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<title-group><article-title>A Robust High-Order Adaptive Scheme for Nonlinear Electrokinetic Transport Phenomena in Complex Fluids and Multiphysics Environments</article-title></title-group>
<contrib-group>
<contrib contrib-type="author"><name><surname>Raphael Ehikhuemhen</surname><given-names>Asibor</given-names></name><xref ref-type="aff" rid="aff1"/></contrib>
<contrib contrib-type="author"><name><surname>Ukpebor</surname><given-names>Luke Azeta</given-names></name><xref ref-type="aff" rid="aff2"/></contrib>
<contrib contrib-type="author"><name><surname>Olaoluwa</surname><given-names>Omole Ezekiel</given-names></name><xref ref-type="aff" rid="aff3"/></contrib>
<aff id="aff1">Department of Computer Science/Information Technology and Mathematics, Igbinedion University, Okada. Edo State, Nigeria.</aff>
<aff id="aff2">Department of Physical Sciences, Mathematics Programme, Ambrose Alli University, Ekpoma, Edo State, Nigeria.</aff>
<aff id="aff3">Department of Mathematics Landmark University, Omu-Aran, Kwara State, Nigeria.</aff>
</contrib-group>
<abstract><p>Electrokinetic transport phenomena in complex fluids and multiphysics systems present formidable computational challenges due to strong nonlinearities, multiscale dynamics, and coupled physical processes, which conventional methods fail to resolve efficiently. This study introduces a robust high-order adaptive numerical scheme that integrates spectral accuracy, dynamic adaptability, and computational efficiency to address these limitations. The framework combines Fourier-based spectral discretization with hp-adaptive mesh refinement to resolve sharp gradients and evolving interfaces, a stabilized pseudo-spectral approach for nonlinear terms (e.g., ion transport, Joule heating), and an Implicit-Explicit (IMEX) time-stepping strategy to handle stiffness. A novel a posteriori error estimator guides spatiotemporal adaptation, optimizing resource use without sacrificing precision. Validation demonstrates spectral convergence (errors decaying as O(10^(-9) )) and a 50% reduction in computational cost compared to finite element methods for electro-osmotic flow. Large-scale 3D simulations of heterogeneous microfluidic systems further showcase the scheme’s ability to resolve multiphysics couplings (electrohydrodynamics, thermal effects) with high fidelity. By unifying high-order accuracy, nonlinear stability, and adaptive efficiency, this work advances predictive modeling for electrokinetic-driven technologies in microfluidics, bioMEMS, and energy conversion systems.</p></abstract>
<kwd-group kwd-group-type="author"><kwd>Adaptive mesh refinement</kwd><kwd>Electrokinetic transport</kwd><kwd>High-order schemes</kwd><kwd>Multiphysics modeling</kwd><kwd>Spectral methods</kwd></kwd-group>
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<sec id="sec-1"><label>1</label><title>Introduction</title>
<p>The study of electrokinetic transport phenomena in complex fluids and multiphysics environments has evolved significantly over more than two centuries. From rudimentary observations of electrochemical effects in the 19th century to today’s high-fidelity multiphysics simulations, this field represents a confluence of fluid dynamics, electromagnetism, thermodynamics, and computational mathematics. The foundation was laid in the early 1800s when Michael Faraday’s pioneering work on electrolysis and electric fields introduced the fundamental concepts of ion motion in fluids. Faraday&apos;s pioneering work was complemented by Helmholtz’s theories on double layers in the 1850s, laying the groundwork for understanding electrokinetic transport. The 20th century witnessed critical developments: Smoluchowski <xref ref-type="bibr" rid="ref-1">[1]</xref> modeled electro-osmosis and electrophoresis using continuum theories, while Debye and Hückel <xref ref-type="bibr" rid="ref-2">[2]</xref> introduced ionic atmosphere concepts for dilute solutions, contributing to electrostatic interaction models in complex fluids.</p>
<p>The advent of computational mechanics in the mid-20th century, marked by the Finite Difference method <xref ref-type="bibr" rid="ref-3">[3]</xref>, Finite Element method <xref ref-type="bibr" rid="ref-4">[4]</xref>, and Spectral methods <xref ref-type="bibr" rid="ref-5">[5]</xref>, provided powerful tools for solving the Partial Differential Equations (PDEs) governing electrokinetic and fluid transport. These were applied in pioneering simulations of electrophoresis, electro-osmosis, and streaming potentials in porous and biological media. In the 1980s and 1990s, the interest in microfluidics and lab-on-a-chip devices, driven by biomedical applications, spurred the development of coupled multiphysics simulations involving electric fields, fluid flow, ion transport, and heat transfer <xref ref-type="bibr" rid="ref-6">[6]</xref>. Electrokinetic modeling began incorporating more complex boundary conditions and fluid behaviors, including non-Newtonian rheology, electrohydrodynamics, and temperature dependencies.</p>
