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Research article · 2022 · Full text

International Journal of Statistics and Applied Mathematics

Oscillatory electro-hydrodynamic (EHD) fluid flow through a microchannel in the presence of radiative heat and a magnetic field

KW BunonyoUC Amadi

Volume 7(3) · Pages 155–166 · DOI: 10.22271/maths.2022.v7.i3b.836 ↗

Research areasNanofluid Flow and Heat TransferFluid Dynamics and Turbulent FlowsSolar Thermal and Photovoltaic Systems

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Abstract

Author-written

In this article, we investigated the oscillatory flow of an electo-hydrodynamic fluid flow through a channel with a radiative heat and magnetic field. The momentum equation, energy equation, and lipid concentration equation were used to represent the problem under consideration. The dimensionless equations were reduced to ordinary differential equations using the oscillatory perturbation parameters after the partial differential equations were scaled to be dimensionless. The ordinary differential equations are directly solved.We obtained some governing parameters during the analysis of the solution, such as thermal Grashof number, nanoparticles Grashof number, Reynolds number, wave number, radiation absorption parameter, thermophoresis parameter, electroosmotic parameter, and Schmidt number, respectively. The study was conducted to investigate the effects of the aforementioned parameters on the various flow profiles, and the results showed that the Grashof number, electroosmotic, and thermophoresis caused the fluid velocity to increase after varying them within a specific range, whereas the Brownian parameter, Reynolds number, and wave number caused the velocity to decrease. The thermophoresis and electroosmotic parameter values, on the other hand, raise the temperature of the fluid. Finally, we were able to develop a coupled system of mathematical models that represent electro-hydrodynamic fluid flow through a channel, solve it, and obtain exact solutions for the velocity profile, temperature profile, and lipid concentration profile.

Summary

Source-checked

Plain-language reading of the full paper, prepared with AI and checked against the text. Each point links to the authors' own words.

  1. Why it matters

    • Electro-osmotic flow (EOF) occurs when an external electric field drives fluid through conduits like microchannels, which is useful for micro-energy systems and liquid chromatography. View evidence ↗

      Why it matters

      Electro-osmotic flow (EOF) occurs when an external electric field drives fluid through conduits like microchannels, which is useful for micro-energy systems and liquid chromatography.

      In the paper's own words

      “According to Resuss, an electrokinetic phenomenon, also known as electroosmosis or electro-osmotic flow (EOF), is defined as the flow of fluid in any conduit (e.g., microchannel, capillary tube) under the influence of an external electric field (1809) [1]. Micro-flow injection analysis, micro-liquid chromatography, and micro-energy systems all benefit from EOF.”

      Page 1

      Found in: Introduction

      Read it in the full textOpen PDF at page 1 ↗
    • Nanofluids are used because they offer better thermophysical properties, such as improved thermal conductivity and diffusivity, compared to standard fluids. View evidence ↗

      Why it matters

      Nanofluids are used because they offer better thermophysical properties, such as improved thermal conductivity and diffusivity, compared to standard fluids.

      In the paper's own words

      “Nanofluids have been found to have improved thermophysical properties (thermal conductivity, thermal diffusivity, and the viscosity of the convective heat transport coefficient) when compared to conventional fluids.”

      Page 1

      Found in: Introduction

      Read it in the full textOpen PDF at page 1 ↗
  2. The question

    • The study aims to investigate the oscillatory flow of an electro-hydrodynamic fluid through a channel subject to a magnetic field and radiative heat. View evidence ↗

      The question

      The study aims to investigate the oscillatory flow of an electro-hydrodynamic fluid through a channel subject to a magnetic field and radiative heat.

      In the paper's own words

      “In this article, we investigated the oscillatory flow of an electo-hydrodynamic fluid flow through a channel with a radiative heat and magnetic field.”

      Page 1

      Found in: Conclusion

      Read it in the full textOpen PDF at page 1 ↗
  3. What they did

    • The researchers used momentum, energy, and lipid concentration equations to mathematically model the fluid flow. View evidence ↗

      What they did

      The researchers used momentum, energy, and lipid concentration equations to mathematically model the fluid flow.

