Application of He's homotopy perturbation method for solving nonlinear wave-like equations with variable coefficients

Size: px
Start display at page:

Download "Application of He's homotopy perturbation method for solving nonlinear wave-like equations with variable coefficients"

Transcription

1 Inrnaional Jornal of Adancs in Alid Mahmaics and Mchanics Volm Iss : Aailabl onlin a IJAAMM ISSN: 47-9 Alicaion of H's homoo rrbaion mhod for soling nonlinar wa-lik qaions wih ariabl cofficins Smi Ga a Dndra Kmar a and Jagd Singh b a Darmn of Mahmaics Jagan Nah Ga Insi of Enginring and Tchnolog Jair- Rajashan India b Darmn of Mahmaics Jagan Nah Unirsi Jair-9 Rajashan India Rcid 7 Ocobr ; Accd in risd rsion Nombr A B S T R A C T In his ar w al homoo rrbaion mhod HPM for soling nonlinar wa-lik qaions wih ariabl cofficins. HPM ilds solion in raid conrgn sris from asil comabl rms and in som cass ilds ac solions in on iraion. Moror his chniq dos no rqir an discrizaion linarizaion or small rrbaions and hrfor rdcs h nmrical comaions o a gra n. Th solion rocdr b HPM is siml highl accra and comars faorabl wih h ac solions obaind arl in h lirar. Th mhodolog rsnd in h ar is sfl for highl nonlinar roblms consising of mor han on diffrnial qaion. Kwords: Homoo rrbaion mhod Nonlinar wa-lik qaions Aroima solions Eac solions Mahmaica. MSC cods: 9B F C IJAAMM Inrodcion Th homoo rrbaion mhod inrodcd b h Chins rsarchr Dr. Ji Han H in 998 has com o b accd as an lgan ool in h hands of rsarchrs looking for siml highl ffci solions o comlicad roblms in man dirs aras of scinc and chnolog. In a sris of ars H 999 has olind and rfind h HPM showing is sflnss b nonlinar diffrnial qaions. As a rl HPM nds o rodc mch mor lgan solions as comard o h ohr coming chniqs sch as homoo analsis mhod HAM rglar rrbaion mhods c. i is no a h cos of accrac. In gnral h solions rodcd b h HPM ar as accra as h solions Corrsonding ahor addrss: dndra.mahs@gmail.com Dndra Kmar

2 Smi Ga al. 66 gin b h ohr aroima mhods. Rcnl H has roidd a highl rliabl accon of h HPM in a monograh H a. Th HPM is in fac a coling of h radiional rrbaion mhod and homoo in oolog H b. Th mhod ilds a r raid conrgnc of h solion sris in mos cass sall onl fw iraions rodc r accra solions. This mhod was alid o fncional ingral qaions Abbasband 7 cold ssm of raciondiffsion qaion Ganji and Sadighi 6 o Hlmholz qaion and fifh-ordr KdV qaion Rafi and Ganji 6 h idmic modl Rafi al. 7 drmining h frqnc-amlid rlaion of a nonlinar oscillaor wih disconini Ozis and Yildirim 7a ralling wa solion of h KdV qaion Ozis and Yildirim 7b. Momani and Odiba 7 and Odiba and Momani 8 sggsd a modifid HPM and sd i for nonlinar arial diffrnial qaions of fracional ordr and qadraic Riccai diffrnial qaion of fracional ordr. I was alid o h hin film flow of a forh grad flid down an inclind lan Siddiq al. 6 o h nonlinar Volra-Frdholm ingral qaion Ghasmi al. 7 o h singlar VIE of scond ordr Chn and Jiang o h linar rogramming roblm alid in oimizaion chniqs in arios indsris Mhrabinzhad and Sabri-Nadjafi o h amromric nzmaic racion modl alid in nclar chmisr Shanmgarajan al. o coninos olaion modls for singl and inrsing scis in Economics Pamk and Pamk o im-dndn fncional diffrnial qaions Ga al. o fracional gas dnamics qaion Singh al. and o fracional ha and wa-lik qaions Singh and Kmar. As i is said in Blndz al. 9a h sd of nonlinar roblm is of crcial imoranc no onl in all aras of hsics b also in nginring and ohr discilins sinc mos hnomna in or world ar ssniall nonlinar and ar dscribd b h nonlinar qaions. I is r imoran o sol nonlinar roblm and in gnral i is ofn mor difficl o g an analic aroimaion han a nmrical on for h gin nonlinar roblm. Blndz al. 9a 9b did a good insigaion on his mhod. Th ahors of Blndz al. 9b mlod homoo rrbaion mhod o obain highr-ordr analical aroimaions o h riodic solions o a nonlinar oscillaor wih disconiniis for which h lasic rsoring forc is an anismmric and consan forc. Eclln agrmn bwn aroima riods and h ac on has bn dmonsrad and discssd. Th HPM is modifid in Blndz al. 7 b rncaing h infini sris corrsonding o h firs ordr aroimaions bfor inrodcing his solion in h scondordr linar diffrnial qaion and so on. Th fond ha h modifid mhod works wll for h whol rang of iniial amlids and h clln agrmn of h aroimaion frqncis and riodic solions wih h ac ons has bn dmonsrad and discssd. Onl on iraion lads o high accrac of h solion wih a minimal rlai rror. In his ar w considr h following nonlinar wa-lik qaions n F k m n Fij i j X G i X G k m ij i i i j i i i H X S X wih h iniial condiions In. J. of Ad. in Al. Mah and Mch. : 6-79.