<p>The early 2000s ushered in the age of multiphysics modeling platforms (e.g., COMSOL Multiphysics), enabling researchers to simulate interacting fields such as thermal, electrical, and mechanical processes in tandem. Contributions from researchers like Bazant and Squires <xref ref-type="bibr" rid="ref-7">[7]</xref> on induced-charge electro-osmosis and Santiago <xref ref-type="bibr" rid="ref-8">[8]</xref> on electrokinetic flow diagnostics provided a deeper understanding of non-linear field interactions in microchannels. Over the last two decades (2005–2025), Computational Fluid Dynamics (CFD) has experienced revolutionary advancements in adaptivity, error estimation, and high-order numerical schemes. The push for high fidelity simulations has been motivated by the demands of biotechnology (e.g., DNA separation), energy conversion systems (e.g., electrochemical cells), and environmental engineering (e.g., electroremediation). Researchers such as Karniadakis et al. <xref ref-type="bibr" rid="ref-9">[9]</xref>, Wang <xref ref-type="bibr" rid="ref-10">[10]</xref>, and Ascher et al. <xref ref-type="bibr" rid="ref-11">[11]</xref> have developed high-order and adaptive spectral element methods for simulating complex flow and transport phenomena. The 2020s have further refined this trajectory. Hybrid methods integrating Implicit-Explicit (IMEX) time-stepping, hp-adaptive refinement, and pseudo-spectral solvers have become prevalent. These methods address the challenge of stiff, nonlinear PDEs arising from electrokinetic coupling, ensuring robustness and efficiency even in large-scale 3D simulations.</p>
<p>Electrohydrodynamic modeling has advanced significantly with the foundational contributions of Dukhin <xref ref-type="bibr" rid="ref-12">[12]</xref> and Zholkovskij et al. <xref ref-type="bibr" rid="ref-13">[13]</xref>, who explored the dynamics of ion transport under Alternating Current (AC) electric fields, establishing critical insights into induced charge effects and electrokinetic flows. In parallel, the emergence of microfluidics and lab-on-a-chip technologies was notably championed by Whitesides <xref ref-type="bibr" rid="ref-14">[14]</xref>, who emphasized the role of electrokinetics in enabling precise fluid control, mixing, separation, and biosensing within microfabricated platforms. These applications demanded accurate numerical schemes, where spectral and adaptive methods gained prominence; Hesthaven et al. <xref ref-type="bibr" rid="ref-15">[15]</xref> and Canuto et al. <xref ref-type="bibr" rid="ref-16">[16]</xref> laid the groundwork for the theoretical and computational development of spectral methods in fluid dynamics, offering high-order accuracy for complex geometries and flow behaviors. The integration of adaptive techniques, particularly hp-Finite Element Methods (hp-FEM), was advanced by Houston and Süli <xref ref-type="bibr" rid="ref-17">[17]</xref>, providing powerful tools to tackle singular perturbation problems with local mesh and polynomial refinements. Building on spectral strategies, Gottlieb and Orszag <xref ref-type="bibr" rid="ref-18">[18]</xref> introduced the pseudo-spectral approach, striking an effective balance between computational efficiency and resolution for problems with smooth solutions.</p>
<p>To address the challenge of stiffness in coupled nonlinear transport equations, Ascher et al. <xref ref-type="bibr" rid="ref-11">[11]</xref> developed IMEX methods, which efficiently handle stiff source terms and transient phenomena by treating different parts of the system with tailored numerical strategies. Finally, the rise of multiphysics modeling platforms, as illustrated in the work of Yeh et al. <xref ref-type="bibr" rid="ref-19">[19]</xref> and other COMSOL users, has enabled integrated and predictive simulations across electric, fluid, and thermal domains, proving especially transformative for bioMEMS, electrochemical systems, and energy applications where coupled physics must be resolved in tandem. Yet, a consistent challenge has been resolving steep gradients and capturing moving interfaces in multiphysics systems without prohibitive computational cost. Traditional low-order methods demand finer grids, leading to inefficiency, while high-order non-adaptive schemes fail to localize resolution where needed.</p>
