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  <titleInfo>
    <title>Multi-level model for hydrodynamic circulation with water quality analysis in bays</title>
  </titleInfo>
  <name type="personal">
    <namePart>Pun, Kwock Leung</namePart>
    <role>
      <roleTerm authority="marcrelator" type="text">creator</roleTerm>
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  </name>
  <name type="personal">
    <namePart>Shibayama, Tomoya</namePart>
    <role>
      <roleTerm type="text">Chairperson</roleTerm>
    </role>
  </name>
  <name type="personal">
    <namePart>Suphat Vongvisessomjai</namePart>
    <role>
      <roleTerm type="text">Examination Committee</roleTerm>
    </role>
  </name>
  <name type="personal">
    <namePart>Tawatchai Tingsanchali</namePart>
    <role>
      <roleTerm type="text">Examination Committee</roleTerm>
    </role>
  </name>
  <name type="corporate">
    <namePart>The Royal Thai Government</namePart>
    <role>
      <roleTerm type="text">Scholarship Donor</roleTerm>
    </role>
  </name>
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  <originInfo>
    <place>
      <placeTerm type="code" authority="marccountry">th</placeTerm>
    </place>
    <place>
      <placeTerm type="text">Bangkok</placeTerm>
    </place>
    <publisher>Asian Institute of Technology</publisher>
    <dateIssued>1991</dateIssued>
    <issuance>monographic</issuance>
  </originInfo>
  <language>
    <languageTerm authority="iso639-2b" type="code">eng</languageTerm>
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    <extent>122 p.</extent>
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  <abstract>A finite difference numerical model is developed to predict the hydrodynamic circulation in  bays. Applying the multi-level approach, the water body is divided into three levels, in which the  interfacial layers are fixed in space. The links between layers are the vertical mass exchange and  momentum transfer in terms of interfacial shear stress. The thickness of upper and middle layers  are decided according to the field measured data taken from Tokyo Bay on May 23, 1983 to represent  an approximate thickness of a thermocline. The formulation of hydrodynamic model is based on  the vertical integration of continuity and momentum equation for each layer. To study the dispersion  of substances in bays, a multi-level approach is also used to formulate a three-level dispersion model.  Mass transport and diffusive flux between layers are included in the model. The formulation of  dispersion model is based on the vertical integration of convection-diffusion equation between the  layer boundaries. An important connection between two models is that the computed layer velocities  and water elevation from the hydrodynamic model serve as input data to the dispersion model.  Consequently, the validity of the three-level hydrodynamic model is examined by comparing  the computed flow condition with the field data measured at 9 sampling points in Tokyo Bay. The  computed results seem in reasonable agreement with the measured data. Moreover, the important  factors which affect the flow condition as well as the dispersion process - such as wind condition,  interfacial shear stress coefficient, residual cunent, initial and boundary conditions - are discussed.  The river discharge does not have much effect on the entire flow pattern except in the vicinity of  the river mouth. Under the wind effect, flow direction is usually deflected in the upper layer and  has a tendency to align with the wind direction. In the middle and lower layer, a return flow is driven  to a direction opposite to the upper layer flow for compensation.</abstract>
  <note>A thesis submitted in partial fulfillment of the requirements for the degree of Master of  Engineering, School of Engineering and Technology</note>
  <note>Thesis (M.Eng.) - Asian Institute of Technology, 1991</note>
  <subject authority="lcsh">
    <topic>Hydrodynamics</topic>
    <topic>Mathematical models</topic>
  </subject>
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    <titleInfo>
      <title>Thesis ; no. WA-91-16</title>
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