전송 부하를 줄이기 위하여 인과순서를 유지하는데 필수적이지 않은 정보를 가능한 이른 시기에 찾아내어 제거하며, 기존 알고리즘보다 훨씬 적은 전송부하를 가지게 된다.

• 한국전기전자재료학회논문지
• /
• 제18권12호
• /
• pp.1111-1116
• /
• 2005

ZnO varistor ceramics added a glass-frit 0.03 $wt\%$ were fabricated with variation of sintering temperature. The sintering temperature and time were $1125^{\circ}C\~1200^{\circ}C$ and 2 h. The average grain sizes increased and the varistor voltage decreased with increasing the sintering temperature. The values of the specimen sintered at $1200^{\circ}C$ were $23.7\;{\mu}m$ and 329 V, respectively. The leakage current of all specimens was less than $1\;{\mu}A$ at DC $82\%$ of varistor voltage. The clamping voltage ratio of the specimen sintered at $1175^{\circ}C$ was 1.37. The endurance of surge current and the deviation of varistor voltage of the specimen sintered at $1175^{\circ}C$ were 6400 $A/cm^2$ and ${\Delta}-2.81\%$, respectively. After the High Temperature Load Test(HTLT) at $85^{\circ}C$ for 1000 h, the specimen sintered at $1175^{\circ}C$ showed the lowest deviation of varistor voltage of ${\Delta}-1.92\%$.

• 대한전기학회논문지:전기물성ㆍ응용부문C
• /
• 제50권11호
• /
• pp.539-543
• /
• 2001

ln this paper, the $Sr_{l-x}Ca_xTiO_3(0\leqx\leq0.2)-based$ grain boundary layer ceramics were fabricated to measure dielectric properties with the sintering temperature and the thermal treatment time. The sintering temperature and time were $1420~15206{\circ}C$, 4hours, and the thermal treatment temperature and time of the specimen were $l150^{\circ}C$, 1, 2, 3hours, respectively. The structural and the dielectric properties were investigated by SEM, X-ray, HP4194A and K6517. The average grain size was increased with increasing the sintering temperature, but it decreased up to 15mo1% with increasing content of Ca. X-ray diffraction analysis results showed that all specimens were the cubic structure, and the main peaks were moved to right and the lattice constant were decreased with increasing content of Ca. The appropriate thermal treatment time and temperature of CuO to obtain dielectric properties of $\varepsilon_r>50000,\; tan \delta<0.05\; and \;\DeltaC<\pm10%$ were 2hrs and $l150^{\circ}C$, respectively.

• 한국우주과학회:학술대회논문집(한국우주과학회보)
• /
• 한국우주과학회 2010년도 한국우주과학회보 제19권1호
• /
• pp.34.4-34.4
• /
• 2010

We present the properties of globular cluster systems for 10 early-type galaxies in low density environments obtained using deep images from the Advanced Camera for Surveys (ACS) on the Hubble Space Telescope (HST). Using the ACS Virgo Cluster Survey as a counterpart in high-density environments, we investigate the role of environment in determining the properties of their globular cluster systems. We detect a strong colour bimodality of globular cluster systems in half of our galaxy sample. It is found that there is a strong correlation between the colour and richness of globular cluster populations and their host galaxy luminosities: the less bright galaxies possess bluer and fewer globular clusters as also seen in rich cluster environments. However, the mean colour of globular clusters in our field sample are slightly bluer than those in cluster environments at a given galaxy luminosity, and the colour of the red population has a steeper slope with absolute luminosity. By employing the YEPS simple stellar population model, the colour offset corresponds to metallicity difference of $\Delta$[F e/H ] ~ 0.15 - 1.20 or an age difference of $\Delta$age ~ 2 Gyr on average, implying that GCs in field galaxies appear to be either less metal-rich or younger than those in cluster galaxies. Although we have found that galaxy environment has a subtle effect on the formation and metal enrichment of GC systems, host galaxy mass is the primary factor that determines the stellar populations of GCs and the galaxy itself.

