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Mathematics Project Topics

Approximate Analytical Solution of Natural Convection Flow With Viscous Dissipation and Variable Viscosity Effects

Approximate Analytical Solution of Natural Convection Flow With Viscous Dissipation and Variable Viscosity Effects

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Approximate Analytical Solution of Natural Convection Flow With Viscous Dissipation and Variable Viscosity Effects

Chapter One

Aimย andย Objectivesย ofย theย study

The aim of this work is to investigate the effects of variable viscosity and viscous dissipation on steady, fully developed natural convection flow of incompressible fluids between infinite vertical parallel plates. This aim will be achieved through the following objectives; which are to:

  • study the effect of varying viscosity on both the velocity and temperature profiles for the fluids in a vertical
  • examine the contribution of suction/injection to both the energy and momentum of the
  • investigate the general effects of viscous dissipation on the fluid flow pattern and

CHAPTERย TWOย 

LITERATUREREVIEW

Introduction

Natural convection flow under suction and injection between vertical infinite parallel platesย has enormous applications in scientific and engineering processes such as in the operationsย of air conditioners, nuclear reactors, the cooling of engines and electrical and electronicย components as well as inย heatย exchangersย toย mention a few.ย A lotย of works existย inย literature that investigated the different physical situations considered in this dissertation.ย Some ofย these worksย are presentedย inย thisย chapterย underย differentย sub-headings.

ย Naturalย convectionย flow

The study of natural convection flow due to steady-periodic heating has received attentionย due to its applicability in different scientific and engineering systems. Natural convection isย still a means of cooling various engineering and control systems as well as electrical andย electronicย componentsย whichย generateย heatย andย areย subjectedย toย heatingย periodically.ย Viscosity is a property of fluid which changes with changing temperatures. Gebhart (1962)ย showed that the heating of fluids by viscous dissipation cannot be neglected for fluids withย high Prandtl number when steady free convective flow is considered because it can greatlyย affectย theย flowย characteristics.ย Again,ย whenย fluidsย areย sheared,ย viscousย dissipationย isย induced by the friction between the different layers of particles of the fluid as they moveย against each other, generating heat in the process. It therefore follows that the rate of shear-ย inducedย heatย generationย withinย aย fluidย isย responsiveย toย variationsย inย viscosity.ย Inspiredย by

the separate works of Sahin (1999) and Tasnim and Mahmud (2009), Jha and Ajibadeย (2011) stated thatย viscosity is the mostย sensitive property of fluid to rising temperatures.ย For instance, 10% rise in the temperature of water results to as much as 140% reduction inย viscosity,ย atย least,ย Schlitchtingย andย Gerstenย (2000).ย Bar-Cohenย andย Roshenowย (1984)ย studied the fully developed fluid flow between two periodically heated parallel plates toย capture miniaturizations of electrical and electronic components. Nanda and Sharma (1963)ย whileย studyingย theย effectsย ofย sinusoidalย variationsย inย surfaceย temperaturesย onย freeย convective laminar flow were able to separate the temperature and velocity into steady andย periodic parts. Wang (1988) investigated the effect of Strouhal number on the developmentย of boundary layers between two periodically heated parallel plates by also separating theย steady and unsteady parts and concluded that Strouhal number exerts an inverse effect onย unsteady flow, but the effect tends to zero as Strouhal number tends to infinity. Barletta andย Rossi di Schio (2004) studied a mixed convection flow in a circular duct whose wall isย subjected to periodic sinusoidal heating and were able to show that there exists a resonanceย frequency where velocity oscillations reach a maximum. Several other authors who haveย taken in hand to investigate natural convection flow under different physical phenomenaย include Muhuri and Gupta (1979), Zacchini (1998), Watanabe and Pop (1994), Barlettaย (1998), Jha and Ajibade (2009), Soundalgekar et al (2004) among others.Jha and Ajibadeย (2011)ย investigatedย theย effectsย of viscousย dissipation onย natural convectionย flowย inย aย vertical channel formedย by twoย infinite parallel plates and concludedย thatย the viscousย dissipation heatingย becomes stronger than those of the plates when the thermal diffusivityย of the fluid is relatively small causing transfer of heat from fluid to plates instead, but theirย results are limited to very narrow range of values of E. Again the viscous dissipationย parameter,ย E, is limited in its role in the work of Jha and Ajibade (2011) as it was used as a perturbationย parameterย only,ย beingย anย off-shootย ofย theย bottleย necksย ofย theย generalย perturbationย method.

