A New Approach for Solving Boundary Value Problem in Partial Differential Equation Arising in Financial Market

Size: px
Start display at page:

Download "A New Approach for Solving Boundary Value Problem in Partial Differential Equation Arising in Financial Market"

Transcription

1 Applied Mahemaics, 6, 7, Published Online May 6 in cires. hp://.scirp.org/journal/am hp://dx.doi.org/.436/am A Ne Approach for olving Boundary Value Problem in Parial Differenial Equaion Arising in Financial Marke Fadugba unday Emmanuel *, Emeka Helen Oluyemisi Deparmen of Mahemaical ciences, Ekii ae Universiy, Ado Ekii, Nigeria Deparmen of Mahemaical and Physical ciences, Afe Babalola Universiy, Ado Ekii, Nigeria Received April 6; acceped 3 May 6; published 6 May 6 Copyrigh 6 by auhors and cienific Research Publishing Inc. This ork is licensed under he Creaive Commons Aribuion Inernaional License (CC BY). hp://creaivecommons.org/licenses/by/4./ Absrac In his paper, e presen a ne approach for solving boundary value problem in parial differenial equaion arising in financial marke by means of he Laplace ransform. The resul shos ha he Laplace ransform for he price of he European call opion hich pays dividend yield reduces o he Black-choles-Meron model. eyords Black-choles-Meron Model, Boundary Value Problem, European Call Opion, Financial Marke, Laplace Transform. Inroducion An opion is a conrac ha gives he righ (no an obligaion) o is holder o buy or sell some amoun of he underlying asse a a fuure dae for a prescribed price. The underlying asses include socks, sock indices, deb insrumens, commodiies and foreign currency. A call opion gives is holder he righ o buy he underlying asse, hereas a pu opion gives is holder he righ o sell. Vanilla opions are acively raded on organized exchanges. They are also subjec o cerain regulariy and sandardizaion condiions. Vanilla opions can be classified as American opions and European opions. An American opion gives a financial agen he righ, bu no obligaion o buy or o sell he underlying asses on or prior o he expiry dae a he specified price called he exercise price. European opion is an opion ha can be exercised only a he expiry dae ih linear payoff. European opion comes in o forms namely European call and pu opions. * Corresponding auhor. Ho o cie his paper: Emmanuel, F.. and Oluyemisi, E.H. (6) A Ne Approach for olving Boundary Value Problem in Parial Differenial Equaion Arising in Financial Marke. Applied Mahemaics, 7, hp://dx.doi.org/.436/am

2 A European call opion is an opion ha can be exercised only a expiry and has a linear payoff given by he difference beeen underlying asse price a mauriy and he exercise price. The payoff for he European call opion is given by ( T, ) ( T ) C T +. () A European pu opion is an opion ha can be exercised only a expiry and has a linear payoff given by he difference beeen he exercise price and underlying asse price a mauriy. The payoff for he European pu opion is given by ( T, ) ( T ) P T +. () The revoluion on derivaive securiies boh in exchange markes and in academic communiies began in he early 97 s. Ho o raionally price an opion as no clear unil 973, hen Black and choles published heir seminal ork on opion pricing in hich hey described a mahemaical frame ork for finding he fair price of a European opion (see []). Moreover, in he same year, [] exended he Black-choles model in several imporan ays. ince is invenion, he Black-choles formula has been idely used by raders o deermine he price of an opion. Hoever his famous formula has been quesioned afer he 987 crash. One of he main concerns abou financial opions is ha he exac values of opions are. For he simples model in he case of consan coefficiens, an exac pricing formula as derived by Black and choles, knon as he Black-choles formula. Hoever, in he general case of ime and space dependen coefficiens he exac pricing formula is no ye esablished, and hus numerical soluions have been used (see [3]). There are many exhausive exs and lieraures in his subjec area such as [4]-[], jus o menion a fe. In his paper, e presen a ne approach for solving boundary value problem in parial differenial equaion arising in financial marke via he Laplace ransform. The res of he paper is organized as follos: ecion presens he Black-choles-Meron parial differenial equaion for he price of European call opion hich pays a dividend yield. In ecion 3, e consider he Laplace ransform and some of is fundamenal properies. ecion 4 presens he Laplace ransform for solving boundary value problem in parial differenial equaion arising in financial marke. We also sho ha our resul reduces o Black-choles-Meron like formula. ecion 5 concludes he paper.. The Black-choles-Meron Parial Differenial Equaion We consider a marke here he underlying asse price, T is governed by he sochasic differenial equaion of he form d r d d + d W, < < (3) here is he volailiy, r is he riskless ineres rae, d is he dividend yield and W is a one-dimensional Wiener process. andard arbirage argumens sho ha any derivaive u(, ) rien on mus saisfy he parial differenial equaion of he form eing u(, ) C(, ) u, u, u, + ( r d ) + ru (, ). (4) in (4), hen e have he Black-choles-Meron parial differenial equaion for he price of European call opion given by ih boundary condiions C, C, C, + ( r d ) + rc (, ) (, ) as on [, ) (, ) as on [, ) C T (6) C T (7) (5) 84

3 and final ime condiion given by + ( T, ) ( T ) ( T ) on [, ) C T f. (8) Equaion (7) saes ha he opion is orhless hen he sock price is zero. 3. The Laplace Transform and Is Fundamenal Properies Le h( x ) be a piece-ise coninuous funcion on every closed inerval { x [ ab, ] x [, )} h: { x [, ) }, h: x h( x) such ha and. Then L ( h( x) ) H( ),for he Laplace ransform of h( x ) and is defined as ( ) e x d,, > here exiss is called L h x H h x x (9) henever he inegral exiss. Conversely, he inverse Laplace ransform of H( ) is defined as L ( H( ) ) h( x) H( ) c > πi Le h( x ) be a piece-ise coninuous ih he Laplace ransform he Laplace ransform hold. ) Lineariy of he Laplace Transform c+ i x e d,. () c i ( ) + ( ) + ( + ) L h x. The fundamenal properies of L e x ah x L bg x ah bg ah x bg x dx. () Equaion () is inermediae from he definiion and he lineariy of he definie inegral. ) caling Propery x L ( ax) h( ax) e d x H, a > a a () 3) hifing Propery 4) Commuaiviy Propery The Laplace ransform is commuaive. i.e. ( e ax ) e ax e x d ( ) L x H a (3) ( ) ( ) ( ) L g x * L h x G * H g x h d 5) The Laplace Transforms on Differeniaion x x d * ( )* ( ) h x g H G L h x L g x Le h( x),for x > be a differeniable funcion ih he derivaive h x M x X hen dh x dx (4) being coninuous. uppose ha α x here exis consan M and X such ha e,, b dh( x) x dh( x) x L ( h( x) ) H ( ) e dx lim e dx H ( ) h( ). (5) Noe ha he condiion 6) Convoluion Propery dx b α x dx b h x Me, x X lim h b e, for > α. (6) b 84

