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Mathieu equation and its application

 

Table Of Contents


Chapter ONE

1.1 Introduction
1.2 Background of Study
1.3 Problem Statement
1.4 Objective of Study
1.5 Limitation of Study
1.6 Scope of Study
1.7 Significance of Study
1.8 Structure of the Research
1.9 Definition of Terms

Chapter TWO

2.1 Overview of Literature Review
2.2 Theoretical Framework
2.3 Historical Perspectives
2.4 Empirical Studies
2.5 Conceptual Framework
2.6 Current Trends
2.7 Critical Analysis
2.8 Research Gaps
2.9 Methodological Approaches
2.10 Comparative Review

Chapter THREE

3.1 Research Methodology Overview
3.2 Research Design
3.3 Data Collection Methods
3.4 Sampling Techniques
3.5 Data Analysis Procedures
3.6 Research Instruments
3.7 Ethical Considerations
3.8 Validity and Reliability

Chapter FOUR

4.1 Introduction to Findings Analysis
4.2 Demographic Analysis
4.3 Quantitative Results Interpretation
4.4 Qualitative Results Interpretation
4.5 Statistical Analysis
4.6 Data Visualization
4.7 Comparative Analysis
4.8 Discussion of Findings

Chapter FIVE

5.1 Conclusion and Summary
5.2 Summary of Findings
5.3 Implications of the Study
5.4 Recommendations for Future Research
5.5 Conclusion Statement

Project Abstract

1.1BriefReviewonMathieuequation

Mathieu equation isa specialcase of a linear second order homogeneousdifferentialequation(Ruby1995).Theequationwasfirstdiscussedin1868,byEmileLeonardMathieuinconnectionwithproblemofvibrationsinellipticalmembrane.HedevelopedtheleadingtermsoftheseriessolutionknownasMathieufunctionoftheellipticalmembranes.Adecadelater,HeinedefinedtheperiodicMathieuAngularFunctionsofintegerorderasFouriercosineandsineseries;furthermore,withoutevaluatingthecorrespondingcoefficient,Heobtainedatranscendentalequationforcharacteristicnumbersexpressedintermsofinfinitecontinuedfractions;andalsoshowedthatonesetofperiodicfunctionsofintegerordercouldbeinaseriesofBesselfunction(Chaos-CadorandLey-Koo2002).Intheearly1880’s,FloquetwentfurthertopublishatheoryandthusasolutiontotheMathieudifferentialequation;hisworkwasnamedafterhimas,‘Floquet’sTheorem’or‘Floquet’sSolution’.StephensonusedanapproximateMathieuequation,andproved,thatitispossibletostabilizetheupperpositionofarigidpendulumbyvibratingitspivotpointverticallyataspecifichighfrequency.(StépánandInsperger2003).Thereexistsanextensiveliteratureontheseequations;andinparticular,awell-highexhaustivecompendiumwasgivenbyMc-Lachlan(1947).TheMathieufunctionwasfurtherinvestigatedbynumberofresearcherswhofoundaconsiderableamountofmathematicalresultsthatwerecollectedmorethan60yearsagobyMc-Lachlan(Gutiérrez-Vegaaetal2002).Whittakerandotherscientistderivedin1900sderivedthehigher-ordertermsoftheMathieudifferentialequation.AvarietyoftheequationexistintextbookwrittenbyAbramowitzandStegun(1964).Mathieudifferentialequationoccursintwomaincategoriesofphysicalproblems.First,applicationsinvolvingellipticalgeometriessuchas,analysisofvibratingmodes2inellipticmembrane,thepropagatingmodesofellipticpipesandtheoscillationsofwaterinalakeofellipticshape.Mathieuequationarisesafterseparatingthewaveequation using ellipticcoordinates.Secondly,problemsinvolving periodicmotionexamplesare,thetrajectoryofan electron in aperiodicarrayofatoms,themechanicsofthequantumpendulumandtheoscillationoffloatingvessels.ThecanonicalformfortheMathieudifferentialequationisgivenby+ y =0, (1.1)dy 2dx2 [a-2qcos(2x)](x)whereaandqarerealconstantsknownasthecharacteristicvalueandparameterrespectively.Closely related to the Mathieu differentialequation is the Modified Mathieudifferentialequationgivenby- y =0, (1.2)dy 2du2 [a-2qcosh(2u)](u)whereu=ixissubstitutedintoequation(1.1).Thesubstitutionoft=cos(x)inthecanonicalMathieudifferentialequation(1.1)abovetransformstheequationintoitsalgebraicformasgivenbelow(1-t) -t + y =0. (1.3) 2 dy 2dt2dydt[a+2q(1-2t2)](t)Thishastwosingularitiesatt=1,-1andoneirregularsingularityatinfinity,whichimpliesthatingeneral(un-likemanyotherspecialfunctions),thesolutionofMathieudifferentialequationcannotbeexpressedintermsofhypergeometricfunctions(Mritunjay2011).ThepurposeofthestudyistofacilitatetheunderstandingofsomeofthepropertiesofMathieufunctionsandtheirapplications.Webelievethatthisstudywillbehelpfulinachievingabettercomprehensionoftheirbasiccharacteristics.ThisstudyisalsointendedtoenlightenstudentsandresearcherswhoareunfamiliarwithMathieufunctions.Inthechaptertwoofthiswork,wediscussedtheMathieu3differentialequationandhowitarisesfromtheellipticalcoordinatesystem.Also,wetalkedabouttheModifiedMathieudifferentialequationandtheMathieudifferentialequationinanalgebraicform.ThechapterthreewasbasedonthesolutionstotheMathieuequationknownasMathieufunctionsandalsotheFloquet’stheory.Inthechapterfour,weshowedhowMathieufunctionscanbeappliedtodescribetheinvertedpendulum,ellipticdrumhead,Radiofrequencyquadrupole,Frequencymodulation,Stabilityofafloatingbody,AlternatingGradientFocusing,thePaultrapforchargedparticlesandtheQuantumPendulum.



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