<p>Classical studies on surfactant-laden droplets in a tubular Poiseuille flow by Pak et al. (J Fluid Mech 753:535–552, 2014) and Dandekar and Ardekani (J Fluid Mech 902:A2, 2020) have elucidated remarkable cross-stream migration phenomena as a second-order effect in low surface Péclet number <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10665_2025_10432_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="27" /> </InlineMediaObject> <EquationSource Format="TEX">\(Pe_\textrm{s}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <msub> <mi>e</mi> <mtext>s</mtext> </msub> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10665_2025_10432_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="83" /> </InlineMediaObject> <EquationSource Format="TEX">\((=V_\textrm{c}a/D_\textrm{s})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mo>=</mo> <msub> <mi>V</mi> <mtext>c</mtext> </msub> <mi>a</mi> <mo stretchy="false">/</mo> <msub> <mi>D</mi> <mtext>s</mtext> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> limit, where <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10665_2025_10432_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(V_\textrm{c}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>V</mi> <mtext>c</mtext> </msub> </math></EquationSource> </InlineEquation> is the characteristic flow velocity, <i>a</i> denotes the droplet radius and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10665_2025_10432_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(D_\textrm{s}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>D</mi> <mtext>s</mtext> </msub> </math></EquationSource> </InlineEquation> is the diffusivity of the surfactant. However, in many biomedical lab-on-a-chip devices, droplet motion occurs between two parallel plates due to combined shear and pressure-driven flow. We unravelled that such a combined flow can lead to better steering of the droplet with enhanced migration velocity. Our model incorporates heat generation by living cells via a thermal dipole within the droplet, surrounded by a non-isothermal medium. We found that the cross-stream migration velocity can be at the leading order in <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10665_2025_10432_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="27" /> </InlineMediaObject> <EquationSource Format="TEX">\(Pe_\textrm{s}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <msub> <mi>e</mi> <mtext>s</mtext> </msub> </mrow> </math></EquationSource> </InlineEquation>, provided the thermocapillary effects combined with the strength of the thermal dipole are strong enough. A novel aspect of this work is the definition of flow control parameters based on a constant volumetric flow rate condition, which governs the droplet migration and flow patterns. We illustrate that a careful transition between flow profiles, specifically from Poiseuille to Couette, provides optimal control in droplet migration, and employing a rectangular geometry instead of a tubular gives better regulation on steering a droplet for accurate microfluidic investigations.</p>

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Steering a Thermocapillary Droplet Motion in Combined Couette–Poiseuille Flow

  • Arindam Basak,
  • Rajaram Lakkaraju,
  • G. P. Raja Sekhar

摘要

Classical studies on surfactant-laden droplets in a tubular Poiseuille flow by Pak et al. (J Fluid Mech 753:535–552, 2014) and Dandekar and Ardekani (J Fluid Mech 902:A2, 2020) have elucidated remarkable cross-stream migration phenomena as a second-order effect in low surface Péclet number \(Pe_\textrm{s}\) P e s \((=V_\textrm{c}a/D_\textrm{s})\) ( = V c a / D s ) limit, where \(V_\textrm{c}\) V c is the characteristic flow velocity, a denotes the droplet radius and \(D_\textrm{s}\) D s is the diffusivity of the surfactant. However, in many biomedical lab-on-a-chip devices, droplet motion occurs between two parallel plates due to combined shear and pressure-driven flow. We unravelled that such a combined flow can lead to better steering of the droplet with enhanced migration velocity. Our model incorporates heat generation by living cells via a thermal dipole within the droplet, surrounded by a non-isothermal medium. We found that the cross-stream migration velocity can be at the leading order in \(Pe_\textrm{s}\) P e s , provided the thermocapillary effects combined with the strength of the thermal dipole are strong enough. A novel aspect of this work is the definition of flow control parameters based on a constant volumetric flow rate condition, which governs the droplet migration and flow patterns. We illustrate that a careful transition between flow profiles, specifically from Poiseuille to Couette, provides optimal control in droplet migration, and employing a rectangular geometry instead of a tubular gives better regulation on steering a droplet for accurate microfluidic investigations.