3 67 Alicaion of H s Homoo Prrbaion Mhod X a X X a X. Hr X n and F ij G i ar nonlinar fncion of X and. F ij Gi ar nonlinar fncion of driais of. Whil H S ar nonlinar fncions and i j k m ar ingrs. Ths s of qaions ar of considrabl significanc in arios filds of alid scincs mahmaical hsics nonlinar hdrodnamics nginring hsics biohsics hman momn scincs asrohsics and lasma hsics. Ths qaions dscrib h olion of sochasic ssms. For aml h dscrib h rraic moions of small aricls ha ar immrsd in flids flcaions of h innsi of lasr ligh loci disribions of flid aricls in rbln flows and h sochasic bhaior of chang ras. Ghorishi al. ha sold his of qaion b Adomain Dcomosiion mhod ADM o aoid nralisic assmions in calclaing h Adomain olnomials. ADM is h mos ransarn mhod for solions of h nonlinar roblms; howr his mhod is inold in h calclaion of comlicad Adomain olnomials which narrows down is alicaions. To orcom his disadanag of h ADM w considr h HPM o sol arios nonlinar wa-lik qaions of ariabl cofficins. Homoo rrbaion mhod HPM To illsra h basic idas of h HPM w considr h following diffrnial qaion H 999 A f r r Ω wih h bondar condiion B n r Γ whr A is a gnral diffrnial oraor B is a bondar oraor f r is a nknown analic fncion Γ is h bondar of h domain Ω. Th oraor A can b diidd ino wo ars L and N whr L is linar and N is nonlinar Eq. hrfor can b wrin as follows L N f r. 4 B h homoo chniq w consrc h homoo ν r : Ω [] R which saisf H [ L L ] [ A f r] [] or H L L L [ N f r] [] 6 whr [ ] is an mbdding aramr is an iniial aroimaion of Eq. which saisf h bondar condiions. In. J. of Ad. in Al. Mah and Mch. : 6-79.

4 Smi Ga al. 68 A and h following qaion can b dformd as H L L 7 and H A f r. 8 Now h Eq. can b wrin as owr sris of :. 9 Sing rsls in aroima solion of Eq. :. Th abo solion is conrgs if N L. Alicaions In his scion w al HPM for hr amls and comard or solion wih ADM. Th n rrors bwn ac solion and homoo solion ar dnod b ϕ ac n φ i i whr φ n ar h aroima solions obaind b h HPM. Eaml.. Considr h following wo dimnsional nonlinar wa-lik qaion wih ariabl cofficins Ghorishi al.. wih h iniial condiions Th ac solion is gin b cos sin. According o h HPM l s considr h following homoo. H 4 Now b HPM w ha In. J. of Ad. in Al. Mah and Mch. : 6-79.