4 Theorem : Convoluion Theorem and Le L( g( x) ) L( h( x )) denoe he Laplace ransforms of g( x) and h( x ), respecively. Then he produc given by L( f ( x) ) L( g( x) h( x) ) is he Laplace ransform of he convoluion of g( x) and h( x ) is denoed by f ( x) ( g* h)( x) and he inegral represenaion x f x g* h x g x h x s ds f ( x) ( h* g)( x) h( x) g( x s) ds x We presen some of he resuls on he exisence and uniqueness of he Laplace ransform belo. Theorem : Exisence of Laplace Transform Le h( x ) be a pieceise coninuous funcion on [, R ] (for every R > ) and have an exponenial order h x M L h x is defined for > β, i.e. a infiniy ih e ax. Then, he Laplace ransform ( ) { } { β} Domain L ( h( x) ) >. Theorem 3: Uniqueness of Laplace Transform Le g( x) and ions ih an exponenial order a infiniy. Assume ha L g( x) L h x, hen g( x) h( x) x [ P] for every P >, excep may be for a finie se of poins. Relaion o he Mellin and he Fourier Transformaions (7) h x be o pieceise coninuous func- ( ),,, Laplace ransformaion is closely relaed o an exended form of oher popular ransforms, paricularly Mellin and Fourier. Boh can be obained hrough a change of variables. By seing z z x e,dx e dz. (8) The Laplace ransform (9) yields M h z e, F h z e, i L h x, (9) here (.), (.) and (.) ( ) ( ) ( ) M F L denoe he Mellin ransform, he Fourier ransform and he Laplace ransform respecively 4. Laplace Transform for olving Boundary Value Problems in Parial Differenial Equaion Arising in Financial Marke By change of variables T, (5) becomes C(, ) C(, ) C(, ) + ( r d ) + rc (, ) () ih boundary condiions C, as on, T () and final ime condiion given by ( ) [ ) (, ) as on [, ) C T () + (, ) ( ) on [, ) C. (3) Le he Laplace ransform for he price of he European call opion be defined as L C, f (4) ( ( )) ( ) and he inverse Laplace ransform for he price of he European call opion be given by ( ( )) (, ) L f C (5) 843

5 here f is he Laplace ransform ih parameer. Taking he Laplace ransform of (5) using (4) e have ha here L is he Laplace operaor and L C, + ( r d ) C, + C, L rc ( (, ) ) (, ) C L f C f + ( ( ) (, )) ( ) ( ) (, ) C f L ( r q) ( r d) ubsiuing (7), (8), (9) and (3) ino (6) yields (, ) C f L ( (, )) ( ) + (6) (7) (8) (9) L rc rf. (3) + f f f r d rf implifying furher and rearranging erms in (3) e have ha f f + r d r + f We consider he folloing o cases as follos. CAE I For, (3) becomes f f + r d r + f The general soluion o (33) can be obained as here f ( ) and f ( ) form c p c p +. (3). (3). (33) f f + f (34) are he complemenary soluion o he homogeneous par of (33) hich is of he and he paricular soluion respecively. We assume ha he soluion o (33) is of he form and f f + + ( r d) r f The firs and he second derivaives of (36) are obained as f (35) f B α. (36) f ( ) ( ) α B α α α B α ubsiuing (36), (37) and (38) ino (35), and simplifying furher, e have ha (37). (38) 844

6 olving (39), e obain he folloing roos α + α ( + ). (39) α B r d r rd + rd + r+ α rd rd + r+ α Hence he complemenary soluion o he homogeneous par of (33) is obained as α α here α and α are given by (4). For he paricular soluion of (33), e assume ha (4) fc B + B, α α (4) f f f j + l j and. (4) p p p Using (4) and (33), and equaing he coefficiens of erms, e obain j l ( + d) ( r + ) ubsiuing (43) and (44) ino he paricular soluion, e have ha ubsiuing (4) and (45) ino (34) f p ( ) ( + d) ( r + ) α α (43). (44) ( + d) ( r + ). (45) f ( ) B + B +, α α. (46) Equaion (46) is he general soluion o (33) for. CAE II For, (33) becomes ih f f + +. ( r d) r f Folloing he above procedures, he general soluion o he las equaion is obained as α α f B + B, α α (47) rd + rd + r+ α rd rd + r+ α 845

7 Equaion (47) coincides ih he complemenary soluion of (33) given by (4). In he case of, e se B o ensure he boundedness of he derivaive f ( ). In he case of, B o ensure ha he opion s value approaches zero as he sock price goes o zero. The soluions for he o cases equaions (46) and (47) become α f( ) B +, α α ( + d) ( r + ) (48) f B α, α α. (49) We an he opion pricing funcion o be coninuous and differeniable a he ransiion poin, Therefore, he values of he funcion and heir firs derivaives from (48) and (49) mus equal o each oher. These condiions can be used o solve for B and B. The funcion values and derivaives a from (48) and (49) are given by α f( ) B + (5) d + r + and and ( ) α B α + f d + (5) f, B α (5) f ( ) Bα α eing (5) (5) and (5) (53) and solving furher, e obain B ( α ) ( α α ) α ( r + ) d + α. (53) ( α ) ( α α ) α B ( r + ) d + α ubsiuing (54) and (55) ino (49) and (48), e have ( α ) α α ( α α ) (54). (55) α f( ) +, α α ( r + ) d + + d r + ( α ) α ( α α ) α α f( ), α α ( r + ) d + respecively. Equaions (56) and (57) can also be rien as f ( ) ( α ) α α ( α α) ( α ) α, α α, for α ( α α ) α +, α α, for ( r + ) d + + d r + α ( r + ) d + Equaion (58) is he Laplace ransform of he price of European call opion hich pays a dividend yield. Theorem 4 (56) (57) (58) 846

8 If, α α, hen he Laplace ransform of he price of European call opion ih dividend yield given by ( α ) α ( α α ) α f ( ) f ( ) reduces o he Black-choles-Meron valuaion formula α ( r + ) d + BM (, ) e d r e (58a) C N d N d (58b) ih ln r d + + d ln r d + d d by means of he Laplace ransform of he form here k g+ a g m+ b ak e L e N e c g + a a+ g + a (58c) r d + r d + ( r + ) α, r d r d + ( r + ) α, b m a and k and bcm,, and g are arbirary consans. c c Proof: From (57) and (58a) e can rie ha eing Therefore, (59) becomes Le us firs consider he erm ( α ) α ( ) α f f α α α ( r + ) ( α α) d + α α A A α α ( r + ) ( α α ) ( α ) α ( d + ) ( α α ) α α (58d). (59) (6). (6) f f A + A. (6) α α A. (63) r r α α ( + ) ( α α) + α α α 847