ย Suctionย andย Injection

Theย significanceย ofย suctionย andย injectionย isย wellย recognizedย inย spaceย scienceย andย aerodynamics in the area of boundary layer control. In the area of mass transfer cooling,ย suction/injection can significantly alter the flow field and by extension affect theย rate ofย heatย transferย onย theย porousย boundaries.ย Theย flowย withย heatย transferย ofย viscousย incompressible fluid between parallel plates has important applications inย many systemsย and devices such as electrostatic precipitation, aerodynamics heating, polymer technologyย and the petroleum industry. Shojaefard et al (2005) investigated flow control on a subsonicย airfoil by suction and injection and concluded that suction significantly increases the liftย coefficientย whileย injectionย decreasesย theย surfaceย skinย frictionย resultingย inย significantย reductionย inย energyย consumptionย ofย suchย aircrafts.ย Thisย byย extensionย willย amountย toย reduced level of air pollutant emission as well as cost for such air crafts. Attia (2005) alsoย investigated the effect of suction and injection on unsteady flow between parallel plates. Byย andย large,ย physicalย phenomenaย inย Medicine,ย Engineeringย andย severalย otherย fieldsย ofย research naturally involves fluids that are Newtonian in nature. Jha and Ajibade (2009)ย studied the influence of suction/injection on natural convection flow of viscous fluid whenย the convection current is induced by the heating of the porous boundaries, but considersย fluid viscosity to be a constant. Recently, Rundora and Makinde (2013) studied the effectsย of suction and injection on unsteady reactive variable viscosity fluid flow with porousย mediumย butย considersย theย fluidย toย be non-Newtonianย inย nature.

 

CHAPTERย THREEย 

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MATHEMATICALย ANALYSES

Introduction

This chapter is preoccupied with the mathematical formulation, derivation and solution ofย both the energy and momentum equations of the two problems under investigation in thisย dissertation.ย Theย dimensionalย energyย andย momentumย equationsย areย firstย putย inย dimensionless forms by the introduction of appropriate non-dimensional quantities. Theย Homotopy Perturbation method is then applied to linearize and uncouple the non-linear andย coupled differential equations before solving by the undetermined coefficient method toย obtain closeย form expressionsย forย both theย velocity and temperatureย fieldsย in the twoย problemsย (seeย Kryszigย E.,ย 1990).ย Theย skinย frictionย andย Nusseltย numberย areย alsoย calculatedย asย wellย as theย phases andย amplitudesย ofย theย unsteadyย velocityย andย temperature.

ย Mathematicalย formulationย andย Geometricalย Description

In this subsection, we formulate a mathematical modelof natural convection flowbetweenย infiniteย verticalย parallelย platesย with viscousย dissipationย andย variableย viscosityย effects.

Considering the flow of viscous dissipating incompressible fluid with temperature dependent viscosity between two vertical and parallel plates of infinite length, the channel formed by the boundary plates are at fixed distances ยฑ on the horizontal axis from the center line,ย  = 0. The direction of flow is taken as the vertically while the direction of heat penetration from the ambient (plates) is taken asย  perpendicular to the direction of flow. The initial temperature of the fluid within the channel is taken as 0.

CHAPTERย FOURย 

SOLUTIONย OFย THEย PROBLEMS

ย Introduction

This chapter provides details of how the solutions of the non-dimensional momentum andย energy equations describing the two problems in this theses were solved as well as theย obtained solutions. It also presents the determination of other quantities of interest such asย the phases and amplitudes of temperature and velocity fields, skin friction at both boundingย platesย as wellas the Nusseltย number.

CHAPTER FIVE

RESULTSย ANDย DISCUSSION

ย Introduction

This chapter presents the discussion of the results obtained from the previous chapter in theย formย ofย valuesย andย lineย graphsย thatย clearlyย revealย theย influencesย ofย theย governingย parameters on theย flowย behaviours. A computer program was written and usedย in theย simulation of the periodic temperature and velocity, Skin friction and Nusselt number forย each of the studied problems. The Phase and amplitude of fluid temperature and velocityย were alsoย simulatedย forย bothย cases.

