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    <identifier>10.57760/sciencedb.39140</identifier>
    <datestamp>2026-06-11T15:16:05Z</datestamp>
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<oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
  <dc:date>2026-06-11</dc:date>
  <dc:title>Supplemental Materials_HYENG-14634</dc:title>
  <dc:identifier>doi:10.57760/sciencedb.39140</dc:identifier>
  <dc:language>en</dc:language>
  <dc:description>The file includes:Figures S1&amp;ndash;S6:S1: Influence of TSKAM parameters S2&amp;ndash;S4: Complete experimental and simulated zinc BTCs for 35‑mesh, 60‑mesh and 100‑mesh sand columns under four flow regimes (Uniform, T60, T40, T20), each with three injection cycles.S5: Comparison of equivalent dispersion coefficient (EDC) vs. velocity‑dependent dispersion (VarD) for bromide transport.S6: Mesh‑independence test results (three grid resolutions).Tables S1&amp;ndash;S2:S1: Simulation accuracy (R&amp;sup2;, RMSE) of the velocity‑dependent dispersion model for Br⁻.S2: Fitted TSKAM parameters and goodness‑of‑fit metrics for all zinc breakthrough experiments.Text sections (within the PDF):Numerical implementation of the variable‑velocity TSKAM: spatial discretization (upwind for advection, central difference for dispersion), time discretization (implicit backward Euler + operator splitting with RK4 for reaction terms), and order of accuracy (first‑order in time, second‑order in space).Mesh‑ and time‑step independence test: quantitative convergence analysis (peak concentration errors &amp;lt;1%).Model calibration and evaluation metrics: definition of R&amp;sup2; and RMSE, parameter determination procedure, boundary and initial conditions.Justification for using an equivalent dispersion coefficient instead of a velocity‑dependent formula under transient flow.Data generationExperimental data: Column breakthrough experiments were conducted using quartz sand of three particle sizes (35‑mesh, 60‑mesh, 100‑mesh). Four flow regimes were tested: steady‑state (Uniform) and sinusoidal flow with periods of 20, 40, and 60 min (T20, T40, T60), all at the same mean flow rate (1 mL/min). Bromide was used as a conservative tracer, and Zn&amp;sup2;⁺ solutions (100 mg/L) were injected in three sequential cycles. Effluent concentrations were measured by ICP‑OES (Zn) and UV‑Vis spectrophotometry (Br⁻).Numerical data: The variable‑flow advection‑dispersion equation (ADE) was used to simulate bromide BTCs, and the Two‑Site Kinetic Attachment Model (TSKAM) was used for Zn&amp;sup2;⁺ transport. Simulations were performed on a one‑dimensional domain (20 cm length) using a finite‑difference method with implicit time stepping. The mesh‑independence test (Fig. S6) verified that a grid spacing of 0.2 cm and time step of 1 s yield converged results (error &amp;lt; 1%).File naming: The file name follows the pattern &amp;quot;Supplemental Materials_HYENG-14634.pdf&amp;quot;, where HYENG-14634 is the manuscript ID.</dc:description>
  <dc:subject>Periodically transient flow regime; Migration of zinc ion; Adsorption-desorption; Particle size</dc:subject>
  <dc:creator>Song WEI</dc:creator>
  <dc:creator>Zhi ZHOU</dc:creator>
  <dc:creator>Yong ZHANG</dc:creator>
  <dc:creator>Hui WEI</dc:creator>
  <dc:creator>Huimei SHAN</dc:creator>
  <dc:rights>PUBLIC</dc:rights>
  <dc:rights>https://creativecommons.org/licenses/by/4.0/</dc:rights>
  <dc:type>dataset</dc:type>
  <dc:publisher>Science Data Bank</dc:publisher>
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