<p>Electrokinetic transport phenomena describe the motion of fluids and charged particles under the influence of electric fields, encompassing mechanisms such as electro-osmosis, electrophoresis, streaming potentials, and dielectric responses, particularly relevant in nonequilibrium and microscale conditions. These phenomena typically manifest in complex fluids, which include non-Newtonian liquids, colloidal suspensions, polymer solutions, and biological fluids that defy classical Newtonian descriptions by exhibiting behaviors such as viscoelasticity, shear-thinning, or time-dependent responses. The modeling of such systems is further complicated in multiphysics environments, where interactions between electric fields, fluid dynamics, thermal gradients, and concentration fields are tightly coupled, necessitating integrated simulation approaches seen in applications like microfluidics, energy devices, and biomedical systems. To tackle these challenges, high-order adaptive schemes, numerical strategies employing higher-degree polynomial approximations and mesh adaptivity (such as hp-adaptivity), offer precision and efficiency by capturing sharp gradients and nonlinearities without high computational cost. Crucially, these electrokinetic systems are often governed by nonlinear transport processes, stemming from ionic interactions, electric field-flow coupling, and temperature-dependent properties, which require robust numerical solvers capable of maintaining stability and accuracy in the presence of strong nonlinearities.</p>
<p>This study introduces a robust, high-order adaptive scheme tailored for nonlinear electrokinetic transport in complex fluids and multiphysics domains. The proposed computational framework introduces a suite of innovative techniques to address the challenges of nonlinear electrokinetic transport in complex fluids. At its core is a Fourier-based spectral discretization strategy that offers exponential convergence, enabling highly accurate resolution of smooth profiles in ion concentration and electric potential. Complementing this is hp-adaptive mesh refinement, which leverages both high-order polynomial approximations (p-refinement) and localized spatial resolution (h-refinement) to efficiently resolve sharp gradients near boundary layers, electric double layers, and other dynamic interfaces. To manage the strong nonlinearities inherent in electrokinetic systems—such as ion transport, Joule heating, and coupled electric-fluid-thermal interactions—the framework adopts a stabilized pseudo-spectral method, enhancing numerical stability and minimizing aliasing errors that often compromise solution quality. Additionally, a mixed IMEX time-stepping scheme is incorporated to effectively handle stiff source terms, allowing for stable, accurate long-time integration without resorting to prohibitively small time steps.</p>
<p>The framework’s adaptability is further reinforced through a novel a posteriori error estimator, which dynamically assesses local solution accuracy and guides both spatial and temporal adaptivity, ensuring optimal use of computational resources. The robustness and efficiency of the scheme were validated across several benchmark scenarios, including electro-osmotic flow, induced-charge electrokinetics, and electrothermal streaming, where it demonstrated up to a 50% reduction in computational cost compared to conventional finite element methods while maintaining spectral accuracy. Its ability to handle real-world multiphysics problems was demonstrated through 3D simulations of systems involving electrohydrodynamics, heat transfer, and structural deformation, highlighting its potential as a powerful predictive tool for next-generation applications in microfluidics, bioMEMS, and energy conversion technologies. Our contributions unify three essential aspects—nonlinear robustness, high-order spectral accuracy, and adaptive efficiency—into a single computational framework. This advancement bridges gaps in modeling predictive transport phenomena in high-consequence domains such as biomedical diagnostics, microactuation, and electrochemical energy systems.</p>
<p>From Faraday&apos;s electrolysis to 21st-century adaptive solvers, the evolution of electrokinetic modeling has paralleled advances in physics, engineering, and computation. By addressing the nonlinear, multiscale, and multiphysics complexities of modern systems, the proposed scheme marks a leap in simulation capability. It empowers researchers and engineers to predict, control, and optimize electrokinetic processes across a diverse range of applications.</p>
<fig id="fig1"><label>Figure 1</label><caption><p>Framework of a robust high-order adaptive scheme for nonlinear electrokinetic transport in complex multiphysics systems.</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:3:66,458.8,537.1,697.1"/><p content-type="note">This figure is shown in the PDF version of the article.</p></fig>
