• 대한기계학회논문집
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• 제19권7호
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• pp.1684-1690
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• 1995

A large time asymptotic solution for an unsteady heat conduction problem of a coated hot wire thermal conductivity measurement process was theoretically found. The solution revealed that the slope of wire temperature versus logarthmic time, which is used to evaluate the thermal conductivity, remains unchanged for large values of time even if a layer of coating is present on the hot wire. The significance of this result is that the thermal conductivity of an electrically conductive fluid can be measured with a coated hot wire using the same conversion relation as for a bare wire.

• 대한기계학회논문집B
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• 제37권12호
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• pp.1147-1152
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• 2013

본 논문에서는 절연된 열선을 이용한 비정상열선법에서 열선의 절연코팅이 선형구간의 초기시점에 미치는 영향을 살펴보기 위하여 이론적인 연구를 수행해 보았다. 이를 위해, 절연된 열선의 온도상승에 관한 해석적 해에서 선형구간의 초기시점에 영향을 미치는 중요한 인자들을 파악해 보았으며, 이러한 인자들의 영향이 무시할 만큼 작아지는 임계시간(critical time)에 대한 연구를 수행해 보았다. 이론적인 연구 결과, 열선의 반경 및 코팅의 두께가 작을수록 절연코팅의 영향이 빠르게 감소하였고, 또한 절연물질의 열전도도가 크고 열확산계수가 작을수록 절연코팅의 영향이 빠르게 감소함을 알 수 있었다. 본 연구의 결과는 절연된 열선을 이용한 비정상열선법에서, 선형구간의 초기시점을 결정하는데 도움이 될 것으로 사료된다.

• 대한기계학회논문집
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• 제8권2호
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• pp.154-161
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• 1984

본 연구에서는 고정밀 아날로그-디지탈 변환기와 마이크로 프로세서(micropr- ocessor) Intel 8085를 사용하여 비정상 아날로그(analog)신호를 왜곡이 없이 디지탈 량으로 직접 변환하여 자료처리하였다. 또한 비정상 열선법은 열선에 전류를 가하여 열선이 열원이며 동시에 온도계의 두 가지 역할을 하므로, 전기전도성이 있는 액체는 적합하지 못한 단점이 있다. 이를 해결하기 위하여 열선에 얇은 절록피복층을 입혀 전기전도성 액체의 열전도율을 측정할 수 있는 가능성에 대한 연구를 시도하였다.

• 대한기계학회논문집B
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• 제35권3호
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• pp.279-285
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• 2011

본 논문에서는 비정상열선법을 이용한 나노유체의 열전도도 측정시, 자연대류 개시점을 수치적 방법을 통하여 파악해 보았다. 측정 유체는 부피비 1, 4, 10% 를 갖는 물-기반 알루미나 나노유체이고, 이에 대한 물성치는 기존 이론모델 및 실험적 상관관계식을 이용하여 계산하였다. 비정상열선법 장치는 FDM 방식으로 모델링 되었으며, 자연대류의 개시점은 중력장하의 열선의 온도변화를 관찰함으로써 파악하였다. 자연대류의 개시점은 물의 경우 11.5 초이고, 10% 부피비에서 Maxwell 모델로 열전도도를 예측한 알루미나 나노유체인 경우 41.6 초로 계산되었다. 특히 부피비가 증가할수록 자연대류가 늦게 발생함을 확인하였으며, 계산된 결과를 이용하여 비정상열선법의 실린더 내부에서 나노유체의 자연대류 개시점을 예측할 수 있는 관계식을 제시하였다. 또한 비정상열선법으로 열전도도를 측정할 때, 기본유체의 자연대류 발생시점 이전에 측정이 이루어진다면 나노유체의 열전도도 측정시 자연대류에 의한 측정오차는 무시할 수 있음을 확인하였다.

