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        <datestamp>2026-09-30T17:40:29Z</datestamp>
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          <dc:title>&lt;p&gt;Pointwise validation of the matching conditions.&lt;/p&gt;</dc:title>
          <dc:creator>Muna Elsadig (25145379)</dc:creator>
          <dc:creator>Muhammad Safdar (1474231)</dc:creator>
          <dc:creator>Hala H. Taha (22838328)</dc:creator>
          <dc:creator>Muhammad Afzal (83943)</dc:creator>
          <dc:subject>Biophysics</dc:subject>
          <dc:subject>Biochemistry</dc:subject>
          <dc:subject>Space Science</dc:subject>
          <dc:subject>Physical Sciences not elsewhere classified</dc:subject>
          <dc:subject>Cell Biology</dc:subject>
          <dc:subject>Neuroscience</dc:subject>
          <dc:subject>Biotechnology</dc:subject>
          <dc:subject>Chemical Sciences not elsewhere classified</dc:subject>
          <dc:subject>Biological Sciences not elsewhere classified</dc:subject>
          <dc:subject>Cancer</dc:subject>
          <dc:subject>Infectious Diseases</dc:subject>
          <dc:subject>whose projection yields</dc:subject>
          <dc:subject>wavepacket &amp;# 8211</dc:subject>
          <dc:subject>wall cosine modes</dc:subject>
          <dc:subject>truncation convergence study</dc:subject>
          <dc:subject>transient treatment follows</dc:subject>
          <dc:subject>precomputed wavenumber grid</dc:subject>
          <dc:subject>form coupling matrix</dc:subject>
          <dc:subject>every matching plane</dc:subject>
          <dc:subject>cavity hybrid resonances</dc:subject>
          <dc:subject>block linear system</dc:subject>
          <dc:subject>power fluxes entering</dc:subject>
          <dc:subject>absorbed power fraction</dc:subject>
          <dc:subject>weighted matrix product</dc:subject>
          <dc:subject>broadband acoustic pulse</dc:subject>
          <dc:subject>membrane &amp;# 8211</dc:subject>
          <dc:subject>dependent acoustic scattering</dc:subject>
          <dc:subject>incident power</dc:subject>
          <dc:subject>vector product</dc:subject>
          <dc:subject>pulse energy</dc:subject>
          <dc:subject>dependent propagation</dc:subject>
          <dc:subject>dependent field</dc:subject>
          <dc:subject>xlink "&gt;</dc:subject>
          <dc:subject>wise reconstruction</dc:subject>
          <dc:subject>velocity continuity</dc:subject>
          <dc:subject>single gaussian</dc:subject>
          <dc:subject>reflection regimes</dc:subject>
          <dc:subject>porous segments</dc:subject>
          <dc:subject>porous model</dc:subject>
          <dc:subject>porous filler</dc:subject>
          <dc:subject>porous core</dc:subject>
          <dc:subject>maximum absorption</dc:subject>
          <dc:subject>lossless limit</dc:subject>
          <dc:subject>fourier approach</dc:subject>
          <dc:subject>field splits</dc:subject>
          <dc:subject>dissipative decay</dc:subject>
          <dc:subject>dissipation audit</dc:subject>
          <dc:subject>computational framework</dc:subject>
          <dc:subject>centre line</dc:subject>
          <dc:description>&lt;p&gt;Reference frequency  Hz with &lt;i&gt;N&lt;/i&gt; = 16 acoustic transverse modes and &lt;i&gt;M&lt;/i&gt; = 22 Galerkin modes; physical parameters &lt;i&gt;a&lt;/i&gt; = 0.05 m, &lt;i&gt;L&lt;/i&gt; = 0.10 m, &lt;i&gt;T&lt;/i&gt; = 350.0 N/m. Panel (a): real part of the fluid normal velocity  in the inlet (dashed) overlaid on the membrane velocity  (solid). Panel (b): real part of  in the left air cavity (dashed) overlaid on  in the porous core (solid). The closed-form elimination of &lt;a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0358579#pone.0358579.e065" target="_blank"&gt;Eq (18)&lt;/a&gt; enforces panel (b) to machine precision; panel (a) is convergent in the truncation. Physical interpretation: the membrane velocity matches the inlet fluid normal velocity – confirming the fluid-structure coupling of &lt;a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0358579#pone.0358579.e044" target="_blank"&gt;Eq (9)&lt;/a&gt; – and the air-porous pressure jump carries the correct factor  from the Delany–Bazley filler.&lt;/p&gt;</dc:description>
          <dc:date>2026-09-30T17:40:25Z</dc:date>
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          <dc:type>Figure</dc:type>
          <dc:identifier>10.1371/journal.pone.0358579.g002</dc:identifier>
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