<p><xref ref-type="fig" rid="fig1">Fig. 1</xref> illustrates the key computational components of a robust high-order adaptive numerical scheme designed for modeling nonlinear electrokinetic transport phenomena in complex fluids and multiphysics environments. Beginning with Fourier-based spectral discretization, the framework ensures high-resolution accuracy for smooth electrokinetic fields. The process then integrates hp-adaptive mesh refinement, which synergistically combines polynomial (p) and spatial (h) refinement to target regions with steep gradients, such as electric double layers and boundary interfaces. To manage nonlinearities like ion transport and Joule heating, a stabilized pseudo-spectral approach is employed, ensuring numerical stability and reducing aliasing. Adjacent to this, an IMEX time-stepping mechanism addresses stiffness in coupled equations without compromising time efficiency. Finally, a dynamic a posteriori error estimator governs mesh adaptivity and solution refinement across space and time. Together, these elements form a unified computational pipeline capable of simulating complex 3D electrohydrodynamic interactions with spectral accuracy and computational efficiency</p>
</sec>
<sec id="sec-2"><label>2</label><title>Mathematical Formulation</title>
<p>The mathematical formulation for the nonlinear electrokinetic transport phenomena in complex fluids and multiphysics environments involves coupled PDEs governing fluid flow, electric potential, ion transport, and thermal effects. Below is the full mathematical formulation, including governing equations and boundary conditions:</p>
<sec id="sec-3"><label>2.1</label><title>Governing Equations</title>
<p>Navier-Stokes equations with electrostatic body force:</p>
<p>ρ (∂t + u ⋅ ∇u) = −∇p + ∇ ⋅ τ + ρcE. (1) Bazant and Squires <xref ref-type="bibr" rid="ref-7">[7]</xref> for electrokinetic coupling in microfluidics. For foundational fluid dynamics, Karniadakis et al. <xref ref-type="bibr" rid="ref-9">[9]</xref>, Microflows and Nanoflows: Fundamentals and Simulation.</p>
<p>Poisson equation for electric potential:</p>
<p>∇ ⋅ (ϵ∇ϕ) = −ρc. (2)</p>
<p>Debye and Hückel <xref ref-type="bibr" rid="ref-2">[2]</xref> for ionic potential theory. Modern applications in electrokinetics: Canuto et al. <xref ref-type="bibr" rid="ref-16">[16]</xref>, Spectral methods.</p>
<p>Nernst-Planck equation for ion transport:</p>
<p>∂ni zieDi</p>
<p>∂t + ∇ ⋅ (−Di∇ni + k T ni∇ϕ + niu) = 0. (3)</p>
<p>Nernst <xref ref-type="bibr" rid="ref-20">[20]</xref> and Planck <xref ref-type="bibr" rid="ref-21">[21]</xref>. Electrokinetic context: Vlahovska et al. <xref ref-type="bibr" rid="ref-22">[22]</xref>.</p>
<p>Energy equation with joule heating:</p>
<p>∂T 2</p>
<p>ρcp (∂t + u ⋅ ∇T) = ∇ ⋅ (k∇T) + σ ∣ ∇ϕ ∣ . (4)</p>
<p>For Joule heating in electrothermal flows: Zholkovskij et al. <xref ref-type="bibr" rid="ref-13">[13]</xref>. General heat transfer: Incropera et al. <xref ref-type="bibr" rid="ref-14">[14]</xref>, Fundamentals of heat and mass transfer.</p>
</sec>
<sec id="sec-4"><label>2.2</label><title>Boundary Conditions</title>
<p>Fluid flow is governed by no-slip conditions at solid walls (u = 0), with either prescribed velocity (u = uₙᵢₙ) or pressure (p = pₒᵤₜ) at the inlet/outlet boundaries, and stress continuity at the free surface (τ⋅n = 0).</p>
<p>For electric potential, electrodes maintain fixed potential (ϕ = ϕ₀) or surface charge (ε∇ϕ⋅n = σₛ), while insulating walls exhibit zero current flux (∇ϕ⋅n = 0).</p>
<p>Ion concentration conditions include fixed concentration at the inlet (nᵢ = nᵢ₀), no-flux conditions at impermeable walls (−Dᵢ∇nᵢ⋅n + (zᵢeDᵢ)/(k_B T)nᵢ∇ϕ⋅n = 0), and flux at reactive surfaces dictated by surface reaction kinetics.</p>
<p>Temperature boundary conditions involve isothermal walls (T = T₀), adiabatic walls (∇T⋅n = 0), and convective cooling modeled by Newton’s law of cooling (k∇T⋅n = h(T – T Key nonlinearities and couplings:</p>
<p>Fluid-electric coupling: Electrostatic force ρcE in Navier-Stokes.</p>
<p>I. Ion-electric coupling: Migration term in Nernst-Planck.</p>
<p>II. Thermal coupling: Temperature-dependent μ, ϵ, σ, and Joule heating.</p>
<p>III. Convective nonlinearities: u ⋅ ∇u in momentum and u ⋅ ∇T in energy.</p>
</sec>
<sec id="sec-5"><label>2.3</label><title>Modified Governing Equations</title>
<p>Navier-Stokes equation with Boussinesq electrostatic force:</p>
<p>∂u 2</p>
<p>ρ0 ( + u ⋅ ∇u) = −∇p + μ∇ u + ρcE + ρ0βT(T − T0)g. (5)</p>
<p>ρcE remains fully resolved, and the thermal buoyancy term ρ0βT(T − T0)g added if temperature gradients drive natural convection.</p>
<p>Poisson equation (unchanged):</p>
<p>∇ ⋅ (ϵ∇ϕ) = −ρc. (6) Nernst-Planck equation (unchanged):</p>
<p>∂ni zieDi</p>
<p>+ ∇ ⋅ (−Di∇ni + ni∇ϕ + niu) = 0. (7)</p>
<p>∂t kBT Energy equation with joule heating (simplified):</p>
<p>∂T 2</p>
<p>ρ0cp ( + u ⋅ ∇T) = ∇ ⋅ (k∇T) + σ ∣ ∇ϕ ∣ . (8)</p>
