A MATHEMATICAL MODEL OF FOUR SPECIES SYN-ECOSYMBIOSIS COMPRISING OF PREY-PREDATION, MUTUALISM AND COMMENSALISMS-I (FULLY WASHED OUT STATE)

Size: px
Start display at page:

Download "A MATHEMATICAL MODEL OF FOUR SPECIES SYN-ECOSYMBIOSIS COMPRISING OF PREY-PREDATION, MUTUALISM AND COMMENSALISMS-I (FULLY WASHED OUT STATE)"

Transcription

1 VOL. 6, NO. 4, APRIL 0 ISSN ARPN Jornl of Engineering nd Applied Sciences Asin Reserch Pblishing Nework (ARPN). All righs reserved. A MATHEMATICAL MODEL OF FOUR SPECIES SYN-ECOSYMBIOSIS COMPRISING OF PREY-PREDATION, MUTUALISM AND COMMENSALISMS-I (FULLY WASHED OUT STATE) R. Srilh nd N. Ch. Pbhirmchryl Reserch Scholr, JNTUH, Kkplly, Hyderbd, Indi Professor (Red.) of Mhemics, NIT, Wrngl, Indi E-Mil: bsrilh8@gmil.com ABSTRACT This invesigion dels wih mhemicl model of for species (S, S, S nd S 4 ) Syn-Ecologicl sysem (Flly Wshed o Se). S is predor srviving on he prey S : he prey is commensl o he hos S which iself is in mlism wih he forh species S 4. S nd S 4 re nerl. The mhemicl model eqions chrcerizing he synecosysem consie se of for firs order non-liner copled differenil eqions. There re in ll sixeen eqilibrim poins. Crieri for he sympoic sbiliy of one of he sixeen eqilibrim poins: he flly wshed o se is esblished. The linerised eqions for he perrbions over he eqilibrim poin re nlyzed o esblish he crieri for sbiliy. The sysem is noiced o be loclly sble. Trjecories of he perrbions hve been illsred. Keywords: mhemicl model, species, syn-ecologicl sysem, mlism, commenslism, differenil eqions. INTRODUCTION Mhemicl modeling is n imporn inerdisciplinry civiy which involves he sdy of some specs of diverse disciplines. Biology, Epidemiodology, Physiology, Ecology, Immnology, Bio-economics, Geneics, Phrmocokineics re some of hose disciplines. This mhemicl modeling hs rised o he zenih in recen yers nd spred o ll brnches of life nd drew he enion of every one. Mhemicl modeling of ecosysems ws iniied by Lok [8] nd by Volerr [4]. The generl concep of modeling hs been presened in he reises of Meyer [9], Cshing [], Pl Colinvx [0], Freedmn [], Kpr [5, 6]. The ecologicl inercions cn be brodly clssified s prey-predion, compeiion, mlism nd so on. N.C. Srinivs [] sdied he compeiive eco-sysems of wo species nd hree species wih regrd o limied nd nlimied resorces. Ler, Lkshmi Nryn [7] hs invesiged he wo species prey-predor models. Recenly sbiliy nlysis of compeiive species ws invesiged by Archn Reddy []. Locl sbiliy nlysis for wospecies ecologicl mlism model hs been invesiged by B. Rvindr Reddy e l., [, ]. The presen invesigion is devoed o n nlyicl sdy of for species Syn-Ecologicl sysem. S is predor srviving on he prey S : he prey is commensl o he hos S which iself is in mlism wih he forh species S 4 ; S nd S 4 re nerl. Figre- shows he Schemic Skech of he sysem nder invesigion. The model eqions of he sysem consie se of for firs order non-liner ordinry differenil copled eqions. In ll he sixeen eqilibrim poins of he sysem re idenified nd he sbiliy nlysis is crried o only for he flly wshed o se. The linerized perrbed eqions over he eqilibrim ses re solved nd he rjecories illsred. Figre-. Schemic skech of he Syn Eco- sysem. BASIC EQUATIONS Noion doped N (): The Poplion of he Prey (S ) N (): The Poplion of he Predor (S ) N (): The Poplion of he Hos (S ) of he Prey (S ) nd ml o S 4 N 4 (): The Poplion of S 4 ml o S : Time insn,,, 4 : Nrl growh res of S, S, S, S 4,,, 44 : Self inhibiion coefficiens of S, S, S, S 4, : Inercion (Prey-Predor) coefficiens of S de o S nd S de o S : Coefficien for commensl for S de o he Hos S 4, 4 : Mlly inercion beween S nd S 4,,, 44 : Crrying cpciies of S, S, S, S 4 Frher he vribles N, N, N, N 4 re nonnegive nd he model prmeers,,, 4 ;,,, 44 ;,,, 4 re ssmed o be non-negive consns. 4

2 VOL. 6, NO. 4, APRIL 0 ISSN ARPN Jornl of Engineering nd Applied Sciences Asin Reserch Pblishing Nework (ARPN). All righs reserved. The model eqions for he growh res of S, S, S, S 4 re d d d N N NN + NN. () N N + NN. () N N + NN. () 4 4 d 4 N N + NN. (4) EQUILIBRIUM STATES The sysem nder invesigion hs sixeen eqilibrim ses defined by i 0, i,,, 4 d re given in he following ble. (5) S. No. Eqilibrim Ses Eqilibrim poin Flly Wshed o se N 0, N 0, N 0, N4 0 Only S 4 srvives 4 N 0, N 0, N 0, N4 44 Only he hos (S )of S srvives N 0, N 0, N, N 0 4 Only he predor S srvives 5 Only he prey S srvives 6 7 Prey (S ) nd predor (S ) wshed o Prey (S ) nd hos (S ) of S wshed o 8 Prey (S ) nd S 4 wshed o 9 Predor (S ) nd Hos (S ) of S wshed o 0 Predor (S ) nd S 4 wshed o Prey (S ) nd predor (S )srvives Only he prey (S ) wshed o Only he predor (S ) wshed o N 0, N, N 0, N 0 N, N 0, N 0, N N 0, N 0, N, N N 0, N, N 0, N 4 44 N 0, N, N, N 0 N, N 0, N 0, N N, N 0, N, N 0 + N, N, N 0, N N 0, N, N, N α + + N, N 0, N, N α where α ( ) + ( 44 44) α ( )

3 VOL. 6, NO. 4, APRIL 0 ISSN ARPN Jornl of Engineering nd Applied Sciences Asin Reserch Pblishing Nework (ARPN). All righs reserved. 4 Only he Hos (S ) of S wshed o + N, N, N 0, N Only S 4 wshed o 6 The co-exisen se (or) Norml sedy se β β N, N, N, N 0 β β where β ( + ) β ( + ) β ( + ) + N N γ + γ γ + γ, N, 4 γ γ + +, N where γ ( + )( ) γ γ ( + )( ) γ ( )( ) The presen pper dels wih he flly wshed o se only. The sbiliy of he oher eqilibrim ses will be presened in he forh coming commnicions. STABILITY OF THE FULLY WASHED OUT EQUILIBRIUM STATE (Sl. No. in he bove Tble) To discss he sbiliy of eqilibrim poin N 0, N 0, N 0, N4 0 Le s consider smll deviions (), (), (), 4 () from he sedy se i.e., N ( ) N + ( ), i,,,4.. (6) i i i Where i () is smll perrbions in he species S i. Sbsiing (6) in (), (), (), (4) nd neglecing prodcs nd higher powers of,,, 4, we ge d d d d d d (7).. (8) (9) d d 4.. (0) 4 4 The chrcerisic eqion of which is ( λ )( λ )( λ )( λ ) 0.. () he roos,,, 4 of which re ll posiive. Hence he Flly Wshed o Se is nsble. The solions of he eqions (7), (8), (9), (0) re 0e () 0e () 0e. (4) 4 4 e. (5) Where 0, 0, 0, re he iniil vles of,,, 4 respecively. There wold rise in ll 576 cses depending pon he ordering of he mgnides of he growh res,,, 4 nd he iniil vles of he perrbions 0 (), 0 (), 0 (), () of he species S, S, S, S 4. Of hese 576 siions some ypicl vriions re illsred hrogh respecive solion crves h wold fcilie o mke some resonble observions. 44