CHAPTERย SIX

ย SUMMARY,ย CONCLUSIONย ANDย RECOMMENDATION

ย ย Summary

In this dissertation, a study of natural convection flow between infinite vertical parallelย platesย withย viscousย dissipationย andย variableย viscosityย effectsย haveย beenย studied.ย Theย problem is further extended to investigate natural convection heat transfer flow in a verticalย channel when the boundary permits movement of fluid in and out (suction/injection). Theย momentum and energy equations of these problems were first separated into steady andย periodic parts before putting in dimensionless form. The strongly non-linear and coupledย odeโ€Ÿs obtained were first subjected to the Homotopy Perturbation technique to break theย non-linearity and coupling, resulting inย linear odeโ€Ÿs which were then solved by means ofย theย undeterminedย coefficientย methodย toย obtainย expressionsย forย bothย temperatureย andย velocityย fieldsย inย theย twoย problems.ย Simulationย ofย theย resultsย wasย carriedย outย usingย MATLAB (R2012b) program and generated numerical values and line graphs were used inย the discussion,ย inferenceย andย drawingย ofย conclusions.

ย Conclusion

In this dissertation, we have been able to overcome the limitations of coupling and non-ย linearityย posedย byย theย governingย differentialย equationsย toย obtain,ย byย theย Homotopyย Perturbation method, model solutions for both the energy and momentum of fluidsin aย verticalย channelย underย theย effectsย ofย viscousย dissipation,ย variableย viscosityย andย suction/injection.

Based on the analysis of the obtained results, the following conclusions are drawn from thisย dissertation:

Firstly, for fluids with > 1, the effect of variable viscosity is dominant over that of viscous dissipation.

Secondly,ย viscous dissipation heating becomes stronger and exerts greater influence onย bothย theย energyย andย momentumย ofย theย workingย fluidย whenย viscosityย hasย beenย increased.

Thirdly, fluid temperature decreases with growing viscous dissipation if the viscosity of theย fluidย decreases withย increasingย temperature.

Fourthly, when viscosity is raised, the rate of heat transfer on the plates decreases with increasing viscous dissipation for all values of .

In addition, suction on a plate increases the velocity and decreases the temperature near itย whileย theย otherย plateย witnessesย decreaseย inย velocity andย increasedย temperatureย underย injection.

Finally, the skin friction on the plates increases with increased suction while it decreasesย withย increasingย injection.

Recommendation

Itย isย herebyย recommendedย thatย theย contributionย ofย variationsย inย conductivityย ofย theย fluidcanย be studiedย onย eachย ofย theย twoย problems asย aย furtherย investigation.

Mixedย convectionย orย pressureย drivenย flowย situationย canย beย studiedย inย either ofย theย casesย toย investigate the effectย ofย pressureย gradientย onย the flowย pattern.

REFERENCES

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  • Ayati Z. andBiazar J.(2015). On the convergence of homotopy perturbation method.ย Journal ofย Theย Egyptian Mathematicalย Society.ย 23:ย 424-428
  • Bar-Cohen A. and Roshenow W.M. (1984). Thermally optimum spacing of vertical, naturalย convectionย cooled parallelย plates.ย Journal ofย Heatย Transferย (ASME)ย 106:116-123.
  • Barletta A. (1998). Laminar mixed convection with viscous dissipation in a vertical channelย Internationalย Journalย ofย Heatย Massย Transferย 41:3501-3513.
  • Barletta A. and Rossi di Schio E. (2004). Mixed convection flow in a vertical circular ductย withย timeย periodicย boundaryย condition:ย steady-periodicย regime.ย Internationalย Journalย ofย Heatย Mass Transfer47:129-40.
  • Biazarย J.andย Ghazviniย H.ย (2009). Heโ€Ÿsย homotopyย perturbationย methodย forย solvingย systemย ofย Volterra integral equations of the second kind. Chaos Solitons Fractals. 39(2):770- 777
  • Biazar J. and Ghazvini H. (2007). Exact solutions for non-linear Schrodinger equations byย Heโ€Ÿsย homotopyย perturbationย method.ย Physicsย Lettersย Aย 336:79-84
  • Chengย P.ย andย Minkowyczย W.ย J.ย (1977).ย Freeย convectionย aboutย aย verticalย flatย plateย embeddedย in aย porousย mediumย withย applicationsย to heatย transferย fromย aย dike.ย Journalย of Geophysical Researchย 82;ย 2040-2044.
  • Domairry G.and Aziz A. (2009). Approximate analysis of MHD squeeze flow between twoย parallel disksย withย suction/injectionย byย homotopyย perturbationย method.ย Mathematicalย Problems inย EngineeringArticle doiย 603916.

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