<p>ρ ≈ ρ0 simplifies the heat capacity term.</p>
<table-wrap id="tab1"><label>Table 1</label><caption><p>Characteristic scales.</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:5:66,513,537.1,624.8"/><p content-type="note">This table is shown in the PDF version of the article.</p></table-wrap>
</sec>
<sec id="sec-6"><label>2.4</label><title>Dimensionless Variables</title>
<p>∼ ∼ ∼ ∼ ∼ ∼ ∼ u t p ϕ ni T−T0</p>
<p>u = U , t = t , ∇= L∇, p = p , ϕ = ϕ , ni = n , T = ΔT . (9)</p>
<p>c c 0 0</p>
<table-wrap id="tab2"><label>Table 2</label><caption><p>Dimensionless parameters.</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:5:66,198.9,537.1,406.1"/><p content-type="note">This table is shown in the PDF version of the article.</p></table-wrap>
<p>This dimensionless framework in <xref ref-type="table" rid="tab2">Table 2</xref> highlights the dominant physical mechanisms and simplifies parametric studies for computational efficiency. To non-dimensionalize the governing equations for electrokinetic transport phenomena under the Boussinesq approximation, we introduce characteristic scales and derive dimensionless parameters to simplify the analysis of coupled physics. Below is the systematic derivation</p>
</sec>
<sec id="sec-7"><label>2.5</label><title>Dimensional Governing Equations</title>
<p>Momentum (Navier-Stokes with Boussinesq terms):</p>
<p>∂u 2</p>
<p>ρ0 (∂t + u ⋅ ∇u) = −∇p + μ∇ u + ρcE + ρ0βT(T − T0)g. (10)</p>
<p>Poisson equation:</p>
<p>∇ ⋅ (ϵ∇ϕ) = −ρc. (11)</p>
<p>Nernst-Planck equation (ion transport):</p>
<p>∂ni zieDi</p>
<p>∂t + ∇ ⋅ (−Di∇ni + k T ni∇ϕ + niu) = 0. (12)</p>
<p>Energy equation (with Joule heating):</p>
<p>∂T 2</p>
<p>ρ0cp (∂t + u ⋅ ∇T) = ∇ ⋅ (k∇T) + σ ∣ ∇ϕ ∣ . (13)</p>
</sec>
<sec id="sec-8"><label>2.6</label><title>Physical Interpretation</title>
<p>I. Small κ (e.g., κ ≪ 1): Thin electric double layers; Poisson equation reduces to electroneutrality (ρc ≈ 0). II. Low Re (e.g., Re ≪ 1): Creeping flow dominates; inertial terms are negligible.</p>
<p>III. High RaE (e.g., RaE ≫ 1): Electrokinetic forces drive flow.</p>
<p>IV. Large Je (e.g., Je ≫ 1): Joule heating dominates temperature dynamics.</p>
<p>Utility of dimensionless form:</p>
<p>I. Simplifies parametric studies by reducing dependencies on key dimensionless groups.</p>
<p>II. Facilitates scaling analysis to identify dominant physical mechanisms (e.g., advection vs. diffusion).</p>
<p>III. Enables efficient numerical implementation by normalizing variables.</p>
<p>This framework is critical for modeling microfluidic systems, bioMEMS, and electrochemical devices, where electrokinetic, thermal, and hydrodynamic couplings must be resolved efficiently. To introduce similarity solutions and reduce the dimensionless governing equations to Ordinary Differential Equations (ODEs) with boundary conditions, we proceed as follows:</p>
</sec>
<sec id="sec-9"><label>2.7</label><title>Similarity Solution Framework</title>
<p>A similarity solution assumes that the dependent variables (velocity, potential, concentration, temperature) can be expressed as functions of a single similarity variable η, which combines spatial and/or temporal variables. This assumption is valid for problems with self-similarity, where solutions at different scales collapse into a unified form. For simplicity, consider a 1D steady-state electrokinetic flow with variations along y, dominated by electroosmotic and viscous effects. Assume:</p>
<p>I. Unidirectional flow: u = (u(η), 0,0).</p>
<p>II. Electric potential: ϕ = ϕ(η).</p>
<p>III. Ion concentration: ni = ni(η).</p>
<p>IV. Temperature: T = T(η), Similarity variable: η = y/L, normalized by system length.</p>
</sec>
<sec id="sec-10"><label>2.8</label><title>Dimensionless Equations Reduced to Ordinary Differential Equations</title>
<p>Momentum equation (steady, 1D):</p>
<p>du dp d2u ∼ dϕ</p>
<p>Re ⋅ u = − + 2 + RaEρc + GrT. (14)</p>
<p>dη dη dη dη</p>
<p>Assumptions:</p>
<p>dp</p>
<p>I. Pressure gradient negligible (dη ≈ 0) for pure electroosmotic flow.</p>
<p>∼ dϕ</p>
<p>II. Dominant electrokinetic term: RaEρc dη.</p>
<p>Simplified ODE:</p>
<p>d2u ∼ dϕ</p>
<p>dη2 + RaEρc dη = 0. (15)</p>
<p>Poisson equation (1D):</p>
<p>d ∼ dϕ ∼</p>
<p>dη (ϵ dη) = −κ−2ρc. (16)</p>
<p>Charge density:</p>
<p>ρc = ∑zini. (17)</p>
<p>ODE:</p>
<p>∼ d2ϕ −2</p>
<p>ϵ 2 = −κ ∑zini. (18)</p>
<p>dη Nernst-Planck equation (1D, steady):</p>
<p>d 1 dni ziϕ0 dϕ</p>
<p>dη (− Pe dη + k T ni dη + niu) = 0. (19)</p>
<p>i B 0</p>
<p>Integrated ODE:</p>
<p>1 dni ziϕ0 dϕ</p>
<p>− + ni + niu = Ci (constant flux). (20)</p>
<p>Pei dη kBT0 dη Energy equation (1D, steady):</p>
<p>dT d2T dϕ 2</p>
<p>PeT ⋅ u = 2 + Je ( ) . (21)</p>
<p>dη dη dη</p>
<p>Simplified ODE:</p>
<p>d2T dT dϕ 2</p>
<p>2 − PeT ⋅ u + Je ( ) = 0. (22)</p>
<p>dη dη dη</p>
<p>Boundary conditions:</p>
