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arxiv: 2504.05834 · v3 · submitted 2025-04-08 · ⚛️ physics.flu-dyn · cond-mat.stat-mech· physics.comp-ph

Geometry-Driven Segregation in Periodically Textured Microfluidic Channels

Pith reviewed 2026-05-22 21:03 UTC · model grok-4.3

classification ⚛️ physics.flu-dyn cond-mat.stat-mechphysics.comp-ph
keywords microfluidic channelsparticle alignmenttextured wallsshear gradientsanisotropic particlespassive sortingReynolds numberfluid dynamics
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0 comments X

The pith

Periodically textured walls in microfluidic channels force elongated particles to align along the centerline.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

Smooth-walled microchannels preserve particle trajectory dependence on initial orientation and position. Adding periodic textures to the walls creates spatially varying shear that repeatedly reorients the particles as they travel. This produces robust alignment to the channel centerline. The alignment strength varies with particle elongation and texture wavelength, reaching a maximum in an optimal range. The effect persists at higher flow speeds, though the distance needed for alignment grows and diverges as Reynolds number rises toward turbulence.

Core claim

Introducing periodically textured walls triggers robust alignment of elongated microparticles along the microchannel centerline through repeated reorientations generated by spatially modulated shear gradients near the textured walls. Alignment efficiency depends on particle elongation and the relative texture wavelength with an optimal range for maximal effect. While the alignment behavior is not limited to low Reynolds numbers, the characteristic alignment length scale diverges as the Reynolds number increases toward the turbulent flow regime.

What carries the argument

Spatially modulated shear gradients near periodically textured walls that generate repeated particle reorientations.

If this is right

  • Alignment becomes independent of starting orientation and lateral position once the periodic texture is introduced.
  • Efficiency reaches a maximum within a specific range of particle elongations and texture wavelengths.
  • The mechanism operates across Reynolds numbers but requires progressively longer distances as flow approaches turbulence.
  • The texture pattern supplies a passive method to sort or focus anisotropic particles without external fields.
  • The approach applies to soft matter transport, biophysical flows, and microfluidic device design.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Texture wavelength could be tuned to select particles of particular aspect ratios for separation in a single device.
  • The same geometry principle might extend to non-periodic or three-dimensional wall patterns for more complex focusing tasks.
  • At high Reynolds numbers the diverging alignment length sets a practical limit on channel length for effective passive control.
  • Direct particle tracking experiments in microfabricated textured channels would test whether the predicted alignment length scales match observations.

Load-bearing premise

The alignment is produced solely by the periodic wall geometry and the modulated shear it creates, independent of particle-wall interactions or initial flow details.

What would settle it

Track orientation distributions of elongated particles in a smooth channel versus an otherwise identical periodically textured channel at fixed flow rate and Reynolds number; if the textured case shows no reduction in dependence on initial orientation, the claim is falsified.

Figures

Figures reproduced from arXiv: 2504.05834 by Fatemeh S. Ahmadi, Hossein Hamzehpour, Reza Shaebani.

Figure 1
Figure 1. Figure 1: FIG. 1. Sketch of the simulation setup. The particle’s orien [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Stationary center-of-mass velocity of a disk as a fun [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 5
Figure 5. Figure 5: The weak dependence of the center-of-mass ve [PITH_FULL_IMAGE:figures/full_fig_p004_5.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Transit time [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Evolution of particle’s lateral position and orient [PITH_FULL_IMAGE:figures/full_fig_p005_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. (A) Transit time [PITH_FULL_IMAGE:figures/full_fig_p005_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. Motion in periodically textured channels. (A) Illus [PITH_FULL_IMAGE:figures/full_fig_p006_6.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8. Evolution of particle’s lateral position and orient [PITH_FULL_IMAGE:figures/full_fig_p007_8.png] view at source ↗
read the original abstract

