본 논문에서는 접지된 유전체평면 위에 변하는 저항율을 갖는 저항띠 격자구조의 전자파 산란문제를 수치해석 방법인 FGMM(Fourier-Galerkin Moment Method)을 이용하여 스트립 폭 및 주기, 유전체층의 비유전율 및 두께, 입사각에 따라 수치 해석하였다. 산란전자계는 Floquet 모드함수의 급수로 전개하였다. 경계조건은 미지의 계수를 구하기 위하여 적용하였고, 저항띠 경계조건은 접선성분의 전계와 스트립의 유도전류와의 관계를 위해 이용하였다. 저항띠의 변하는 저항율은 저항띠의 양끝에서 0으로 변하는 경우를 취급하였고, 이때 유도되는 표면 전류밀도는 2종 Chebyshev 다항식의 급수로 전개하였다. 본 논문에서 변하는 저항율이 0을 갖는 도체띠에 대한 정규화 된 반사전력은 기존 논문의 결과와 매우 잘 일치하였다.
본 논문에서는 접지된 2개의 유전체평면 위에 저항띠 양끝에서 0으로 변하는 저항율을 갖는 저항띠 격자구조의 전자파 산란문제를 수치해석 방법인 FGMM(Fourier-Galerkin Moment Method)을 이용하여 스트립 폭 및 주기, 유전체층의 비유전율 및 두께, 입사각에 따라 수치해석하였다. 산란전자계는 Floquet 모드함수의 급수로 전개하였다. 경계조건은 미지의 계수를 구하기 위하여 적용하였고, 저항띠 경계조건은 접선성분의 전계와 스트립의 유도전류와의 관계를 위해 이용하였다. 저항띠의 변하는 저항율은 저항띠의 양끝에서 0으로 변하는 경우를 취급하였고, 이때 유도되는 표면 전류밀도는 2종 Chebyshev 다항식의 급수로 전개하였다. 본 논문에서 변하는 저항율이 0을 갖는 정규화된 반사전력은 기존 논문의 결과와 매우 잘 일치하였다.
Two polyethylene tubes were inserted into the esophagus of anesthetized rabbit in order to record the fluctuation of the intraluminal pressure through the orifices located near the tips of the tubes. The orifice of the first tube was 10 cm apart from the incisor of the rabbit and the orifice of the second tube was 5 cm below that of the first one. The tubes were filled with saline solution running at various rates ranging from 1.5 ml/min. to 4.2 ml/min. The tubes were connected to the pressure transducers and the electrical signals were recorded by the physiograph. When the peristaltic wave approached to the orifice a rise in the pressure was recorded, returning to the base line when the portion of the orifice was quiescent. The frequency of the peristaltic motion and the velocity of the wave were studied in connection with the flow rate of saline solution through the tubes and in the case of massive acute hemorrhage. The results obtained were as follows: 1. There was reflux of fluid induced during the procedure of the experiment. This outwrad flow through the pharynx seemed to elicite swallowing reflexes. Accordingly, the frequency of peristalsis of the esophagus was largely dependent on the flow rate of the fluid through the inserted tubes. By the flow rate of 1.5 ml/min., 2.5 ml/min., or 4.2 ml/min., the frequencies of the peristalsis were revealed to be
The gas hydrate exploration using seismic reflection data, the detection of BSR(Bottom Simulating Reflector) on the seismic section is the most important work flow because the BSR have been interpreted as being formed at the base of a gas hydrate zone. Usually, BSR has some dominant qualitative characteristics on seismic section i.e. Wavelet phase reversal compare to sea bottom signal, Parallel layer with sea bottom, Strong amplitude, Masking phenomenon above the BSR, Cross bedding with other geological layer. Even though a BSR can be selected on seismic section with these guidance, it is not enough to conform as being true BSR. Some other available methods for verifying the BSR with reliable analysis quantitatively i.e. Interval velocity analysis, AVO(Amplitude Variation with Offset)analysis etc. Usually, AVO analysis can be divided by three main parts. The first part is AVO analysis, the second is AVO modeling and the last is AVO inversion. AVO analysis is unique method for detecting the free gas zone on seismic section directly. Therefore it can be a kind of useful analysis method for discriminating true BSR, which might arise from an Possion ratio contrast between high velocity layer, partially hydrated sediment and low velocity layer, water saturated gas sediment. During the AVO interpretation, as the AVO response can be changed depend upon the water saturation ratio, it is confused to discriminate the AVO response of gas layer from dry layer. In that case, the AVO modeling is necessary to generate synthetic seismogram comparing with real data. It can be available to make conclusions from correspondence or lack of correspondence between the two seismograms. AVO inversion process is the method for driving a geological model by iterative operation that the result ing synthetic seismogram matches to real data seismogram wi thin some tolerance level. AVO inversion is a topic of current research and for now there is no general consensus on how the process should be done or even whether is valid for standard seismic data. Unfortunately, there are no well log data acquired from gas hydrate exploration area in Korea. Instead of that data, well log data and seismic data acquired from gas sand area located nearby the gas hydrate exploration area is used to AVO analysis, As the results of AVO modeling, type III AVO anomaly confirmed on the gas sand layer. The Castagna's equation constant value for estimating the S-wave velocity are evaluated as A=0.86190, B=-3845.14431 respectively and water saturation ratio is
