• 제목/요약/키워드: Transition region

검색결과 956건 처리시간 0.03초

Change in the Order of the Phase Transition in Triglycine Selenate Crystal

  • Song, Yong-Won
    • The Korean Journal of Ceramics
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    • 제6권1호
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    • pp.6-8
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    • 2000
  • The specific heat of a partly deuterated triglycine selenage (DTGSe) crystal under $\gamma$-irradiation was measured. It was shown that $\gamma$-irradiation defects changed the thermodynamic behavior of DTGSe crystal in a small dose region. The order of the phase transition changed from the first to the second at D=0.3 MR.

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Analysis of Mixed Grade Transition in Continuous Thin Slab Casting with EMBR

  • J.H. Ahn;J.K. Yoon;이정의
    • 소성∙가공
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    • 제8권3호
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    • pp.271-271
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    • 1999
  • A concentration change during grade transition operation in thin slab casting is investigated through computer simulation and the results are compared with experimental measurements. Fluid flow and mixing patterns in various tundish levers and flow rates were analysed by a three-dimensional mathematical model. Based on the contained results, a simple, efficient and accurate computational model is suggested to predict the concentration profile at the outlet of the tundish. Based on the model, mixing in and below the mold was analyzed considering electromagnetic braking force. The predicted concentration profiles show good agreements with the measured values. It is found that the lower vortices in the mold are suppressed by the electromagnetic field and a plug-like flow region develops, which decreases the intermixing of two different grades of steel and shortens the length of transition region.

수중익 경계층의 천이영역에 미치는 표면조도의 영향 (Surface Roughness Effects on Boundary Layer Transition Region for Hydrofoil)

  • 문철진;김시영
    • 수산해양기술연구
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    • 제30권2호
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    • pp.116-124
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    • 1994
  • There has been studied a lot of two dimensional hydrofoil sections for the boundary layers. This paper suggests that the plaiable roughness effects on boundary layer transition region of suction side for NACA 4412 hydrofoil sections provided by auxieiary shape factor and lag-entrainment effects. These results show that the laminar sepration. Transition and end of transition of the boundary layer due to pitting roughness effects, to the foil Reynold's number as well as to the angle of attack were delayed a little. And comparisons with valuable the other calculations and measurements show qualitative agreements.

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DSMC법을 이용한 터보분자펌프 다단 익렬의 2차원 유동장 해석 (Analysis of two-dimensional flow fields in the multi-stage turbomolecular pump using the DSMC method)

  • 황영규;허중식;박종윤
    • 설비공학논문집
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    • 제12권1호
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    • pp.83-94
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    • 2000
  • The performance of a turbomolecular pump(TMP) in both molecular and transition flow regions is predicted by the numerical solutions of the Boltzmann equation obtained by the direct simulation Monte Carlo method. The compression characteristics of the TMP are investigated for a wide range of the Knudsen number( Kn ). The maximum compression ratios strongly depend on Kn in transition region, while do they weakly on Kn in free molecular flow region. The present numerical results of the single blade row in both molecular and transition regions are used to predict the overall performance of a TMP, which has three kinds of blade with 24-rows.

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자연대류 경계층의 천이특성에 대한 실험적 연구 (Experimental study of natural transition in natural convection boundary layer)

  • 황성충;요시프 무스타파;임희창
    • 한국가시화정보학회지
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    • 제20권1호
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    • pp.29-37
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    • 2022
  • We carried out a laboratory experiment about the thermo-fluidic characteristics of natural convection boundary layer over a vertical heated plate under constant heat flux condition. Particle image velocimetry has been applied to observe the surface convection velocity close to the vertical plate submerged in the water chamber with the condition of Ra = 7 × 109 and Pr = 8.1. The velocity distributions indicate that the distinct stripe-like structures appears in the upstream (earlier transition region) and the distinct negative-positive and Λ(λ)-shaped flow structures in the downstream (mid-transition region). In addition, the temporal variation of spanwise and streamwise velocity is also presented.

다층 층간분리된 적층 판의 유한요소 자유진동해석 (Finite Element Analysis for Free Vibration of Laminated Plates Containing Multi-Delamination)

  • Taehyo Park;Seokoh Ma
    • 한국전산구조공학회:학술대회논문집
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    • 한국전산구조공학회 2003년도 가을 학술발표회 논문집
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    • pp.37-44
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    • 2003
  • In this proposed work, computational, finite element model far multi-delaminated plates will be developed. In the current analysis procedures of multi-delaminated plates, different elements are used at delaminated and undelaminated region separately. In the undelaminated region, plate element based on Mindlin plate theory is used in order to obtain accurate results of out-of-plane displacement of thick plate. And for delaminated region, plate element based on Kirchhoff plate theory is considered. To satisfy the displacement continuity conditions, displacement vector based on Kirchhoff theory is transformed to displacement of transition element. Element mass and stiffness matrices of each region (delaminated, undelaminated and transition region) will be assembled for global matrix.