4 VOL. 6, NO. 4, APRIL 0 ISSN ARPN Jornl of Engineering nd Applied Sciences Asin Reserch Pblishing Nework (ARPN). All righs reserved. Cse (i): If 0 < 0 < 0 <, < < < 4 In his cse prey (S ) hs he les nrl birh re nd S 4 domines he prey (S ), predor (S ) nd he hos (S ) of S in nrl growh re s well s in is poplion srengh. Cse (iv): If 0<<0<0, <<<4 In his cse he hos (S ) of S hs he les nrl birh re. Iniilly he hos (S ) of S domines over S 4 nd he predor (S ) ill he imes insn * 4, * respecively. Therefer he dominnce is reversed. ; * * Also he prey (S ) domines over S 4, Predor (S ) ill he ime insn * 4, * respecively nd herefer he dominnce is reversed. ; * * Figre- Cse (ii): If 0 < 0 < 0 <, < < < 4 In his cse predor (S ) hs he les nrl birh re. Iniilly he predor (S ) domines over he prey (S ) ill he ime insn * 0 0 nd here-fer he prey (S ) domined he predor (S ). The * ime my be clled he dominnce ime of he predor (S ) over he prey (S ). Figre-4 Cse (v): If 0 < 0 < 0 <, < < 4 < In his cse he Hos (S ) of S hs he les nrl birh re. Iniilly i is domines over he predor (S ) ill he ime insn * 0 0 nd herefer he dominnce is reversed. Also S 4 domines over he prey (S ) ill he ime insn * 4 nd herefer he dominnce is 4 0 Figre- Cse (iii): If 0 < 0 < < 0, < < < 4 In his cse predor (S ) hs he les nrl birh re. Iniilly he predor (S ) domines over S 4, hos (S ) of S nd prey (S ) ill he ime insn,, respecively nd here fer he dominnce is * * * 4 reversed * * 0 * 0 4,, Figre-5 45

5 VOL. 6, NO. 4, APRIL 0 ISSN ARPN Jornl of Engineering nd Applied Sciences Asin Reserch Pblishing Nework (ARPN). All righs reserved. Cse (vi): If 0 < 0 < < 0, < 4 < < In his cse he prey (S ) hs he les nrl birh re. Iniilly he prey (S ) domines over is hos, S 4 nd Predor (S ) ill he ime insn *, * 4, * respecively nd herefer he dominnce is reversed. Also S 4 domines over he hos (S ) of S, nd he predor (S ) ill he ime insn * 4, * 4 nd herefer he dominnce is reversed. Similrly, he hos (S ) of S domines over he predor (S ) ill he ime insn * nd he dominnce ges reversed herefer. ; ; * 0 * * Cse (viii): If 0 < 0 < 0 <, < < 4 < In his cse he predor (S ) hs he les nrl birh re. Iniilly he predor (S ) domines over he prey (S ), hos (S ) of S ill he ime insn *, * respecively nd herefer he dominnce is reversed. Also he prey (S ) domines over is hos ill he ime insn * nd herefer he dominnce is reversed. Similrly S 4 domines over he hos (S ) of S ill he ime insn * 4 he dominnce ges reversed fer. ; ; * * * Figre-8 Figre-6 Cse (vii): If 0 < 0 < 0 <, < 4 < < In his cse he hos (S ) of S hs he les nrl birh re. Iniilly S 4 domines over boh he prey (S ) nd predor (S ) ill he ime insn * 4, * 4 respecively nd herefer he dominnce is reversed. Also he Prey (S ) domines over he Predor (S ) po he ime insn * nd he dominnce ges reversed fer. nd ; * * * 0 0 ; * 0 * ; * 0 * Cse (ix): If 0 < 0 < < 0, < 4 < < In his cse he prey (S ) hs he les nrl birh re. Iniilly he prey (S ) domines over is hos, predor (S ) nd S 4 ill he ime insn *, *, * 4 respecively nd here fer he dominnce is reversed. Also S 4 domines over he predor (S ) nd he hos (S ) of S ill he imes insn * 4 nd * 4 nd herefer he dominnce is reversed. ; ; * 0 * 0 * nd ; * * Figre-7 46

6 VOL. 6, NO. 4, APRIL 0 ISSN ARPN Jornl of Engineering nd Applied Sciences Asin Reserch Pblishing Nework (ARPN). All righs reserved. ; * * ; * 0 * nd * Figre-9 Cse (x): If < 0 < 0 < 0, < < 4 < In his cse he prey (S ) hs he les nrl birh re. Iniilly he prey (S ) domines over S 4 ill he ime insn * 4 nd herefer he dominnce is reversed. Also he predor (S ) domines over S nd S 4 ill he ime insns *, * 4 respecively nd herefer he dominnce is reversed. * * 4 ; 4 nd * 0 0 Figre- Cse (xii): If < 0 < 0 < 0, 4 < < < In his cse S 4 hs he les nrl birh re. Iniilly he prey (S ) domines over is hos nd predor (S ) ill he ime insn *, * respecively nd herefer he dominnce is reversed. * 0 * 0 ; 0 0 Figre-0 Cse (xi): If < 0 < 0 < 0, < < < 4 In his cse he predor (S ) hs he les nrl birh re. Iniilly he predor (S ) domines over S 4 nd prey (S ) ill he ime insn * 4, * respecively nd herefer he dominnce is reversed. Also he hos (S ) of S domines over he prey (S ) nd S 4 ill he ime insn *, * 4 respecively nd herefer he dominnce is reversed. Similrly he prey (S ) domines over S 4 ill he ime insn * 4 nd he dominnce ges reversed fer. Figre- TRAJECTORIES OF PERTURBATIONS The rjecories in he - plne given by ( ) ( ) nd re shown in Figre

7 VOL. 6, NO. 4, APRIL 0 ISSN ARPN Jornl of Engineering nd Applied Sciences Asin Reserch Pblishing Nework (ARPN). All righs reserved. [4] George F Simmons: Differenil Eqions wih pplicions nd hisoricl noes. T McGrw- Hill, New Delhi. [5] Kpr J. N Mhemicl Modeling. Wiley - Esern. [6] Kpr J.N Mhemicl Models in Biology nd Medicine Affilied Es - Wes. Figre- Also he rjecories in he plne given by ( ) ( ) nd re shown in Figre Similrly he rjecories in he - 4, -, - 4, plnes re ( ) ( ),( ) ( ), ( ) ( ),( ) ( ) respecively. 0 0 [7] Lkshmi Nryn K A Mhemicl sdy of Prey-Predor Ecologicl Models wih pril covers for he prey nd lernive food for he predor. PhD Thesis. J. N. T. Universiy. [8] Lok A. j. 95. Elemens of Physicl biology. Willims nd Wilkins, Blimore. [9] Meyer W.J Conceps of Mhemicl Modeling. McGrw - Hill. [0] Pl Colinvx Ecology. John Wiley nd Sons Inc., New York. [] Rvindr Reddy B., Lkshmi Nryn, K. nd Pbhirmchryl N.Ch A model of wo mlly inercing species wih limied resorces for boh he species. Inernionl J. of Engg. Reserch nd Ind. Appls. (II): 8-9. REFERENCES Figre-4 [] Rvindr Reddy B., Lkshmi Nryn K. nd Pbhirmchryl N.Ch. 00. A model of wo mlly inercing species wih limied resorces nd hrvesing of boh he species consn re. Inernionl J. of Mh. Sci nd Engg. Appls. (IJMSEA). 4(III): [] Srinivs N.C. 99. Some Mhemicl specs of modeling in Bio Medicl Sciences. PhD Thesis. Kkiy Universiy. [4] Volerr V. 9. Leconssen l heorie mhemiqe de l leie po lvie. Ghier - Villrs, Pris. [] Archn Reddy R On he sbiliy of some mhemicl models in biosciences- inercing species. PhD Thesis. JNTU. [] Cshing J. M Inegro - differenil eqions nd Dely Models in Poplion Dynmics. Lecre Noes in Biomhemics. Springer- Verlg, Heidelberg. Vol. 0. [] Freedmn H. I Deerminisic Mhemicl Models in Poplion Ecology. Mrcel - Decker, New York. 48