9 Using he values of and Therefore (63) yields r d r d + r + α ( α α ) r d + ( r + ). α r d + r d + ( r + ) A ( r ) + r d + ( r + ) Thus, r d r d ( r ) ln α e ( r + ) r d + r + ln α e r d + ( r + q) r d + r d + r + ln α e r d + r d + ( r + ) A ( r + ) r d + ( r + ) r d + r d + ( r + ) ubsiuing he value of α ino (64) and simplifying furher, e obain ln rd + ( r+ ) r d ln e e A r d r d r d ( r + + ) + + ( r + ) (64) (65) 848

10 Comparing (65) ih (58c), e have ha,, ln, r d b g ra,, c ln m k. c b r d c m Taking he inverse Laplace ransform of (65), e obain here We also consider he erm r ( ) e r (66) A e N d N d (67) A d ln r d +. (68) ( α ) α ( d + ) ( α α ) ( α ) ( α α ) α d + ubsiuing he values of α and α ino (69) yields A implifying (7) furher, e obain A α r d ( r ) r d ln ln. (69) e e r d r d + r d ( r ) ( r ) ln r d r d ln (7) e e. (7) r d + r d + r d Once again e compare (7) ih (58c), e deduce ha 849

11 +,, ln, r d b + g da,, c ln m k c b r d c m Taking he Laplace ransform of (7), e have ha e d (7) A N d (73) here ln r d + + d. (74) The inverse Laplace ransform of (6) is obained as (, ) (, ) ubsiuing (67), (68), (73) and (74) ino (75) yields C C A + A. (75) d r (, ) (, ) e e (, ) C C N d N d C BM ln r d + + d ln r d + d d This complees he proof. Theorem 5 If, α α, hen he Laplace ransform of he price of European call opion ih dividend yield given by (, ) C ( α ) α α ( α α ) α ( r + ) d + + d r + + reduces o he Black-choles-Meron valuaion formula given by BM d r (, ) e e (76) C N d N d (76a) ih ln r d + + d ln r d + d d by means of he Laplace ransform given by 85

12 here k g+ a g m+ b ak e L e N e c g + a a+ g + a (76b) r d + r d + ( r + ) α, r d r d + ( r + ) α, b m a and k and bcm,, and g are arbirary consans. c c Remark ) The proof of Theorem 5 follos from Theorem 4, since (56) and (57) have he same inverse Laplace ransforms. The above resuls sho ha he prices of European call opion ih dividend yield given by (56) and (57) coincide ih he Black-choles-Meron model given by (58b) by means of (58c). 5. Conclusion Finance is one of he fases developing areas in he modern corporae and banking orld. In his paper, e have considered he boundary value problem in parial differenial equaion arising in financial marke. We used a ne approach for solving he Black-choles-Meron parial differenial equaion for he price of European call opion hich pays a dividend yield by means of he Laplace ransform. The same approach can be used for European pu opion ih dividend paying sock. The resuls sho ha he Laplace ransform for he price of he European call opion ih dividend paying sock coincides ih he Black-choles-Meron model; i is very effecive and is a good ool for solving parial differenial equaions arising in financial marke and oher areas such as engineering and applied sciences. References [] Black, F. and choles, M. (973) The Pricing of Opions and Corporae Liabiliies. Journal of Poliical Economy, 8, hp://dx.doi.org/.86/66 [] Meron, R.C. (973) Theory of Raional Opion Pricing. Bell Journal of Economics and Managemen cience, 4, hp://dx.doi.org/.37/3343 [3] Lee, H. and heen, D. (9) Laplace Transformaion Mehod for he Black-choles Equaion. Inernaional Journal of Numerical Analysis and Modelling, 6, [4] Cohen, A.M. (7) Numerical Mehods for Laplace Transform Inversion. pringer, Ne York. [5] Nozo, C.R. and Fadugba,.E. (4) Performance Measure of Laplace Transforms for Pricing Pah Dependen Opions. Inernaional Journal of Pure and Applied Mahemaics, 94, hp://dx.doi.org/.73/ijpam.v94i.5 [6] Fadugba,.E. and Ogunrinde, R.B. (4) Black-choles Parial Differenial Equaion in he Mellin Transform Domain. Inernaional Journal of cienific and Technology Research, 3, -6. [7] Lee, R. (3) Opion Pricing by Transform Mehods: Exension, Unificaion and Error Conrol. anford Universiy, Working Paper. [8] Perella, G. and uo,.g. (4) Numerical Pricing of Discree Barrier and Lookback Opions via Laplace Transforms. Journal of Compuaional Finance, 8, -37. [9] Zieneb, E. and Rokiah, R.A. (3) olving an Asian Opions PDE via Laplace Transform. cience Asia, 39, hp://dx.doi.org/.36/scienceasia [] himko, D.C. (99) Finance in Coninuous Time. A Primer, olb Publishing. (76c) 85

A New Technique for Solving Black-Scholes Equation for Vanilla Put Options

A New Technique for Solving Black-Scholes Equation for Vanilla Put Options Briish Journal of Mahemaics & Compuer Science 9(6): 483-491, 15, Aricle no.bjmcs.15.19 ISSN: 31-851 SCIENCEDOMAIN inernaional www.sciencedomain.org A New Technique for Solving Blac-Scholes Equaion for

More information

Chapter 2. First Order Scalar Equations

Chapter 2. First Order Scalar Equations Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.

More information

Ann. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL:

Ann. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL: Ann. Func. Anal. 2 2011, no. 2, 34 41 A nnals of F uncional A nalysis ISSN: 2008-8752 elecronic URL: www.emis.de/journals/afa/ CLASSIFICAION OF POSIIVE SOLUIONS OF NONLINEAR SYSEMS OF VOLERRA INEGRAL EQUAIONS

More information

10. State Space Methods

10. State Space Methods . Sae Space Mehods. Inroducion Sae space modelling was briefly inroduced in chaper. Here more coverage is provided of sae space mehods before some of heir uses in conrol sysem design are covered in he

More information

Sumudu Decomposition Method for Solving Fractional Delay Differential Equations

Sumudu Decomposition Method for Solving Fractional Delay Differential Equations vol. 1 (2017), Aricle ID 101268, 13 pages doi:10.11131/2017/101268 AgiAl Publishing House hp://www.agialpress.com/ Research Aricle Sumudu Decomposiion Mehod for Solving Fracional Delay Differenial Equaions

More information

An Introduction to Backward Stochastic Differential Equations (BSDEs) PIMS Summer School 2016 in Mathematical Finance.