5 Alicaion of H s Homoo Prrbaion Mhod In. J. of Ad. in Al. Mah and Mch. : Using Eq. in Eq. 4 and comaring h cofficins of arios owrs of w g : : 6 : and so on. Soling abo diffrnial qaions ndr h iniial condiions m ν m for m w g and so on. Thrfor h aroima solion is gin b which conrgs o h ac solion and sam as obaind b ADM Ghorishi al..

6 Smi Ga al. In. J. of Ad. in Al. Mah and Mch. : Eaml.. Considr h following nonlinar wa-lik qaion wih ariabl cofficins Ghorishi al wih h iniial condiions. Th ac solion is gin b. According o h HPM considr h following homoo H. 8 Now b HPM w ha. Using Eq. in Eq. and comaring h cofficins of arios owrs of w finds : 8 : : ]. 8 Soling abo diffrnial qaions w g

7 7 Alicaion of H s Homoo Prrbaion Mhod and so on. Thrfor h aroima solion is gin b which is h ac solion and is sam as obaind b ADM Ghorishi al.. Eaml.. Considr h following nonlinar wa-lik qaion wih ariabl cofficins Ghorishi al.. < < > 6 wih h iniial condiions. 7 Th ac solion of Eq. 6 is gin b sin. According o h HPM firs w consrc h homoo in h following form H. 8 Now b HPM w ha. 9 In. J. of Ad. in Al. Mah and Mch. : 6-79.

8 Smi Ga al. 7 Using Eq. 9 in Eq. 8 and comaring h cofficins of arios owrs of w finds ha h following Eq. 8 is dcomosd in o infini no of linar arial diffrnial qaions soling hs qaions ndr h iniial condiions w g!! and so on. 7 7! Thrfor h aroima solion is gin b 7 sin!! 7! which is an ac solion and is sam as obaind b ADM Ghorishi al.. 4 Tabls Tabl : Th following abl shows absol rrorϕ 7 for ariabls and aris from. o. for Eaml E- 9.6E-.E-8.89E-7.686E-6.6E-.9866E-.8666E E-7.966E E-.66E-.689E E-7.86E E 9.6E-.E-8.44E-7.86E-6 In. J. of Ad. in Al. Mah and Mch. : 6-79.

9 7 Alicaion of H s Homoo Prrbaion Mhod Tabl : Th following abl shows absol rror ϕ 8 for ariabl and aris from. o. for Eaml E-.764E-.647E-8.689E-7.984E E-.6E E E E E E-.689E E-7.96E-6.986E- 9.86E- 8.E E E-6 Tabl : Th following abl shows absol rror ϕ for ariabl and aris from. o. for Eaml E E E-7.686E-....9E E E-7.6E-7 Figrs HPM Eac Figr : Comarison of ac solion and HPM solion of Eaml. a. In. J. of Ad. in Al. Mah and Mch. : 6-79.

10 Smi Ga al HPM Eac. 4 6 Figr : Comarison of ac solion and HPM solion of Eaml HPM Eac Figr : Comarison of ac solion and HPM solion of Eaml...E- 9.E-6 8.E-6 7.E-6 6.E-6.E-6 4.E-6.E-6.E-6.E-6.E..7.9 Figr 4: Errors of Eaml. form arios als of o a. In. J. of Ad. in Al. Mah and Mch. : 6-79.

11 7 Alicaion of H s Homoo Prrbaion Mhod.E- 8.E-6 6.E-6 4.E-6.E-6.E Figr : Errors of Eaml. from arios als of o Figr 6: Eac solion grah of Eaml. for o Figr 7: Aroima solion grah of Eaml. o fifh aroimaion for o. In. J. of Ad. in Al. Mah and Mch. : 6-79.

12 Smi Ga al Figr 8: Eac solion grah of Eaml. for o Figr 9: Aroima solion grah of Eaml. o fifh aroimaion for o Figr : Aroima solion grah of Eaml. o fifh aroimaion for o. In. J. of Ad. in Al. Mah and Mch. : 6-79.

