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        <identifier>oai:www.ideals.illinois.edu:2142/26017</identifier>
        <datestamp>2023-07-10</datestamp>
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        <thesis xmlns="http://www.ndltd.org/standards/metadata/etdms/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:dc="http://purl.org/dc/elements/1.1/" xsi:schemaLocation="http://www.ndltd.org/standards/metadata/etdms/1.1/ http://www.ndltd.org/standards/metadata/etdms/1.1/etdms11.xsd http://purl.org/dc/elements/1.1/ http://www.ndltd.org/standards/metadata/etdms/1.1/etdmsdc.xsd">
          <dc:contributor>Gioia, Gustavo</dc:contributor>
          <dc:contributor>Gioia, Gustavo</dc:contributor>
          <dc:contributor>Christensen, Kenneth T.</dc:contributor>
          <dc:contributor>Freund, Jonathan B.</dc:contributor>
          <dc:contributor>Goldenfeld, Nigel D.</dc:contributor>
          <dc:creator>Tran, Tuan A.</dc:creator>
          <dc:date>2011-08-25T22:09:05Z</dc:date>
          <dc:date>2011-08-25T22:09:05Z</dc:date>
          <dc:date>2011-08</dc:date>
          <dc:date>2011-08-25T22:09:05Z</dc:date>
          <dc:date>2011-08</dc:date>
          <dc:description>We carry out unprecedented experimental measurements
 of the frictional drag in 
 turbulent soap-film flows over smooth walls. 
 These flows are effectively two-dimensional,
   and we are able to create soap-film flows
 with the two types of turbulent spectrum 
 that are theoretically possible in two dimensions:
 the ``enstrophy cascade,''
 for which the spectral exponent $\alpha=3$,
 and the ``inverse energy cascade,''
 for which the spectral exponent $\alpha=5/3$.
 We find that the functional relation
 between the frictional
 drag $f$ and the Reynolds number Re depends on the
 spectral exponent:  where $\alpha=3$, $f \propto {\Re^{-1/2}}$;
  where $\alpha=5/3$, $f \propto {\Re^{-1/4}}$.
 
These findings cannot be 
 reconciled with the classic theory of the 
 frictional drag. The classic theory
 provides no means of distinguishing
   between one type of turbulent spectrum and
 another, and cannot account for the existence
 of a ``spectral link'' between the frictional
 drag and the turbulent spectrum.
 In view of our experimental results, 
 we conclude that the 
  classic theory must be considered incomplete.
 In contrast, our findings are consistent with
 a recently proposed spectral theory of the frictional
  drag.  In this theory the frictional
   drag of turbulent flows on smooth
 walls is predicted to be
 $f\propto {\rm Re}^{(1-\alpha)/(1+\alpha)}$, 
 where $\alpha$ is the spectral exponent. 
 This prediction is in exact 
 accord with our experiments on soap-film flows.
  It is also in accord with the available
 experimental data on
 three-dimensional pipe flows, where
 a single type of spectrum is possible:
 the ``energy cascade,'' for which $\alpha=5/3$
 (the same as for the inverse energy cascade).
  In fact, for $\alpha=5/3$ the 
   prediction of the spectral theory 
 coincides with the emprirical law of Blasius
 ($f \propto {\Re^{-1/4}}$),
 which gives the best 
  representation of the available experimental 
results for three-dimensional
  pipe flows of moderate turbulent strength 
 (starting from ${\rm  Re} \approx 2,500$ and  up to
 ${\rm Re}\approx 100,000$).
 In carrying out our experiments on the frictional drag,
 we discover the spontaneous occurrence 
 in unobstructed soap-film flows of a type of 
  shock related to the elasticity of the film.
  By means of extensive experimental measurements,
  we verify that these shocks are dissipative and diffusive;
  that they give rise to fluctuations independently from
  the boundaries, with
  a strong but circumscribed effect
  on the spatial distribution of turbulent intensity; 
  and that they
  alter the structure
  of the turbulent spectrum downstream from the 
  shock. 
We show that a simple one--dimensional model 
  is capable of capturing the most salient features
  of our experimental measurements and observations
 on the shocks. In this model the
steady-state equation of momentum balance 
 contains four terms: the inertial force,
  the elastic force, the gravitational force, 
  and the drag force of the ambient air.
 The elastic force consists of the 
  gradient of the surface tension, and it can be 
 computed under the assumption (which 
   is satisfied in our experiments) that 
 the film is in the Marangoni regime, i.e., 
 that as the flow moves through the shock
  there is no time 
  for diffusional exchange of soap molecules between the bulk and the
  faces of the film, so that
  the concentration of soap molecules in the 
  bulk of the film remains invariant.</dc:description>
          <dc:description>Item withdrawn by Alexis Thompson (athmpsn1@illinois.edu) on 2011-04-22T20:58:16Z
Item was in collections:
University of Illinois Theses &amp; Dissertations (ID: 1)
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          <dc:identifier>http://hdl.handle.net/2142/26017</dc:identifier>
          <dc:language>en</dc:language>
          <dc:rights>Copyright 2010 Tuan Anh Tran.</dc:rights>
          <dc:subject>Turbulence</dc:subject>
          <dc:subject>Two-dimensional turbulence</dc:subject>
          <dc:subject>Friction factor</dc:subject>
          <dc:subject>Frictional drag</dc:subject>
          <dc:subject>Energy spectrum</dc:subject>
          <dc:subject>Enstrophy cascade</dc:subject>
          <dc:subject>Inverse energy cascade</dc:subject>
          <dc:subject>Marangoni</dc:subject>
          <dc:subject>Shocks</dc:subject>
          <dc:subject>Soap-film flows</dc:subject>
          <dc:subject>Soap-film channel</dc:subject>
          <dc:title>Experiments in turbulent soap-film flows: Marangoni shocks, frictional drag, and energy spectra</dc:title>
          <degree>
            <department>Mechanical Sci &amp; Engineering</department>
            <departmentCode>1917</departmentCode>
            <discipline>Theoretical &amp; Applied Mechans</discipline>
            <disciplineCode>0242</disciplineCode>
            <grantor>University of Illinois at Urbana-Champaign</grantor>
            <level>Dissertation</level>
            <name>Ph.D.</name>
            <program>PHD:Theor&amp;Appl Mechanics -UIUC</program>
            <programCode>10KS0242PHD</programCode>
          </degree>
        </thesis>
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