An Introduction to Backward Stochastic Differential Equations (BSDEs) PIMS Summer School 2016 in Mathematical Finance. 1 An Inroducion o Backward Sochasic Differenial Equaions (BSDEs) PIMS Summer School 2016 in Mahemaical Finance June 25, 2016 Chrisoph Frei cfrei@ualbera.ca This inroducion is based on Touzi [14], Bouchard

More information

Stochastic Model for Cancer Cell Growth through Single Forward Mutation

Stochastic Model for Cancer Cell Growth through Single Forward Mutation Journal of Modern Applied Saisical Mehods Volume 16 Issue 1 Aricle 31 5-1-2017 Sochasic Model for Cancer Cell Growh hrough Single Forward Muaion Jayabharahiraj Jayabalan Pondicherry Universiy, jayabharahi8@gmail.com

More information

Fractional Method of Characteristics for Fractional Partial Differential Equations

Fractional Method of Characteristics for Fractional Partial Differential Equations Fracional Mehod of Characerisics for Fracional Parial Differenial Equaions Guo-cheng Wu* Modern Teile Insiue, Donghua Universiy, 188 Yan-an ilu Road, Shanghai 51, PR China Absrac The mehod of characerisics

More information

Chulhan Bae and Doobae Jun

Chulhan Bae and Doobae Jun Korean J. Mah. 5 07 No. pp. 9 46 hps://doi.org/0.568/kjm.07.5..9 ANALYIC SOLUIONS FOR AMERICAN PARIAL ARRIER OPIONS Y EXPONENIAL ARRIERS Chulhan ae and Doobae Jun Absrac. his paper concerns barrier opion

More information

On the Fourier Transform for Heat Equation

On the Fourier Transform for Heat Equation Applied Mahemaical Sciences, Vol. 8, 24, no. 82, 463-467 HIKARI Ld, www.m-hikari.com hp://dx.doi.org/.2988/ams.24.45355 On he Fourier Transform for Hea Equaion P. Haarsa and S. Poha 2 Deparmen of Mahemaics,

More information

E β t log (C t ) + M t M t 1. = Y t + B t 1 P t. B t 0 (3) v t = P tc t M t Question 1. Find the FOC s for an optimum in the agent s problem.

E β t log (C t ) + M t M t 1. = Y t + B t 1 P t. B t 0 (3) v t = P tc t M t Question 1. Find the FOC s for an optimum in the agent s problem. Noes, M. Krause.. Problem Se 9: Exercise on FTPL Same model as in paper and lecure, only ha one-period govenmen bonds are replaced by consols, which are bonds ha pay one dollar forever. I has curren marke

More information

FINM 6900 Finance Theory

FINM 6900 Finance Theory FINM 6900 Finance Theory Universiy of Queensland Lecure Noe 4 The Lucas Model 1. Inroducion In his lecure we consider a simple endowmen economy in which an unspecified number of raional invesors rade asses

More information

arxiv: v1 [math.ca] 15 Nov 2016

arxiv: v1 [math.ca] 15 Nov 2016 arxiv:6.599v [mah.ca] 5 Nov 26 Counerexamples on Jumarie s hree basic fracional calculus formulae for non-differeniable coninuous funcions Cheng-shi Liu Deparmen of Mahemaics Norheas Peroleum Universiy

More information

On the Separation Theorem of Stochastic Systems in the Case Of Continuous Observation Channels with Memory

On the Separation Theorem of Stochastic Systems in the Case Of Continuous Observation Channels with Memory Journal of Physics: Conference eries PAPER OPEN ACCE On he eparaion heorem of ochasic ysems in he Case Of Coninuous Observaion Channels wih Memory o cie his aricle: V Rozhova e al 15 J. Phys.: Conf. er.

More information

Differential Equations

Differential Equations Mah 21 (Fall 29) Differenial Equaions Soluion #3 1. Find he paricular soluion of he following differenial equaion by variaion of parameer (a) y + y = csc (b) 2 y + y y = ln, > Soluion: (a) The corresponding

More information

6.2 Transforms of Derivatives and Integrals.

6.2 Transforms of Derivatives and Integrals. SEC. 6.2 Transforms of Derivaives and Inegrals. ODEs 2 3 33 39 23. Change of scale. If l( f ()) F(s) and c is any 33 45 APPLICATION OF s-shifting posiive consan, show ha l( f (c)) F(s>c)>c (Hin: In Probs.

More information

ENGI 9420 Engineering Analysis Assignment 2 Solutions

ENGI 9420 Engineering Analysis Assignment 2 Solutions ENGI 940 Engineering Analysis Assignmen Soluions 0 Fall [Second order ODEs, Laplace ransforms; Secions.0-.09]. Use Laplace ransforms o solve he iniial value problem [0] dy y, y( 0) 4 d + [This was Quesion

More information

Cash Flow Valuation Mode Lin Discrete Time

Cash Flow Valuation Mode Lin Discrete Time IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728,p-ISSN: 2319-765X, 6, Issue 6 (May. - Jun. 2013), PP 35-41 Cash Flow Valuaion Mode Lin Discree Time Olayiwola. M. A. and Oni, N. O. Deparmen of Mahemaics

More information

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes Represening Periodic Funcions by Fourier Series 3. Inroducion In his Secion we show how a periodic funcion can be expressed as a series of sines and cosines. We begin by obaining some sandard inegrals

More information

LAPLACE TRANSFORM AND TRANSFER FUNCTION

LAPLACE TRANSFORM AND TRANSFER FUNCTION CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION Professor Dae Ryook Yang Spring 2018 Dep. of Chemical and Biological Engineering 5-1 Road Map of he Lecure V Laplace Transform and Transfer funcions

More information

IMPACT OF AN OBLIQUE BREAKING WAVE ON A WALL

IMPACT OF AN OBLIQUE BREAKING WAVE ON A WALL Source: Physics of Fluids Vol 6 No pp 6-64 4 DOI: 6/64445 IMPACT OF AN OIQUE REAKING WAVE ON A WA Jian-Jun SHU School of Mechanical & Aerospace Engineering Nanyang Technological Universiy 5 Nanyang Avenue

More information

ADVANCED MATHEMATICS FOR ECONOMICS /2013 Sheet 3: Di erential equations

ADVANCED MATHEMATICS FOR ECONOMICS /2013 Sheet 3: Di erential equations ADVANCED MATHEMATICS FOR ECONOMICS - /3 Shee 3: Di erenial equaions Check ha x() =± p ln(c( + )), where C is a posiive consan, is soluion of he ODE x () = Solve he following di erenial equaions: (a) x

More information

The Optimal Stopping Time for Selling an Asset When It Is Uncertain Whether the Price Process Is Increasing or Decreasing When the Horizon Is Infinite

The Optimal Stopping Time for Selling an Asset When It Is Uncertain Whether the Price Process Is Increasing or Decreasing When the Horizon Is Infinite American Journal of Operaions Research, 08, 8, 8-9 hp://wwwscirporg/journal/ajor ISSN Online: 60-8849 ISSN Prin: 60-8830 The Opimal Sopping Time for Selling an Asse When I Is Uncerain Wheher he Price Process

More information

MATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence

MATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence MATH 433/533, Fourier Analysis Secion 6, Proof of Fourier s Theorem for Poinwise Convergence Firs, some commens abou inegraing periodic funcions. If g is a periodic funcion, g(x + ) g(x) for all real x,