13 77 Alicaion of H s Homoo Prrbaion Mhod -.. Figr : Aroima solion grah of Eaml. o fifh aroimaion for o. 6 Conclsions In his ar h HPM has bn sccssfll mlod o obain h aroima analical solions of h nonlinar wa-lik qaions wih ariabl cofficins. In Eamls - w obsr ha HPM solions ar mor accra han h ADM. Figs. o show ha h solions obaind b HPM ar mch closr o h ac solion for arios als of im aramr. Tabl o dnos h lss rror for h solion obaind b HPM and ac solion. HPM aoids h difficlis arising in finding h Adomain olnomials. In addiion h calclaions inold in HPM ar r siml and sraigh forward. I is shown ha h HPM is a romising ool for boh linar and nonlinar arial diffrnial qaions. Mahmaica. has bn sd for nmrical comaions in his ar. Rfrncs Abbasband S. 7: Alicaion of H's homoo rrbaion mhod o fncional ingral qaions. Chaos Solions Fracals Blndz A. Pascal C. Orno M. Gallgo S. and Ni C. 7: Alicaion of modifid H's homoo rrbaion mhod o obain highr ordr aroimaions of a forc nonlinar oscillaor. Phsics Lrs A Blndz A. Pascal C. Blndz T. and Hrnandz A. 9a: Solion for an anismmric qadraic nonlinar oscillaor b a modifid H's homoo rrbaion mhod. Nonlinar Analsis RWA Blndz A. Pascal C. Orno M. Blndz T. and Gallgo S. 9b: Alicaion of modifid H's homoo rrbaion mhod o obain highr ordr aroimaions o a nonlinar oscillaor wih disconiniis. Nonlinar Analsis RWA Chn Z. and Jiang W. : Picwis homoo rrbaion mhod for soling linar and nonlinar wakl singlar VIE of scond ordr. Alid Mahmaics and Comaion In. J. of Ad. in Al. Mah and Mch. : 6-79.

14 Smi Ga al. 78 Ganji D. D. and Sadighi A. 6: Alicaion of H's homoo rrbaion mhod o nonlinar cold ssm of racion-diffsion qaions. Inrnaional Jornal of Nonlinar Scincs and Nmrical Simlaion Ghasmi M. Taassoli M. and Babolian E. 7: Nmrical solions of h nonlinar Volra-Frdholm ingral qaions b sing homoo rrbaion mhod. Alid Mahmaics and Comaion Ghorishi M. Ismail A. I. B. and Ali N. H. M. : Adomain dcomosiion mhod for nonlinar wa-lik qaion wih ariabl cofficins. Alid Mahmaical Scincs Ga S. Singh J. and Kmar D. : Alicaions of homoo rrbaion ransform mhod for soling im-dndn fncional diffrnial qaions. Inrnaional Jornal of Nonlinar Scinc H J. H. 999: Homoo rrbaion chniqs. Comr Mhods in Alid Mchanics and Enginring H J. H. a: A riw on som nw rcnl dlod nonlinar analical chniqs. Inrnaional Jornal of Nonlinar Scincs and Nmrical Simlaion. 7. H J. H. b: A coling of homoo chniq and rrbaion chniq for nonlinar roblms. Inrnaional Jornal of Nonlinar Mchanics H J. H. : Homoo rrbaion mhod: a nw nonlinar analical chniq. Alid Mahmaics and Comaion Mhrabinzhad M. and Sabri-Nadjafi J. : Alicaion of H's homoo rrbaion mhod o linar rogramming roblm Inrnaional Jornal of Comr Mahmaics Momani S. and Odiba Z. 7: Homoo rrbaion mhod for nonlinar arial diffrnial qaions of fracional ordr. Phsics Lrs A Odiba Z. and Momani S. 8: Modifid homoo rrbaion mhod: Alicaion o Riccai diffrnial qaion. Chaos Solions Fracals Ozis T. and Yildirim A. 7a: A comarai sd of H's homoo rrbaion mhod for drmining frqnc-amlid rlaion of a nonlinar oscillaors wih disconini. Inrnaional Jornal of Nonlinar Scinc and Nmrical Simlaion Ozis T. and Yildirim A. 7b: Tralling wa solion of KdV qaion sing H' homoo rrbaion mhod. Inrnaional Jornal of Nonlinar Scinc and Nmrical Simlaion Pamk S. and Pamk N. : H's homoo rrbaion mhod for coninos olaion modl for singl and inracing scis. Comrs and Mahmaics wih Alicaions In. J. of Ad. in Al. Mah and Mch. : 6-79.