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Conformational Transition of Form II to Form Ⅰ PoLy(L-proline) and the Aggregation of Form Ⅰ in the Transition: Water-Propanol Solvent System

  • 김현돈
    • Bulletin of the Korean Chemical Society
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    • 제18권9호
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    • pp.922-928
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    • 1997
  • The conformational transition of poly(L-proline) (PLP), Form Ⅱ → Form Ⅰ and the intermolecular aggregation of the product, Form Ⅰ, during and after the transition in water-propanol (1:7, 1:9, 1:15.7, and 1:29 v/v) were studied. For the study, the viscosity change and excess light scattering intensity were measured in the course of the transition which was determined by the Form Ⅰ fraction, fI of the sample solution. For the PLP sample of molecular weight Mv=31,000 the experimental results show that the reaction course is roughly divided into three regions: in the first region [fI=0.27 to 0.40 (- [α]D=400 to 330)], the conformational change of Form Ⅱ → Form Ⅰ occurs with decrease of viscosity, in the second region [fI=0.40 to 0.80 (- [α]D=330 to 120)], a partial side-by-side (p-S-S) type aggregation in which Form Ⅰ blocks interact with each other, which induces the increase of viscosity, starts to occur, and in the third region [fI=0.80 to 1.00 (- [α]D=120 to 15)], a side-by-side type (raft like) aggregation of Form Ⅰ or an end-to-end (E-E) type aggregation occurs according to the solvent situation, i.e., in a water-rich medium [water-propanol (1:9 or 1:7 v/v)], the (S-S) type aggregation with a gross decrease in viscosity occurs while in a water-poor medium [water-propanol (1:29 or 1:15.7 v/v), the (E-E) type aggregation with a large increase in viscosity occurs. The (S-S) type aggregation was promoted at high temperatures. Based on the structure of PLP, a reasonable mechanism for the (p-S-S) and (S-S) aggregation which occurs with the transition of Form Ⅱ → Form Ⅰ is considered. The suggested mechanism was also supported by the result of chain length effect of PLP for the aggregation.

발달하는 원형제트의 간헐적 유동에 관한 실험적 연구 (An Experimental Study About The Intermittent Flow Field in The Transition Region of a Turbulent Round Jet)

  • 김숭기;조지룡;정명균
    • 대한기계학회논문집
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    • 제14권1호
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    • pp.230-240
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    • 1990
  • 본 연구에서는 원형제트의 천이영역에서 속도신호를 측정하고 이로부터 간헐 도와 간헐주파수를 구하며 이를 사용한 지역평균법으로 난류특성량들을 구하여 천이영 역에서의 난류구조를 해석하고 난류 모델링을 위해 필요한 기초자료를 제공하고자 한 다. 난류강도, 레이놀즈응력, 속도성분의 3차상관 관계등의 레이놀즈평균과 지역평 균들을 제시하였고, 편평도, 비대칭도등의 통계학적인 해석과 확산항에 대한 검토도 행하였다.

파형벽면이 있는 채널 유동의 응집 구조 연구 (COHERENT STRUCTURES IN DEVELOPING FLOW OVER A WAVY WALL)

  • 장경식
    • 한국전산유체공학회지
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    • 제17권2호
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    • pp.93-99
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    • 2012
  • The present study focuses on the case of developing flow with in a channel containing a long array of sinusoidal waves (2a/${\lambda}$=0.1, ${\lambda}$=h, ${\lambda}$ is the wavelength, 2a is the wave height, h is the mean channel depth) at the bottom wall. The Reynolds number defined with channel height, h and the mean velocity, U, is Re=6,700. The channel is sufficiently long such that transition is completed and the flow is fully developed over the downstream half of the channel. For the case of an incoming steady flow with no resolved turbulence, the instantaneous flow fields in the transition region are characterized by the formation of arrays of highly-organized large-scale hairpin vortices whose dimensions scale with that of the roughness elements. The paper explains the mechanism for the formation of these arrays of hairpin vortices and shows these eddies play the primary role in the formation of the large-scale streaks of high and low velocity over the wavy wall region. The presence of resolved turbulence in the incoming flow, reduces the streamwise distance needed for the streaks to develop over the wavy region, but does not affect qualitatively the transition process. In the fully-developed region, isolated and trains of large-scale hairpins play an important role in the dynamics of the streaks over the wavy wall.

NONTHERMAL BROADENING OF UV LINES OBSERVED AT THE LIMB OF THE QUIET SUN

  • LEE HVUNSOOK;YUN HONG SIK;CHAE JONGCHUL
    • 천문학회지
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    • 제33권1호
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    • pp.57-73
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    • 2000
  • We have done a spectroscopic study of the solar transition region using high resolution UV & EUV data obtained by SUMER(Solar Ultraviolet Measurements of Emitted Radiation) on board SOHO(Solar and Heliospheric Observatory). Optically thin and conspicuous emission lines observed at the solar limb are carefully selected to acquire average values of physical parameters for the quiet region as a function of radial distance. Our main results found from the present study can be summarized as follows. 1) Nonthermal velocities estimated from various UV lines do not decrease with height at least within one total line intensity scale height above the limb. 2) Nonthermal velocity distribution with temperature is very similar to that of the disk center, in the sense that its peak is located around $2{\times}10^5 K$, but the value is systematically larger than that of the disk. 3) It is found that nonthermal velocity is inversely proportional. to quadratic root of electron density up to about 10 arc seconds above the limb, i.e. ${\xi}\~N_e^{-1/4}$, implying that the observed nonthermal broadening can be attributed to Alfven waves passing through the medium. 41 Electron density estimated from the O V 629/760 line ratio is found to range from about $1{\times}10^{10}cm^{-3}$ to $2{\times} 10^{12}cm^{-3}$ in the transition region.

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