Available online at Pelagia Research Library. Advances in Applied Science Research, 2011, 2 (3):

Available online at   Pelagia Research Library. Advances in Applied Science Research, 2011, 2 (3): Avilble online www.pelgireserchlibrry.com Pelgi Reserch Librry Advnces in Applied Science Reserch 0 (): 5-65 ISSN: 0976-860 CODEN (USA): AASRFC A Mhemicl Model of For Species Syn-Ecosymbiosis Comprising

More information

A Model of two mutually interacting Species with Mortality Rate for the Second Species

A Model of two mutually interacting Species with Mortality Rate for the Second Species Avilble online t www.pelgireserchlibrry.com Advnces in Applied Science Reserch, 0, 3 ():757-764 ISS: 0976-860 CODE (USA): AASRFC A Model of two mutully intercting Species with Mortlity Rte for the Second

More information

The Dynamics of Two Harvesting Species with variable Effort Rate with the Optimum Harvest Policy

The Dynamics of Two Harvesting Species with variable Effort Rate with the Optimum Harvest Policy Inernionl OPEN ACCESS Journl Of Modern Engineering Reserch (IJMER) The Dynmics of Two Hrvesing Species wih vrible Effor Re wih he Opimum Hrves Policy Brhmpl Singh; nd Professor Suni Gkkhr; Deprmen of Mhemics,

More information

ON THE STABILITY OF DELAY POPULATION DYNAMICS RELATED WITH ALLEE EFFECTS. O. A. Gumus and H. Kose

ON THE STABILITY OF DELAY POPULATION DYNAMICS RELATED WITH ALLEE EFFECTS. O. A. Gumus and H. Kose Mhemicl nd Compuionl Applicions Vol. 7 o. pp. 56-67 O THE STABILITY O DELAY POPULATIO DYAMICS RELATED WITH ALLEE EECTS O. A. Gumus nd H. Kose Deprmen o Mhemics Selcu Universiy 47 Kony Turey ozlem@selcu.edu.r

More information

Solutions for Nonlinear Partial Differential Equations By Tan-Cot Method

Solutions for Nonlinear Partial Differential Equations By Tan-Cot Method IOSR Journl of Mhemics (IOSR-JM) e-issn: 78-578. Volume 5, Issue 3 (Jn. - Feb. 13), PP 6-11 Soluions for Nonliner Pril Differenil Equions By Tn-Co Mehod Mhmood Jwd Abdul Rsool Abu Al-Sheer Al -Rfidin Universiy

More information

3. Renewal Limit Theorems

3. Renewal Limit Theorems Virul Lborories > 14. Renewl Processes > 1 2 3 3. Renewl Limi Theorems In he inroducion o renewl processes, we noed h he rrivl ime process nd he couning process re inverses, in sens The rrivl ime process

More information

Contraction Mapping Principle Approach to Differential Equations

Contraction Mapping Principle Approach to Differential Equations epl Journl of Science echnology 0 (009) 49-53 Conrcion pping Principle pproch o Differenil Equions Bishnu P. Dhungn Deprmen of hemics, hendr Rn Cmpus ribhuvn Universiy, Khmu epl bsrc Using n eension of

More information

Motion. Part 2: Constant Acceleration. Acceleration. October Lab Physics. Ms. Levine 1. Acceleration. Acceleration. Units for Acceleration.

Motion. Part 2: Constant Acceleration. Acceleration. October Lab Physics. Ms. Levine 1. Acceleration. Acceleration. Units for Acceleration. Moion Accelerion Pr : Consn Accelerion Accelerion Accelerion Accelerion is he re of chnge of velociy. = v - vo = Δv Δ ccelerion = = v - vo chnge of velociy elpsed ime Accelerion is vecor, lhough in one-dimensionl

More information

Think of the Relationship Between Time and Space Again

Think of the Relationship Between Time and Space Again Repor nd Opinion, 1(3),009 hp://wwwsciencepubne sciencepub@gmilcom Think of he Relionship Beween Time nd Spce Agin Yng F-cheng Compny of Ruid Cenre in Xinjing 15 Hongxing Sree, Klmyi, Xingjing 834000,

More information

5.1-The Initial-Value Problems For Ordinary Differential Equations

5.1-The Initial-Value Problems For Ordinary Differential Equations 5.-The Iniil-Vlue Problems For Ordinry Differenil Equions Consider solving iniil-vlue problems for ordinry differenil equions: (*) y f, y, b, y. If we know he generl soluion y of he ordinry differenil

More information

Necessary and Sufficient Conditions for Asynchronous Exponential Growth in Age Structured Cell Populations with Quiescence

Necessary and Sufficient Conditions for Asynchronous Exponential Growth in Age Structured Cell Populations with Quiescence JOURNAL OF MATEMATICAL ANALYSIS AND APPLICATIONS 25, 49953 997 ARTICLE NO. AY975654 Necessry nd Sufficien Condiions for Asynchronous Exponenil Growh in Age Srucured Cell Populions wih Quiescence O. Arino

More information

f t f a f x dx By Lin McMullin f x dx= f b f a. 2

f t f a f x dx By Lin McMullin f x dx= f b f a. 2 Accumulion: Thoughs On () By Lin McMullin f f f d = + The gols of he AP* Clculus progrm include he semen, Sudens should undersnd he definie inegrl s he ne ccumulion of chnge. 1 The Topicl Ouline includes

More information

Solutions to Problems from Chapter 2

Solutions to Problems from Chapter 2 Soluions o Problems rom Chper Problem. The signls u() :5sgn(), u () :5sgn(), nd u h () :5sgn() re ploed respecively in Figures.,b,c. Noe h u h () :5sgn() :5; 8 including, bu u () :5sgn() is undeined..5

More information

A RECURSIVE PROCEDURE FOR COMMENSAL- HOST ECOLOGICAL MODEL WITH REPLENISHMENT RATE FOR BOTH THE SPECIES - A NUMERICAL APPROACH

A RECURSIVE PROCEDURE FOR COMMENSAL- HOST ECOLOGICAL MODEL WITH REPLENISHMENT RATE FOR BOTH THE SPECIES - A NUMERICAL APPROACH VOL. 5, NO., OCTOBER ISSN 89-668 6- Asian Research Publishing Network (ARPN). All rights reserved. A RECURSIVE PROCEDURE FOR COMMENSAL- HOST ECOLOGICAL MODEL WITH REPLENISHMENT RATE FOR BOTH THE SPECIES

More information

1. Find a basis for the row space of each of the following matrices. Your basis should consist of rows of the original matrix.

1. Find a basis for the row space of each of the following matrices. Your basis should consist of rows of the original matrix. Mh 7 Exm - Prcice Prolem Solions. Find sis for he row spce of ech of he following mrices. Yor sis shold consis of rows of he originl mrix. 4 () 7 7 8 () Since we wn sis for he row spce consising of rows

More information

Neural assembly binding in linguistic representation

Neural assembly binding in linguistic representation Neurl ssembly binding in linguisic represenion Frnk vn der Velde & Mrc de Kmps Cogniive Psychology Uni, Universiy of Leiden, Wssenrseweg 52, 2333 AK Leiden, The Neherlnds, vdvelde@fsw.leidenuniv.nl Absrc.