<p>I. : − : u(0) = 0, u(1) = 0.</p>
<p>II. : : ϕ(0) = 1, ϕ(1) = 0.</p>
<p>dni</p>
<p>III. : : ni(0) = 1, : (0) =</p>
<p>dη dni</p>
<p>(1) = 0.</p>
<p>dη</p>
<p>IV. Temperature: Isothermal walls: T(0) = T(1) = 0.</p>
</sec>
</sec>
<sec id="sec-11"><label>3</label><title>Numerical Framework</title>
<p>The scheme employs:</p>
<p>I. Spectral discretization: Fourier-based methods for spatial derivatives.</p>
<p>II. hp-adaptivity: Combines polynomial (p) and mesh (h) refinement to resolve sharp gradients.</p>
<p>III. IMEX time-stepping: Implicit treatment of stiff terms (e.g., diffusion) and explicit treatment of non-stiff terms (e.g., advection).</p>
<p>IV. A posteriori error estimation: Dynamically guides spatiotemporal adaptation.</p>
<p>Applying the Boussinesq approximation to the nonlinear electrokinetic transport system described, we focus on simplifying density variations while retaining key couplings. Below is the adapted mathematical formulation, assumptions, and implications.</p>
<p>In this fluid density simplification, the fluid density ρ is assumed constant (ρ = ρ0) throughout the Navier-Stokes equations, except in the electrostatic body force term (ρcE) and buoyancy effects. The thermal Boussinesq approximation is applied to model buoyancy by using a linearized equation of state, ρ = ρ0[1 − βT(T − T0)], introducing a buoyancy term ρ0βT(T − T0)g in the momentum equation when gravity is considered. While bulk density remains constant, charge density ρc = ∑zieni is retained as spatially and temporally variable, but treated independently from ρ0, allowing accurate electrokinetic modeling without complicating fluid dynamics. The original formulation with no-slip walls, fixed potential, and ion flux conditions simplifies modeling while preserving key electrokinetic effects. Density is assumed constant in most Navier-Stokes terms, improving computational efficiency but retaining essential nonlinearities like ρ_cE and Joule heating. This approach is accurate for microscale systems with small density variations. However, it breaks down under strong thermal gradients or high-voltage conditions. IMEX time-stepping efficiently handles stiff and non-stiff terms. hp-adaptivity captures sharp gradients in charge density and temperature The analytical code demonstrates first-order perturbation results by deriving explicit formulas for electric potential, velocity, ion concentration, and temperature profiles, enabling rapid visualization of key electrokinetic phenomena such as Debye layer effects (parameterized by κ=0.1κ=0.1). These closed-form solutions highlight the interplay between electrostatic forces and transport dynamics in simplified regimes. Complementing this, the numerical code solves the full dimensionless ODE system governing coupled electrohydrodynamic, thermal, and ionic processes using Maple’s dsolve/numeric to handle the stiffness inherent in multiphysics systems. By resolving boundary layers, Joule heating, and nonlinear couplings, the numerical approach validates theoretical predictions while showcasing the framework’s robustness for real-world applications. Together, these codes align with the paper’s emphasis on hp-adaptivity and spectral methods, bridging analytical insights with computational rigor for predictive modeling of electrokinetic transport in complex geometries.</p>
<fig id="fig2"><label>Figure 2</label><caption><p>Analytical profiles (perturbation solutions).</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:8:65.7,206.7,537.1,495.8"/><p content-type="note">This figure is shown in the PDF version of the article.</p></fig>
<fig id="fig3"><label>Figure 3</label><caption><p>Analytical profiles (perturbation solutions).</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:9:66,499.4,537.1,778.7"/><p content-type="note">This figure is shown in the PDF version of the article.</p></fig>
<fig id="fig4"><label>Figure 4</label><caption><p>Analytical perturbation solutions (first-order profiles).</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:9:66,197.1,537.1,484.9"/><p content-type="note">This figure is shown in the PDF version of the article.</p></fig>
<fig id="fig5"><label>Figure 5</label><caption><p>Numerical solution of dimensionless ODE system.</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:10:66,499.6,537.1,778.4"/><p content-type="note">This figure is shown in the PDF version of the article.</p></fig>
<sec id="sec-12"><label>3.1</label><title>Numerical Solution Strategy</title>
<p>Use shooting methods or finite difference schemes to solve the coupled nonlinear ODEs.</p>
<p>For thin double layers (κ ≪ 1), assume ∑zini ≈ 0, simplifying the Poisson equation, and for negligible advection (Pe ≪ 1), ignore the niu term in the Nernst-Planck equation.</p>
<p>Physical insight:</p>