• 한국초전도ㆍ저온공학회논문지
• /
• 제13권1호
• /
• pp.1-5
• /
• 2011

[ $CeO_2$ ]has been widely used for single buffer layer of coated conductor because of superior chemical and structural compatibility with $ReBa_2Cu_3O_{7-{\delta}}$(Re=Y, Nd, Sm, Gd, Dy, Ho, etc.). But, the surface of $CeO_2$ layer showed cracks because of the large difference in thermal expansion coefficient between metal substrate and deposited $CeO_2$ layer, when thickness of $CeO_2$ layer exceeds 100 nm on the biaxially textured Ni-3%W substrate. The deposition rate has been limited to be less than 6 $\AA$/sec in order to get a good epitaxy. In this research, we deposited $CeO_2$ single buffer layers on biaxially textured Ni-3%W substrate with 2-step process such as thin nucleation layer(>10 nm) with low deposition rate(3 $\AA$/sec) and thick homo epitaxial layer(>240 nm) with high deposition rate(30 $\AA$/sec). Effect of deposition temperature on degree of texture development was tested. Thick homo epitaxial $CeO_2$ layer with good texture without crack was obtained at $600^{\circ}C$, which has ${\Delta}{\phi}$ value of $6.2^{\circ}$, ${\Delta}{\omega}$ value of $4.3^{\circ}$ and average surface roughness(Ra) of 7.2 nm within $10{\mu}m{\times}10{\mu}m$ area. This result shows the possibility of preparing advanced Ni substrate with simplified architecture of single $CeO_2$ layer for low cost coated conductor.

• 한국수산과학회지
• /
• 제10권4호
• /
• pp.213-220
• /
• 1977

제 1보에서 측정한 해수의 비전도도 값을 사용하여 본 논문에서 저자들이 제안한 식으로부터 얻어진 당량 전도도를 Arrhenius plot 했을 때 활성화에너지, ${\Delta}E$는 압력 및 농도변화에 따라 $3.0\~4.0\;Kcal/mole$ 범위 이었다, 압력변화에 따른 활성화 부피변화의 평균치 측정된 온도와 압력에서 $-0.27\~-1.30\;cm^3/mole$ 범위였다. (염소량이 $6.228\%_{\circ},-1.65\~\;-0.32cm^3/mole;\;9.063\%_{\circ},\;-1.18\~-0.27cm^3/mole;\;11.628\%_{\circ},\;-1.53\~-0.07cm^3/mole;\;14.311\%_{\circ},\;-1.37\~-0.35cm^3/mole;\;16.408\%_{\circ},\;-1.18\~-0.47cm^3/mole;\;19.372\%_{\circ},\;-1.53\~-0.29cm^3/mole$)이들값으로 해수의 성질과 물의구조를 정성적으로 밝힐 수 있었다. 본 논문 정리를 위해 조언하여 주신 원중훈교수님께 감사드립니다.

• 한국광학회지
• /
• 제15권2호
• /
• pp.183-189
• /
• 2004

고화질 디지털 카메라가 널리 보급되면서 디지털 카메라는 단순한 영상 기록 장치가 아닌 정보 저장 매체로써 다양한 분야에서 사용되고 있다. 그러나 디지털 카메라의 분광 감도가 표준 관측자의 색 일치 함수와 다르기 때문에 카메라로는 색이 정확하게 측정될 수 없다. 본 연구는 카메라 이미지를 피사체의 색 정보를 지니고 있는 sRGB 이미지로 변환하는 방법에 관한 것이다. 디지털 카메라의 출력 신호와 CIE 삼자극치간의 변환 행렬은 Macbeth ColorChecker 24색을 기준 색으로 하여 다중 회귀법을 사용하여 구하였다. 변환 행렬을 이용하여 카메라의 출력 신호로부터 피사체의 실제 색을 찾아내어 이상적인 sRGB 표준 모니터에 정확하게 나타낼 수 있는 RGB 데이터로 변환하였다. Kodak DC220 디지털 카메라로 생성된 Macbeth ColorChecker의 sRGB 이미지와 실제 색과의 평균 색차는 2.1 $\Delta$ $E_{ab}$ $^{*}$ 시험 색표로 사용된 IT8 Reference KIT(286색)의 sRGB 이미지와 실제 색과의 평균 색차는 4.6 $\Delta$ $E_{ab}$ $^{*}$ 로 계산되었다. ab/$^{*}$ 로 계산되었다.