More information

GENERALIZATION OF SOME INEQUALITIES VIA RIEMANN-LIOUVILLE FRACTIONAL CALCULUS

GENERALIZATION OF SOME INEQUALITIES VIA RIEMANN-LIOUVILLE FRACTIONAL CALCULUS - TAMKANG JOURNAL OF MATHEMATICS Volume 5, Number, 7-5, June doi:5556/jkjm555 Avilble online hp://journlsmhkueduw/ - - - GENERALIZATION OF SOME INEQUALITIES VIA RIEMANN-LIOUVILLE FRACTIONAL CALCULUS MARCELA

More information

An Integral Two Space-Variables Condition for Parabolic Equations

An Integral Two Space-Variables Condition for Parabolic Equations Jornl of Mhemics nd Sisics 8 (): 85-9, ISSN 549-3644 Science Pblicions An Inegrl Two Spce-Vribles Condiion for Prbolic Eqions Mrhone, A.L. nd F. Lkhl Deprmen of Mhemics, Lborory Eqions Differenielles,

More information

A Kalman filtering simulation

A Kalman filtering simulation A Klmn filering simulion The performnce of Klmn filering hs been esed on he bsis of wo differen dynmicl models, ssuming eiher moion wih consn elociy or wih consn ccelerion. The former is epeced o beer

More information

e t dt e t dt = lim e t dt T (1 e T ) = 1

e t dt e t dt = lim e t dt T (1 e T ) = 1 Improper Inegrls There re wo ypes of improper inegrls - hose wih infinie limis of inegrion, nd hose wih inegrnds h pproch some poin wihin he limis of inegrion. Firs we will consider inegrls wih infinie

More information

A Simple Method to Solve Quartic Equations. Key words: Polynomials, Quartics, Equations of the Fourth Degree INTRODUCTION

A Simple Method to Solve Quartic Equations. Key words: Polynomials, Quartics, Equations of the Fourth Degree INTRODUCTION Ausrlin Journl of Bsic nd Applied Sciences, 6(6): -6, 0 ISSN 99-878 A Simple Mehod o Solve Quric Equions Amir Fhi, Poo Mobdersn, Rhim Fhi Deprmen of Elecricl Engineering, Urmi brnch, Islmic Ad Universi,

More information

RESPONSE UNDER A GENERAL PERIODIC FORCE. When the external force F(t) is periodic with periodτ = 2π

RESPONSE UNDER A GENERAL PERIODIC FORCE. When the external force F(t) is periodic with periodτ = 2π RESPONSE UNDER A GENERAL PERIODIC FORCE When he exernl force F() is periodic wih periodτ / ω,i cn be expnded in Fourier series F( ) o α ω α b ω () where τ F( ) ω d, τ,,,... () nd b τ F( ) ω d, τ,,... (3)

More information

Probability, Estimators, and Stationarity

Probability, Estimators, and Stationarity Chper Probbiliy, Esimors, nd Sionriy Consider signl genered by dynmicl process, R, R. Considering s funcion of ime, we re opering in he ime domin. A fundmenl wy o chrcerize he dynmics using he ime domin

More information

How to prove the Riemann Hypothesis

How to prove the Riemann Hypothesis Scholrs Journl of Phsics, Mhemics nd Sisics Sch. J. Phs. Mh. S. 5; (B:5-6 Scholrs Acdemic nd Scienific Publishers (SAS Publishers (An Inernionl Publisher for Acdemic nd Scienific Resources *Corresonding

More information

I = I = I for this case of symmetry about the x axis, we find from

I = I = I for this case of symmetry about the x axis, we find from 8-5. THE MOTON OF A TOP n his secion, we shll consider he moion of n xilly symmeric body, sch s op, which hs fixed poin on is xis of symmery nd is ced pon by niform force field. The op ws chosen becse

More information

1.0 Electrical Systems

1.0 Electrical Systems . Elecricl Sysems The ypes of dynmicl sysems we will e sudying cn e modeled in erms of lgeric equions, differenil equions, or inegrl equions. We will egin y looking fmilir mhemicl models of idel resisors,

More information

The order of reaction is defined as the number of atoms or molecules whose concentration change during the chemical reaction.

The order of reaction is defined as the number of atoms or molecules whose concentration change during the chemical reaction. www.hechemisryguru.com Re Lw Expression Order of Recion The order of recion is defined s he number of oms or molecules whose concenrion chnge during he chemicl recion. Or The ol number of molecules or

More information

On the Pseudo-Spectral Method of Solving Linear Ordinary Differential Equations

On the Pseudo-Spectral Method of Solving Linear Ordinary Differential Equations Journl of Mhemics nd Sisics 5 ():136-14, 9 ISS 1549-3644 9 Science Publicions On he Pseudo-Specrl Mehod of Solving Liner Ordinry Differenil Equions B.S. Ogundre Deprmen of Pure nd Applied Mhemics, Universiy

More information

M r. d 2. R t a M. Structural Mechanics Section. Exam CT5141 Theory of Elasticity Friday 31 October 2003, 9:00 12:00 hours. Problem 1 (3 points)

M r. d 2. R t a M. Structural Mechanics Section. Exam CT5141 Theory of Elasticity Friday 31 October 2003, 9:00 12:00 hours. Problem 1 (3 points) Delf Universiy of Technology Fculy of Civil Engineering nd Geosciences Srucurl echnics Secion Wrie your nme nd sudy numer he op righ-hnd of your work. Exm CT5 Theory of Elsiciy Fridy Ocoer 00, 9:00 :00

More information

IX.1.1 The Laplace Transform Definition 700. IX.1.2 Properties 701. IX.1.3 Examples 702. IX.1.4 Solution of IVP for ODEs 704

IX.1.1 The Laplace Transform Definition 700. IX.1.2 Properties 701. IX.1.3 Examples 702. IX.1.4 Solution of IVP for ODEs 704 Chper IX The Inegrl Trnform Mehod IX. The plce Trnform November 4, 7 699 IX. THE APACE TRANSFORM IX.. The plce Trnform Definiion 7 IX.. Properie 7 IX..3 Emple 7 IX..4 Soluion of IVP for ODE 74 IX..5 Soluion

More information

A Time Truncated Improved Group Sampling Plans for Rayleigh and Log - Logistic Distributions

A Time Truncated Improved Group Sampling Plans for Rayleigh and Log - Logistic Distributions ISSNOnline : 39-8753 ISSN Prin : 347-67 An ISO 397: 7 Cerified Orgnizion Vol. 5, Issue 5, My 6 A Time Trunced Improved Group Smpling Plns for Ryleigh nd og - ogisic Disribuions P.Kvipriy, A.R. Sudmni Rmswmy

More information

Asymptotic relationship between trajectories of nominal and uncertain nonlinear systems on time scales

Asymptotic relationship between trajectories of nominal and uncertain nonlinear systems on time scales Asympoic relionship beween rjecories of nominl nd uncerin nonliner sysems on ime scles Fim Zohr Tousser 1,2, Michel Defoor 1, Boudekhil Chfi 2 nd Mohmed Djemï 1 Absrc This pper sudies he relionship beween

More information

A LIMIT-POINT CRITERION FOR A SECOND-ORDER LINEAR DIFFERENTIAL OPERATOR IAN KNOWLES

A LIMIT-POINT CRITERION FOR A SECOND-ORDER LINEAR DIFFERENTIAL OPERATOR IAN KNOWLES A LIMIT-POINT CRITERION FOR A SECOND-ORDER LINEAR DIFFERENTIAL OPERATOR j IAN KNOWLES 1. Inroducion Consider he forml differenil operor T defined by el, (1) where he funcion q{) is rel-vlued nd loclly