The purpose of this paper is to seek ways to improve the competitiveness of Korea's fashion industry by utilizing the source of competitiveness of Japan's fashion industry, which represents the world's leading countries in terms of fashion, so that Korea can better enter the global fashion market. The study shall first compare the competitiveness of the Japanese and Korean fashion industries by utilizing the generalized double diamond model; second, provide an understanding of what the Japanese fashion industry can offer to Korean fashion industry and companies - that is, understand what the Japanese fashion industry's competitive edge is; and third, study the kind of global competitiveness that Korea's fashion industry must achieve. To adopt a generalized double diamond model to compare the competitiveness of the Korean and Japanese fashion industries, we selected 31 sub-variables to act as determinants of the model. That is, we extracted 31sub-variables by doing research of literature to analyze national competitiveness of the fashion industries. To measure these 31 sub-variables, secondary data was gathered. We collected data related to each sub-variable from various sources of Korea and Japan. And to calculate the competitiveness index, we took three steps with reference to previous studies. We found that status of the fashion industry of the two countries as it stands. That is, Japan is an advanced country of which fashion industry is domestic market-oriented while Korea is a small open economy that mainly focuses on the foreign market. Out of 31 proxy variables, Korea's fashion industry shows higher measurements relating to production and export than Japan, but Japan's fashion industry reports higher measurements than Korea in the fields of R&D, design and brand power, the rate of value added, the efficiency of companies and globalization. In order for Korea's fashion industry to achieve competitiveness in the global market, it should pursue the following development direction. First, it is very difficult for Korea to follow the footsteps of the U.S. and Japanese fashion industries that are able to take advantage of economies of scale, because Korea is smaller than those countries. Therefore, in the case of small economies such as Singapore, strengthening of international activities will practically improve domestic determinants that Korea should improve its domestic diamond by enhancing the current competitiveness of its international diamond. In other words, Korea needs to further endeavor to develop and expand global resources and markets as well as improve its competitiveness in terms of R&D, design and brand power, the rate of value-added, and the efficiency of companies. As the Korean fashion industry shows relatively advanced level of information technology and the fashion education system, it has considerable potential to grow. Korea is expected to have a huge growth potential since it has relatively higher level of information technology, fashion education system and activities than those of Japan in both the domestic diamond and international diamond. In particular, a better environment is laid out before Korea to gain competitiveness in the fashion industry due to the recently growing influence of the Korean Wave that Korea is expected to grow as a leader in the Asian market as well as in the global market.
현대사회의 병리현상 중에서 매우 심각하게 문제를 야기하는 "중독(中毒)" 현상에 대한 도가철학적 해석과 해결 방안을 모색하는 것이 본고의 의도이다. 이를 위해 철학적 사유의 지평에서 중독을 관조는 법을 구명하였다. 질병은 고정불변의 실체를 지니는 존재자가 아니라 균형과 조화를 상실한 일종의 현상으로서 파악해야 한다. 이에 대한 치료는 해독약으로서의 약(藥)을 처방할 수 있다. 약 자체가 독약과 양약의 구분이 모호한 물질적 존재로서, 조화와 균형의 시각에서 약을 다루어야만 중독 현상의 해결에 유효할 수 있다. 중독 현상을 보는 도가철학의 관점은 만물의 개별자가 지니는 욕망의 일탈 또는 욕망의 과잉으로 빚어진 병리 현상이다. 개별자는 우주자연의 변화과정 속에 일시적으로 존재하는 과정적 존재일 뿐이다. 이런 도가적 세계관을 계승하는 유파로서의 한의철학이 있다. 도가적 한의철학의 지평에서 중독 현상은 마음의 조화와 균형을 잃는 것에서 온다. 해결의 방법도 마음의 혼란 상태[마(魔)]를 안정시키는 것에서 시작한다. 병리현상으로서의 중독은 실제로는 실체적 본질이 없다. 질병 현상은 삶의 어떤 계기나 인연에 의하여 조금씩 쌓여 견고하게 굳어진 일종의 일시적 현상일 뿐, 영원한 본질이 있는 악의 표상이 아니다. 이런 이치를 자각하는 순간 그런 병리현상에서 벗어날 수 있는 길이 열린다. 도가철학의 진단과 처방은 단호하다. 욕망의 일탈이 바로 병리현상을 일으킨다. 과유불급(過猶不及)이다. 과(過)와 불급(不及) 사이의 조화와 균형을 찾는 일이 중요하다. 그리하면 병리적 중독과 같은 모든 시름은 우주변화의 풍랑에 씻기어 간다.
