• 제목/요약/키워드: x-t Diagram

검색결과 37건 처리시간 0.023초

A central limit theorem for sojourn time of strongly dependent 2-dimensional gaussian process

  • Jeon, Tae-Il
    • 대한수학회지
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    • 제32권4호
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    • pp.725-737
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    • 1995
  • Let $X_t = (X_t^(1), X_t^(2))', t \geqslant 0$, be a real stationary 2-dimensional Gaussian process with $EX_t^(1) = EX_t^(2) = 0$ and $$ EX_0 X'_t = (_{\rho(t) r(t)}^{r(t) \rho(t)}), $$ where $r(t) \sim $\mid$t$\mid$^-\alpha, 0 < \alpha < 1/2, \rho(t) = o(r(t)) as t \to \infty, r(0) = 1, and \rho(0) = \rho (0 \leqslant \rho < 1)$. For $t > 0, u > 0, and \upsilon > 0, let L_t (u, \upsilon)$ be the time spent by $X_s, 0 \leqslant s \leqslant t$, above the level $(u, \upsilon)$.

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터널에서의 고속철도 압력파에 관한 X-t선도 이론 해석 (Theoretical x-t Diagram Analysis on Pressure Waves of High Speed Train in Tunnel)

  • 남성원;권혁빈
    • 한국철도학회논문집
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    • 제7권3호
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    • pp.200-207
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    • 2004
  • Theoretical study has been conducted to clarify pressure characteristics of KTX (Korea Train eXpress) in tunnel. The severe pressure change in tunnel may give rise to the ear-discomfort for passenger and fatigue for car body. Critical tunnel lengths which are induced by x-t diagram analysis can be applied to the experimental results measured by using the running test with atmospheric pressure sensors and portable data acquisition system in previous study. In this study, the tunnels from 200m to 4000m in length have been chosen for the investigation of tunnel length effects. We found that there are similar patterns of external pressure change for each critical tunnel length. The critical tunnel lengths are governed by train speed, train length and sonic velocity. And, the patterns of pressure wave in tunnel are classified into eight groups.

Possible Role of Disorder on Magnetostructural Transition in La1-xBaxMnO3

  • Kim, N.G.;Jung, J.H.
    • Journal of Magnetics
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    • 제12권3호
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    • pp.103-107
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    • 2007
  • Magnetic field induced structural transition has been systematically investigated for $La_{1-x}Ba_xMnO_3$ with the fine control of carrier doping $(0.15{\leq}x{\leq}0.20)$. Application of a magnetic field results in the suppression of the rhombohedral-orthorhombic transition temperature $(T_s)$ and the increase of insulator-metal transition temperature $(T_{MI})$. Near x = 0.17, where $T_S$ is similar to $T_{MI}$ at zero magnetic field, we found that the $T_S$ smoothly decreased with magnetic field even though it intersected the $T_{MI}$ near 3 T. Also, the magnetostructural phase diagram obtained from the temperature sweep and from the magnetic field sweep is not significantly modified. By comparing the magnetostructural transition in $La_{1-x}Sr_xMnO_3$, we have suggested that the large disorder originated from ionic size differences between La and Ba may weaken the sensitivity of the kinetic energy of $e_g$ electrons on the degree of lattice distortion in $La_{1-x}Ba_xMnO_3$.

INFRARED AND HARD X-RAY DIAGNOSTICS OF AGN IDENTIFICATION FROM THE AKARI AND SWIFT/BAT ALL-SKY SURVEYS

  • Matsuta, K.;Gandhi, P.;Dotani, T.;Nakagawa, T.;Isobe, N.;Ueda, Y.;Ichikawa, K.;Terashima, Y.;Oyabu, S.;Yamamura, I.;Stawarz, L.
    • 천문학논총
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    • 제27권4호
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    • pp.285-286
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    • 2012
  • We combine data from two all-sky surveys, the Swift/Burst Alert Telescope 22 Month Source Catalog and the AKARI Point Source Catalogue, in order to study the connection between the hard X-ray (> 10 keV) and infrared (IR) properties of local active galactic nuclei (AGN). We find two photometric diagnostics are useful for source classification: one is the X-ray luminosity vs. IR color diagram, in which type 1 radio-loud AGN are well isolated from other AGN. The second one uses the X-ray vs. IR color-color diagram as a redshift-independent indicator for identifying Compton-thick (CT) AGN. Importantly, CT AGN and starburst galaxies in composite systems can also be separated in this plane based upon their hard X-ray fluxes and dust temperatures. This diagram may be useful as a new indicator to classify objects in new surveys such as with WISE and NuSTAR.