15 79 Alicaion of H s Homoo Prrbaion Mhod Rafi M. and Ganji D. D. 6: Elici solions of Hlmholz qaion and fifh-ordr KdV qaion sing homoo rrbaion mhod. Inrnaional Jornal of Nonlinar Scincs and Nmrical Simlaion Rafi M. Ganji D. D. and Daniali D. 7: Solion of idmic modl b homoo rrbaion mhod. Alid Mahmaics and Comaion Shanmgarajan A. Alwaraan S. Somasndaram S. and Lakshmanan R. : Analic solion of amromric nzmaic racion basd on homoo rrbaion mhod. Elcrochimica Aca Siddiq A. M. Mahmood R. and Ghori Q. K. 6: homoo rrbaion mhod for hin film flow of a forh grad flid down an inclind lan. Phsics Lrs A Singh J. Kmar D. and Kilicman A. : Homoo rrbaion mhod for fracional gas dnamics qaion sing smd ransform. Absrac and Alid Analsis Aricl ID ags. Singh J. and Kmar D. : An alicaion of homoo rrbaion ransform mhod o fracional ha and wa-lik qaions. Jornal of Fracional Calcls and Alicaions In. J. of Ad. in Al. Mah and Mch. : 6-79.

Simplified Mathieu s equation with linear friction

Simplified Mathieu s equation with linear friction Simplifid Mahi s qaion wih linar fricion Nicola MARCOV*, *Corrsponding ahor *AEROSPACE Consling, B-dl Ili Mani, Bchars 66, Romania Unirsi of Bchars, Facl of Mahmaics and Compr Scinc, Sr. Acadmii nr. 4,

More information

Feedback Control and Synchronization of Chaos for the Coupled Dynamos Dynamical System *

Feedback Control and Synchronization of Chaos for the Coupled Dynamos Dynamical System * ISSN 746-7659 England UK Jornal of Informaion and Comping Scinc Vol. No. 6 pp. 9- Fdbac Conrol and Snchroniaion of Chaos for h Copld Dnamos Dnamical Ssm * Xdi Wang Liin Tian Shmin Jiang Liqin Y Nonlinar

More information

On the Derivatives of Bessel and Modified Bessel Functions with Respect to the Order and the Argument

On the Derivatives of Bessel and Modified Bessel Functions with Respect to the Order and the Argument Inrnaional Rsarch Journal of Applid Basic Scincs 03 Aailabl onlin a wwwirjabscom ISSN 5-838X / Vol 4 (): 47-433 Scinc Eplorr Publicaions On h Driais of Bssl Modifid Bssl Funcions wih Rspc o h Ordr h Argumn

More information

SIMPLIFIED METHOD ON MATHEMATICAL MODEL OF TRANSONIC AXIAL COMPRESSORS

SIMPLIFIED METHOD ON MATHEMATICAL MODEL OF TRANSONIC AXIAL COMPRESSORS ICAS CONRESS SIMPLIIED MEHOD ON MAHEMAICAL MODEL O RANSONIC AXIAL COMPRESSORS Árád ERESS Ph. D. sdn BDAPES NIERSIY O ECHNOLOY AND ECONOMICS Darmn o Aircra and Shis Kords: CD, rbomachinar, C, C, ini olm

More information

A Mathematical model to Solve Reaction Diffusion Equation using Differential Transformation Method

A Mathematical model to Solve Reaction Diffusion Equation using Differential Transformation Method Inernaional Jornal of Mahemaics Trends and Technology- Volme Isse- A Mahemaical model o Solve Reacion Diffsion Eqaion sing Differenial Transformaion Mehod Rahl Bhadaria # A.K. Singh * D.P Singh # #Deparmen

