• 보존과학회지
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• 제25권1호
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• pp.61-76
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• 2009

광주읍성은 구 전남도청이 위치한 국립 아시아 문화전당 건립부지 내에서 지표조사 결과 확인된 유적이다. 성벽의 길이는 일부 유실구간을 제외하고 총 85.1m이며, 석벽을 축조하기 위하여 총 10종의 암석이 사용된 것으로 나타났다. 이중에서 석영안산암이 41.1%, 안산암이 35.7%로 가장 높은 점유율을 보였다. 석영안산암은 성벽을 축성하는 주석재로 사용되었으며, 안산암은 주로 큰 부재 사이를 채우기 위한 사잇돌로 사용되었다. 암석학적 및 지형학적으로 볼 때 축성암석의 산지일 가능성이 높을 것으로 판단되는 무등산 일대에 분포하는 암석들을 대상으로 각각의 성인적 동질성을 검토한 결과, 산출상태, 전암대자율, 구성광물의 종류, 상대적 함량 및 조직, 지구화학적 특징이 서로 아주 유사하였다. 또한 무등산 남서쪽 사면의 증심사 계곡을 따라 석영안산암의 노두에서는 암석의 채석 흔적이 산재한다. 따라서 광주읍성의 축성에 사용된 대량의 석재는 무등산 남서 사면에서 조달하였으며, 석재의 이동은 광주천을 이용하였을 가능성이 높았을 것으로 해석된다.

• 한국소음진동공학회논문집
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• 제14권7호
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• pp.604-611
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• 2004

It is well known that wall impedance essentially determines how sound wave transmits from one place to another. The wall impedance is related with its dynamic properties : for example, the mass, stiffness, and damping characteristics. It is noteworthy, however, that the wall impedance is also function of spatial characteristics of two spaces that is separated by the wall. This is often referred that the wall is not locally reacting. In this paper, we have attempted to see how the acoustic characteristics of the two spaces is affected by various structure parameters such as density, applied tension, and a normalized length of the wall. Calculations are conducted for two different modally reacting boundary conditions by modal expansion method. The variation of the Helmholtz mode and the structural-dominated mode are analyzed as the structure parameters vary. The displacement distribution of the structure, pressure and active intensity of the inside and outside cavity are presented at the Helmholtz mode and the structure-dominated mode. It is shown that the frequency characteristics are governed by both structure-and fluid-dominated mode. The results exhibit that the density of the structure is the most sensitive design parameter on the frequency characteristics for the coupling system as we could imagine in the beginning. The Helmholtz mode frequency decrease as density increases. However. it increases as applied tension and an opening size increase. The bandwidth of the Helmholtz mode is mainly affected by density of the structure and its opening size.

• 대한소아치과학회지
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• 제44권4호
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• pp.446-454
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• 2017

최근 개발된 bulk-fill 복합레진에 대한 연구가 많이 이루어지고 있지만 소아환자 치료에 사용할 수 있는 적절한 재료인지에 대한 연구는 부족한 실정이다. 따라서 본 연구의 목적은 유구치의 2급 와동에서 bulk-fill 복합레진과 전통적 복합레진의 와동 적합성을 비교 평가하는 것이다. 발치 된 80개의 유구치의 근심 또는 원심에 2급 와동을 형성한 후 4개의 군으로 무작위로 나누었다. 대조군은 전통적 복합레진인 Filtek$^{TM}$ Z-350 XT(FZ)으로 수복하고 나머지 3개의 군은 bulk-fill 복합레진인 Filtek$^{TM}$ Bulk Fill Posterior Restorative(FB), Tetric N-Ceram$^{(R)}$ BulkFill(TNC)과 Filtek$^{TM}$ Bulk Fill Flowable Restorative(FBF)으로 수복하였다. 모든 시편을 열순환 시행한 후 50% 질산은($AgNO_3$)용액에 침적시켰다. Micro-CT를 이용하여 전체 질산은의 침투 부피와 치경부의 변연누출 정도를 측정하였고 기포의 개수, 크기, 위치를 평가하였다. 질산은의 침투 부피에서 FB가 FZ보다 유의하게 낮은 값을 보였고(p < 0.05), TNC와 FBF는 FZ와 비슷한 값을 보였다. 치경부 부분의 변연누출 정도는 FBF가 FZ와 FB보다 유의하게 낮은 값을 보였다(p < 0.05). 기포의 개수와 크기는 4개 군 모두 유의한 차이가 없었으나 기포의 위치는 전통적 복합레진에서는 전체 기포의 83.3%가 수복물 내부에 분포하였고, bulk-fill 복합레진에서는 치은축면 선각에 많이 분포하였다. 유구치 2급 와동에서 bulk-fill 복합레진과 전통적 복합레진의 와동에 대한 적합성은 유사한 결과를 보여주었다. 따라서 소아의 치아우식증 수복치료 시 bulk-fill 복합레진이 유용하게 사용될 수 있을 것으로 보인다.