      In the paper's own words

      “The momentum equation, energy equation, and lipid concentration equation were used to represent the problem under consideration.”

      Page 1

      Found in: Introduction

      Read it in the full textOpen PDF at page 1 ↗
    • Partial differential equations were scaled to be dimensionless and then reduced to ordinary differential equations using oscillatory perturbation parameters. View evidence ↗

      What they did

      Partial differential equations were scaled to be dimensionless and then reduced to ordinary differential equations using oscillatory perturbation parameters.

      In the paper's own words

      “The dimensionless equations were reduced to ordinary differential equations using the oscillatory perturbation parameters after the partial differential equations were scaled to be dimensionless.”

      Page 1

      Found in: Mathematical Models

      Read it in the full textOpen PDF at page 1 ↗
    • The problem was solved using analytical methods and numerical simulations performed with Wolfram Mathematica version 12. View evidence ↗

      What they did

      The problem was solved using analytical methods and numerical simulations performed with Wolfram Mathematica version 12.

      In the paper's own words

      “This article showed analytical solution of the formulated problem and numerical simulation done using Wolfram Mathematica, version 12.”

      Page 6

      Found in: Conclusion

      Read it in the full textOpen PDF at page 6 ↗
  4. What they found

    • An increase in the Brownian parameter results in a decrease in the velocity of the fluid. View evidence ↗

      What they found

      An increase in the Brownian parameter results in a decrease in the velocity of the fluid.

      In the paper's own words

      “The fluid velocity decreases as the Brownian parameter increases.”

      Page 11

      Found in: Conclusion

      Read it in the full textOpen PDF at page 11 ↗
    • The fluid temperature increases as the nanoparticles Grashof number increases. View evidence ↗

      What they found

      The fluid temperature increases as the nanoparticles Grashof number increases.

      In the paper's own words

      “An increase in nanoparticles, the Grashof number, increases the fluid temperature.”

      Page 11

      Found in: Reynolds number and wave number increases cause a

      Read it in the full textOpen PDF at page 11 ↗
    • An increase in the Schmidt number causes the fluid temperature to decrease. View evidence ↗

      What they found

      An increase in the Schmidt number causes the fluid temperature to decrease.

      In the paper's own words

      “The Schmidt number increase decreases the fluid temperature.”

      Page 11

      Found in: Reynolds number and wave number increases cause a

      Read it in the full textOpen PDF at page 11 ↗
  5. What it means

    • The authors concluded that they successfully developed and solved a coupled system of mathematical models to determine exact profiles for velocity, temperature, and lipid concentration. View evidence ↗

      What it means

      The authors concluded that they successfully developed and solved a coupled system of mathematical models to determine exact profiles for velocity, temperature, and lipid concentration.

      In the paper's own words

      “Finally, we were able to develop a coupled system of mathematical models that represent electro-hydrodynamic fluid flow through a channel, solve it, and obtain exact solutions for the velocity profile, temperature profile, and lipid concentration profile.”

      Page 1

      Found in: Method of Solution

      Read it in the full textOpen PDF at page 1 ↗

Visual summary

1 visuals

Illustrations explain the paper; they do not show study data.

AI-generated illustration
AI-generated conceptual illustration (electro-hydrodynamic fluid in a glass microchannel). It explains the idea and does not show study data.↗ Enlarge
Conceptual Model of EHD Flow
AI-generated conceptual illustration (electro-hydrodynamic fluid in a glass microchannel). It explains the idea and does not show study data.

AI-generated conceptual illustration (electro-hydrodynamic fluid in a glass microchannel). It explains the idea and does not show study data.

Open full-size image ↗

Conceptual Model of EHD Flow

AI-generated conceptual illustration (electro-hydrodynamic fluid in a glass microchannel). It explains the idea and does not show study data.

