The paper (Ram & Ramachandran, Purdue, arXiv:2609.06393) models elongated swimmers (aspect ratio q=10, Jeffery reorientation ) in Womersley oscillatory channel flow , using 5×10⁵-particle Langevin simulations, a 2D Fokker-Planck equation, and a reduced 1D orientational FPE with Fourier-harmonic perturbation analysis. The four governing groups are Pef=S/DR, Pec=VaDR, Wo=a√(n/ν), and β=DR/n .
The analytical curve above shows the exact closed-form factor: depletion is ~β²-scaled for β≪1 (strong suppression) and saturates at unity for β≫1, matching the reported 2D-FPE verification in Figure 16.
The mild parabolic-in-ŷ concentration above (depletion at centerline, wall accumulation) is reconstructed from the paper's Eq. 3.13 with σ=α/6(1−α²/20); it reproduces the shape of the verified profiles in Figure 15.
Strengths: rigorous Langevin↔FPE cross-validation, exact symmetry proofs (π-periodicity of C despite 2π forcing), and a falsifiable closed-form depletion law verified over β∈[10⁻³,10³]. Limitations: entirely theoretical/dilute; the 1D asymptotics require Pec≪1 and Pef≪1; large-Pef scalings (A=0.13Pef^0.18, ŷ*=0.52Pef^-0.17) are empirical fits, not derivations; wall hydrodynamics, finite concentration, 3D effects, and living-cell validation are absent. Nothing here is experimentally tested, so physiological relevance (e.g., pulsatile blood) remains a conjecture.
A simulation or experiment showing centerline depletion strengthening with increasing Wo or decreasing β would falsify the central suppression claim; the paper's own 2D-FPE vs Langevin agreement would fail if swimmer–flow feedback (non-dilute) or wall hydrodynamics dominate.
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