• 한국수산과학회지
• /
• 제44권4호
• /
• pp.423-430
• /
• 2011

The most satisfactory split-beam transducer for fish sizing maintains a wide bearing angle region for correct fish tracking without interference from side lobes and lower sensitivity to fish echoes outside of the main lobe region to correctly measure the angular location of free-swimming fishes in the sound beam. To evaluate the performance of an experimentally developed 50 kHz split-beam transducer, the angular location of a target was derived from the electrical phase difference between the resultant signals for the pair of transducer quadrants in the horizontal and vertical planes consisting of 32 transducer elements. The electrical phase difference was calculated by cross-spectral density analysis for the signals from the pair of receiving transducer quadrants, and the directivity correction factor for a developed split-beam transducer was estimated as the fourth-order polynomial of the off-axis beam angle for the angular location of the target. The experimental results demonstrate that the distance between the acoustic centers for the pair of receiving transducer quadrants can be controlled to less than one wavelength by optimization with amplitude-weighting transformers, and a smaller center spacing provides a range of greater angular location for tracking of a fish target. In particular, a side lobe level of -25.2 dB and an intercenter spacing of $0.96\lambda$($\lambda$= wavelength) obtained in this study suggest that the angular location of fish targets distributing within a range of approximately ${\pm}28^{\circ}$ without interference from side lobes can be measured.

• 한국우주과학회:학술대회논문집(한국우주과학회보)
• /
• 한국우주과학회 2011년도 한국우주과학회보 제20권1호
• /
• pp.20.1-20.1
• /
• 2011

We present the results of far-ultraviolet (FUV) observations of comet C/2001 Q4 (NEAT) obtained with Far-ultraviolet Imaging Spectrograph (FIMS) on board the Korean microsatellite STSAT-1, which operated at an altitude of 700 km in a sun-synchronous orbit. FIMS is a dual-channel imaging spectrograph (S channel 900-1150 ${\AA}$, L channel 1350-1750 ${\AA}$, ${\lambda}/{\Box}{\lambda}$ ~ 550) with large image fields of view (S: $4^{\circ}.0{\times}4'.6$, L: $7^{\circ}.5{\times}4'.3$, angular resolution 5'-10') optimized for the observation of diffuse emission of astrophysical radiation. Comet C/2001 Q4 (NEAT) was observed with a scanning survey mode when it was located around the perihelion between 8 and 15 May 2004. Several important emission lines were detected including S I (1425, 1474 ${\AA}$), C I (1561, 1657 ${\AA}$) and several emission lines of CO $A1{\cap}-X1{\sum}+$ system in the L channel. We estimated QCO = ($2.58\;{\pm}\;0.64)\;{\times}\;1028$ s-1 from the production rate of CO 1510 ${\AA}$. We obtained L-channel image which have map size of $5^{\circ}{\times}5^{\circ}$. The image was constructed for the wavelength band of L-channel (1350-1750 ${\AA}$).We also obtained radial profile of S I, C I, CO with line fitting from central coma.

• 정보처리학회논문지B
• /
• 제11B권6호
• /
• pp.625-632
• /
• 2004

H.264 부호화 기법은 단방향 및 양방향 예측 모드를 채택하고 있으며, 가변 길이 부호화를 사용하기 때문에 비디오 부호기에서 발생되는 데 이터량은 시간에 따라 변한다. 전송채널 용량이 제한된 고정 비트율 부호기에서는 출력 비트량을 제어하기 위해 버퍼가 사용되는데, 버퍼가 넘치거나(overflow) 고갈되는 것(underflow)을 막기 위해 발생 비트량을 적절한 영역 내에서 제한해야 한다. 기존의 비트량 제어방법 에서는 영상데이터의 왜곡 값과 양자화 계수간의 $\lambda_{MODE}$가 정규 값을 벗어나기 때문에 화질이 열화 된다. 본 논문에서는 H.264 동영상의 왜곡 값에 대한 새로운 양자화 계수론 도출하여 피드백 함으로써 버퍼의 넘침이나 고갈을 방지할 수 있는 알고리즘을 제안하였다. 제안한 기법을 6개의 실험데이터에 적용한 견과 PSNR 값은 기존 방법에서와 비슷하면서도 비트율은 최대 8%까지 감소하였다.