We investigate the transport dynamics of elongated microparticles in microchannel flows. While smooth-walled channels preserve the dependence of particle trajectories on initial orientation and lateral position, we show that introducing periodically textured walls can trigger robust alignment of the particle along the channel centerline. This geometry-driven alignment arises from repeated reorientations generated by spatially modulated shear gradients near the textured walls. The alignment efficiency depends on particle elongation and the relative texture wavelength, with an optimal range for maximal effect. While the observed alignment behavior is not limited to low Reynolds numbers, the characteristic alignment length scale diverges as the Reynolds number increases toward the turbulent flow regime. These findings offer a predictive framework for designing microfluidic devices that passively sort or focus anisotropic particles, with implications for soft matter transport, biophysical flows, and microfluidic engineering.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript investigates transport of elongated microparticles in microchannel flows. It claims that periodically textured walls induce robust centerline alignment via repeated reorientations from spatially modulated shear gradients near the walls, in contrast to smooth walls where trajectories retain dependence on initial orientation and lateral position. Alignment efficiency depends on particle elongation and texture wavelength (with an optimal range), while the characteristic alignment length diverges as Reynolds number increases toward turbulence. The work positions this as a predictive framework for passive sorting or focusing of anisotropic particles in microfluidic devices.

Significance. If the central mechanism is confirmed, the result would be significant for microfluidic engineering by providing a purely geometric route to passive particle alignment and focusing that overrides initial-condition dependence. This has clear implications for soft-matter transport, biophysical flows, and device design where external forcing is undesirable. The reported dependence on elongation, wavelength, and Reynolds number supplies concrete design guidelines.

major comments (2)
  1. [Numerical Methods / particle equation of motion] The claim that alignment is driven purely by periodic wall geometry and modulated shear (independent of particle-wall interactions or initialization details) is load-bearing. The abstract supplies no information on the particle equation of motion, wall boundary treatment, or sampling of initial position/orientation phase space; any short-range hydrodynamic corrections or contact forces could introduce an alternative centering mechanism. Please add this specification and robustness tests in the numerical-methods section.
  2. [Results] Quantitative support for 'robust alignment' and the 'optimal range' is needed. The abstract is entirely qualitative; the results section should report metrics such as alignment fraction versus initial conditions, alignment length versus wavelength and aspect ratio, and any error bars or ensemble statistics.
minor comments (2)
  1. [Discussion] Clarify the Reynolds-number scaling of the alignment length (e.g., with a plot or asymptotic argument) rather than stating only that it diverges.
  2. [Figures] Add a schematic or trajectory plot illustrating the repeated reorientation events near the textured walls for a representative particle.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for highlighting points that improve its clarity and rigor. We address each major comment below and have revised the manuscript accordingly.

read point-by-point responses
  1. Referee: [Numerical Methods / particle equation of motion] The claim that alignment is driven purely by periodic wall geometry and modulated shear (independent of particle-wall interactions or initialization details) is load-bearing. The abstract supplies no information on the particle equation of motion, wall boundary treatment, or sampling of initial position/orientation phase space; any short-range hydrodynamic corrections or contact forces could introduce an alternative centering mechanism. Please add this specification and robustness tests in the numerical-methods section.

    Authors: We agree that explicit specification of the particle dynamics and boundary treatment is necessary to support the geometry-driven claim. The revised Numerical Methods section now details the particle equation of motion (integration of hydrodynamic torques and forces from the resolved flow field, without short-range corrections or contact forces), the no-slip treatment of the periodically textured walls, and the sampling protocol over initial lateral positions and orientations. New robustness tests confirm that centerline alignment occurs consistently across the sampled phase space when the texture wavelength lies in the reported optimal range, with no evidence of alternative centering mechanisms. revision: yes

  2. Referee: [Results] Quantitative support for 'robust alignment' and the 'optimal range' is needed. The abstract is entirely qualitative; the results section should report metrics such as alignment fraction versus initial conditions, alignment length versus wavelength and aspect ratio, and any error bars or ensemble statistics.