View source evidence ↗

Figures & tables

From the original paper
The Effect of thermal Grashof number on velocity profile, withFigure 1Page 6The effect of thermophoresis parameter on velocity profile, withFigure 2Page 7The effect of Brownian motion parameter on velocity profile, withFigure 3Page 7The effect of Reynolds number on velocity profile, withFigure 4Page 7The effect of wave number on velocity profile, withFigure 5Page 8The effect of electroosmotic parameter on velocity profile, withFigure 6Page 8The effect of nanoparticles Grashof number on nanoparticles fraction profile, withFigure 7Page 8The effect of thermophoresis on nanoparticles fraction profile, withFigure 8Page 9The effect of Schmidt number on nanoparticles fraction profile, withFigure 9Page 9The effect of radiation absorption on temperature profile, withFigure 10Page 9The effect of wave number on temperature profile, withFigure 11Page 10The effect of oscillatory parameter on temperature profile, withFigure 12Page 10The effect of an electroosmotic values on concentration profile, withFigure 13Page 10
FULL TEXT Original article · reflowed for reading

Introduction

According to Resuss, an electrokinetic phenomenon, also known as electroosmosis or electroosmotic flow (EOF), is defined as the flow of fluid in any conduit (e.g., microchannel, capillary tube) under the influence of an external electric field (1809) [1] . Micro-flow injection analysis, micro-liquid chromatography, and micro-energy systems all benefit from EOF. Other authors' research is included below. Patankar et al. 1998 [2] studied the electro-osmotic flow through a microchannel. Yang et al. 2021 [3] investigated EOF in microfluidics. Tang et al. 2009 [4] investigated the EOF in the context of a power-law model. Miller et al. 2001 [5] predicted EOF using a carbon nanotube membrane later on. Nanofluids have been found to have improved thermophysical properties (thermal conductivity, thermal diffusivity, and the viscosity of the convective heat transport coefficient) when compared to conventional fluids. Nano-liquid elements have shown colossal potential applications in many fields. The endoscopic effect of nanofluids in peristalsis was dissected by Akbar et al. 2011 [6] . Noreen 2013 [7] explored nanofluids under initiated attractive fields and blended convection. Moreover, Tripathi et al. 2014 [8] contemplated the peristaltic movement of nanofluid. Reddy et al. (2015) [9] suggested the peristaltic stream of nanofluid through objection dividers. Ebaid et al. 2018 [10] inspected the peristaltic movement of nanofluid under convective circumstances. Shao et al. 2016 [11] read up a reference answer for twofold dispersion convection. Twofold diffusive convection is a liquid element peculiarity that describes a type of convection driven if at the point when the temperature contrast is held consistent, warm dispersion delivers a focused inclination. Taking into account the wide uses of twofold diffusive convection, it was concentrated in a nano-fluidic stream model with peristaltic siphoning. Huppert et al. 1981 [12] examined the utilization of twofold dispersion convection. Essentially, Bég et al. 2011 [13] depicted the peristaltic siphoning of nano-liquids through twofold diffusive convection. Kefayati 2014 [14] made sense of twofold dispersion convection for pseudoplastic liquids. The peristaltic movement of the MHD course through twofold diffusive convection was concentrated by Rout 2014 et al. [15] Unstable electrokinetic transport through peristaltic microchannels was concentrated by Tripathi et al. 2016 [16] Tripathi et al. 2017 [17] investigated the peristaltic movement of the couple-stress liquid through the microchannel. In Prakash et al. 2018 [18] they analyzed the peristaltic movement of Williamson ionic nanofluid in the tightened microchannel. Tripathi et al. 2018 [19] likewise concentrated on the blood stream balanced by electroosmosis. Additionally, Tripathi et al. 2018 [20] concentrated on the consolidated impact of electroosmosis and peristalsis through the microchannel. Likewise, Tripathi et al. 2018 [21] uncovered the peristaltic transport of nanofluids with a light impact by means of a microchannel. The effect of intensity and mass on the joined impact of electroosmosis and peristalsis was concentrated by Waheed et al. 2019 [22] . Noreen et al. 2019 [23] examined the impact of intensity on EOF through peristaltic siphoning. In another review, Noreen et al. 2019 [24] suggested the vehicle of MHD nanofluid through the peristaltic microchannel. Entropy age in peristaltically prompted microchannels is a quickly arising area of interest. The investigation of entropy within the framework is important because it aids in tracing the sources of available energy. Various sources of irreversibility include intensity course through the limited temperature slope, convective intensity move characteristics, and consistency and dissemination impacts. Entropy can be limited to save energy quality for the ideal plan of any warm framework. As of now, the examination subject of limiting entropy age has acquired unique status among researchers around the world. Restricted examinations have researched the entropy creation in electro-osmotically prompted peristaltic microchannels. Kefayati 2016 [25] made sense of entropy creation for non-Newtonian nanofluids through a permeable depression. Kefayati 2016 [26] has likewise portrayed entropy creation and twofold diffusive convection for power-regulation liquids. In the previously mentioned referenced works, nobody has had the option to take a gander at them in an oscillatory stream and concoct a consequence of some kind or another. Accordingly, the ongoing examination expects to fill this hole. The discoveries of the current investigation can be utilized for clinical purposes like cell treatment, drug conveyance frameworks, pharmaco-dynamic siphons, and molecule filtration. Likewise, to extend how we might interpret thermosolutal convection, unique consideration was paid to concentrating on entropy age.

