• Advances in nano research
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• 제15권3호
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• pp.263-275
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• 2023

The electron transport properties of Y-type zigzag branched carbon nanotubes (CNTs) are of great significance for micro and nano carbon-based electronic devices and their interconnection. Based on the semi-empirical method combining tight-binding density functional theory and non-equilibrium Green's function, the electron transport properties between the branches of Y-type zigzag branched CNT are studied. The results show that the drain-source current of semiconducting Y-type zigzag branched CNT (8, 0)-(4, 0)-(4, 0) is cut-off and not affected by the gate voltage in a bias voltage range [-0.5 V, 0.5 V]. The current presents a nonlinear change in a bias voltage range [-1.5 V, -0.5 V] and [0.5 V, 1.5 V]. The tangent slope of the current-voltage curve can be changed by the gate voltage to realize the regulation of the current. The regulation effect under negative bias voltage is more significant. For the larger diameter semiconducting Y-type zigzag branched CNT (10, 0)-(5, 0)-(5, 0), only the value of drain-source current increases due to the larger diameter. For metallic Y-type zigzag branched CNT (12, 0)-(6, 0)-(6, 0), the drain-source current presents a linear change in a bias voltage range [-1.5 V, 1.5 V] and is symmetrical about (0, 0). The slope of current-voltage line can be changed by the gate voltage to realize the regulation of the current. For three kinds of Y-type zigzag branched CNT with different diameters and different conductivity, the current-voltage curve trend changes from decline to rise when the branch of drain-source is exchanged. The current regulation effect of semiconducting Y-type zigzag branched CNT under negative bias voltage is also more significant.

• 대한족부족관절학회지
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• 제21권2호
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• pp.61-65
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• 2017

Purpose: The purpose of this study was to determine the correlation and ratio between the calcaneal length and width for predicting the width of calcaneus. Materials and Methods: A total of 190 feet (190 patients) were included based on computed tomography scans. The length of calcaneus (CL) was measured on the line connecting the center of a circle tangent to the cortical margin in the anterior and posterior parts of the calcaneus in a sagittal plane (W1, W2). The width of the calcaneus was defined as the horizontal line of each part (W1, W2, W3) on the same axial plane. The relationship between the measurement was determined through a correlation analysis. The reliability was assessed based on intraclass correlation coefficients. Results: The CL and widths of calcaneus (W1, W2, W3) had a good positive correlation (r=0.848 [W1/CL], r=0.738 [W2/CL], r=0.769 [W3/CL]; p<0.001). The mean CL and widths ratios were 0.33 (W1/CL), 0.37 (W2/CL), and 0.37 (W3/CL). Using these ratios to estimate the widths by multiplying each ratio by the measured calcaneal length, we found a difference between the estimated calcaneal widths and the actual measured calcaneal widths values was 0.25 mm, 0.43 mm, and 0.16 mm. All measurements showed good-to-excellent inter- and intraobserver reliability. Conclusion: This study analyzed the correlation and ratio between the length and width of the calcaneus. The results will help orthopedic surgeons fixate screws in a stable manner to prevent iatrogenic injuries to the medial neurovascular structures of the calcaneus.

• 대한토목학회논문집
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• 제34권2호
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• pp.515-527
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• 2014

