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        검색결과 105

        101.
        2001.04 KCI 등재 서비스 종료(열람 제한)
        The atmospheric conditions and the transport mechanism of long-range transport of air pollutants from coastal area to inland area were investigated using regular meteorological data and air pollution data obtatined from the southeastern area of Korea. Daytime temperature over the inland area(Taegu) was higher than that over the coastal area(Pusan) and the temperature difference of about 5∼6℃ when the thermal low was most fully developed and the sea level pressure over Taegu was lower than that over Pusan by about 4∼5 hPa at that time. Therefore this low pressure appeared to the thermally induced low. Air mass polluted from the coastal area during the morning period was transported inland area, at first by the sea breeze and by the large scale wind system toward the thermal low generated in the mountainous inland region. This was explained by the fact that the concentration of air pollutants over Taegu increased throughtout the late afternoon.
        102.
        1999.10 KCI 등재 서비스 종료(열람 제한)
        A sea/land breeze circulation system and a regional scale circulation system are formed at a region which has complex terrain around coastal area and affect to the dispersion and advection of air pollutants. Therefore, it is important that atmospheric circulation model should be well designed for the simulation of regional dispersion of air pollutants. For this, Local Circulation Model, LCM which has an ability of high resolution is used. To verify the propriety of a LCM, we compared the simulation result of LCM with an exact solution of a linear theory over a simple topography. Since they presented almost the same value and pattern of a vertical velocity at the level of 1 ㎞, we had a reliance of a LCM. For the prediction of dispersion and advection of air pollutants, the wind field should be calculated with high accuracy. A numerical simulation using LCM will provide more accurate results over a complex terrain around coastal area.
        103.
        1998.06 KCI 등재 서비스 종료(열람 제한)
        Effects of uniform flow on a two-dimensional mesoscale horizontal convection were investigated by using the vorticity and thermodynamic equations. For this purpose, We simulated properties of a thermal convection in a stably stratified Boussinesq fluid caused by partial heating at the center of a lower boundary. If we don`t consider effects of the uniform flow, the convection takes the form of axisymmetric with respect to the z-axis. But when uniform flow is strong, velocity field and temperature field consist of a single cell structure which spreads upstream side of the partial heating area. The flow pattern for strong uniform flows takes the form of positive temperature near the ground and negative temperature perturbation aloft over the partial heating area, and downward motion directly over the upwind portion of the partial heating area and upward motion on the downstream side. The downstream edge of the upstream cell is shifted in the downstream direction with the increase of uniform flow almost linearly.
        104.
        1998.04 KCI 등재 서비스 종료(열람 제한)
        This study is concerned with properties of a thermal convection in a stably stratified Boussinesq fluid caused by partial heating at the lower boundary. For this purpose, two-dimensional, nonrotating system was employed. If the heating is very strong, convection takes the form of a turbulent plume. Otherwise, remains laminar. If the partial heating at the bottom boundary is symmetric, the convection takes the form of axisymmetric with respect to the z-axis. but heating form is not so significant as to alter the main features of the horizontal convection. The convective motion consists of two-cell with the convergence in the lower layer at the center of the partial heating area. The temperature perturbation is characterized by the temperature `Cross-Over` over the partial heating area. These features are cleared according to the increase of temperature difference between the center and side part of the bottom boundary.
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