More information

15/03/1439. Lecture 4: Linear Time Invariant (LTI) systems

15/03/1439. Lecture 4: Linear Time Invariant (LTI) systems Lecre 4: Liner Time Invrin LTI sysems 2. Liner sysems, Convolion 3 lecres: Implse response, inp signls s coninm of implses. Convolion, discree-ime nd coninos-ime. LTI sysems nd convolion Specific objecives

More information

ENGR 1990 Engineering Mathematics The Integral of a Function as a Function

ENGR 1990 Engineering Mathematics The Integral of a Function as a Function ENGR 1990 Engineering Mhemics The Inegrl of Funcion s Funcion Previously, we lerned how o esime he inegrl of funcion f( ) over some inervl y dding he res of finie se of rpezoids h represen he re under

More information

4.8 Improper Integrals

4.8 Improper Integrals 4.8 Improper Inegrls Well you ve mde i hrough ll he inegrion echniques. Congrs! Unforunely for us, we sill need o cover one more inegrl. They re clled Improper Inegrls. A his poin, we ve only del wih inegrls

More information

How to Prove the Riemann Hypothesis Author: Fayez Fok Al Adeh.

How to Prove the Riemann Hypothesis Author: Fayez Fok Al Adeh. How o Prove he Riemnn Hohesis Auhor: Fez Fok Al Adeh. Presiden of he Srin Cosmologicl Socie P.O.Bo,387,Dmscus,Sri Tels:963--77679,735 Emil:hf@scs-ne.org Commens: 3 ges Subj-Clss: Funcionl nlsis, comle

More information

Hermite-Hadamard-Fejér type inequalities for convex functions via fractional integrals

Hermite-Hadamard-Fejér type inequalities for convex functions via fractional integrals Sud. Univ. Beş-Bolyi Mh. 6(5, No. 3, 355 366 Hermie-Hdmrd-Fejér ype inequliies for convex funcions vi frcionl inegrls İmd İşcn Asrc. In his pper, firsly we hve eslished Hermie Hdmrd-Fejér inequliy for

More information

New Inequalities in Fractional Integrals

New Inequalities in Fractional Integrals ISSN 1749-3889 (prin), 1749-3897 (online) Inernionl Journl of Nonliner Science Vol.9(21) No.4,pp.493-497 New Inequliies in Frcionl Inegrls Zoubir Dhmni Zoubir DAHMANI Lborory of Pure nd Applied Mhemics,

More information

Soliton Scattering on the External Potential in Weakly Nonlocal Nonlinear Media

Soliton Scattering on the External Potential in Weakly Nonlocal Nonlinear Media Mlysin Journl of Mhemicl Sciences 1(S) Februry: 219 226 (216) Specil Issue: The 3 rd Inernionl Conference on Mhemicl Applicions in Engineering 214 (ICMAE 14) MALAYSIAN JOURNAL OF MATHEMATICAL SCIENCES

More information

Procedia Computer Science

Procedia Computer Science Procedi Compuer Science 00 (0) 000 000 Procedi Compuer Science www.elsevier.com/loce/procedi The Third Informion Sysems Inernionl Conference The Exisence of Polynomil Soluion of he Nonliner Dynmicl Sysems

More information

A PREY-PREDATOR MODEL WITH AN ALTERNATIVE FOOD FOR THE PREDATOR AND OPTIMAL HARVESTING OF THE PREDATOR

A PREY-PREDATOR MODEL WITH AN ALTERNATIVE FOOD FOR THE PREDATOR AND OPTIMAL HARVESTING OF THE PREDATOR VOL. 7, O. 8, AUGUST ISS 89-668 ARP Journal of Engineering and Applied Sciences 6- Asian Research Publishing ework (ARP). All righs reserved. A PREY-PREDATOR MODEL WITH A ALTERATIVE FOOD FOR THE PREDATOR

More information

Physics 2A HW #3 Solutions

Physics 2A HW #3 Solutions Chper 3 Focus on Conceps: 3, 4, 6, 9 Problems: 9, 9, 3, 41, 66, 7, 75, 77 Phsics A HW #3 Soluions Focus On Conceps 3-3 (c) The ccelerion due o grvi is he sme for boh blls, despie he fc h he hve differen

More information

LAPLACE TRANSFORM OVERCOMING PRINCIPLE DRAWBACKS IN APPLICATION OF THE VARIATIONAL ITERATION METHOD TO FRACTIONAL HEAT EQUATIONS

LAPLACE TRANSFORM OVERCOMING PRINCIPLE DRAWBACKS IN APPLICATION OF THE VARIATIONAL ITERATION METHOD TO FRACTIONAL HEAT EQUATIONS Wu, G.-.: Lplce Trnsform Overcoming Principle Drwbcks in Applicion... THERMAL SIENE: Yer 22, Vol. 6, No. 4, pp. 257-26 257 Open forum LAPLAE TRANSFORM OVEROMING PRINIPLE DRAWBAKS IN APPLIATION OF THE VARIATIONAL

More information

September 20 Homework Solutions

September 20 Homework Solutions College of Engineering nd Compuer Science Mechnicl Engineering Deprmen Mechnicl Engineering A Seminr in Engineering Anlysis Fll 7 Number 66 Insrucor: Lrry Creo Sepember Homework Soluions Find he specrum

More information

Temperature Rise of the Earth

Temperature Rise of the Earth Avilble online www.sciencedirec.com ScienceDirec Procedi - Socil nd Behviorl Scien ce s 88 ( 2013 ) 220 224 Socil nd Behviorl Sciences Symposium, 4 h Inernionl Science, Socil Science, Engineering nd Energy

More information

Positive and negative solutions of a boundary value problem for a

Positive and negative solutions of a boundary value problem for a Invenion Journl of Reerch Technology in Engineering & Mngemen (IJRTEM) ISSN: 2455-3689 www.ijrem.com Volume 2 Iue 9 ǁ Sepemer 28 ǁ PP 73-83 Poiive nd negive oluion of oundry vlue prolem for frcionl, -difference

More information

Average & instantaneous velocity and acceleration Motion with constant acceleration

Average & instantaneous velocity and acceleration Motion with constant acceleration Physics 7: Lecure Reminders Discussion nd Lb secions sr meeing ne week Fill ou Pink dd/drop form if you need o swich o differen secion h is FULL. Do i TODAY. Homework Ch. : 5, 7,, 3,, nd 6 Ch.: 6,, 3 Submission

More information

IX.1.1 The Laplace Transform Definition 700. IX.1.2 Properties 701. IX.1.3 Examples 702. IX.1.4 Solution of IVP for ODEs 704

IX.1.1 The Laplace Transform Definition 700. IX.1.2 Properties 701. IX.1.3 Examples 702. IX.1.4 Solution of IVP for ODEs 704 Chper IX The Inegrl Trnform Mehod IX. The plce Trnform November 6, 8 699 IX. THE APACE TRANSFORM IX.. The plce Trnform Definiion 7 IX.. Properie 7 IX..3 Emple 7 IX..4 Soluion of IVP for ODE 74 IX..5 Soluion

More information

Magnetostatics Bar Magnet. Magnetostatics Oersted s Experiment

Magnetostatics Bar Magnet. Magnetostatics Oersted s Experiment Mgneosics Br Mgne As fr bck s 4500 yers go, he Chinese discovered h cerin ypes of iron ore could rc ech oher nd cerin mels. Iron filings "mp" of br mgne s field Crefully suspended slivers of his mel were

More information

Journal of Mathematical Analysis and Applications. Two normality criteria and the converse of the Bloch principle