    Authors: We have augmented the Results section with the requested quantitative metrics. New figures and text report the alignment fraction (fraction of trajectories reaching within 0.1 channel widths of the centerline) as a function of initial position and orientation, the characteristic alignment length versus texture wavelength and particle aspect ratio (with error bars from ensembles of several hundred trajectories), and statistical summaries confirming the existence and location of the optimal wavelength range. These additions provide direct, quantitative support for the claims of robust, geometry-driven alignment. revision: yes

Circularity Check

0 steps flagged

No circularity detected; derivation self-contained

full rationale

The paper presents a geometry-driven alignment mechanism based on modulated shear gradients in textured channels, grounded in standard fluid mechanics without any quoted self-definitional steps, fitted inputs renamed as predictions, or load-bearing self-citations that reduce the central claim to its inputs. The abstract describes the effect as arising from repeated reorientations due to spatially modulated shear, with dependence on elongation and wavelength, but supplies no equations or derivations that loop back to the result by construction. No evidence of ansatz smuggling, uniqueness theorems from prior self-work, or renaming of known results appears in the provided text. The derivation remains independent of the target outcome and relies on external hydrodynamic principles.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract-only review provides no explicit free parameters, axioms, or invented entities; standard assumptions of low-to-moderate Reynolds number flow and rigid particle dynamics are presumed but unstated.

pith-pipeline@v0.9.0 · 5677 in / 1059 out tokens · 35294 ms · 2026-05-22T21:03:33.706411+00:00 · methodology

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Reference graph

Works this paper leans on

52 extracted references · 52 canonical work pages

  1. [1]

    Alignment also depends on boundary roughness, captured by the dimensionless ratio ε1= ∆ x δ

    5D1≲∆ x≲2D1. Alignment also depends on boundary roughness, captured by the dimensionless ratio ε1= ∆ x δ . For ε1≪ 1, strongly overlapping disks smooth the wall and reduce shear gradients; for ε1≫ 1, shear zones be- come widely separated and alignment degrades. Opti- mal alignment occurs for 0 . 1≲ε1≲2, with effects van- ishing beyond ε1>5. Another key par...

  2. [2]

    Fluid mechanics of microrheology,

    T. M. Squires and T. G. Mason, “Fluid mechanics of microrheology,” Annu. Rev. Fluid Mech. 42, 413–438 (2010)

  3. [3]

    Microfluidics: Fluid physics at the nanoliter scale,

    T. M. Squires and S. R. Quake, “Microfluidics: Fluid physics at the nanoliter scale,” Rev. Mod. Phys. 77, 977– 1026 (2005)

  4. [4]

    Nonlinear microfluidics,

    D. Stoecklein and D. Di Carlo, “Nonlinear microfluidics, ” Anal. Chem. 91, 296–314 (2019)

  5. [5]

    Computational models for active mat- ter,

    R. Shaebani, A. Wysocki, R. G. Winkler, G. Gompper, and H. Rieger, “Computational models for active mat- ter,” Nat. Rev. Phys. 2, 181–199 (2020)

  6. [6]

    Microtubule polymeriza- tion generates microtentackles important in circulating tumor cell invasion,

    L. Kainka, R. Shaebani, K. Kaiser, J. Bosche, L. San- ten, and F. Lautenschl¨ ager, “Microtubule polymeriza- tion generates microtentackles important in circulating tumor cell invasion,” Biophys. J. 124, 2161–2175 (2025)

  7. [7]

    Cell-free layer de- velopment and spatial organization of healthy and rigid red blood cells in a microfluidic bifurcation,

    Y. Rashidi, O. Aouane, A. Darras, T. John, J. Harting, C. Wagner, and S. M. Recktenwald, “Cell-free layer de- velopment and spatial organization of healthy and rigid red blood cells in a microfluidic bifurcation,” Soft Matter 19, 6255 (2023)

  8. [8]

    Red blood cell lingering modulates hematocrit dis- tribution in the microcirculation,

    Y. Rashidi, G. Simionato, Q. Zhou, T. John, A. Kihm, M. Bendaoud, T. Kr¨ uger, M. O. Bernabeu, L. Kaestner, M. W. Laschke, M. D. Menger, C. Wagner, and A. Dar- ras, “Red blood cell lingering modulates hematocrit dis- tribution in the microcirculation,” Biophy. J. 122, 1526 (2023)

  9. [9]

    Cell-free layer of red blood cells in a constricted microfluidic channel under steady and time-dependent flow conditions,