More information

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales Advances in Dynamical Sysems and Applicaions. ISSN 0973-5321 Volume 1 Number 1 (2006, pp. 103 112 c Research India Publicaions hp://www.ripublicaion.com/adsa.hm The Asympoic Behavior of Nonoscillaory Soluions

More information

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients Secion 3.5 Nonhomogeneous Equaions; Mehod of Undeermined Coefficiens Key Terms/Ideas: Linear Differenial operaor Nonlinear operaor Second order homogeneous DE Second order nonhomogeneous DE Soluion o homogeneous

More information

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes Half-Range Series 2.5 Inroducion In his Secion we address he following problem: Can we find a Fourier series expansion of a funcion defined over a finie inerval? Of course we recognise ha such a funcion

More information

EXERCISES FOR SECTION 1.5

EXERCISES FOR SECTION 1.5 1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler

More information

A Note on the Equivalence of Fractional Relaxation Equations to Differential Equations with Varying Coefficients

A Note on the Equivalence of Fractional Relaxation Equations to Differential Equations with Varying Coefficients mahemaics Aricle A Noe on he Equivalence of Fracional Relaxaion Equaions o Differenial Equaions wih Varying Coefficiens Francesco Mainardi Deparmen of Physics and Asronomy, Universiy of Bologna, and he

More information

On the Solutions of First and Second Order Nonlinear Initial Value Problems

On the Solutions of First and Second Order Nonlinear Initial Value Problems Proceedings of he World Congress on Engineering 13 Vol I, WCE 13, July 3-5, 13, London, U.K. On he Soluions of Firs and Second Order Nonlinear Iniial Value Problems Sia Charkri Absrac In his paper, we

More information

An Introduction to Malliavin calculus and its applications

An Introduction to Malliavin calculus and its applications An Inroducion o Malliavin calculus and is applicaions Lecure 5: Smoohness of he densiy and Hörmander s heorem David Nualar Deparmen of Mahemaics Kansas Universiy Universiy of Wyoming Summer School 214

More information

2. Nonlinear Conservation Law Equations

2. Nonlinear Conservation Law Equations . Nonlinear Conservaion Law Equaions One of he clear lessons learned over recen years in sudying nonlinear parial differenial equaions is ha i is generally no wise o ry o aack a general class of nonlinear

More information

Undetermined coefficients for local fractional differential equations

Undetermined coefficients for local fractional differential equations Available online a www.isr-publicaions.com/jmcs J. Mah. Compuer Sci. 16 (2016), 140 146 Research Aricle Undeermined coefficiens for local fracional differenial equaions Roshdi Khalil a,, Mohammed Al Horani

More information

Class Meeting # 10: Introduction to the Wave Equation

Class Meeting # 10: Introduction to the Wave Equation MATH 8.5 COURSE NOTES - CLASS MEETING # 0 8.5 Inroducion o PDEs, Fall 0 Professor: Jared Speck Class Meeing # 0: Inroducion o he Wave Equaion. Wha is he wave equaion? The sandard wave equaion for a funcion

More information

ME 391 Mechanical Engineering Analysis

ME 391 Mechanical Engineering Analysis Fall 04 ME 39 Mechanical Engineering Analsis Eam # Soluions Direcions: Open noes (including course web posings). No books, compuers, or phones. An calculaor is fair game. Problem Deermine he posiion of

More information

Lecture #31, 32: The Ornstein-Uhlenbeck Process as a Model of Volatility

Lecture #31, 32: The Ornstein-Uhlenbeck Process as a Model of Volatility Saisics 441 (Fall 214) November 19, 21, 214 Prof Michael Kozdron Lecure #31, 32: The Ornsein-Uhlenbeck Process as a Model of Volailiy The Ornsein-Uhlenbeck process is a di usion process ha was inroduced

More information

CHAPTER 2 Signals And Spectra

CHAPTER 2 Signals And Spectra CHAPER Signals And Specra Properies of Signals and Noise In communicaion sysems he received waveform is usually caegorized ino he desired par conaining he informaion, and he undesired par. he desired par

More information

On the Integro-Differential Equation with a Bulge Function by Using Laplace Transform

On the Integro-Differential Equation with a Bulge Function by Using Laplace Transform Applied Mahemaical Sciences, Vol. 9, 15, no. 5, 9-34 HIKARI Ld, www.m-hikari.com hp://dx.doi.org/1.1988/ams.15.411931 On he Inegro-Differenial Equaion wih a Bulge Funcion by Using Laplace Transform P.

More information

Solutions to Assignment 1

Solutions to Assignment 1 MA 2326 Differenial Equaions Insrucor: Peronela Radu Friday, February 8, 203 Soluions o Assignmen. Find he general soluions of he following ODEs: (a) 2 x = an x Soluion: I is a separable equaion as we

More information

u(x) = e x 2 y + 2 ) Integrate and solve for x (1 + x)y + y = cos x Answer: Divide both sides by 1 + x and solve for y. y = x y + cos x

u(x) = e x 2 y + 2 ) Integrate and solve for x (1 + x)y + y = cos x Answer: Divide both sides by 1 + x and solve for y. y = x y + cos x . 1 Mah 211 Homework #3 February 2, 2001 2.4.3. y + (2/x)y = (cos x)/x 2 Answer: Compare y + (2/x) y = (cos x)/x 2 wih y = a(x)x + f(x)and noe ha a(x) = 2/x. Consequenly, an inegraing facor is found wih

More information

Problem Set on Differential Equations

Problem Set on Differential Equations Problem Se on Differenial Equaions 1. Solve he following differenial equaions (a) x () = e x (), x () = 3/ 4. (b) x () = e x (), x (1) =. (c) xe () = + (1 x ()) e, x () =.. (An asse marke model). Le p()

More information

Application of a Stochastic-Fuzzy Approach to Modeling Optimal Discrete Time Dynamical Systems by Using Large Scale Data Processing

Application of a Stochastic-Fuzzy Approach to Modeling Optimal Discrete Time Dynamical Systems by Using Large Scale Data Processing Applicaion of a Sochasic-Fuzzy Approach o Modeling Opimal Discree Time Dynamical Sysems by Using Large Scale Daa Processing AA WALASZE-BABISZEWSA Deparmen of Compuer Engineering Opole Universiy of Technology

More information

Lecture 10: The Poincaré Inequality in Euclidean space

Lecture 10: The Poincaré Inequality in Euclidean space Deparmens of Mahemaics Monana Sae Universiy Fall 215 Prof. Kevin Wildrick n inroducion o non-smooh analysis and geomery Lecure 1: The Poincaré Inequaliy in Euclidean space 1. Wha is he Poincaré inequaliy?