Journal of Mathematical Analysis and Applications. Two normality criteria and the converse of the Bloch principle J. Mh. Anl. Appl. 353 009) 43 48 Conens liss vilble ScienceDirec Journl of Mhemicl Anlysis nd Applicions www.elsevier.com/loce/jm Two normliy crieri nd he converse of he Bloch principle K.S. Chrk, J. Rieppo

More information

Analytic solution of linear fractional differential equation with Jumarie derivative in term of Mittag-Leffler function

Analytic solution of linear fractional differential equation with Jumarie derivative in term of Mittag-Leffler function Anlyic soluion of liner frcionl differenil equion wih Jumrie derivive in erm of Mig-Leffler funcion Um Ghosh (), Srijn Sengup (2), Susmi Srkr (2b), Shnnu Ds (3) (): Deprmen of Mhemics, Nbdwip Vidysgr College,

More information

Minimum Squared Error

Minimum Squared Error Minimum Squred Error LDF: Minimum Squred-Error Procedures Ide: conver o esier nd eer undersood prolem Percepron y i > for ll smples y i solve sysem of liner inequliies MSE procedure y i = i for ll smples

More information

Minimum Squared Error

Minimum Squared Error Minimum Squred Error LDF: Minimum Squred-Error Procedures Ide: conver o esier nd eer undersood prolem Percepron y i > 0 for ll smples y i solve sysem of liner inequliies MSE procedure y i i for ll smples

More information

A new model for limit order book dynamics

A new model for limit order book dynamics Anewmodelforlimiorderbookdynmics JeffreyR.Russell UniversiyofChicgo,GrdueSchoolofBusiness TejinKim UniversiyofChicgo,DeprmenofSisics Absrc:Thispperproposesnewmodelforlimiorderbookdynmics.Thelimiorderbookconsiss

More information

EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR A SECOND-ORDER ITERATIVE BOUNDARY-VALUE PROBLEM

EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR A SECOND-ORDER ITERATIVE BOUNDARY-VALUE PROBLEM Elecronic Journl of Differenil Equions, Vol. 208 (208), No. 50, pp. 6. ISSN: 072-669. URL: hp://ejde.mh.xse.edu or hp://ejde.mh.un.edu EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR A SECOND-ORDER ITERATIVE

More information

Bioeconomic modelling of a prey predator system using differential algebraic equations

Bioeconomic modelling of a prey predator system using differential algebraic equations MuliCrf Inernionl Journl of ngineering Science nd Technolog Vol. No. pp. -4 INTRNATIONAL JOURNAL OF NGINRING SCINC AN TCHNOLOGY www.ijes-ng.com MuliCrf Limied. All righs reserved Bioeconomic modelling

More information

0 for t < 0 1 for t > 0

0 for t < 0 1 for t > 0 8.0 Sep nd del funcions Auhor: Jeremy Orloff The uni Sep Funcion We define he uni sep funcion by u() = 0 for < 0 for > 0 I is clled he uni sep funcion becuse i kes uni sep = 0. I is someimes clled he Heviside

More information

A PREY-PREDATOR MODEL WITH COVER FOR THE PREY AND AN ALTERNATIVE FOOD FOR THE PREDATOR AND CONSTANT HARVESTING OF BOTH THE SPECIES *

A PREY-PREDATOR MODEL WITH COVER FOR THE PREY AND AN ALTERNATIVE FOOD FOR THE PREDATOR AND CONSTANT HARVESTING OF BOTH THE SPECIES * Jordn Journl of Mthemtics nd Sttistics (JJMS) (), 009, pp. 43-54 A PREY-PREATOR MOEL WITH COVER FOR THE PREY A A ALTERATIVE FOO FOR THE PREATOR A COSTAT HARVESTIG OF BOTH THE SPECIES * K. LAKSHMI ARAYA.PATTABHIRAMACHARYULU

More information

Thermal neutron self-shielding factor in foils: a universal curve

Thermal neutron self-shielding factor in foils: a universal curve Proceedings of he Inernionl Conference on Reserch Recor Uilizion, Sfey, Decommissioning, Fuel nd Wse Mngemen (Snigo, Chile, -4 Nov.3) Pper IAEA-CN-/, IAEA Proceedings Series, Vienn, 5 Therml neuron self-shielding

More information

..,..,.,

..,..,., 57.95. «..» 7, 9,,. 3 DOI:.459/mmph7..,..,., E-mil: yshr_ze@mil.ru -,,. -, -.. -. - - ( ). -., -. ( - ). - - -., - -., - -, -., -. -., - - -, -., -. : ; ; - ;., -,., - -, []., -, [].,, - [3, 4]. -. 3 (

More information

1. Introduction. 1 b b

1. Introduction. 1 b b Journl of Mhemicl Inequliies Volume, Number 3 (007), 45 436 SOME IMPROVEMENTS OF GRÜSS TYPE INEQUALITY N. ELEZOVIĆ, LJ. MARANGUNIĆ AND J. PEČARIĆ (communiced b A. Čižmešij) Absrc. In his pper some inequliies

More information

The solution is often represented as a vector: 2xI + 4X2 + 2X3 + 4X4 + 2X5 = 4 2xI + 4X2 + 3X3 + 3X4 + 3X5 = 4. 3xI + 6X2 + 6X3 + 3X4 + 6X5 = 6.

The solution is often represented as a vector: 2xI + 4X2 + 2X3 + 4X4 + 2X5 = 4 2xI + 4X2 + 3X3 + 3X4 + 3X5 = 4. 3xI + 6X2 + 6X3 + 3X4 + 6X5 = 6. [~ o o :- o o ill] i 1. Mrices, Vecors, nd Guss-Jordn Eliminion 1 x y = = - z= The soluion is ofen represened s vecor: n his exmple, he process of eliminion works very smoohly. We cn elimine ll enries

More information

UNIQUENESS OF AMMENSAL & COMMENSAL MATHEMATICAL MODELS WITH LIMITED RESOURCES IN FULLY WASHED-OUT STATE

UNIQUENESS OF AMMENSAL & COMMENSAL MATHEMATICAL MODELS WITH LIMITED RESOURCES IN FULLY WASHED-OUT STATE UNIQUENESS OF AMMENSAL & COMMENSAL MATHEMATICAL MODELS WITH LIMITED RESOURCES IN FULLY WASHED-OUT STATE 1 Dr. K.V.L.N.Acharyulu & Dr.N.Phani Kumar 1 Associate Professor, Department of Mathematics, Bapatla

More information

Some Inequalities variations on a common theme Lecture I, UL 2007

Some Inequalities variations on a common theme Lecture I, UL 2007 Some Inequliies vriions on common heme Lecure I, UL 2007 Finbrr Hollnd, Deprmen of Mhemics, Universiy College Cork, fhollnd@uccie; July 2, 2007 Three Problems Problem Assume i, b i, c i, i =, 2, 3 re rel

More information

Convergence of Singular Integral Operators in Weighted Lebesgue Spaces

Convergence of Singular Integral Operators in Weighted Lebesgue Spaces EUROPEAN JOURNAL OF PURE AND APPLIED MATHEMATICS Vol. 10, No. 2, 2017, 335-347 ISSN 1307-5543 www.ejpm.com Published by New York Business Globl Convergence of Singulr Inegrl Operors in Weighed Lebesgue

More information

CALDERON S REPRODUCING FORMULA FOR DUNKL CONVOLUTION

CALDERON S REPRODUCING FORMULA FOR DUNKL CONVOLUTION Avilble online hp://scik.org Eng. Mh. Le. 15, 15:4 ISSN: 49-9337 CALDERON S REPRODUCING FORMULA FOR DUNKL CONVOLUTION PANDEY, C. P. 1, RAKESH MOHAN AND BHAIRAW NATH TRIPATHI 3 1 Deprmen o Mhemics, Ajy