본 연구에서는 국내 모래의 공학적 특성을 파악하기 위하여 표준사, 욕지사, 낙동강사를 이용하여 구속압 조건, $K_0$ 조건, 과압밀 조건, 상대밀도 조건을 다르게하여 삼축압축시험을 실시하였다. 삼축압축시험 결과, 변형률 ${\epsilon}_1$에 따른 축차응력 $\acute{q}$의 변화는 구속압 ${\sigma}_3$와 상대밀도 $D_r$이 클수록 크게 변화하였으나, $K_0$ 조건과 과압밀 조건변화와 크게 상관이 없었다. 모래의 최대 내부마찰각(${\phi}_{max}$)은 구속압이 클수록 입자간의 접촉력이 크게 되어 작아지는 경향을 나타내었고, $K_0$ 조건과 과압밀 조건에 따라서는 거의 변화가 없는 것으로 나타났으며, 상대밀도에 따라서는 상대밀도가 감소함에 따라 내부마찰각도 작아지는 경향을 나타내었다. 체적변형률(${\epsilon}_u$)은 구속압이 클수록 입자의 파쇄성과 입자간의 재배열에 의해 체적 팽창이 작게 나타났으며, $K_0$ 조건과 과압밀 조건에서는 조건에 상관없이 거의 같은 거동을 보였고, 상대밀도에 따라서는 상대밀도가 커질수록 초기에는 압축되다가 축변형률(${\epsilon}_1$)이 증가할수록 팽창하는 경향이 뚜렷하게 나타났다. 변형률 변화에 따른 탄성계수 $E_{sec}$는 변형률이 커질수록 차츰 수렴하는 경향을 나타내었고, 축차응력($\acute{q}$)-변형률(${\epsilon}_1$) 관계에서 초기할선 탄성계수($E_{ini}$)>할선 탄성계수($E_{sec}$)>접선 탄성계수($E_{tan}$) 순으로 탄성계수의 크기가 산정되었으며, 구속압 및 상대밀도가 증가함에 따라 탄성계수가 증가하는 경향을 보였고, $K_0$ 및 과압밀에 따라서는 거의 비슷한 탄성계수를 나타내었다. 접선 탄성계수에 의한 정규화에 대해서는 다양한 증가비로 증가하는 경향을 보였다. 한계상태선의 기울기 M은 구속압이 증가함에 따라 감소하는 경향을 나타내었고, $K_0$ 및 구속압, 상대밀도에 따라서는 동일선상에 표현되며, 상대밀도가 증가할수록 한계상태선의 기울기 M도 증가하는 경향을 보였다.

• 수산해양기술연구
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• 제53권2호
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• pp.177-186
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• 2017

This study is intended to provide navigator with specific information necessary to assist in the avoidance of collision and in operation of ships to evaluate the maneuverability of research vessel Jera. Authors carried out full-scale sea trials for turning test, zig-zag test, and spiral test at actual sea-going condition, which were performed on starboard and port sides with 10-20 rudder angle at service speed of 10 knots. The turning circle was much different at both of the turning of port and starboard which was longer at the starboard than at the port. In the zig-zag test results, the port and starboard was $10^{\circ}$ the first and second overshoot angles were $6.0^{\circ}$, $5.8^{\circ}$ and $6.3^{\circ}$, $7.1^{\circ}$ respectively and the first overshoot angles were $16.4^{\circ}$, $17.6^{\circ}$ when using $20^{\circ}$. Her maneuverability index T and N can be easily determined by using an analogue computer with the data obtained from the zig-zag tests where K is a constant representing the turning ability and T is a constant representing her quick response. In the zig-zag tests under $10^{\circ}$ or $20^{\circ}$ at rudder angle, the value K is 0.149. 0.123 sec- and T is 11.853 and 6.193 sec and angular velocity is $0.937^{\circ}/sec$ and $1.636^{\circ}/sec$. In the spiral test, the loop width was unstable at $+0.51^{\circ}$ and $-1.19^{\circ}$ around the midship of rudder, but the tangent line at $0^{\circ}$ was close to vertical. From the sea trial results, we found that she did comply with the present criterion in the standards of maneuverability of IMO.

• 터널과지하공간
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• 제15권3호
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• pp.223-227
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• 2005

국내의 일부 지역에서만 발견되는 유리질화산암중 삼호지역에 분포하고 있는 암석을 대상으로 암석의 물리적$cdot$역학적 특성에 대하여 살펴보았다. 본 연구를 수행하기 위하여 암석의 기본 물리적 성질 시험인 비중, 함수비, 흡수율, 공극률, 초음파 속도, 그리고 역학적 성질 시험인 일축 및 삼축 압축, 압열인장 강도, 점하중 강도 등 실내 시험 방법을 이용하였다. 유리질화산암에서 나타나는 비중의 크기는 2.28이였으며, 함수비와 흡수율은 $1.67\%$와 $1.72\%$로써 비슷한 값을 보였다 공극률은 3.87\%$로 낮게 나타난 반면, 초음파 속도는 P파가 5330m/s, S파가 2980 m/s로써 비교적 높은 값을 보였다. 유리질화산암의 압열인장 강도는 7.2MPa 점하중 강도는 2.6MPa로 나타났다. 점하중 강도로부터 추정한 일축압축 강도는 62.4MPa로 실제 일축압축 시험으로부터 구한 66.0MPa과 매우 잘 일치하였다. 일축압축 시험에서 구한 탄성계수 영률은 E=43.2 GPa이였으며, 포아송비는 v=0.28로 나타났다. 또한, Mohr-Coulomb 파괴포락선으로부터 구한 유리질화산암의 점착력은 c=20.1MPa 내부 마찰각은 $\Phi=28.6^{\circ}$로 나타났다.