More information

Utility maximization in incomplete markets

Utility maximization in incomplete markets Uiliy maximizaion in incomplee markes Marcel Ladkau 27.1.29 Conens 1 Inroducion and general seings 2 1.1 Marke model....................................... 2 1.2 Trading sraegy.....................................

More information

Math 334 Test 1 KEY Spring 2010 Section: 001. Instructor: Scott Glasgow Dates: May 10 and 11.

Math 334 Test 1 KEY Spring 2010 Section: 001. Instructor: Scott Glasgow Dates: May 10 and 11. 1 Mah 334 Tes 1 KEY Spring 21 Secion: 1 Insrucor: Sco Glasgow Daes: Ma 1 and 11. Do NOT wrie on his problem saemen bookle, excep for our indicaion of following he honor code jus below. No credi will be

More information

Properties Of Solutions To A Generalized Liénard Equation With Forcing Term

Properties Of Solutions To A Generalized Liénard Equation With Forcing Term Applied Mahemaics E-Noes, 8(28), 4-44 c ISSN 67-25 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Properies Of Soluions To A Generalized Liénard Equaion Wih Forcing Term Allan Kroopnick

More information

t 2 B F x,t n dsdt t u x,t dxdt

t 2 B F x,t n dsdt t u x,t dxdt Evoluion Equaions For 0, fixed, le U U0, where U denoes a bounded open se in R n.suppose ha U is filled wih a maerial in which a conaminan is being ranspored by various means including diffusion and convecion.

More information

Solution of Integro-Differential Equations by Using ELzaki Transform

Solution of Integro-Differential Equations by Using ELzaki Transform Global Journal of Mahemaical Sciences: Theory and Pracical. Volume, Number (), pp. - Inernaional Research Publicaion House hp://www.irphouse.com Soluion of Inegro-Differenial Equaions by Using ELzaki Transform

More information

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t... Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger

More information

On Volterra Integral Equations of the First Kind with a Bulge Function by Using Laplace Transform

On Volterra Integral Equations of the First Kind with a Bulge Function by Using Laplace Transform Applied Mahemaical Sciences, Vol. 9, 15, no., 51-56 HIKARI Ld, www.m-hikari.com hp://dx.doi.org/1.1988/ams.15.41196 On Volerra Inegral Equaions of he Firs Kind wih a Bulge Funcion by Using Laplace Transform

More information

Matrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality

Matrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality Marix Versions of Some Refinemens of he Arihmeic-Geomeric Mean Inequaliy Bao Qi Feng and Andrew Tonge Absrac. We esablish marix versions of refinemens due o Alzer ], Carwrigh and Field 4], and Mercer 5]

More information

On a Fractional Stochastic Landau-Ginzburg Equation

On a Fractional Stochastic Landau-Ginzburg Equation Applied Mahemaical Sciences, Vol. 4, 1, no. 7, 317-35 On a Fracional Sochasic Landau-Ginzburg Equaion Nguyen Tien Dung Deparmen of Mahemaics, FPT Universiy 15B Pham Hung Sree, Hanoi, Vienam dungn@fp.edu.vn

More information

Continuous Time. Time-Domain System Analysis. Impulse Response. Impulse Response. Impulse Response. Impulse Response. ( t) + b 0.

Continuous Time. Time-Domain System Analysis. Impulse Response. Impulse Response. Impulse Response. Impulse Response. ( t) + b 0. Time-Domain Sysem Analysis Coninuous Time. J. Robers - All Righs Reserved. Edied by Dr. Rober Akl 1. J. Robers - All Righs Reserved. Edied by Dr. Rober Akl 2 Le a sysem be described by a 2 y ( ) + a 1

More information

Generalized Chebyshev polynomials

Generalized Chebyshev polynomials Generalized Chebyshev polynomials Clemene Cesarano Faculy of Engineering, Inernaional Telemaic Universiy UNINETTUNO Corso Viorio Emanuele II, 39 86 Roma, Ialy email: c.cesarano@unineunouniversiy.ne ABSTRACT

More information

arxiv: v1 [math.fa] 9 Dec 2018

arxiv: v1 [math.fa] 9 Dec 2018 AN INVERSE FUNCTION THEOREM CONVERSE arxiv:1812.03561v1 [mah.fa] 9 Dec 2018 JIMMIE LAWSON Absrac. We esablish he following converse of he well-known inverse funcion heorem. Le g : U V and f : V U be inverse

More information

15. Vector Valued Functions

15. Vector Valued Functions 1. Vecor Valued Funcions Up o his poin, we have presened vecors wih consan componens, for example, 1, and,,4. However, we can allow he componens of a vecor o be funcions of a common variable. For example,

More information

AMartingaleApproachforFractionalBrownian Motions and Related Path Dependent PDEs

AMartingaleApproachforFractionalBrownian Motions and Related Path Dependent PDEs AMaringaleApproachforFracionalBrownian Moions and Relaed Pah Dependen PDEs Jianfeng ZHANG Universiy of Souhern California Join work wih Frederi VIENS Mahemaical Finance, Probabiliy, and PDE Conference

More information

Pade and Laguerre Approximations Applied. to the Active Queue Management Model. of Internet Protocol

Pade and Laguerre Approximations Applied. to the Active Queue Management Model. of Internet Protocol Applied Mahemaical Sciences, Vol. 7, 013, no. 16, 663-673 HIKARI Ld, www.m-hikari.com hp://dx.doi.org/10.1988/ams.013.39499 Pade and Laguerre Approximaions Applied o he Acive Queue Managemen Model of Inerne

More information

Some New Uniqueness Results of Solutions to Nonlinear Fractional Integro-Differential Equations

Some New Uniqueness Results of Solutions to Nonlinear Fractional Integro-Differential Equations Annals of Pure and Applied Mahemaics Vol. 6, No. 2, 28, 345-352 ISSN: 2279-87X (P), 2279-888(online) Published on 22 February 28 www.researchmahsci.org DOI: hp://dx.doi.org/.22457/apam.v6n2a Annals of

More information

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728, p-issn: 2319-765X. Volume 1, Issue 6 Ver. II (Nov - Dec. 214), PP 48-54 Variaional Ieraion Mehod for Solving Sysem of Fracional Order Ordinary Differenial

More information

Bifurcation Analysis of a Stage-Structured Prey-Predator System with Discrete and Continuous Delays

Bifurcation Analysis of a Stage-Structured Prey-Predator System with Discrete and Continuous Delays Applied Mahemaics 4 59-64 hp://dx.doi.org/.46/am..4744 Published Online July (hp://www.scirp.org/ournal/am) Bifurcaion Analysis of a Sage-Srucured Prey-Predaor Sysem wih Discree and Coninuous Delays Shunyi

More information

Research Article Existence and Uniqueness of Positive and Nondecreasing Solutions for a Class of Singular Fractional Boundary Value Problems