• Current Photovoltaic Research
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• 제1권1호
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• pp.63-68
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• 2013

We investigated the effects of Au eutectic reaction on Si thin film growth by hot wire chemical vapor deposition. Small SiC and Si nano-particles fabricated through a wet etching process were coated and biased at 50 V on micro-textured Si p-n junction solar cells. Au thin film of 10 nm and a Si thin film of 100 nm were then deposited by an electron beam evaporator and hot wire chemical vapor deposition, respectively. The Si and SiC nano-particles and the Au thin film were structurally embedded in Si thin films. However, the Au thin film grew and eventually protruded from the Si thin film in the form of Au silicide nano-balls. This is attributed to the low eutectic bonding temperature ($363^{\circ}C$) of Au with Si, and the process was performed with a substrate that was pre-heated at a temperature of $450^{\circ}C$ during HWCVD. The nano-balls and structures showed various formations depending on the deposited metals and Si surface. Furthermore, the samples of Au nano-balls showed low reflectance due to surface plasmon and quantum confinement effects in a spectra range of short wavelength spectra range.

• 한국분말재료학회지
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• 제15권4호
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• pp.285-291
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• 2008

Fe based ($Fe_{68.2}C_{5.9}Si_{3.5}B_{6.7}P_{9.6}Cr_{2.1}Mo_{2.0}Al_{2.0}$) amorphous powder were produced by a gas atomization process, and then ductile Cu powder fabricated by the electric explosion of wire(EEW) were mixed in the liquid (methanol) consecutively. The Fe-based amorphous - nanometallic Cu composite powders were compacted by a spark plasma sintering (SPS) processes. The nano-sized Cu powders of ${\sim}\;nm$200 produced by EEW in the methanol were mixed and well coated with the atomized Fe amorphous powders through the simple drying process on the hot plate. The relative density of the compacts obtained by the SPS showed over 98% and its hardness was also found to reach over 1100 Hv.

• Journal of Welding and Joining
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• 제33권2호
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• pp.23-31
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• 2015

Stainless steel is used in automobile muffler and exhaust systems. However, in comparison with other steels it has a high thermal expansion rate and low thermal conductivity, and undergoes excessive thermal deformation after welding. To address this problem, we evaluated the use of arc brazing in place of welding for the processing of an exhaust system, and investigated the parameters that affect the joint characteristics. Muffler parts STS439 and hot-dipped Al coated steel were used as test specimens, and CuAl brazing wire was used as the filler metal for the cold metal transfer (CMT) welding machine, which is a low heat input arc welder. In addition, a Box-Behnken design of experiment was used, which is a response surface methodology. The main process parameters (current, speed, and torch angle) were used to determine the appropriate welding quality and the mechanical properties of the brazing part was evaluated at the optimal welding condition. The optimal processing condition for arc brazing was 135A current, 51cm/min speed and $74^{\circ}$ torch angle. The process was applied to an actual exhaust system muffler and the prototype was validated by thermal fatigue, thermal shock, and endurance limit tests.

• 대한기계학회논문집B
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• 제25권12호
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• pp.1869-1878
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• 2001

Experiments are carried out to investigate the effect of pulsations on the flow and heat transfer characteristics of an axisymmetric impinging jet on a flat plate heated by using a gold coated aim. Vertex motion in the impinging jet is visualized using a fog generator, and a thermochromatic liquid crystal (TLC) technique is used to measure the time averaged local temperature distributions on the impingement plate. In addition, the quantitative data for mean velocity and turbulence intensity are obtained employing hot-wire anemometer. Parameters such as pulsating frequency (f = 0, 10 and 20 Hz) and the nozzle-to-palate spacing (H/D = 2, 10) are considered at the jet Reynolds number of 20,000. Consequently, the significant changes of flow structure and local Nusselt number distribution due to pulsations are observed. In the case of H/D = 2, the enhanced heat transfer coefficient exceeding 30 % is observed at the stagnation point. At the high H/D, heat transfer rate increases with pulsation frequency.