• Title/Summary/Keyword: dispersion simulation

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Numerical Simulation of the Wind Flow Over a Triangular Prism with a Porous Windbreak (다공성 방풍벽이 설치된 삼각프리즘 주위 유동장의 수치모사)

  • 김현구;임희창;이정묵
    • Journal of Korean Society for Atmospheric Environment
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    • v.15 no.3
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    • pp.223-233
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    • 1999
  • The wind-flow characteristics over a two-dimensional triangular prism with a porous windbreak are numerically investigated. The geometry is a simplified model of large outdoor stack with a frontal wall-type windbreak which is used to prevent particle dispersion by reducing wind speed over stak surface. In the present numerical model, the RNG k-$\varepsilon$ model, the orthogonal grid system and the QUICK scheme are employed for the successful simulation of separated flow. The predicted results are compared and validated with the associated wind-tunnel experiments. In addition, the trajectories of dispersed particles and their sedimentation characteristics are quantitatively investingated using a Lagrangian turbulent-dispersion model.

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Study on Urban Temperature Prediction Method Using Lagrangian Particle Dispersion Model (라그랑지안 입자모델을 활용한 도시기온 예측기법의 연구)

  • Kim, Seogcheol;Yun, Jeongim
    • Journal of Korean Society for Atmospheric Environment
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    • v.33 no.1
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    • pp.45-53
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    • 2017
  • A high resolution model is proposed for calculating the temperature field of a large city, based upon a Lagrangian particle model. Utilizing the analogy between the heat and mass transport phenomena in turbulent flows, a Lagrangian particle model, originally developed for air pollutant dispersion problems, is adapted for simulating heat transport. In the model conceptual heat particles are released into the atmosphere from the heat sources and move along with the turbulent winds in accordance with the Markov process. The potential temperature assumed to be conserved along with heat particles serves as a tag, so the temperature fields can be deduced from the distribution of particles. The wind fields are constructed from a diagnostic meteorology model incorporating a morphological model designed for building flows. Test run shows the robustness of the modeling system.

Simulation Modelling of the Pollutant Concentration in Vehicle Tunnels (차량터널 오염물질 농도 예측 시뮬레이션 모델 연구)

  • 이창우;양원철;이송희
    • Tunnel and Underground Space
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    • v.6 no.1
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    • pp.57-63
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    • 1996
  • The goal of this study is to develop a simulation model of the pollutant dispersion in vehicle tunnels, which can be utilized to optimize the tunnel ventilation system. Contaminant dispersion is modelled using a FDM solution of advective diffusion equation. Taking into consideration the local vehicle emission rates by year, it is user-oriented and its logic is generalized. Therefore, differences in the ventilation scheme can be easily adapted. The results of its application to a urban tunnel show that the relative errors are 1.1~6.8% for the natural velocity, 1.3% for the traffic-induced velocity and 2.9% for the total air quantity. Simulated CO concentrations along the entire tunnel show about 13% of the relative error.

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Dispersion Pattern Simulation of Tungsten Impactors According to Mass and Shape of Explosives (폭약 질량과 형상에 따른 텅스텐 충격자의 분산 패턴 시뮬레이션)

  • Sakong, Jae;Woo, Sung-Choong;Bae, Yong-Woon;Choi, Yeoun-Jin;Cha, Jung-Phil;Ga, In-Han;Kim, Tae-Won
    • Transactions of the Korean Society of Mechanical Engineers A
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    • v.38 no.12
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    • pp.1325-1333
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    • 2014
  • The dispersion pattern of a near miss neutralizer has a great effect on the disablement of a threatening projectile. This study numerically investigated the dispersion pattern of cylindrical tungsten impactors by an explosion in the near miss neutralizer. The mass and shape of the explosive were considered as influencing factors on the dispersion pattern. The explosives were set using two shape models: a parallel shape with the same upper and lower thicknesses and a tapered shape with different upper and lower thicknesses. In the simulation results, the dispersed impactors formed a ring-shaped pattern on a two-dimensional plane in an arbitrary space. In addition, the fire net area increased with the explosive mass when the explosive shapes were identical. In particular, the tapered shape explosive formed a larger fire net area than the parallel shape explosive. Based on the analysis of the fire net area along with the dispersion density, both the explosive mass and shape representing the physical characteristics should be considered for controlling the dispersion pattern of impactors in a near miss neutralizer.