Research Article Existence and Uniqueness of Positive and Nondecreasing Solutions for a Class of Singular Fractional Boundary Value Problems Hindawi Publishing Corporaion Boundary Value Problems Volume 29, Aricle ID 42131, 1 pages doi:1.1155/29/42131 Research Aricle Exisence and Uniqueness of Posiive and Nondecreasing Soluions for a Class of

More information

Math 333 Problem Set #2 Solution 14 February 2003

Math 333 Problem Set #2 Solution 14 February 2003 Mah 333 Problem Se #2 Soluion 14 February 2003 A1. Solve he iniial value problem dy dx = x2 + e 3x ; 2y 4 y(0) = 1. Soluion: This is separable; we wrie 2y 4 dy = x 2 + e x dx and inegrae o ge The iniial

More information

EXISTENCE OF NON-OSCILLATORY SOLUTIONS TO FIRST-ORDER NEUTRAL DIFFERENTIAL EQUATIONS

EXISTENCE OF NON-OSCILLATORY SOLUTIONS TO FIRST-ORDER NEUTRAL DIFFERENTIAL EQUATIONS Elecronic Journal of Differenial Equaions, Vol. 206 (206, No. 39, pp.. ISSN: 072-669. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu fp ejde.mah.xsae.edu EXISTENCE OF NON-OSCILLATORY SOLUTIONS TO

More information

Chapter 14 Wiener Processes and Itô s Lemma. Options, Futures, and Other Derivatives, 9th Edition, Copyright John C. Hull

Chapter 14 Wiener Processes and Itô s Lemma. Options, Futures, and Other Derivatives, 9th Edition, Copyright John C. Hull Chaper 14 Wiener Processes and Iô s Lemma Copyrigh John C. Hull 014 1 Sochasic Processes! Describes he way in which a variable such as a sock price, exchange rae or ineres rae changes hrough ime! Incorporaes

More information

On Option Pricing by Quantum Mechanics Approach

On Option Pricing by Quantum Mechanics Approach On Opion Pricing by Quanum Mechanics Approach Hiroshi Inoue School of Managemen okyo Universiy of Science Kuki, Saiama 46-851 Japan e-mail:inoue@mskukiusacp Absrac We discuss he pah inegral mehodology

More information

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,

More information

On Gronwall s Type Integral Inequalities with Singular Kernels

On Gronwall s Type Integral Inequalities with Singular Kernels Filoma 31:4 (217), 141 149 DOI 1.2298/FIL17441A Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma On Gronwall s Type Inegral Inequaliies

More information

18.03SC Unit 3 Practice Exam and Solutions

18.03SC Unit 3 Practice Exam and Solutions Sudy Guide on Sep, Dela, Convoluion, Laplace You can hink of he ep funcion u() a any nice mooh funcion which i for < a and for > a, where a i a poiive number which i much maller han any ime cale we care

More information

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson PROCEEDINGS OF THE FOURTH INTERNATIONAL CONFERENCE ON DYNAMICAL SYSTEMS AND DIFFERENTIAL EQUATIONS May 4 7, 00, Wilmingon, NC, USA pp 0 Oscillaion of an Euler Cauchy Dynamic Equaion S Huff, G Olumolode,

More information

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is UNIT IMPULSE RESPONSE, UNIT STEP RESPONSE, STABILITY. Uni impulse funcion (Dirac dela funcion, dela funcion) rigorously defined is no sricly a funcion, bu disribuion (or measure), precise reamen requires

More information

On the Timing Option in a Futures Contract

On the Timing Option in a Futures Contract On he Timing Opion in a Fuures Conrac Francesca Biagini, Mahemaics Insiue Universiy of Munich Theresiensr. 39 D-80333 Munich, Germany phone: +39-051-2094459 Francesca.Biagini@mahemaik.uni-muenchen.de Tomas

More information

Math Final Exam Solutions

Math Final Exam Solutions Mah 246 - Final Exam Soluions Friday, July h, 204 () Find explici soluions and give he inerval of definiion o he following iniial value problems (a) ( + 2 )y + 2y = e, y(0) = 0 Soluion: In normal form,

More information

4.6 One Dimensional Kinematics and Integration

4.6 One Dimensional Kinematics and Integration 4.6 One Dimensional Kinemaics and Inegraion When he acceleraion a( of an objec is a non-consan funcion of ime, we would like o deermine he ime dependence of he posiion funcion x( and he x -componen of

More information

1. Consider a pure-exchange economy with stochastic endowments. The state of the economy

1. Consider a pure-exchange economy with stochastic endowments. The state of the economy Answer 4 of he following 5 quesions. 1. Consider a pure-exchange economy wih sochasic endowmens. The sae of he economy in period, 0,1,..., is he hisory of evens s ( s0, s1,..., s ). The iniial sae is given.

More information

Ordinary Differential Equations

Ordinary Differential Equations Lecure 22 Ordinary Differenial Equaions Course Coordinaor: Dr. Suresh A. Karha, Associae Professor, Deparmen of Civil Engineering, IIT Guwahai. In naure, mos of he phenomena ha can be mahemaically described

More information

Chapter 8 The Complete Response of RL and RC Circuits

Chapter 8 The Complete Response of RL and RC Circuits Chaper 8 The Complee Response of RL and RC Circuis Seoul Naional Universiy Deparmen of Elecrical and Compuer Engineering Wha is Firs Order Circuis? Circuis ha conain only one inducor or only one capacior

More information

Improved Approximate Solutions for Nonlinear Evolutions Equations in Mathematical Physics Using the Reduced Differential Transform Method

Improved Approximate Solutions for Nonlinear Evolutions Equations in Mathematical Physics Using the Reduced Differential Transform Method Journal of Applied Mahemaics & Bioinformaics, vol., no., 01, 1-14 ISSN: 179-660 (prin), 179-699 (online) Scienpress Ld, 01 Improved Approimae Soluions for Nonlinear Evoluions Equaions in Mahemaical Physics

More information

A Sharp Existence and Uniqueness Theorem for Linear Fuchsian Partial Differential Equations

A Sharp Existence and Uniqueness Theorem for Linear Fuchsian Partial Differential Equations A Sharp Exisence and Uniqueness Theorem for Linear Fuchsian Parial Differenial Equaions Jose Ernie C. LOPE Absrac This paper considers he equaion Pu = f, where P is he linear Fuchsian parial differenial

More information

( ) 2. Review Exercise 2. cos θ 2 3 = = 2 tan. cos. 2 x = = x a. Since π π, = 2. sin = = 2+ = = cotx. 2 sin θ 2+

( ) 2. Review Exercise 2. cos θ 2 3 = = 2 tan. cos. 2 x = = x a. Since π π, = 2. sin = = 2+ = = cotx. 2 sin θ 2+ Review Eercise sin 5 cos sin an cos 5 5 an 5 9 co 0 a sinθ 6 + 4 6 + sin θ 4 6+ + 6 + 4 cos θ sin θ + 4 4 sin θ + an θ cos θ ( ) + + + + Since π π, < θ < anθ should be negaive. anθ ( + ) Pearson Educaion

