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<front>
<journal-meta>
<journal-id journal-id-type="publisher">ESurfD</journal-id>
<journal-title-group>
<journal-title>Earth Surface Dynamics Discussions</journal-title>
<abbrev-journal-title abbrev-type="publisher">ESurfD</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Earth Surf. Dynam. Discuss.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">2196-6338</issn>
<publisher><publisher-name></publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.5194/esurfd-1-437-2013</article-id>
<title-group>
<article-title>Flocculation processes and sedimentation of fine sediments in the open annular flume – experiment and numerical modeling</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Klassen</surname>
<given-names>I.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hillebrand</surname>
<given-names>G.</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Olsen</surname>
<given-names>N. R. B.</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Vollmer</surname>
<given-names>S.</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Lehmann</surname>
<given-names>B.</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Nestmann</surname>
<given-names>F.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>Institute for Water and River Basin Management, Karlsruhe Institute of Technology, Germany</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Federal Institute of Hydrology, Koblenz, Germany</addr-line>
</aff>
<aff id="aff3">
<label>3</label>
<addr-line>Department of Hydraulic and Environmental Engineering, Norwegian University of Science and Technology, Trondheim, Norway</addr-line>
</aff>
<aff id="aff4">
<label>4</label>
<addr-line>Institute for Hydraulic Engineering and Water Management, Technical University Darmstadt, Germany</addr-line>
</aff>
<pub-date pub-type="epub">
<day>14</day>
<month>10</month>
<year>2013</year>
</pub-date>
<volume>1</volume>
<issue>1</issue>
<fpage>437</fpage>
<lpage>481</lpage>
<permissions>
<copyright-statement>Copyright: &#x000a9; 2013 I. Klassen et al.</copyright-statement>
<copyright-year>2013</copyright-year>
<license license-type="open-access">
<license-p>This work is licensed under the Creative Commons Attribution 3.0 Unported License. To view a copy of this licence, visit <ext-link ext-link-type="uri"  xlink:href="https://creativecommons.org/licenses/by/3.0/">https://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions>
<self-uri xlink:href="https://esurf.copernicus.org/preprints/1/437/2013/esurfd-1-437-2013.html">This article is available from https://esurf.copernicus.org/preprints/1/437/2013/esurfd-1-437-2013.html</self-uri>
<self-uri xlink:href="https://esurf.copernicus.org/preprints/1/437/2013/esurfd-1-437-2013.pdf">The full text article is available as a PDF file from https://esurf.copernicus.org/preprints/1/437/2013/esurfd-1-437-2013.pdf</self-uri>
<abstract>
<p>The prediction of cohesive sediment transport requires numerical models
which include the dominant physico-chemical processes of fine sediments.
Mainly in terms of simulating small scale processes, flocculation of fine
particles plays an important role since aggregation processes affect the
transport and settling of fine-grained particles. Flocculation algorithms
used in numerical models are based on and calibrated using experimental
data. A good agreement between the results of the simulation and the
measurements is a prerequisite for further applications of the transport
functions.
&lt;br&gt;&lt;br&gt;
In this work, the sediment transport model (SSIIM) was extended by
implementing a physics-based aggregation process model based on McAnally
(1999). SSIIM solves the Navier-Stokes-Equations in a three-dimensional,
non-orthogonal grid using the k-ε turbulence model. The program
calculates the suspended load with the convection-diffusion equation for the
sediment concentration.
&lt;br&gt;&lt;br&gt;
Experimental data from studies in annular flumes (Hillebrand, 2008; Klassen, 2009)
is used to test the flocculation algorithm. Annular flumes are
commonly used as a test rig for laboratory studies on cohesive sediments
since the flocculation processes are not interfered with by pumps etc. We
use the experiments to model measured floc sizes, affected by aggregation
processes, as well as the sediment concentration of the experiment. Within
the simulation of the settling behavior, we use different formulas for
calculating the settling velocity (Stokes, 1850 vs. Winterwerp, 1998) and
include the fractal dimension to take into account the structure of flocs.
&lt;br&gt;&lt;br&gt;
The aim of the numerical calculations is to evaluate the flocculation
algorithm by comparison with the experimental data. The results from these
studies have shown, that the flocculation process and the settling behaviour
are very sensitive to variations in the fractal dimension. We get the best
agreement with measured data by adopting a characteristic fractal dimension
&lt;i&gt;n&lt;/i&gt;&lt;sub&gt;&lt;i&gt;f&lt;/i&gt;&lt;/sub&gt;&lt;sub&gt;c&lt;/sub&gt;&lt;/sub&gt; to 1.4. Insufficient results were obtained when neglecting
flocculation processes and using Stokes settling velocity equation, as it is
often done in numerical models which do not include a flocculation
algorithm.
&lt;br&gt;&lt;br&gt;
These numerical studies will be used for further applications of the
transport functions to the SSIIM model of reservoirs of the Upper Rhine
River, Germany.</p>
</abstract>
<counts><page-count count="45"/></counts>
</article-meta>
</front>
<body/>
<back>
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