• Restorative Dentistry and Endodontics
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• 제20권2호
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• pp.627-643
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• 1995

The resistance to fracture of the restored tooth may be influenced by many factors, among these are the cavity dimension and the physical properties of the restorative material. The placement of direct composite resin restorations has generally been found to have a strengthening effect on the prepared teeth. It is the purpose of this investigation to study the relationship between the cavity isthmus and the fracture resistance of a tooth in composite resin restorations. In this study, MO cavity was prepared on the maxillary left first molar and then filled with composite resin. Three dimentional model with 3049 nodes and 2450 8-node blick elements was made by the serial photographic method and isthmus (1/4, 1/3, 1/2 and 2/3 of intercusplal distance between mesiobuccal cusp tip and mesiolingual cusp tip) was varied. Two types of model(B and R model) were developed. B model was assumed perfect bonding between the restoration and cavity wall and R model was left unfilled. A load of 1500N was applied vertically on the node from the lingual slope of the mesiobuccal cusp. The results were as follows : 1. There was a significant decrease of stress resulting in increase of fracture resistance in B model when compared with R model. 2. When it comes to stress distribution, the stress was concentrated in the facio-gingival line angle and the buccal side of the distal margin of the cavity in both Band R model. 3. With the increase of the isthmus width, the stress decreased in the area of the facio-gingival line angle, and increased in the area of facio-gingival line angle as well as the buccal side of the distal margin of the cavity in B model. In R model, the stress increased both in the area of facio-gingival line angle and the buccal side of the distal margin of the cavity, therefore the possibility of crack increased. 4. As the width of cavity increased, in B model, the direction of crack moved from horizontal to vertical on the facio-gingival line angle and the facio-pulpal line angle. In R model, the direction of the crack was horizontal on the facio-gingival line angle and moved from horizontal to the $45^{\circ}$ direction on the facio-pulpal line angle.

• 대한전자공학회논문지TC
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• 제38권7호
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• pp.14-21
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• 2001

본 논문에서는 유전체가 삽입된 공진기를 이용하여 C-band용 대역통과 여파기를 설계, 제작하였다. 공진기의 높이는 인접 유전체 공진기의 도파관 차단 주파수로부터 결정된다. 공진기의 지름은 도체 손실을 고려하여 유전체의 두 배로 결정하였다. 유전체 공진기의 공진주파수는 비소멸(non-decaying) 모드 해석법으로 계산하였다. 일반적으로 원통형 유전체 공진기의 공진주파수는 Cohn 모델로 해석하였는데, 이것은 공진기의 벽과 유전체벽 사이에서 전자파가 소멸(decaying)된다는 가정 하에 해석한 방법이다. 그러나， 이 방법은 근사적인 해석방법이다. 외부양호도(external quality factor)인 $Q_{ex}$는 Ansoft의 Maxwell 시뮬레이션 툴을 사용하여 결정하였다. 유전율 45인 유전체를 사용하여 설계한 대역통과 여파기는 5.065GHz의 중심주파수를 가졌다. 삽입손실은 1dB, 밴드 폭은 20MHz, 감쇠 특성은 30dB$(f_0{\pm}15MHz)$)로 설계목표에 만족함을 알 수 있다.

