• 한국산학기술학회논문지
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• 제22권3호
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• pp.13-19
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• 2021

n형 SiC 반도체에서 적층 결함이 열전 물성에 미치는 영향에 대해 연구하였다. ��-SiC 분말 성형체를 질소 분위기에서 1600~2100 ℃, 20~120분간 열처리해서 30~42 %의 기공률을 갖는 다공질 SiC 반도체를 제작하였다. X선 회절 분석으로 적층 결함량, 격자 스트레인 및 격자 상수를 산출하였고, 미세 구조 분석을 위해서 기공률 및 비표면적 측정과 함께, 주사 전자현미경 (SEM), 투과 전자현미경 (TEM) 및 고분해능 전자현미경 (HREM) 등을 관찰하였다. Ar 분위기 550~900 ℃에서 도전율과 Seebeck 계수를 측정 및 산출하였다. 열처리 온도가 높을수록, 처리 시간이 길어질수록 캐리어 농도 증가 및 입자와 입자간의 연결성 향상에 의해 도전율이 향상되었다. 도너로 작용하는 질소의 고용으로 Seebeck 계수는 음(-)의 값을 나타내었고, 도전율과 마찬가지로 열처리 온도 및 시간이 상승함에 따라 Seebeck 계수의 절대 값이 증가하였다. 이는 적층 결함의 감소, 즉 입자 및 결정 성장과 함께 적층 결함 밀도의 감소에 의해 포논의 평균 자유 행정이 증가해서 결과적으로 포논-드랙 효과에 의한 Seebeck 계수의 향상으로 나타난 것으로 판단된다.

• Wind and Structures
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• 제35권1호
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• pp.1-20
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• 2022

This research work presents an experimental study's outcomes to reveal the impact of an O-ring on the flow control over a sphere placed in a turbulent boundary layer. The investigation is performed quantitatively and qualitatively using particle image velocimetry (PIV) and dye visualization. The sphere model having a diamater of 42.5 mm is located in a turbulent boundary layer flow over a smooth plate for gap ratios of 0≤G/D≤1.5 at Reynolds number of 5 × 10³. Flow characteristics, including patterns of instantaneous vorticity, streaklines, time-averaged streamlines, velocity vectors, velocity fluctuations, Reynolds stress correlations, and turbulence kinetic energy (), are compared and discussed for a naked sphere and spheres having O-rings. The boundary layer velocity gradient and proximity of the sphere to the flat plate profoundly influence the flow dynamics. At proximity ratios of G/D=0.1 and 0.25, a wall jet is formed between lower side of the sphere and flat plate, and velocity fluctuations increase in regions close to the wall. At G/D=0.25, the jet flow also induces local flow separations on the flat plate. At higher proximity ratios, the velocity gradient of the boundary layer causes asymmetries in the mean flow characteristics and turbulence values in the wake region. It is observed that the O-ring with various placement angles (𝜃) on the sphere has a considerable alteration in the flow structure and turbulence statistics on the wake. At lower placement angles, where the O-ring is closer to the forward stagnation point of the sphere, the flow control performance of the O-ring is limited; however, its impact on the flow separation becomes pronounced as it is moved away from the forward stagnation point. At G/D=1.50 for O-ring diameters of 4.7 (2 mm) and 7 (3 mm) percent of the sphere diameter, the -ring exhibits remarkable flow control at 𝜃=50° and 𝜃=55° before laminar flow separation occurrence on the sphere surface, respectively. This conclusion is yielded from narrowed wakes and reductions in turbulence statistics compared to the naked sphere model. The O-ring with a diameter of 3 mm and placement angle of 50° exhibits the most effective flow control. It decreases, in sequence, streamwise velocity fluctuations and length of wake recovery region by 45% and 40%, respectively, which can be evaluated as source of decrement in drag force.

• Wind and Structures
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• 제34권1호
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• pp.115-125
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• 2022

The high-Reynolds number flow around a rectangular cylinder, having streamwise to crossflow length ratio equal to 5 is analyzed in the present paper. The flow is characterized by shear-layer separation from the upstream edges. Vortical structures of different size form from the roll-up of these shear layers, move downstream and interact with the classical vortex shedding further downstream in the wake. The corresponding mean flow is characterized by a recirculation region along the lateral surface of the cylinder, ending by mean flow reattachment close to the trailing edge. The mean flow features on the cylinder side have been shown to be highly sensitive to set-up parameters both in numerical simulations and in experiments. The results of 21 Large Eddy Simulations (LES) are analyzed herein to highlight the impact of the lateral mean recirculation characteristics on the near-wake flow features and on some bulk quantities. The considered simulations have been carried out at Reynolds number Re=DU_∞/ν=40 000, being D the crossflow dimension, U_∞ the freestream velocity and ν the kinematic viscosity of air; the flow is set to have zero angle of attack. Some simulations are carried out with sharp edges (Mariotti et al. 2017), others with different values of the rounding of the upstream edges (Rocchio et al. 2020) and an additional LES is carried out to match the value of the roundness of the upstream edges in the experiments in Pasqualetto et al. (2022). The dimensions of the mean recirculation zone vary considerably in these simulations, allowing us to single out meaningful trends. The streamwise length of the lateral mean recirculation and the streamwise distance from the upstream edge of its center are the parameters controlling the considered quantities. The wake width increases linearly with these parameters, while the vortex-shedding non-dimensional frequency shows a linear decrease. The drag coefficient also linearly decreases with increasing the recirculation length and this is due to a reduction of the suctions on the base. However, the overall variation of C_D is small. Finally, a significant, and once again linear, increase of the fluctuations of the lift coefficient is found for increasing the mean recirculation streamwise length.