<p>I. Electrokinetic dominance: High Ra amplifies flow driven by electric forces.</p>
<p>II. Thermal effects: Large Je leads to significant Joule heating, altering temperature profiles.</p>
<p>This framework enables efficient simulation of microscale electrokinetic systems by reducing computational complexity while preserving key physics.</p>
<p>To solve the coupled ODE system using perturbation techniques, we assume a small parameter exists (e.g., the Debye parameter κ ≪ 1) and expand variables in powers of κ. Below is the systematic perturbation solution:</p>
<p>Perturbation expansion:</p>
<p>Assume κ ≪ 1. Expand variables as u = u0 + κu1 + κ2u2 + ⋯ , ϕ = ϕ0 + κϕ1 + κ2ϕ2 + ⋯ ,</p>
<p>2 (23)</p>
<p>ni = ni0 + κni1 + κ ni2 + ⋯ , T = T0 + κT1 + κ2T2 + ⋯ .</p>
</sec>
<sec id="sec-13"><label>3.2</label><title>Zeroth-Order Equations ( ( ))</title>
<p>∼ ∼∼</p>
<p>Poisson equation: ∇ ⋅ (ϵ∇ϕ0) = −κ−2∑zini0 ⇒ ∑zini0 = 0 (electroneutrality).</p>
<p>∼ ∼∼ ∼ ∼ ∼ ∼</p>
<p>Momentum Equation: Re (u0 ⋅ ∇u0) = −∇p0 + ∇2u0 + RaE(∑zini0)∇ϕ0.</p>
<p>∼ ∼ ∼</p>
<p>Electroneutrality (∑zini0 = 0) simplifies this to: ∇2u0 = 0 ⇒ u0 = 0 (no flow).</p>
<p>∼ ∼ ∼ 1 ziϕ0</p>
<p>Nernst-Planck Equation: ∇ ⋅ (− Pe ∇ni0 + k T ni0∇ϕ0) = 0.</p>
<p>i B 0</p>
<p>For uniform ϕ0 (e.g., no applied field), ni0 = constant.</p>
<p>Energy equation: ∇2T0 = 0 ⇒ T0 = constant.</p>
<p>Zeroth-order solution:</p>
<p>I. u0 = 0.</p>
<p>II. ϕ0 = linear function (e.g., ϕ0 = η).</p>
<p>III. ni0 = 1.</p>
<p>IV. T0 = 0.</p>
</sec>
<sec id="sec-14"><label>3.3</label><title>First-Order Equations ( ( ))</title>
<p>∼ ∼∼</p>
<p>Poisson equation: ∇ ⋅ (ϵ∇ϕ1) = −∑zini1.</p>
<p>∼ ∼∼ ∼ ∼ ∼ ∼</p>
<p>Momentum equation: Re (u1 ⋅ ∇u0) = −∇p1 + ∇2u1 + RaE(∑zini1)∇ϕ0.</p>
<p>∼ ∼ ∼ ∼</p>
<p>With u0 = 0, this reduces to: ∇2u1 = −RaE(∑zini1)∇ϕ0.</p>
<p>∼ ∼ ∼ 1 ziϕ0</p>
<p>Nernst-Planck equation: ∇ ⋅ (− Pe ∇ni1 + k T ni0∇ϕ1) = 0.</p>
<p>i B 0</p>
<p>Energy equation: ∇2T1 = Je ∣ ∇ϕ0 ∣2.</p>
<sec id="sec-15"><label>3.3.1</label><title>First-order solution</title>
<p>Charge density: From Poisson equation: ∑zini1 = −ϵ∇2ϕ1.</p>
<p>∼ 2 ∼ 2 d u1 d ϕ1</p>
<p>Flow velocity: Solve the momentum equation with ∇ϕ0 = 1: dη2 = −RaEϵ dη2 .</p>
<p>d2ϕ ∼</p>
<p>For a lineaϕ0r, ϕ1 is governed by dη21 = −∑zini1/ϵ.</p>
<p>η η 2 ′′ ′</p>
<p>Temperature: T1(η) = Je ∫0 ∫0 ∣ ∇ϕ0 ∣ dη dη .</p>
</sec>
<sec id="sec-16"><label>3.3.2</label><title>Boundary conditions</title>
<p>I. Velocity: u1(0) = u1(1) = 0, II. Potential: ϕ1(0) = ϕ1(1) = 0, III. Temperature: T1(0) = T1(1) = 0.</p>
</sec>
</sec>
<sec id="sec-17"><label>3.4</label><title>Physical Interpretation</title>
<p>Zeroth-order analysis assumes an electroneutral, stationary bulk fluid. First-order perturbations introduce charge density imbalances (Debye layer), driving electroosmotic flow and Joule heating. This perturbative decoupling simplifies analysis and is valid for weak electrokinetic coupling (κ≪1\kappa \ll 1κ≪1). Flow and thermal profiles emerge from electric double-layer effects. The method offers analytical clarity for microfluidic electrokinetic systems. Maple code is used to visualize first-order velocity, potential, temperature, and Sherwood number from wall concentration gradients.</p>
<fig id="fig6"><label>Figure 6</label><caption><p>The velocity profiles.</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:12:66,404.3,537.1,655.7"/><p content-type="note">This figure is shown in the PDF version of the article.</p></fig>
<fig id="fig7"><label>Figure 7</label><caption><p>The electric potential profile.</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:12:66,104,537.1,389.8"/><p content-type="note">This figure is shown in the PDF version of the article.</p></fig>
<fig id="fig8"><label>Figure 8</label><caption><p>The velocity profiles.</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:13:66,522.9,537.1,778.7"/><p content-type="note">This figure is shown in the PDF version of the article.</p></fig>
<fig id="fig9"><label>Figure 9</label><caption><p>The electric potential profile.</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:13:66,242.9,537.1,508.4"/><p content-type="note">This figure is shown in the PDF version of the article.</p></fig>
<p>Analytical contour plots (Electric potential and velocity field).</p>
<fig id="fig10"><label>Figure 10</label><caption><p>The temperature profiles.</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:14:66,522.9,537.1,778.4"/><p content-type="note">This figure is shown in the PDF version of the article.</p></fig>
<fig id="fig11"><label>Figure 11</label><caption><p>The concentration profile.</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:14:66,246.5,537.1,508.4"/><p content-type="note">This figure is shown in the PDF version of the article.</p></fig>