• 한국재료학회지
• /
• 제9권4호
• /
• pp.355-361
• /
• 1999

가용성 폴리이마드 주쇄에 Disperse-Red 1 크로모포를 공유결합 시킨 옆사술계 비선형 전기광학 고분자를 합성하였다. 합성된 고분자의 유리전이온도 빛 열분해온도 는 각각 $225^{\circ}C, 310^{\circ}C$이었으며 광통신 파장에서 광학적으로 투명하였다. $100 V/\mu\textrm{m}$의 전기장으로 폴링했을 때, 유전상수는 10 kHz에서 3.37이며, 파장 1300 nm에서, 굴절률은 $n_{TE} 및 n_{TM}$ 모두 1.631로같았으며, 전기광학계수는 4.6 ~ 9.2 pm/V이였다. 폴링한 후 $180^{\circ}C$에서 1시간 동안 유지시킨 시편의 전기광학계수의 값은 감소되지 않 았으며, 장기적인 관점에서 $90^{\circ}C$에서 500 시간 동안 유지시킨 시편의 전기광학계수도 변함이 없었다.

• 대한화학회지
• /
• 제39권5호
• /
• pp.350-355
• /
• 1995

요오드와 테트라메틸주석간의 전하이동에 따른 상호작용을 사염화탄소 용매내에서 분광학적 방법으로 연구하였다. 이들의 결과로부터 일시적인 전하이동 착물의 흡수 스펙트 럼(${\lambda}_{max}=270nm$)이 관찰되었으며, 흡수스펙트럼의 후속적인 감소현상으로 요오드에 의한 테트라메틸주석의 분해반응임을 알았다(iodoedestannylation). 따라서 Iodoedestannylation에 대한 속도 상수를 온도 10, 25 및 $35^{\circ}C$ 압력을 1200 bar까지 변화 시켜가면서 측정하였으며, 이때의 반응속도상수는 온도와 압력에 따라 증가함을 알았다. 이 반응속도 상수로부터 ${\Delta}V^{\neq},\;{\Delta}{\beta}^{\neq},\;{\Delta}H^{\neq}$ 및 ${\Delta}S^{\neq}$의 값을 구했으며 이들 값으로부터 전이상태의 용매구조 변 화 및 메카니즘을 규명하였다. 이러한 사실로부터 본 반응은 $S_F2$ 메카니즘이 지배적 이며 압력이 증가함에 따라 $S_F2$의 성격이 약화됨을 알았다.

• 한국결정학회지
• /
• 제15권1호
• /
• pp.24-28
• /
• 2004

X-선 회절법을 이용하여 $C_{12}H_{15}N_3O_3$의 분자 및 결정구조를 해석하였다. 이 결정의 결정계는 Monoclinic이고 공간군은 $P2_1/c$이며, 단위포 상수는 a = 12.9955(9) ${\AA}$, b = 7.7137(5) ${\AA}$, c = 13.4699(11) ${\AA}$, ${\beta}$ = 107.86(1)$^{\circ}$, V = 1285.2(1) ${\AA}^3$, T = 296 K, Z = 4, $D_c$ = 1.350 $Mgm^{-3}$이다. 회절반점들의 세기는 Enraf-Nonius CAD-4 Diffractometer로 얻었으며 Mo $K{\alpha}$선(${\lambda}$ = 1.71073 ${\AA}$)을 사용하였다. 분자구조는 Direct method로 풀었으며, $F_0\;>\;4{\sigma}(F_0)$인 1644개의 독립 회절 데이터에 대하여 최소자승법으로 193개의 변수를 정밀화하여 최종 신뢰도 값 R = 4.19%을 얻었다.

• 한국신재생에너지학회:학술대회논문집
• /
• 한국신재생에너지학회 2007년도 추계학술대회 논문집
• /
• pp.281-284
• /
• 2007

Recently, we have developed p-i-n a-Si:H single junction thin film solar cells with RF (13.56MHz) plasma enhanced chemical vapor deposition (PECVD) system, and also successfully fabricated the mini modules ($>300cm^2$), using the laser patterning technique to form an integrated series connection. The efficiency of a mini module was 7.4% ($Area=305cm^2$, Isc=0.25A, Voc=14.74V, FF=62%). To fabricate large area modules, it is important to optimise the integrated series connection, without damaging the cell. We have newly installed the laser patterning equipment that consists of two different lasers, $SHG-YVO_4$ (${\lambda}=0.532{\mu}m$) and YAG (${\lambda}=1.064{\mu}m$). The mini-modules are formed through several scribed lines such as pattern-l (front TCO), pattern-2 (PV layers) and pattern-3 (BR/back contact). However, in the case of pattern-3, a high-energy part of laser shot damaged the textured surface of the front TCO, so that the resistance between the each cells decreases due to an incomplete isolation. In this study, the re-deposition of SnOx from the front TCO, Zn (BR layer) and Al (back contact) on the sidewalls of pattern-3 scribed lines was observed. Moreover, re-crystallization of a-Si:H layers due to thermal damage by laser patterning was evaluated. These cause an increase of a leakage current, result in a low efficiency of module. To optimize a-Si:H single junction thin film modules, a laser beam profile was changed, and its effect on isolation of scribed lines is discussed in this paper.