• Advances in nano research
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• 제16권4호
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• pp.325-340
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• 2024

There are several novel uses for dispersing many nanoparticles into a conventional fluid, including dynamic sealing, damping, heat dissipation, microfluidics, and more. Therefore, melting heat and mass transfer characteristics of a 3-D MHD Hybrid Nanofluid flow over a rotating disc with presenting dufour and soret effects are assessed numerically in this study. In this instance, we investigated both ferric sulfate and molybdenum disulfide as nanoparticles suspended within base fluid water. The governing partial differential equations are transformed into linked higher-order non-linear ordinary differential equations by the local similarity transformation. The collection of these deduced equations is then resolved using a Chebyshev spectral collocation-based algorithm built into the Mathematica software. To demonstrate how different instances of hybrid/ nanofluid are impacted by changes in temperature, velocity, and the distribution of nanoparticle concentration, examples of graphical and numerical data are given. For many values of the material parameters, the computational findings are shown. Simulations conducted for different physical parameters in the model show that adding hybrid nanoparticle to the fluid mixture increases heat transfer in comparison to simple nanofluids. It has been identified that hybrid nanoparticles, as opposed to single-type nanoparticles, need to be taken into consideration to create an effective thermal system. Furthermore, porosity lowers the velocities of simple and hybrid nanofluids in both cases. Additionally, results show that the drag force from skin friction causes the nanoparticle fluid to travel more slowly than the hybrid nanoparticle fluid. The findings also demonstrate that suction factors like magnetic and porosity parameters, as well as nanoparticles, raise the skin friction coefficient. Furthermore, It indicates that the outcomes from different flow scenarios correlate and are in strong agreement with the findings from the published literature. Bar chart depictions are altered by changes in flow rates. Moreover, the results confirm doctors' views to prescribe hybrid nanoparticle and particle nanoparticle contents for achalasia patients and also those who suffer from esophageal stricture and tumors. The results of this study can also be applied to the energy generated by the melting disc surface, which has a variety of industrial uses. These include, but are not limited to, the preparation of semiconductor materials, the solidification of magma, the melting of permafrost, and the refreezing of frozen land.

• 암석학회지
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• 제18권1호
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• pp.19-30
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• 2009

울산시 울주군 언양읍 북부 신흥마을 입구에 북서-남동 방향으로 트렌치된 단면에서 양산단층대의 주단층과 제4기 단층이 관찰되었다. 본 논문은 신흥마을 입구의 트렌치 단면에서 조사된 양산단층대의 기반암 단층(신흥단층)과 제4기 단층(제4기 신흥단층)의 기하학적 운동학적 특성연구로부터 양산단층대 남부의 단층 운동사를 해석하였다 신흥마을 입구 트렌치 단면에서는 단층접촉으로 반복되어 산출하는 백악기 하양층군의 퇴적암류와 유천층군의 화산암류 그리고 이들 기반암류를 부정 합으로 피복하는 제4기 퇴적층 등이 산출하고, 본 연구결과 양산단층대의 형성과 관련된 적어도 2회의 주향-이동 단층운동 (D1, D2)과 이후 적어도 2회의 역-이동 단층운동(D3, D4)이 인지된다 (1) D1 단층운동: 양산단층대의 주 단층을 향하여 퇴적암류의 층리를 고각화시키는 주향-이동 단층운동. (2) D2 단층운동: 고각화된 층리를 단층면으로 하는 우수 주향-이동 단층운동 주요 특징적인 구조요소로서는 북북동 방향의 준 수평적인 우세한 단층조선과 준 수직적인 우세한 단층엽리 등이 있다. 양산단층대의 주요 단층암류는 D2 단층운동에 의해 형성되었다. (3) D3 단층운동: (동) 북동 주향에 (남)남동 내지 (북)북서 방향으로 중각 경사하는 단층면을 갖는 공역성 역-이동 단층운동 주요 특징적인 구조요소로서는 주향 방향의 단층조선을 중첩하는 경사 방향의 단층조선, D2 단층비지에 발달하는 S-C 구조 엽리, 비탈과 평탄 기하의 단층면, 단층운동에 수반된 비대칭 및 끌림 습곡과 붕괴구조 등이 있다. 양산단층대 주 단층면의 방향성은 주로 D3 단층운동에 의해 분산되었다. (4) D4 단층운동: 제4기 퇴적층내에 5-C 구조 엽리의 발달과 함께 제4기 퇴적층을 수 cm 변위시키는 제4기 역-이동 단층운동 양산단층대의 다른 제4기 단층과 같이 D4 단층면은 기반암의 D3 역-이동 단층면의 연장선상에 놓이고, 이들 단층은 동일한(북)북서-(남)남동 방향의 압축응력에 의해 형성되었다.