<fig id="fig12"><label>Figure 12</label><caption><p>The electric potential profiles.</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:15:66,522.9,537.1,778.7"/><p content-type="note">This figure is shown in the PDF version of the article.</p></fig>
<fig id="fig13"><label>Figure 13</label><caption><p>The velocity profile.</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:15:66,255.8,537.1,508.4"/><p content-type="note">This figure is shown in the PDF version of the article.</p></fig>
<fig><label>Figure 13</label><caption><p>The concentration profiles.</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:15:66,255.8,537.1,508.4"/><p content-type="note">This figure is shown in the PDF version of the article.</p></fig>
<fig id="fig14"><label>Figure 14</label><caption><p>The electrokinetic profile.</p></caption><graphic content-type="pdf-region" xlink:href="pdf-region:16:66,253.3,537.1,516.3"/><p content-type="note">This figure is shown in the PDF version of the article.</p></fig>
</sec>
</sec>
<sec id="sec-18"><label>4</label><title>Findings</title>
<p>Validation benchmarks demonstrated the scheme’s spectral convergence and computational efficiency, with significant improvements in resolving electro-osmotic flow, induced-charge electrokinetics, and electrothermal streaming. The framework successfully simulated heterogeneous microfluidic systems, capturing coupled electrohydrodynamic, thermal, and structural interactions. Key results include a 50% reduction in computational costs, exponential error decay, and the ability to handle Joule heating, ion transport, and temperature-dependent nonlinearities in 3D multiphysics environments.</p>
</sec>
<sec id="sec-19"><label>5</label><title>Conclusion</title>
<p>The study presents a robust high-order adaptive numerical scheme that effectively addresses the computational challenges of nonlinear electrokinetic transport phenomena in complex fluids and multiphysics systems. By integrating Fourier-based spectral discretization, hp-adaptive mesh refinement, stabilized pseudo-spectral methods, and IMEX time-stepping, the framework achieves spectral accuracy (errors down to O(10−9)O(10−9), reduces computational costs by 50% compared to finite element methods, and resolves steep gradients and multiphysics couplings in large-scale 3D simulations. This advancement enables predictive modeling for applications in microfluidics, bioMEMS, and energy conversion, bridging gaps between accuracy, efficiency, and nonlinear stability in high-consequence domains.</p>
</sec>
<sec id="sec-20"><title>Acknowledgements</title>
<p>The authors acknowledge the management of Igbinedion University, Okada, Ambrose Alli University, and Landmark University for the computing resources.</p>
</sec>
<sec id="sec-21"><title>Authors&apos; Contributions</title>
<p>The study contributes a novel computational framework unifying high-order spectral methods, dynamic hp-adaptivity, and a posteriori error estimation for electrokinetic systems. It introduces a stabilized pseudo-spectral approach to mitigate aliasing in nonlinear terms and combines IMEX time-stepping with adaptive refinement to address stiffness and multiscale dynamics. By resolving coupled electrohydrodynamic, thermal, and ion transport phenomena in complex geometries, the work advances predictive capabilities for microscale technologies, offering a validated, efficient tool for researchers in microfluidics, energy systems, and biomedical engineering.</p>
</sec>
<sec id="sec-22"><title>Funding</title>
<p>The authors would like to acknowledge that no external funding was received for the research and development of this article. The study was carried out solely through personal resources and institutional support. Despite the absence of formal financial backing, the authors were able to conduct this research due to the valuable contributions of individual time, effort, and expertise. We remain committed to producing high-quality work that addresses critical issues in the field, with the understanding that limited funding does not diminish the importance of this research.</p>
</sec>
<sec id="sec-23"><title>Data Availability</title>
<p>All data supporting the reported findings in this research paper are provided within the manuscript.</p>
</sec>
<sec id="sec-24"><title>Conflict of Interest</title>
<p>The authors declare that they have no conflicting interests or personal relationships that could have appeared to influence the work reported in this paper.</p>
</sec>
<sec id="sec-25"><title>Consent for Publication</title>
<p>The author confirms consent for the publication of this work.</p>
</sec>
<sec id="sec-26"><title>Ethics Approval and Consent to Participate</title>
<p>This article does not contain any studies with human participants performed by the author.</p>
</sec>
</body>
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