More information

LAGRANGIAN AND HAMILTONIAN MECHANICS WITH FRACTIONAL DERIVATIVES

LAGRANGIAN AND HAMILTONIAN MECHANICS WITH FRACTIONAL DERIVATIVES LAGRANGIAN AND HAMILTONIAN MEHANIS WITH FRATIONAL DERIVATIVES EMIL POPESU 2,1 1 Asronomicl Insiue of Romnin Acdemy Sr uiul de Argin 5, 40557 Buchres, Romni 2 Technicl Universiy of ivil Engineering, Bd

More information

Scalar Conservation Laws

Scalar Conservation Laws MATH-459 Nmerical Mehods for Conservaion Laws by Prof. Jan S. Heshaven Solion se : Scalar Conservaion Laws Eercise. The inegral form of he scalar conservaion law + f ) = is given in Eq. below. ˆ 2, 2 )

More information

USING ITERATIVE LINEAR REGRESSION MODEL TO TIME SERIES MODELS

USING ITERATIVE LINEAR REGRESSION MODEL TO TIME SERIES MODELS Elecronic Journl of Applied Sisicl Anlysis EJASA (202), Elecron. J. App. S. Anl., Vol. 5, Issue 2, 37 50 e-issn 2070-5948, DOI 0.285/i20705948v5n2p37 202 Universià del Sleno hp://sib-ese.unile.i/index.php/ejs/index

More information

Tax Audit and Vertical Externalities

Tax Audit and Vertical Externalities T Audi nd Vericl Eernliies Hidey Ko Misuyoshi Yngihr Ngoy Keizi Universiy Ngoy Universiy 1. Inroducion The vericl fiscl eernliies rise when he differen levels of governmens, such s he federl nd se governmens,

More information

Physic 231 Lecture 4. Mi it ftd l t. Main points of today s lecture: Example: addition of velocities Trajectories of objects in 2 = =

Physic 231 Lecture 4. Mi it ftd l t. Main points of today s lecture: Example: addition of velocities Trajectories of objects in 2 = = Mi i fd l Phsic 3 Lecure 4 Min poins of od s lecure: Emple: ddiion of elociies Trjecories of objecs in dimensions: dimensions: g 9.8m/s downwrds ( ) g o g g Emple: A foobll pler runs he pern gien in he

More information

Solitary Wave Solutions for the Boussinesq and Fisher Equations by the Modified Simple Equation Method

Solitary Wave Solutions for the Boussinesq and Fisher Equations by the Modified Simple Equation Method Mhemics Leers ; (): -8 hp://www.sciencepblishinggrop.com/j/ml doi:.48/j.ml.. Soliry Wve Solions for he Bossinesq nd Fisher Eqions by he Modified Simple Eqion Mehod Md. Ashrfzzmn Khn, M. Ali Akbr, Fehi

More information

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 9: The High Beta Tokamak

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 9: The High Beta Tokamak .65, MHD Theory of Fusion Sysems Prof. Freidberg Lecure 9: The High e Tokmk Summry of he Properies of n Ohmic Tokmk. Advnges:. good euilibrium (smll shif) b. good sbiliy ( ) c. good confinemen ( τ nr )

More information

MATH 124 AND 125 FINAL EXAM REVIEW PACKET (Revised spring 2008)

MATH 124 AND 125 FINAL EXAM REVIEW PACKET (Revised spring 2008) MATH 14 AND 15 FINAL EXAM REVIEW PACKET (Revised spring 8) The following quesions cn be used s review for Mh 14/ 15 These quesions re no cul smples of quesions h will pper on he finl em, bu hey will provide

More information

PARABOLA. moves such that PM. = e (constant > 0) (eccentricity) then locus of P is called a conic. or conic section.

PARABOLA. moves such that PM. = e (constant > 0) (eccentricity) then locus of P is called a conic. or conic section. wwwskshieducioncom PARABOLA Le S be given fixed poin (focus) nd le l be given fixed line (Direcrix) Le SP nd PM be he disnce of vrible poin P o he focus nd direcrix respecively nd P SP moves such h PM

More information

ON NEW INEQUALITIES OF SIMPSON S TYPE FOR FUNCTIONS WHOSE SECOND DERIVATIVES ABSOLUTE VALUES ARE CONVEX

ON NEW INEQUALITIES OF SIMPSON S TYPE FOR FUNCTIONS WHOSE SECOND DERIVATIVES ABSOLUTE VALUES ARE CONVEX Journl of Applied Mhemics, Sisics nd Informics JAMSI), 9 ), No. ON NEW INEQUALITIES OF SIMPSON S TYPE FOR FUNCTIONS WHOSE SECOND DERIVATIVES ABSOLUTE VALUES ARE CONVEX MEHMET ZEKI SARIKAYA, ERHAN. SET

More information

PHYSICS 1210 Exam 1 University of Wyoming 14 February points

PHYSICS 1210 Exam 1 University of Wyoming 14 February points PHYSICS 1210 Em 1 Uniersiy of Wyoming 14 Februry 2013 150 poins This es is open-noe nd closed-book. Clculors re permied bu compuers re no. No collborion, consulion, or communicion wih oher people (oher

More information

Predict Global Earth Temperature using Linier Regression

Predict Global Earth Temperature using Linier Regression Predict Globl Erth Temperture using Linier Regression Edwin Swndi Sijbt (23516012) Progrm Studi Mgister Informtik Sekolh Teknik Elektro dn Informtik ITB Jl. Gnesh 10 Bndung 40132, Indonesi 23516012@std.stei.itb.c.id

More information

1. Consider a PSA initially at rest in the beginning of the left-hand end of a long ISS corridor. Assume xo = 0 on the left end of the ISS corridor.

1. Consider a PSA initially at rest in the beginning of the left-hand end of a long ISS corridor. Assume xo = 0 on the left end of the ISS corridor. In Eercise 1, use sndrd recngulr Cresin coordine sysem. Le ime be represened long he horizonl is. Assume ll ccelerions nd decelerions re consn. 1. Consider PSA iniilly res in he beginning of he lef-hnd

More information

S Radio transmission and network access Exercise 1-2

S Radio transmission and network access Exercise 1-2 S-7.330 Rdio rnsmission nd nework ccess Exercise 1 - P1 In four-symbol digil sysem wih eqully probble symbols he pulses in he figure re used in rnsmission over AWGN-chnnel. s () s () s () s () 1 3 4 )

More information

A SPECIAL CASE OF ECOLOGICAL COMMENSALISM- PHASE PLANE ANALYSIS

A SPECIAL CASE OF ECOLOGICAL COMMENSALISM- PHASE PLANE ANALYSIS A SPECIAL CASE OF ECOLOGICAL COMMENSALISM- PHASE PLANE ANALYSIS Dr. K.V. L. N. Acharyulu Associate Professor, Department of Mathematics, Bapatla Engineering College, Bapatla, (India) n whet ABSTRACT The

More information

ON THE OSTROWSKI-GRÜSS TYPE INEQUALITY FOR TWICE DIFFERENTIABLE FUNCTIONS

ON THE OSTROWSKI-GRÜSS TYPE INEQUALITY FOR TWICE DIFFERENTIABLE FUNCTIONS Hceepe Journl of Mhemics nd Sisics Volume 45) 0), 65 655 ON THE OSTROWSKI-GRÜSS TYPE INEQUALITY FOR TWICE DIFFERENTIABLE FUNCTIONS M Emin Özdemir, Ahme Ock Akdemir nd Erhn Se Received 6:06:0 : Acceped

More information

A Prey-Predator Model with an Alternative Food for the Predator and Optimal Harvesting of the Prey

