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        <datestamp>2026-09-29T09:06:52Z</datestamp>
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          <dc:title>Experimental study of the flow in and above very flexible vegetation</dc:title>
          <dc:creator>Louis Vallier (25136213)</dc:creator>
          <dc:creator>Ludovic Cassan (25136216)</dc:creator>
          <dc:creator>Frédéric Y. Moulin (25136219)</dc:creator>
          <dc:subject>Physical Sciences not elsewhere classified</dc:subject>
          <dc:subject>Medicine</dc:subject>
          <dc:subject>Neuroscience</dc:subject>
          <dc:subject>Physiology</dc:subject>
          <dc:subject>Ecology</dc:subject>
          <dc:subject>Information Systems not elsewhere classified</dc:subject>
          <dc:subject>Developmental Biology</dc:subject>
          <dc:subject>Inorganic Chemistry</dc:subject>
          <dc:subject>Infectious Diseases</dc:subject>
          <dc:subject>Plant Biology</dc:subject>
          <dc:subject>Double-averaging</dc:subject>
          <dc:subject>flexible vegetation</dc:subject>
          <dc:subject>logarithmic law</dc:subject>
          <dc:subject>plant–flow interactions</dc:subject>
          <dc:subject>rough-wall boundary layers</dc:subject>
          <dc:description>&lt;p&gt;Optical measurements were performed in an open-channel tilting flume filled with vegetation surrogates in regimes of strong deformation at high values of the Cauchy number, Ca, in [1720;22766]. Multi-plane telecentric 2D particle image velocimetry (PIV) measurements gave access to flow components both above and inside the vegetation. We show that the canopy layer separates into two distinct sub-layers. In the lower part, the wake sub-layer, located below the maximum vegetation density height hν, vegetation behaves as a simply reconfigured canopy, hν decreasing with Ca following laws found for flexible canopies. Above hν, a flapping sub-layer appears, whose upper boundary hc scales with the water depth &lt;i&gt;H&lt;/i&gt;. There, vegetation band excursions homogenize the mean velocity field, erasing all dispersive terms, and profiles of the double-averaged longitudinal velocity follow a log law, as in sparse vegetation canopies, with an inflection point in the velocity profiles found just above hν.&lt;/p&gt;</dc:description>
          <dc:date>2026-09-29T09:06:52Z</dc:date>
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          <dc:identifier>10.6084/m9.figshare.34022216.v1</dc:identifier>
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