X선 반가폭을 이용한 Al 2024-T3 합금의 피로수명예측에 관한 연구 (A Study on the Prediction of Fatigue Life in 2024-T3 Aluminium using X-ray Half-Value Breadth)

  • 조석수;김순호;주원식
    • 한국정밀공학회지
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    • 제17권1호
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    • pp.145-152
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    • 2000
  • X-ray diffraction method detects change of crystal lattice distance under material surface using diffraction angle 2$\theta$. This technique can be applied to the behavior on slip band and micro crack due to material degradation. The relation between half-value breadth and number of cycle has three stages which constitute rapid decrease in initial number of cycles, slight decrease in middle number of cycles and rapid decrease in final number of cycles. The ratio of half-value breadth takes a constant value on B/B$_{0}$-N diagram with loading condition except early part of fatigue life. The ratio of half-value breadth B/B$_{0}$ with respect to number of cycle to failure N$_{f}$ has linear behavior on B/B$_{0}$-log N$_{f}$ diagram. Therefore, in this paper the estimation of fatigue life by average gradient method has much less estimated mean error than the estimation of fatigue life by log B/B$_{0}$-log N/N$_{f}$ relation.elation.ation.

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2-프로판올과 톨루엔 혼합물질의 인화점 측정에 관한 연구 (Study on the Flash Point Determination of 2-Propanol-Toluene Mixtures)

  • 목연수;최재욱;김영일;최일곤;하동명
    • 한국안전학회지
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    • 제12권3호
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    • pp.114-119
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    • 1997
  • The lower flash points and upper flash points of 2-propanol and toluene mixtures were determined by air-blowing method instead of Tag-closed flash point tester. The relations between the flash points and the composition of the mixtures are as follows, $T_{F.L}=4.3182+6.0909X_1$ $T_{F.U}=39.3636-2.9091X_1$ As results, the experimental data and the estimated values from the relations are considerably agreed, and we could plotted the relative diagram between flash points and the explosive range.

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$(TMTSF)_2BF_4$의 압력-온도 상태도 연구 (Pressure-Temperature Phase Diagram of $(TMTSF)_2BF_4$)

  • 조연정
    • Progress in Superconductivity
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    • 제14권1호
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    • pp.24-29
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    • 2012
  • $(TMTSF)_2BF_4$ containing non-centrosymmetric anions is well known to exhibit a metal insulator transition around 37 K by ordering of the anions with a $q_2$=(1/2, 1/2, 1/2) wave vector. We established pressure-temperature phase diagram of the $(TMTSF)_2BF_4$ compound and showed that it can belong to the general phase diagram of the $(TMTSF)_2X$ family. Application of hydrostatic pressure decreases the anion ordering transition temperature and the superconducting state is finally stabilized below 3.77 K under 7.7 kbar. Magnetoresistance measurement on the $(TMTSF)_2BF_4$ under 7.8 kbar is performed but neither the field-induced spin-density-wave state nor the rapid oscillation is observed up to 9 T.

터널내 교행 열차의 풍압에 대한 특성법 해석 (Analysis for Characteristics Method on Wind Pressure of Trains Crossing in Tunnel)

  • 남성원
    • 한국철도학회논문집
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    • 제16권6호
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    • pp.454-459
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    • 2013
  • 열차가 터널에 고속으로 진입하면, 압력파가 발생한다. 열차 선두부의 진입에 의하여 발생한 압축파는 터널을 따라 진행되어 터널 출구에서 반사되어 팽창파로 되돌아오며, 후미부의 진입에 의하여 발생한 팽창파도 터널을 따라 전파되어 터널 출구에서 압축파로 반사되어 터널 입구로 되돌아 온다. 열차 선두부 및 후미부에 의하여 발생한 이러한 압력파는 터널 입구 및 출구에서 각각 반사되어 터널 내부를 왕복하며, 차량 객실에 탑승한 승객들에게는 이명감을 일으키고, 터널 출구에서는 환경소음의 일종인 미기압파를 발생시킨다. 터널에서의 큰 압력 변동은 터널의 최적 단면적 설계에도 주요 인자로 고려되고 있으며, 차체의 반복 피로 하중으로 작용하므로, 이에 대한 정량적 및 정성적 분석이 필요하다. 본 연구에서는 고정 격자계를 이용하여 개발한 특성 해법을 교행하는 열차에 대하여 적용하였으며, 교행시의 열차 선두부 및 후미부의 경계 조건식을 개발하여, X-t선도와 같이 해석하였다. 해석 결과, 교행 열차의 특정 터널진입 시간에 압력파 간의 상쇄가 일어남을 알 수 있었다.

철 초전도체에서 스핀 밀도 파와 $\pi$ 위상 차 초전도성의 상전이 그림 (Phase Diagram of Spin Density Wave and $\pi$ Phase Shifted Superconductivity in the Fe Pnictide Superconductors)

  • 이나영;최한용
    • Progress in Superconductivity
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    • 제11권2호
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    • pp.112-117
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    • 2010
  • We examine phase transition of the spin density wave and $\pi$ phase shifted superconductivity in the Fe pnictide superconductors. The phase diagram is described in the plane of the temperature T and the doping x with the combination of Ginzburg-Landau expansion of the free energy near the multi-critical temperature $T_c$ and the self-consistent numerical iterations of the gap equations. The phase separation or coexistence is determined by computing the 4-th order terms of the free energy which is confirmed by the numerical calculations. We can show the phase coexistence when the spin density wave is incommensurate. And the first order phase transition is observed near the boundary between commensurate and incommensurate spin density wave.