• 한국전산유체공학회지
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• 제10권1호
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• pp.80-86
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• 2005

In order to control the transonic flow field with a shock wave, a condensing flow was produced by an expansion of moist air on a circular bump model and shock waves were occurred in the supersonic parts of the fields. Furthermore, the additional passive technique of shock-boundary layer interaction using the porous wall with a cavity underneath was adopted in this flow field. The effects of these methods on the shock wave characteristics were investigated numerically. The result showed that the flow fields might be effectively controlled by the suitable combination between non-equilibrium condensation and the position of porous wall.

• 대한기계학회논문집
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• 제18권5호
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• pp.1288-1300
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• 1994

Mathematical modeling and numerical calculation on the flow and thermal characteristics induced by fire in a partial enclosure are performed. The solution procedures include the Shvab-Zeldovich approximation for the physical transport equations, low Reynolds number k-.epsilon. model for the turbulent fluid flow and Discrete Ordinate method(DOM) to calculate the radiative heat transfer. PMMA(Polymethylmethacrylate) is adopted as a solid fuel. Two different cases are considered : combustions with and without gas radiation occuring in a open cavity for variable pyrolyzing location of PMMA. When the fire source is located at the left-wall, the flow region of flame gas is limited at the left-wall and ceiling and recirculation region of inlet gas is formulated at neat the floor. In case of neglecting the radiative heat transfer, more large flame size and higher temperature is predicted. It is essential to consider the radiative heat transfer for analysis of fire phenomenon.

• 소성∙가공
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• 제21권2호
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• pp.96-100
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• 2012

Conventional injection molding system for producing extremely thin-wall parts such as Light Guide Plates(LGP's) for mobile displays is at the limit of its capability due to its tendency to develop frozen layers and the critical speed of injection. The molten polymer in the cavity freezes quickly as its heat is rapidly transferred to the mold base. Many attempts have been tried in the past to overcome this problem. The present study used the injection/compression molding technology to produce a thin-wall part, with enhanced features such as an automated mechanism for cutting gates. As a result, the total cycle time was reduced by almost 35 seconds, resulting in a productivity increase by 30%.

• 한국전산유체공학회:학술대회논문집
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• 한국전산유체공학회 2003년도 The Fifth Asian Computational Fluid Dynamics Conference
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• pp.187-188
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• 2003

In order to control the transonic flow field with shock wave, a condensing flow was produced by an expansion of moist air on a circular bump model and shock waves were occurred in the supersonic parts of the fields. Furthermore, the additional passive technique of shock - boundary layer interaction using the porous wall with a cavity underneath was adopted in this flow field. The effects of these methods on the shock wave characteristics were investigated numerically. The result showed that the flow fields might be effectively controlled by the suitable combination between non-equilibrium condensation and the position of porous wall.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2002년도 학술대회지
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• pp.159-160
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• 2002

New S-shaped aeroelastic mesoflaps are utilized to control normal shock/boundary-layer interactions. New generation of the mesoflaps is designed f3r a better rigidness and a good flow uniformity across the ulteractions. ,Major advantages of the mesoflap system can be a better total pressure recovery downstream of the interactions due to the lambda shock structure over the flap system, and a rehabilitation of the thickened boundary layer due to bleeding through a cavity underneath the flap system. Skin friction has been measured downstream of the interactions, using the laser interferometer skin friction (LISF) meter, which optically detects the rate of thinning of an oil film applied to the test surface. Various flap-thicknesses of the S-shaped mesoflap arrays are tested, and the results are compared to the solid-wall reference case. Overall, not much difference in the level of skin friction is noticed for the S-shaped flap arrays of various thicknesses, and its level is lower than the skin friction downstream of the solid-wall interaction