More information

Appendix 14.1 The optimal control problem and its solution using

Appendix 14.1 The optimal control problem and its solution using 1 Appendix 14.1 he opimal conrol problem and is soluion using he maximum principle NOE: Many occurrences of f, x, u, and in his file (in equaions or as whole words in ex) are purposefully in bold in order

More information

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3 and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or

More information

Monotonic Solutions of a Class of Quadratic Singular Integral Equations of Volterra type

Monotonic Solutions of a Class of Quadratic Singular Integral Equations of Volterra type In. J. Conemp. Mah. Sci., Vol. 2, 27, no. 2, 89-2 Monoonic Soluions of a Class of Quadraic Singular Inegral Equaions of Volerra ype Mahmoud M. El Borai Deparmen of Mahemaics, Faculy of Science, Alexandria

More information

Numerical Approximation of Partial Differential Equations Arising in Financial Option Pricing

Numerical Approximation of Partial Differential Equations Arising in Financial Option Pricing Numerical Approximaion of Parial Differenial Equaions Arising in Financial Opion Pricing Fernando Gonçalves Docor of Philosophy Universiy of Edinburgh 27 (revised version) To Sílvia, my wife. Declaraion

More information

Variation of Parameters for Causal Operator Differential Equations

Variation of Parameters for Causal Operator Differential Equations Applied Mahemaics, 217, 8, 1883-192 hp://wwwscirporg/journal/am ISSN Online: 2152-7393 ISSN Prin: 2152-7385 Variaion of Parameers for Causal Operaor Differenial Equaions Reza R Ahangar Mahemaics Deparmen,

More information

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Simulaion-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Week Descripion Reading Maerial 2 Compuer Simulaion of Dynamic Models Finie Difference, coninuous saes, discree ime Simple Mehods Euler Trapezoid

More information

Vehicle Arrival Models : Headway

Vehicle Arrival Models : Headway Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where

More information

11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu

11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu ON EQUATIONS WITH SETS AS UNKNOWNS BY PAUL ERDŐS AND S. ULAM DEPARTMENT OF MATHEMATICS, UNIVERSITY OF COLORADO, BOULDER Communicaed May 27, 1968 We shall presen here a number of resuls in se heory concerning

More information

CONTRIBUTION TO IMPULSIVE EQUATIONS

CONTRIBUTION TO IMPULSIVE EQUATIONS European Scienific Journal Sepember 214 /SPECIAL/ ediion Vol.3 ISSN: 1857 7881 (Prin) e - ISSN 1857-7431 CONTRIBUTION TO IMPULSIVE EQUATIONS Berrabah Faima Zohra, MA Universiy of sidi bel abbes/ Algeria

More information

On some Properties of Conjugate Fourier-Stieltjes Series

On some Properties of Conjugate Fourier-Stieltjes Series Bullein of TICMI ol. 8, No., 24, 22 29 On some Properies of Conjugae Fourier-Sieljes Series Shalva Zviadadze I. Javakhishvili Tbilisi Sae Universiy, 3 Universiy S., 86, Tbilisi, Georgia (Received January

More information

IMPROVED HYPERBOLIC FUNCTION METHOD AND EXACT SOLUTIONS FOR VARIABLE COEFFICIENT BENJAMIN-BONA-MAHONY-BURGERS EQUATION

IMPROVED HYPERBOLIC FUNCTION METHOD AND EXACT SOLUTIONS FOR VARIABLE COEFFICIENT BENJAMIN-BONA-MAHONY-BURGERS EQUATION THERMAL SCIENCE, Year 015, Vol. 19, No. 4, pp. 1183-1187 1183 IMPROVED HYPERBOLIC FUNCTION METHOD AND EXACT SOLUTIONS FOR VARIABLE COEFFICIENT BENJAMIN-BONA-MAHONY-BURGERS EQUATION by Hong-Cai MA a,b*,

More information

CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR

CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR Annales Academiæ Scieniarum Fennicæ Mahemaica Volumen 31, 2006, 39 46 CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR Joaquim Marín and Javier

More information

(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4)

(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4) Phase Plane Analysis of Linear Sysems Adaped from Applied Nonlinear Conrol by Sloine and Li The general form of a linear second-order sysem is a c b d From and b bc d a Differeniaion of and hen subsiuion

More information

Intermediate Differential Equations Review and Basic Ideas

Intermediate Differential Equations Review and Basic Ideas Inermediae Differenial Equaions Review and Basic Ideas John A. Burns Cener for Opimal Design And Conrol Inerdisciplinary Cener forappliedmahemaics Virginia Polyechnic Insiue and Sae Universiy Blacksburg,

More information

dy dx = xey (a) y(0) = 2 (b) y(1) = 2.5 SOLUTION: See next page

dy dx = xey (a) y(0) = 2 (b) y(1) = 2.5 SOLUTION: See next page Assignmen 1 MATH 2270 SOLUTION Please wrie ou complee soluions for each of he following 6 problems (one more will sill be added). You may, of course, consul wih your classmaes, he exbook or oher resources,

More information

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems.

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems. Mah 2250-004 Week 4 April 6-20 secions 7.-7.3 firs order sysems of linear differenial equaions; 7.4 mass-spring sysems. Mon Apr 6 7.-7.2 Sysems of differenial equaions (7.), and he vecor Calculus we need

More information

6. Stochastic calculus with jump processes

6. Stochastic calculus with jump processes A) Trading sraegies (1/3) Marke wih d asses S = (S 1,, S d ) A rading sraegy can be modelled wih a vecor φ describing he quaniies invesed in each asse a each insan : φ = (φ 1,, φ d ) The value a of a porfolio

More information

Fractional Laplace Transform and Fractional Calculus

Fractional Laplace Transform and Fractional Calculus Inernaional Mahemaical Forum, Vol. 12, 217, no. 2, 991-1 HIKARI Ld, www.m-hikari.com hps://doi.org/1.12988/imf.217.71194 Fracional Laplace Transform and Fracional Calculus Gusavo D. Medina 1, Nelson R.

More information

Stochastic Reservoir Systems with Different Assumptions for Storage Losses

Stochastic Reservoir Systems with Different Assumptions for Storage Losses American Journal of Operaions Research, 26, 6, 44-423 hp://www.scirp.org/journal/ajor ISSN Online: 26-8849 ISSN Prin: 26-883 Sochasic Reservoir Ssems wih Differen Assumpions for Sorage Losses Carer Browning,

More information

The Brock-Mirman Stochastic Growth Model

The Brock-Mirman Stochastic Growth Model c December 3, 208, Chrisopher D. Carroll BrockMirman The Brock-Mirman Sochasic Growh Model Brock and Mirman (972) provided he firs opimizing growh model wih unpredicable (sochasic) shocks. The social planner

More information