A Prey-Predator Model with an Alternative Food for the Predator and Optimal Harvesting of the Prey Available online a www.pelagiaresearchlibrary.com Advances in Applied Science Research, 0, (4):45-459 A Prey-Predaor Model wih an Alernaive Food for he Predaor and Opimal Harvesing of he Prey K. Madhusudhan

More information

Non-oscillation of perturbed half-linear differential equations with sums of periodic coefficients

Non-oscillation of perturbed half-linear differential equations with sums of periodic coefficients Hsil nd Veselý Advnces in Difference Equions 2015 2015:190 DOI 10.1186/s13662-015-0533-4 R E S E A R C H Open Access Non-oscillion of perurbed hlf-liner differenil equions wih sums of periodic coefficiens

More information

MASS, STIFFNESS, AND DAMPING MATRICES FROM MEASURED MODAL PARAMETERS

MASS, STIFFNESS, AND DAMPING MATRICES FROM MEASURED MODAL PARAMETERS IS 74 Inernionl Insrmenion-omion Conference & Exhibi Ocober, 974 MSS, STIFFNESS, ND DMPING MTRICES FROM MESURED MODL PRMETERS Ron Poer nd Mr Richrdson Digil Signl nlysis HEWLETT-PCKRD COMPNY Sn Clr, Cliforni

More information

IX.2 THE FOURIER TRANSFORM

IX.2 THE FOURIER TRANSFORM Chper IX The Inegrl Trnsform Mehods IX. The Fourier Trnsform November, 7 7 IX. THE FOURIER TRANSFORM IX.. The Fourier Trnsform Definiion 7 IX.. Properies 73 IX..3 Emples 74 IX..4 Soluion of ODE 76 IX..5

More information

LAPLACE TRANSFORMS. 1. Basic transforms

LAPLACE TRANSFORMS. 1. Basic transforms LAPLACE TRANSFORMS. Bic rnform In hi coure, Lplce Trnform will be inroduced nd heir properie exmined; ble of common rnform will be buil up; nd rnform will be ued o olve ome dierenil equion by rnforming

More information

ON A NEW SOLUTION OF FRACTIONAL DIFFERENTIAL EQUATION USING COMPLEX TRANSFORM IN THE UNIT DISK

ON A NEW SOLUTION OF FRACTIONAL DIFFERENTIAL EQUATION USING COMPLEX TRANSFORM IN THE UNIT DISK Mhemicl Compionl pplicions Vol 9 No pp 5-6 4 ON NEW SOLUTION OF FRCTIONL IFFERENTIL EQUTION USING COMPLEX TRNSFORM IN THE UNIT ISK Rbh W Ibrhim Mslin rs Insie of Mhemicl Sciences Universiy Mly 563 Kl Lmpr

More information

A new model for solving fuzzy linear fractional programming problem with ranking function

A new model for solving fuzzy linear fractional programming problem with ranking function J. ppl. Res. Ind. Eng. Vol. 4 No. 07 89 96 Journl of pplied Reserch on Indusril Engineering www.journl-prie.com new model for solving fuzzy liner frcionl progrmming prolem wih rning funcion Spn Kumr Ds

More information

Application on Inner Product Space with. Fixed Point Theorem in Probabilistic

Application on Inner Product Space with. Fixed Point Theorem in Probabilistic Journl of Applied Mhemics & Bioinformics, vol.2, no.2, 2012, 1-10 ISSN: 1792-6602 prin, 1792-6939 online Scienpress Ld, 2012 Applicion on Inner Produc Spce wih Fixed Poin Theorem in Probbilisic Rjesh Shrivsv

More information

2k 1. . And when n is odd number, ) The conclusion is when n is even number, an. ( 1) ( 2 1) ( k 0,1,2 L )

2k 1. . And when n is odd number, ) The conclusion is when n is even number, an. ( 1) ( 2 1) ( k 0,1,2 L ) Scholrs Journl of Engineering d Technology SJET) Sch. J. Eng. Tech., ; A):8-6 Scholrs Acdemic d Scienific Publisher An Inernionl Publisher for Acdemic d Scienific Resources) www.sspublisher.com ISSN -X

More information

Chapter 2. Motion along a straight line. 9/9/2015 Physics 218

Chapter 2. Motion along a straight line. 9/9/2015 Physics 218 Chper Moion long srigh line 9/9/05 Physics 8 Gols for Chper How o describe srigh line moion in erms of displcemen nd erge elociy. The mening of insnneous elociy nd speed. Aerge elociy/insnneous elociy

More information

Chapter Direct Method of Interpolation

Chapter Direct Method of Interpolation Chper 5. Direc Mehod of Inerpolion Afer reding his chper, you should be ble o:. pply he direc mehod of inerpolion,. sole problems using he direc mehod of inerpolion, nd. use he direc mehod inerpolns o

More information

Fault-Tolerant Guaranteed Cost Control of Uncertain Networked Control Systems with Time-varying Delay

Fault-Tolerant Guaranteed Cost Control of Uncertain Networked Control Systems with Time-varying Delay IJCSNS Inernionl Journl of Compuer Science nd Nework Securiy VOL.9 No.6 June 9 3 Ful-olern Gurneed Cos Conrol of Uncerin Neworked Conrol Sysems wih ime-vrying Dely Guo Yi-nn Zhng Qin-ying Chin Universiy

More information

FURTHER GENERALIZATIONS. QI Feng. The value of the integral of f(x) over [a; b] can be estimated in a variety ofways. b a. 2(M m)

FURTHER GENERALIZATIONS. QI Feng. The value of the integral of f(x) over [a; b] can be estimated in a variety ofways. b a. 2(M m) Univ. Beogrd. Pul. Elekroehn. Fk. Ser. M. 8 (997), 79{83 FUTHE GENEALIZATIONS OF INEQUALITIES FO AN INTEGAL QI Feng Using he Tylor's formul we prove wo inegrl inequliies, h generlize K. S. K. Iyengr's

More information

ON PREY-PREDATOR MODEL WITH HOLLING-TYPE II AND LESLIE-GOWER SCHEMES AHMED BUSERI ASHINE

ON PREY-PREDATOR MODEL WITH HOLLING-TYPE II AND LESLIE-GOWER SCHEMES AHMED BUSERI ASHINE Journl of Mthemtics nd Computer Applictions Reserch (JMCAR) ISSN(P): 5-48; ISSN(E): Applied Vol 3, Issue 1, Dec 16, 7-34 TJPRC Pvt Ltd ON PREY-PREDATOR MODEL WITH HOLLING-TYPE II AND LESLIE-GOWER SCHEMES

More information

Hermite-Hadamard and Simpson Type Inequalities for Differentiable Quasi-Geometrically Convex Functions

Hermite-Hadamard and Simpson Type Inequalities for Differentiable Quasi-Geometrically Convex Functions Trkish Jornl o Anlysis nd Nmer Theory, 4, Vol, No, 4-46 Aville online h://ssciecom/jn/// Science nd Edcion Plishing DOI:69/jn--- Hermie-Hdmrd nd Simson Tye Ineliies or Dierenile Qsi-Geomericlly Convex

More information

graph of unit step function t

graph of unit step function t .5 Piecewie coninuou forcing funcion...e.g. urning he forcing on nd off. The following Lplce rnform meril i ueful in yem where we urn forcing funcion on nd off, nd when we hve righ hnd ide "forcing funcion"

More information

Green s Functions and Comparison Theorems for Differential Equations on Measure Chains

Green s Functions and Comparison Theorems for Differential Equations on Measure Chains Green s Funcions nd Comprison Theorems for Differenil Equions on Mesure Chins Lynn Erbe nd Alln Peerson Deprmen of Mhemics nd Sisics, Universiy of Nebrsk-Lincoln Lincoln,NE 68588-0323 lerbe@@mh.unl.edu

More information