A comprehensive numerical study is carried out to investigate for the understanding of the flow evolution and flame development in a supersonic combustor with normal injection of ncumally injecting hydrogen in airsupersonic flows. The formulation treats the complete conservation equations of mass, momentum, energy, and species concentration for a multi-component chemically reacting system. For the numerical simulation of supersonic combustion, multi-species Navier-Stokes equations and detailed chemistry of H2-Air is considered. It also accommodates a finite-rate chemical kinetics mechanism of hydrogen-air combustion GRI-Mech. 2.11[1], which consists of nine species and twenty-five reaction steps. Turbulence closure is achieved by means of a k-two-equation model (2). The governing equations are spatially discretized using a finite-volume approach, and temporally integrated by means of a second-order accurate implicit scheme (3-5).The supersonic combustor consists of a flat channel of 10 cm height and a fuel-injection slit of 0.1 cm width located at 10 cm downstream of the inlet. A cavity of 5 cm height and 20 cm width is installed at 15 cm downstream of the injection slit. A total of 936160 grids are used for the main-combustor flow passage, and 159161 grids for the cavity. The grids are clustered in the flow direction near the fuel injector and cavity, as well as in the vertical direction near the bottom wall. The no-slip and adiabatic conditions are assumed throughout the entire wall boundary. As a specific example, the inflow Mach number is assumed to be 3, and the temperature and pressure are 600 K and 0.1 MPa, respectively. Gaseous hydrogen at a temperature of 151.5 K is injected normal to the wall from a choked injector.A series of calculations were carried out by varying the fuel injection pressure from 0.5 to 1.5MPa. This amounts to changing the fuel mass flow rate or the overall equivalence ratio for different operating regimes. Figure 1 shows the instantaneous temperature fields in the supersonic combustor at four different conditions. The dark blue region represents the hot burned gases. At the fuel injection pressure of 0.5 MPa, the flame is stably anchored, but the flow field exhibits a high-amplitude oscillation. At the fuel injection pressure of 1.0 MPa, the Mach reflection occurs ahead of the injector. The interaction between the incoming air and the injection flow becomes much more complex, and the fuel/air mixing is strongly enhanced. The Mach reflection oscillates and results in a strong fluctuation in the combustor wall pressure. At the fuel injection pressure of 1.5MPa, the flow inside the combustor becomes nearly choked and the Mach reflection is displaced forward. The leading shock wave moves slowly toward the inlet, and eventually causes the combustor-upstart due to the thermal choking. The cavity appears to play a secondary role in driving the flow unsteadiness, in spite of its influence on the fuel/air mixing and flame evolution. Further investigation is necessary on this issue. The present study features detailed resolution of the flow and flame dynamics in the combustor, which was not typically available in most of the previous works. In particular, the oscillatory flow characteristics are captured at a scale sufficient to identify the underlying physical mechanisms. Much of the flow unsteadiness is not related to the cavity, but rather to the intrinsic unsteadiness in the flowfield, as also shown experimentally by Ben-Yakar et al. [6], The interactions between the unsteady flow and flame evolution may cause a large excursion of flow oscillation. The work appears to be the first of its kind in the numerical study of combustion oscillations in a supersonic combustor, although a similar phenomenon was previously reported experimentally. A more comprehensive discussion will be given in the final paper presented at the colloquium.