Numerical Simulation of Volcanic Ash Dispersion and Deposition during 2011 Eruption of Mt. Kirishima (2011년 기리시마 화산 분화에 따른 화산재 이동 및 침적에 관한 수치모의실험)

  • Lee, Soon-Hwan;Jang, Eun-Suk;Yun, Sung-Hyo
    • Journal of the Korean earth science society
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    • v.35 no.4
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    • pp.237-248
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    • 2014
  • To analyze the characteristics of deposition and dispersion of volcanic ash emitted from Mt. Kirishima on January 26, 2011, several numerical simulations were carried out by using the numerical models including Weather and Research Forecast (WRF) and FLEXPART. The dispersion of ash located under 1 km high tends to be concentrated along the prevailing wind direction on January 26 2011. On the other hand, volcanic ash released on the following day spreads to Kirishima bay due to the intensified high pressure air mass in southern Kyushu. When Siberian air mass was intensified January 26, 2011, the deposition of volcanic ash is concentrated restrictedly in the narrow area along the wind direction of the downwind side of Mt. Kirishima. The development of high pressure air mass over the eruption area tends to induce the intensified horizontal diffusion of volcanic ash. Since the estimated deposition of volcanic ash is agreed well with observed values, the proposed numerical simulation is reasonable to use the assessment on the behavior of volcanic ash.

Application of Practical Dispersion-Correction Scheme for Simulation of Tsunami Propagation (지진해일 전파 수치해석을 위한 실용적인 분산보정기법 적용)

  • Choi, Moon-Kyu;Ha, Tae-Min;Cho, Yong-Sik
    • Journal of the Korean Society of Hazard Mitigation
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    • v.8 no.4
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    • pp.145-152
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    • 2008
  • The initial wave lengths of tsunamis can be several tens to hundreds kilometers. Thus, the importance of the frequency dispersive effects in proportion to variation of the wave length, and should be properly considered in numerical simulation of tsunami propagation for a better accuracy. Recently, a practical dispersion-correction scheme has been developed by adding dispersion-correction terms(Cho et al., 2007). The new model employing the numerical technique has been verified by comparing numerical results with available analytic solutions, however, the new model has not yet been applied on a real topography. In this study, the new model is applied on a real topography and its applicability is examined. To study the applicability of the new model, two historical tsunami events are simulated for Sokcho, Mukho and Pohang harbors, with the tide gage records. Numerical results, the arrival time and the maximum water level at the tidal stations, are compared with observed data at each harbor.

A Study on Comparison between the Propagation of Uncertainty by GUM and Monte-Carlo Simulation (측정 불확도 표현 지침서(GUM)와 Monte-Carlo Simulation에 의한 불확도 전파 결과의 비교 연구)

  • Jungkee Shu;Hyungsik Min;Minsu Park;Jin-Chun Woo;Jongsang Kim
    • Journal of the Korean Chemical Society
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    • v.47 no.1
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    • pp.31-37
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    • 2003
  • The expanded uncertainties calculated by the application of GUM -approximation and Monte-Carlo simulation were compared about the model equation of one-point calibration which is widely used for the measurements and chemical analysis. For the comparisons, we assumed a set of artificial data at the various level of concentration and dispersion of t or normal distribution. Mistakes of more then 50 % was revealed at the values calculated by GUM-approximation in comparison with those of Monte-Carlo simulation because of the excess dispersion from t-distribution and non-linearity by division in the equation. In contrary, the mistake of calculation due to non-linearity of the equation was not observed in the level of detection limits with the equation of one-point calibration, because of the relatively large values of uncertainty in response.