Mathematical Formulation

The microchannel is restricted by some growth at the upper wall of the channel caused by cholesterol, which causes a periodic wave at a velocity along the axial direction of the channel. The temperature and the nanoparticles at the lower part of the channel are taken as respectively. According to Mohan and Satheesh 2016 [27] , the mathematical representation of the geometry at the upper wall is expressed is:

Mathematical Models

The models governing the physical problem electro-hydrodynamic (EHD) flow of nanofluid through a restricted microchannel with radiative heat following, Bunonyo and Amos 2021 [28] and Noreen et al. 2019 [23,24] are:

The Poisson-Boltzmann equation according to Tripathi et al. 2017 [17] is

The transformational and the dimensionless parameters are:

Using equation ( 6) in simplifying equations ( 1)-( 5), we have the following:

Applying Debye-Huckel linearization approximation according to Prakash and Tripathi (2018) [18] and equation ( 6), then equation (5) becomes:

Equations ( 8)-( 11) are subject to the following boundary conditions:

Method of Solution

Let us assume that the flow is oscillatory in the channel, following Bunonyo and Amos (2020) [29] , we present the solution to be the form:

Solving equation ( 14), we have

Solving equation ( 19) using the boundary condition in equation ( 18), we have

Solving equation ( 16), we have

Rd Pr     Differentiate equation ( 21) twice and substitute the result into equation (17), which is

The homogenous and particular solutions of equation ( 22) are

So, the solution to equation ( 22) is

Solving equation ( 25) using the boundary conditions in equation ( 18), we have 20), ( 21) and ( 26) into equation ( 15), we have:

The velocity prolife is obtained after substituting equation ( 29) into equation ( 13), we have

The nanoparticles concentration is obtained after substituting equation ( 13) into equation ( 26), we have

The temperature profile is obtained after substituting equation ( 21) into equation ( 13), we have

The electric potential distribution is obtained after substituting equation ( 20) into equation ( 13

The effect of thermophoresis parameter on velocity profile, with 0

The effect of Brownian motion parameter on velocity profile, with 0

Conclusion

The study was carried out to investigate the oscillatory flow of an electro-hydrodynamic (EHD) fluid flow through a microchannel with radiative heat and magnetic field by representing the problem mathematically. The analytical solutions were analyzed and simulation was done using Wolfram Mathematica, focusing on varying the pertinent parameters, and the results were revealed as follows:

1. The thermal Grashof number, electroosmotic and thermophoresis values increase the fluid velocity. 2. The fluid velocity decreases as the Brownian parameter increases.

Reynolds number and wave number increases cause a

decrease in fluid velocity. 4. An increase in nanoparticles, the Grashof number, increases the fluid temperature. 5. Thermophoresis increased and caused an increase in fluid temperature. 6. The Schmidt number increase decreases the fluid temperature. 7. The electroosmotic value increase caused the lipid concentration in the fluid to increase.