• 대기
• /
• 제23권3호
• /
• pp.265-273
• /
• 2013

To investigate properties of cloud and rainfall occurred at Boseong on 10 July 2012, Raindrop Size distributions (RSDs) and other parameters were analyzed using observation data collected by Micro Rain Radar (MRR) and PARticle SIze and VELocity (PARSIVEL) disdrometer located in the National center for intensive observation of severe weather at Boseong in the southwest of the Korean peninsula. In addition, time series of RSD parameters, relationship between reflectivity-rain rate, and vertical variation of rain rates-fall velocities below melting layer were examined. As a result, good agreements were found in the reflectivity-rain rate time series as well as their power relationships between MRR and PARSIVEL disdrometer. The rain rate was proportional to reflectivity, mean diameter, and inversely proportional to shape (${\mu}$), slope (${\Lambda}$), intercept ($N_0$) parameter of RSD. In comparison of the RSD, as rain rate was increased, the slope of RSD became less steep and the mean diameter became larger. Also, it was verified that reflectivities are classified in three categories (Category 1: Z (reflectivity) > 40 dBZ, Category 2: 30 dBZ < Z < 40 dBZ, Category 3: Z < 30 dBZ). As reflectivity was increased, rain rate was intensified and larger raindrops were existed, while reflectivity was decreased, shape (${\mu}$), slope (${\Lambda}$), intercept ($N_0$) parameter of RSD were increased. We expected that these results will lead to better understanding of microphysical process in convective rainfall system occurred during short-term period over Korean peninsula.

• 한국항공우주학회지
• /
• 제43권3호
• /
• pp.224-231
• /
• 2015

람다 날개 형상의 공력 계수에 대한 실험적 연구를 국방과학연구소의 중형아음속 풍동에서 수행하였다. 본 연구의 주목적은 옆미끄럼각의 변화에 따라 다양한 공력 계수가 어떻게 변화하는지를 조사하는 것이다. 옆미끄럼각이 $0^{\circ}C$인 경우, 피칭 모멘트가 급격히 불안정해지는 현상을 확인하였으며, 옆미끄럼각이 증가함에 따라 pitch break 현상이 더 높은 받음각에서 발생하는 것을 확인하였다. 롤링 모멘트는 옆미끄럼각이 있는 경우 pitch break와 유사한 특성을 보여준다. 이런 경향은 옆미끄럼각이 증가할수록 더 심하게 나타났다. 요잉 모멘트는 높은 받음각에서 옆미끄럼각에 따라 기울기가 크게 변화하였고 불안정한 방향 안정성이 뚜렷이 나타났다. 모멘트의 이런 특성들은 비행 제어를 위해서는 보다 효과적인 조종성 증가 장치가 필수적이란 것을 의미하고 있다.

• Fisheries and Aquatic Sciences
• /
• 제19권2호
• /
• pp.8.1-8.11
• /
• 2016

To quantitatively estimate the influence of cuttlebone on the target strength (TS) of golden cuttlefish, the cuttlebone was carefully extracted from 19 live cuttlefish caught using traps in the inshore waters around Geojedo, Korea, in early May 2010 and the TS was measured using split-beam echosounders (Simrad ES60 and EY500). The TS-length relationships for the cuttlefish (before the extraction of cuttlebone, Fish Aquat Sci. 17:361-7, 2014) and the corresponding cuttlebone were compared. The cuttlebone length ($L_b$) ranged from 151 to 195 mm (mean $L_b$ = 168.3 mm) and the mass ($W_b$) ranged from 29.3 to 53.2 g (mean $W_b$ = 38.8 g). The mean TS values at 70 and 120 kHz were -33.60 dB (std = 1.12 dB) and -32.24 dB (std = 1.87 dB), respectively. The mean TS values of cuttlebone were 0.19 dB and 0.04 dB lower than those of cuttlefish at 70 and 120 kHz, respectively. For 70 and 120 kHz combined, the mean TS value of cuttlebone was -32.87 dB, 0.11 dB lower than that of cuttlefish (-32.76 dB). On the other hand, the mean TS value of cuttlebone predicted by the regression ($TS_b$ = 24.86 $log_{10}$ $L_b$ - 4.86 $log_{10}$ ${\lambda}$ - 22.58, $r^2$ = 0.85, N = 38, P < 0.01) was -33.10 dB, 0.04 dB lower than that of cuttlefish predicted by the regression ($TS_c$ = 24.62 $log_{10}$ $L_c$ - 4.62 $log_{10}$ ${\lambda}$ - 22.64, $r^2$ = 0.85, N = 38, P < 0.01). That is, the contribution of cuttlebone to the cuttlefish TS determined by the measured results was slightly greater than that by the predicted results. These results suggest that cuttlebone is responsible for the TS of cuttlefish, and the contribution is estimated to be at least 99 % of the total echo strength.