    S. M. Recktenwald, K. Graessel, Y. Rashidi, J. N. Steuer, T. John, S. Gekle, and C. Wagner, “Cell-free layer of red blood cells in a constricted microfluidic channel under steady and time-dependent flow conditions,” Phys. Rev. Fluids 8, 074202 (2023)

  10. [10]

    Continuous particle separation through deterministic lateral displacement,

    L. R. Huang, E. C. Cox, R. H. Austin, and J. C. Sturm, “Continuous particle separation through deterministic lateral displacement,” Science 304, 987–990 (2004)

  11. [11]

    Particle separati on using virtual deterministic lateral displacement (vdld),

    D. J. Collins, T. Alan, and A. Neild, “Particle separati on using virtual deterministic lateral displacement (vdld), ” Lab Chip 14, 1595–1603 (2014)

  12. [12]

    Deterministic microfluidic ratchet,

    K. Loutherback, J. Puchalla, R. H. Austin, and J. C. Sturm, “Deterministic microfluidic ratchet,” Phys. Rev. Lett. 102, 045301 (2009)

  13. [13]

    Geometric structure design of passive label-free microfluidic system s for biological micro-object separation,

    H. Tang, J. Niu, H. Jin, S. Lin, and D. Cui, “Geometric structure design of passive label-free microfluidic system s for biological micro-object separation,” Microsyst Nano- eng 8, 62 (2022)

  14. [14]

    Finite element simula- tions of hydrodynamic trapping in microfluidic particle- trap array systems,

    X. Xu, Z. Li, and A. Nehorai, “Finite element simula- tions of hydrodynamic trapping in microfluidic particle- trap array systems,” Biomicrofluidics 7, 054108 (2013)

  15. [15]

    Particle separation and sorting in microfluidic devices: a review,

    P. Sajeesh and A. K. Sen, “Particle separation and sorting in microfluidic devices: a review,” Microfluid. Nanofluidics 17, 1–52 (2014)

  16. [16]

    Continuous separation of cells and particles in microfluidic systems,

    A. Lenshof and T. Laurell, “Continuous separation of cells and particles in microfluidic systems,” Chem. Soc. Rev. 39, 1203–1217 (2010)

  17. [17]

    Active mi- crofluidic systems for cell sorting and separation,

    M. Sivaramakrishnan, R. Kothandan, D. K. Govindara- jan, Y. Meganathan, and K. Kandaswamy, “Active mi- crofluidic systems for cell sorting and separation,” Curr. Opin. Biomed. Eng. 13, 60–68 (2020)

  18. [18]

    Active par- ticle motion in poiseuille flow through rectangular chan- nels,

    R. N. Valani, B. Harding, and Y. M. Stokes, “Active par- ticle motion in poiseuille flow through rectangular chan- nels,” Phys. Rev. E 110, 034603 (2024)

  19. [19]

    Acoustophoretic particle motion in a spherical microchamber,

    B. Sailer, R. Barnkob, and O. Hayden, “Acoustophoretic particle motion in a spherical microchamber,” Phys. Rev. Appl. 22, 044034 (2024)

  20. [20]

    A review of acoustofluidic separation of bioparticles,

    F. Hossein and P. Angeli, “A review of acoustofluidic separation of bioparticles,” Biophys. Rev. 15, 2005–2025 (2023)

  21. [21]

    Continuous fo- cusing of microparticles using inertial lift force and vor- ticity via multi-orifice microfluidic channels,

    J.-S. Park, S.-H. Song, and H.-I. Jung, “Continuous fo- cusing of microparticles using inertial lift force and vor- ticity via multi-orifice microfluidic channels,” Lab Chip 9, 939 (2009)

  22. [22]

    Enhanced size- dependent trapping of particles using microvortices,

    J. Zhou, S. Kasper, and I. Papautsky, “Enhanced size- dependent trapping of particles using microvortices,” Mi- crofluid. Nanofluid. 15, 611 (2013)

  23. [23]

    A deterministic model for bubble propagation through simple and cas- 9 caded loops of microchannels in power-law fluids,

    J. Mandal, S. Sarkar, and S. Sen, “A deterministic model for bubble propagation through simple and cas- 9 caded loops of microchannels in power-law fluids,” Phys. Fluids 33, 072008 (2021)

  24. [24]