Figures and tables from the paper

Figure 1. The Effect of thermal Grashof number on velocity profile, with
The Effect of thermal Grashof number on velocity profile, with↗ Enlarge
Figure 1
The Effect of thermal Grashof number on velocity profile, with

The Effect of thermal Grashof number on velocity profile, with

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Original paper figureSource PDF · page 6 ↗
Figure 2. The effect of thermophoresis parameter on velocity profile, with
The effect of thermophoresis parameter on velocity profile, with↗ Enlarge
Figure 2
The effect of thermophoresis parameter on velocity profile, with

The effect of thermophoresis parameter on velocity profile, with

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Original paper figureSource PDF · page 7 ↗
Figure 3. The effect of Brownian motion parameter on velocity profile, with
The effect of Brownian motion parameter on velocity profile, with↗ Enlarge
Figure 3
The effect of Brownian motion parameter on velocity profile, with

The effect of Brownian motion parameter on velocity profile, with

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Original paper figureSource PDF · page 7 ↗
Figure 4. The effect of Reynolds number on velocity profile, with
The effect of Reynolds number on velocity profile, with↗ Enlarge
Figure 4
The effect of Reynolds number on velocity profile, with

The effect of Reynolds number on velocity profile, with

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Original paper figureSource PDF · page 7 ↗
Figure 5. The effect of wave number on velocity profile, with
The effect of wave number on velocity profile, with↗ Enlarge
Figure 5
The effect of wave number on velocity profile, with

The effect of wave number on velocity profile, with

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Original paper figureSource PDF · page 8 ↗
Figure 6. The effect of electroosmotic parameter on velocity profile, with
The effect of electroosmotic parameter on velocity profile, with↗ Enlarge
Figure 6
The effect of electroosmotic parameter on velocity profile, with

The effect of electroosmotic parameter on velocity profile, with

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Original paper figureSource PDF · page 8 ↗
Figure 7. The effect of nanoparticles Grashof number on nanoparticles fraction profile, with
The effect of nanoparticles Grashof number on nanoparticles fraction profile, with↗ Enlarge
Figure 7
The effect of nanoparticles Grashof number on nanoparticles fraction profile, with

The effect of nanoparticles Grashof number on nanoparticles fraction profile, with

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Original paper figureSource PDF · page 8 ↗
Figure 8. The effect of thermophoresis on nanoparticles fraction profile, with
The effect of thermophoresis on nanoparticles fraction profile, with↗ Enlarge
Figure 8
The effect of thermophoresis on nanoparticles fraction profile, with

The effect of thermophoresis on nanoparticles fraction profile, with

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Original paper figureSource PDF · page 9 ↗
Figure 9. The effect of Schmidt number on nanoparticles fraction profile, with
The effect of Schmidt number on nanoparticles fraction profile, with↗ Enlarge
Figure 9
The effect of Schmidt number on nanoparticles fraction profile, with

The effect of Schmidt number on nanoparticles fraction profile, with

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Original paper figureSource PDF · page 9 ↗
Figure 10. The effect of radiation absorption on temperature profile, with
The effect of radiation absorption on temperature profile, with↗ Enlarge
Figure 10
The effect of radiation absorption on temperature profile, with

The effect of radiation absorption on temperature profile, with

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Original paper figureSource PDF · page 9 ↗
Figure 11. The effect of wave number on temperature profile, with
The effect of wave number on temperature profile, with↗ Enlarge
Figure 11
The effect of wave number on temperature profile, with

The effect of wave number on temperature profile, with

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Original paper figureSource PDF · page 10 ↗
Figure 12. The effect of oscillatory parameter on temperature profile, with
The effect of oscillatory parameter on temperature profile, with↗ Enlarge
Figure 12
The effect of oscillatory parameter on temperature profile, with

The effect of oscillatory parameter on temperature profile, with

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Original paper figureSource PDF · page 10 ↗
Figure 13. The effect of an electroosmotic values on concentration profile, with
The effect of an electroosmotic values on concentration profile, with↗ Enlarge
Figure 13
The effect of an electroosmotic values on concentration profile, with

The effect of an electroosmotic values on concentration profile, with

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Original paper figureSource PDF · page 10 ↗

References

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