• Bulletin of the Korean Chemical Society
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• 제23권2호
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• pp.325-329
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• 2002

In this study, the dependency of the behavior of propagating front on the reaction condition in frontal polymerization reaction has been studied. We have used some multifunctional acrylates as a monomer and ammonium persulfate as an initiator for the polymerization reactions. In frontal polymerization, a method of producing polymeric materials via a thermal front that propagates through the unreacted monomer/initiator solution, the behavior of self propagating front shows various dynamic patterns depending on the reaction condition. We have obtained some spin modes of propagating front in the number of 'hot spots' or 'spin heads' by changing the reaction condition. The effect of the reactor tube diameter on the mode of propagating front has also been studied by using some reactor tubes with different size of tube diameter and it has been examined in some detail by adopting an experimental method of two-tubes system.

• 대한기계학회논문집B
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• 제30권1호
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• pp.67-73
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• 2006

This investigation deals with the spin-up flows in a circular container of aspect ratio, 2.0. Shear front is generated in the transient spin-up process and propagating from the side wall to the central axis in a rotating container. Propagation of the shear front to the axis in a rotating container means the region acquires an angular momentum transfer from the solid walls. Propagating speed of the shear front depends on the apparent viscosity of polymer solution. Two kinds of polymer solutions are considered as a working fluid: one is CMC and the other is CTAB solution. CMC solution has larger apparent viscosity than that of water, and CTAB shows varying apparent viscosities depending on the applied shear rates. Transient and spatial variations of the apparent viscosities of the present polymer solutions (CTAB and CMC) cause different speeds of the propagating shear front. In practice, CMC solution that has larger values of apparent viscosity than that of water always shows rapid approach to the steady state in comparison of the behavior of the flows with water. However, for the CTAB solution, the speed of the propagating of the shear front changes with the local magnitude of its apparent viscosity. Consequently, the prediction of Wedemeyer's model quantitatively agrees with the present experimental results.

• 대한기계학회논문집
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• 제1권4호
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• pp.182-189
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• 1977

The propagating flame temperature of the Propane-Air premixture by using 30.$\mu$ and 50.$\mu$ diameter platinum sensing wires, that is, Two Wires Correction Method, Through the constant volume burining inside the 150mm diameter, 30mm height combustion chamber under the circumstances of the atomospheric pressure, and the room temperature was determined. Also the temperature distribution across High Temperature Region, i.e. Flame Front, and the temperature profile behind the flame the front have been obtained.

• Journal of Advanced Marine Engineering and Technology
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• 제29권8호
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• pp.849-854
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• 2005

The laminar flame concept in turbulent reacting flow is considered applicable to many practical combustion systems For turbulent premixed combustion under widely used flamelet concept, the flame surface is described as an infinitely thin propagating surface that such a Propagating front can be represented as a level contour of a continuous function G. In this study, for the Purpose of validating the LES of G-equation combustion model. LES of turbulent Premixed combustion with dynamic SGS model of G-equation in turbulent channel flow are carried out A constant density assumption is used. The Predicted flame propagating speed is goof agreement with the DNS result of G. Bruneaux et al.

• 한국가스학회지
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• 제12권1호
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• pp.54-61
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• 2008

Experimental investigations were performed to assess the influences of different multiple obstacles on flame propagation in a rectangular confinement. Three different multiple obstacles were used: circular, triangular and square cross-sections with blockage ratios of 15% and 30%. The same method described in Park et al. [13] to investigate the interaction between the propagating flame and the obstacle was applied. Before the freely propagating flame impinged on the obstacle, the flame propagation speed remains close to the laminar burning velocity, regardless of the obstacles used. The reported data revealed that the trend in increase of the local flame propagation speed is a result of the interaction between the obstacle and the propagating flame front behind the obstacle. The local speed was found to increase from a circular to a triangular and a square obstacle. The mean flame speed was found to be less dependent on both the obstacle types and the different blockage ratios used.

• 한국추진공학회:학술대회논문집
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• 한국추진공학회 2008년 영문 학술대회
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• pp.364-370
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• 2008

Spinning detonations propagating in a circular tube were numerically investigated with a one-step irreversible reaction model governed by Arrhenius kinetics. The time evolution of the simulation results was utilized to reveal the propagation mechanism of single-headed spinning detonation. The track angle of soot record on the tube wall was numerically reproduced with various levels of activation energy, and the simulated unique angle was the same as that of the previous reports. The maximum pressure histories of the shock front on the tube wall showed stable and unstable pitch modes for the lower and higher activation energies, respectively. The shock front shapes and the pressure profiles on the tube wall clarified the mechanisms of two modes. The maximum pressure history in the stable pitch remained nearly constant, and the single Mach leg existing on the shock front rotated at a constant speed. The high and low frequency pressure oscillations appeared in the unstable pitch due to the generation and decay of complex Mach interaction on the shock front shape. The high frequency oscillation was self-induced because the intensity of the transverse wave was changed during propagation in one cycle. The high frequency behavior was not always the same for each cycle, and therefore the low frequency oscillation was also induced in the pressure history.