    Morphology and kinematics of a train of power-law droplets in a corrugated microchan- nel,

    J. Mandal and S. Sarkar, “Morphology and kinematics of a train of power-law droplets in a corrugated microchan- nel,” Chem. Eng. Sci. 274, 118691 (2023)

  25. [25]

    Universal correlation for droplet fragmentation in a microfluidic t-junction,

    J. Mandal and S. Sarkar, “Universal correlation for droplet fragmentation in a microfluidic t-junction,” Lang- muir 40, 17489 (2024)

  26. [26]

    Thermal marangoni stress induced droplet mobilization in a mi- crofluidic confinement,

    J. Mandal, D. Sanyal, and S. Sarkar, “Thermal marangoni stress induced droplet mobilization in a mi- crofluidic confinement,” Phys. Fluids 37, 081704 (2025)

  27. [27]

    Modeling transport of soft particles in porous media,

    S. Li, H.-h. Yu, and J. Fan, “Modeling transport of soft particles in porous media,” Phys. Rev. E 104, 025112 (2021)

  28. [28]

    Deterministic lateral displacement for particle separation: a review,

    J. McGrath, M. Jimenez, and H. Bridle, “Deterministic lateral displacement for particle separation: a review,” Lab Chip 14, 4139–4158 (2014)

  29. [29]

    Current status and further development of deterministic lateral displacemen t for micro-particle separation,

    A. Zhbanov, Y. S. Lee, and S. Yang, “Current status and further development of deterministic lateral displacemen t for micro-particle separation,” Micro Nano Syst. Lett. 11, 11 (2023)

  30. [30]

    A review on deter- ministic lateral displacement for particle separation and detection,

    T. Salafi, Y. Zhang, and Y. Zhang, “A review on deter- ministic lateral displacement for particle separation and detection,” Nano-Micro Lett. 11, 77 (2019)

  31. [31]

    Dynamic control of particle separation in deterministic lateral displacement separator with viscoelastic fluids,

    Y. Li, H. Zhang, Y. Li, X. Li, J. Wu, S. Qian, and F. Li, “Dynamic control of particle separation in deterministic lateral displacement separator with viscoelastic fluids,” Sci. Rep. 8, 3618 (2018)

  32. [32]

    Particle focusing in a suspension flow through a corrugated tube,

    G. F. Hewitt and J. S. Marshall, “Particle focusing in a suspension flow through a corrugated tube,” J. Fluid Mech. 660, 258 (2010)

  33. [33]

    Inertial focusi ng of small particles in wavy channels: Asymptotic analysis at weak particle inertia,

    T. Nizkaya, J. Angilella, and M. Bues, “Inertial focusi ng of small particles in wavy channels: Asymptotic analysis at weak particle inertia,” Physica D 268, 91 (2014)

  34. [34]

    Pore-scale modelling of particle transport in a porous bed,

    R. Storm and J. S. Marshall, “Pore-scale modelling of particle transport in a porous bed,” J. Fluid Mech. 979, A9 (2024)

  35. [35]

    Particle focus - ing in a wavy channel,

    X. Mao, I. Bischofberger, and A. Hosoi, “Particle focus - ing in a wavy channel,” J. Fluid Mech. 968, A25 (2023)

  36. [36]

    The motion of ellip- soidal particles immersed in a viscous fluid,

    G. B. Jeffery and L. N. G. Filon, “The motion of ellip- soidal particles immersed in a viscous fluid,” Proc. R. Soc. Lond. 102, 161–179 (1922)

  37. [37]

    Par- ticle shape influences settling and sorting behavior in mi- crofluidic domains,

    H. Basagaoglu, S. Succi, D. Wyrick, and J. Blount, “Par- ticle shape influences settling and sorting behavior in mi- crofluidic domains,” Sci. Rep. 8, 8583 (2018)

  38. [38]

    Rotational separation of non-spherical bioparticles using i-shaped pillar arrays in a microfluidic device,

    K. K. Zeming, S. Ranjan, and Y. Zhang, “Rotational separation of non-spherical bioparticles using i-shaped pillar arrays in a microfluidic device,” Nat. Commun. 4, 1625 (2013)

  39. [39]