본 연구는 세계 최대의 프랜차이즈 시장으로 부상하고 있는 중국 프랜차이즈 시장에서 가맹 본부와 가맹점 간의 재계약 성과에 영향을 미치는 요인에 관한 연구이다. 선행 연구를 토대로 하여 프랜차이즈 재계약 결정요인으로서 가맹본부특성, 가맹점 특성, 본부와 가맹점간 관계적 특성, 환경적 특성 등 4가지로 설정하고, 가맹본부 특성, 가맹점 특성, 관계적 특성, 환경적 특성을 본부의 경영성과와 가맹점에 대한 만족도 영향변수로, 본부의 경영성과와 본부의 가맹점에 대한 만족도를 재계약의도의 영향변수로 하여 연구모형을 설정하였다. 이러한 연구모형을 실증적으로 검증하기 위하여 중국 프랜차이즈 시장에서 가맹본부를 중심으로 설문조사를 실시하여 실증분석을 하였다. 설정한 가설 중에서 경영성과 영향요인으로서 본부특성, 가맹점특성, 관계적 특성, 환경적 특성 요인이 영향을 미치는 것으로 나타났으나, 본부특성 구성요인 중 가맹점에 대한 통제와 관계적 특성 중 몰입은 경영성과에 유의한 영향을 미치지 않는 것으로 나타났다. 본부의 가맹점에 대한 만족도 영향요인으로는 가맹점 특성이 채택되었지만 관계적 특성인 신뢰, 몰입과 갈등 변수등도 유의하지 않은 것으로 나타났다. 가맹본부의 경영성과와 가맹점에 대한 만족은 가맹본부의 재계약 의도를 높이는 것으로 나타났다. 이러한 연구분석 결과는 중국 시장에 이미 진출해 있거나 향후 진출하려는 국제 프랜차이즈 기업의 전략적 분석과 수립에 도움이 될 구체적인 실무지식을 제공해 줄 수 있을 것으로 기대된다.
The wall shear stress in the vicinity of end-to end anastomoses under steady flow conditions was measured using a flush-mounted hot-film anemometer(FMHFA) probe. The experimental measurements were in good agreement with numerical results except in flow with low Reynolds numbers. The wall shear stress increased proximal to the anastomosis in flow from the Penrose tubing (simulating an artery) to the PTFE: graft. In flow from the PTFE graft to the Penrose tubing, low wall shear stress was observed distal to the anastomosis. Abnormal distributions of wall shear stress in the vicinity of the anastomosis, resulting from the compliance mismatch between the graft and the host artery, might be an important factor of ANFH formation and the graft failure. The present study suggests a correlation between regions of the low wall shear stress and the development of anastomotic neointimal fibrous hyperplasia(ANPH) in end-to-end anastomoses. 30523 T00401030523 ^x Air pressure decay(APD) rate and ultrafiltration rate(UFR) tests were performed on new and saline rinsed dialyzers as well as those roused in patients several times. C-DAK 4000 (Cordis Dow) and CF IS-11 (Baxter Travenol) reused dialyzers obtained from the dialysis clinic were used in the present study. The new dialyzers exhibited a relatively flat APD, whereas saline rinsed and reused dialyzers showed considerable amount of decay. C-DAH dialyzers had a larger APD(11.70
The wall shear stress in the vicinity of end-to end anastomoses under steady flow conditions was measured using a flush-mounted hot-film anemometer(FMHFA) probe. The experimental measurements were in good agreement with numerical results except in flow with low Reynolds numbers. The wall shear stress increased proximal to the anastomosis in flow from the Penrose tubing (simulating an artery) to the PTFE: graft. In flow from the PTFE graft to the Penrose tubing, low wall shear stress was observed distal to the anastomosis. Abnormal distributions of wall shear stress in the vicinity of the anastomosis, resulting from the compliance mismatch between the graft and the host artery, might be an important factor of ANFH formation and the graft failure. The present study suggests a correlation between regions of the low wall shear stress and the development of anastomotic neointimal fibrous hyperplasia(ANPH) in end-to-end anastomoses. 30523 T00401030523 ^x Air pressure decay(APD) rate and ultrafiltration rate(UFR) tests were performed on new and saline rinsed dialyzers as well as those roused in patients several times. C-DAK 4000 (Cordis Dow) and CF IS-11 (Baxter Travenol) reused dialyzers obtained from the dialysis clinic were used in the present study. The new dialyzers exhibited a relatively flat APD, whereas saline rinsed and reused dialyzers showed considerable amount of decay. C-DAH dialyzers had a larger APD(11.70