• 한국세라믹학회지
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• 제31권10호
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• pp.1099-1106
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• 1994

It is suggested that the microstructural toughening process in the initial rising portion of R-curves observed in polycrystalline alumina should be different from the grain bridging mechanism identified in the long crack regime. Microcracking in the advancing crack front seems to be a prerequisite for the development of unbroken bridging ligaments behind the crack tip. In order to test such a proposition, attempts were made to identify experimentally the presence of microcracks in the frontal zone of propagating cracks. In-situ observation is made of crack growth in a miniature double cantilever beam specimen of a average grain size of 10 ${\mu}{\textrm}{m}$ alumina. Presence of a few microcracks was identified in front of crack tip on the propagating crack plane. The R-curves were re-evaluated based on the observation.

• 한국안전학회지
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• 제26권2호
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• pp.32-35
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• 2011

다중 장애물을 가지는 폭발챔버에서 전파하는 화염과 국부 장애물의 상관관계를 조사하기 위하여 실험적 연구를 수행하였다. 폭발챔버 높이 235 mm, 단면적 $1,000{\times}950\;mm^2$, 벤트면적 $1,000{\times}320\;mm^2$를 가지는 폭발챔버를 제작하였으며, 30% blockage ratio를 가지는 장애물을 챔버내에 설치하였다. 전파하는 화염과 장애물의 상관관계를 조사하기 위해 고속카메리를 사용하였다. 고속카메라로 얻어진 화염 이미지로부터 장애물 주위의 국부 화염전파 거동은 2가지 다른 방법, 즉 전파하는 화염전면(flame front)의 각 pixel point에서 산정된 평균 화염전파속도와 연소면적 증가(incremental burnt area)/화염전면 길이(flame front length) 관점에서 분석하였다. 분석결과, 2가지 방법으로 얻은 결과는 거의 일치하는 경향을 나타났으며, 전파하는 화염이 장애물의 전면과 상호 작용할 때 화염속도는 급격히 증가하다가 장애물의 후단면에서 약간 감소하고, 화염이 장애물 후단에서 재결합될 때 다시 급격히 증가하였다.

• 한국전자파학회논문지
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• 제8권6호
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• pp.665-680
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• 1997

본 논문에서는 350 MHz와 900 MHz 평면파에 노출된 다양한 모델의 인체 두부 내 비흡수율(specific abs sorption rate, SAR)의 분포를 해석하였다. 해석 방법은 유한차분시간영역(finite-difference time-domain, FDTD) 방법이며, 인체 두부 모델로서 균질 매질의 구형모델, 균질의 실질적인 형태를 갖는 모텔 그리고 실질적인 형태를 갖는 비균질 모델이 사용된다. 입사 평면파의 편파는 인체 길이방향과 일치하며, 진행방향은 뒤에서 암으로, 그리고 앞에서 뒤로 향하는 두 가지 경우를 다룬다. 얻어진 연구결과는 다음과 같다. 1) 세 가지 모델의 평균 SAR은 비슷하나 국부 SAR은 큰 차이가 있다. 2) 주파수가 900 MHz보다 두부의 공진이 일어나는 대역인 350 MHz에서 복사전력이 더 깊이 침투한다. 3) 후방입사 평변파의 경우에는 두부가 아닌 목 부근에서 "hot spot"이 일어난다. 4) 전방입사 평면파의 경우에는 900 MHz에서는 코, 350 MHz의 경우에는 입술 위와 턱 부분에 "hot spot"이 나타난다.

• 대한기계학회논문집
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• 제19권5호
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• pp.1280-1290
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• 1995

In order to investigate the compression wave propagating in a high-speed railway tunnel, a numerical calculation was applied to the wave phenomenon occurring in a model tunnel. Unsteady, one-dimensional inviscid or viscous flows were solved by an explicit TVD scheme, and the calculated flows were compared with the results of measurement in real tunnels. Tunnel noises caused by emission of the compression wave were characterized in terms of excess pressure of compression wave, pressure gradient in the wave front and width of the compression wave. Calculated attenuation, pressure gradient and width of compression wave with the propagating distance agreed with the results of measurement in the real tunnels. The results also show that tunnel noises are proportional to the train velocity entering the tunnel.