    Engi- neering particle trajectories in microfluidic flows using particle shape,

    W. E. Uspal, H. Burak Eral, and P. S. Doyle, “Engi- neering particle trajectories in microfluidic flows using particle shape,” Nat. Commun. 4, 2666 (2013)

  40. [40]

    Universal motion of mirror-symmetric microparticles in confined stokes flow,

    R. N. Georgiev, S. O. Toscano, W. E. Uspal, B. Bet, S. Samin, R. van Roij, and H. B. Eral, “Universal motion of mirror-symmetric microparticles in confined stokes flow,” Proc. Natl. Acad. Sci. U.S.A. 117, 21865– 21872 (2020)

  41. [41]

    Small asymmetric brownian objects self-align in nanofluidic channels,

    G. Fiorucci, J. T. Padding, and M. Dijkstra, “Small asymmetric brownian objects self-align in nanofluidic channels,” Soft Matter 15, 321–330 (2019)

  42. [42]

    Oscillations of confined fibres transported in microchannels,

    M. Nagel, P.-T. Brun, H. Berthet, A. Lindner, F. Gal- laire, and C. Duprat, “Oscillations of confined fibres transported in microchannels,” J. Fluid Mech. 835, 444– 470 (2018)

  43. [43]

    Numerical simulations of a stick-slip spherical particle in poiseuil le flow,

    M. Trofa, G. DAvino, and P. L. Maffettone, “Numerical simulations of a stick-slip spherical particle in poiseuil le flow,” Phys. Fluids 31, 083603 (2019)

  44. [44]

    Particle motion nearby rough surfaces,

    C. Kurzthaler, L. Zhu, A. A. Pahlavan, and H. A. Stone, “Particle motion nearby rough surfaces,” Phys. Rev. Flu- ids 5, 082101 (2020)

  45. [45]

    An experimental study and modelling of roughness effects on laminar flow in microchannels,

    G. Gamrat, M. Favre-Marinet, S. Le Person, R. Baviere, and F. Ayela, “An experimental study and modelling of roughness effects on laminar flow in microchannels,” J. Fluid Mech. 594, 399–423 (2008)

  46. [46]

    Effect of roughness on elongated particles in turbulent channel flow,

    D. Saccone, C. Marchioli, and M. De Marchis, “Effect of roughness on elongated particles in turbulent channel flow,” Int. J. Multiphase Flow 152, 104065 (2022)

  47. [47]

    Surface rough- ness analysis of microchannels featuring microfluidic devices fabricated by three different materials and methods,

    J. M. Acosta-Cuevas, M. A. Garcia-Ramirez, G. Hinojosa-Ventura, A. J. Martinez-Gomez, V. H. Perez-Luna, and O. Gonzalez-Reynoso, “Surface rough- ness analysis of microchannels featuring microfluidic devices fabricated by three different materials and methods,” Coatings 13, 1676 (2023)

  48. [48]

    S. M. Richardson, Fluid Mechanics (Hemisphere, New York, 1989)

  49. [49]

    Lagrangian-eulerian finite element formulation for in- compressible viscous flows,

    T. J. Hughes, W. K. Liu, and T. K. Zimmermann, “Lagrangian-eulerian finite element formulation for in- compressible viscous flows,” Comput. Methods Appl. Mech. Eng. 29, 329–349 (1981)

  50. [50]

    Acoustic tweezing of microparticles in microchannels with sinusoidal cross sections,

    E. A. Jannesar and H. Hamzehpour, “Acoustic tweezing of microparticles in microchannels with sinusoidal cross sections,” Sci. Rep. 11, 17902 (2021)

  51. [51]

    Acoustic interaction force between two particles immersed in a viscoelastic fluid,

    F. Eslami, H. Hamzehpour, S. Derikvandi, and S. Amir Bahrani, “Acoustic interaction force between two particles immersed in a viscoelastic fluid,” Phys. Fluids 35, 031707 (2023)

  52. [52]

    Radial particle displace - ments in poiseuille flow of suspensions,

    G. Segr´ e and A. Silberberg, “Radial particle displace - ments in poiseuille flow of suspensions,” Nature 189, 209–210 (1961)