More information

Elementary Differential Equations and Boundary Value Problems

Elementary Differential Equations and Boundary Value Problems Elmnar Diffrnial Equaions and Boundar Valu Problms Boc. & DiPrima 9 h Ediion Chapr : Firs Ordr Diffrnial Equaions 00600 คณ ตศาสตร ว ศวกรรม สาขาว ชาว ศวกรรมคอมพ วเตอร ป การศ กษา /55 ผศ.ดร.อร ญญา ผศ.ดร.สมศ

More information

Boyce/DiPrima 9 th ed, Ch 2.1: Linear Equations; Method of Integrating Factors

Boyce/DiPrima 9 th ed, Ch 2.1: Linear Equations; Method of Integrating Factors Boc/DiPrima 9 h d, Ch.: Linar Equaions; Mhod of Ingraing Facors Elmnar Diffrnial Equaions and Boundar Valu Problms, 9 h diion, b William E. Boc and Richard C. DiPrima, 009 b John Wil & Sons, Inc. A linar

More information

Ratio-Product Type Exponential Estimator For Estimating Finite Population Mean Using Information On Auxiliary Attribute

Ratio-Product Type Exponential Estimator For Estimating Finite Population Mean Using Information On Auxiliary Attribute Raio-Produc T Exonnial Esimaor For Esimaing Fini Poulaion Man Using Informaion On Auxiliar Aribu Rajsh Singh, Pankaj hauhan, and Nirmala Sawan, School of Saisics, DAVV, Indor (M.P., India (rsinghsa@ahoo.com

More information

A Mixed Formulation Triangular Mindlin Plate Finite Element with Cubic Displacements and Quadratic Moments

A Mixed Formulation Triangular Mindlin Plate Finite Element with Cubic Displacements and Quadratic Moments Rcn Adancs in Enginring Mchanics Srcrs and Urban lanning A Mid Forlaion rianglar Mindlin la Fini Eln ih Cbic isplacns and Qadraic Mons AAM ÓSA VALENIN-VASILE UNGUREANU IOAN LUCIAN CÎRSOLOVEAN MIRCEA HORNEł

More information

SOLITON SOLUTIONS OF NONLINEAR PARTIAL DIFFERENTIAL EQUATIONS OF FRACTIONAL ORDER

SOLITON SOLUTIONS OF NONLINEAR PARTIAL DIFFERENTIAL EQUATIONS OF FRACTIONAL ORDER . Kamran AYUB. Nawab KAN. M Yaqb KAN. Aia RANI. Mhammad ASRAF. Jaria AYUB. Qazi MAMOOD-UL-ASSAN. Madiha AFZAL SOLITON SOLUTIONS OF NONLINEAR PARTIAL DIFFERENTIAL EQUATIONS OF FRACTIONAL ORDER. Dparmn of

More information

Numerical Simulation for the 2-D Heat Equation with Derivative Boundary Conditions

Numerical Simulation for the 2-D Heat Equation with Derivative Boundary Conditions IOSR Joural of Applid Chmisr IOSR-JAC -ISSN: 78-576.Volum 9 Issu 8 Vr. I Aug. 6 PP 4-8 www.iosrjourals.org Numrical Simulaio for h - Ha Equaio wih rivaiv Boudar Codiios Ima. I. Gorial parm of Mahmaics

More information

Homotopy Perturbation Method for Solving Partial Differential Equations

Homotopy Perturbation Method for Solving Partial Differential Equations Inernaional OPEN ACCESS Jornal Of Modern Engineering Research (IJMER) Homooy Perrbaion Mehod for Solving Parial Differenial Eqaions R. Ashokan, M. Syed Ibrahim, L. Rajendran,* Dearmen of Mahemaics, Madrai

More information

On the Speed of Heat Wave. Mihály Makai

On the Speed of Heat Wave. Mihály Makai On h Spd of Ha Wa Mihály Maai maai@ra.bm.hu Conns Formulaion of h problm: infini spd? Local hrmal qulibrium (LTE hypohsis Balanc quaion Phnomnological balanc Spd of ha wa Applicaion in plasma ranspor 1.

More information

a dt a dt a dt dt If 1, then the poles in the transfer function are complex conjugates. Let s look at f t H t f s / s. So, for a 2 nd order system:

a dt a dt a dt dt If 1, then the poles in the transfer function are complex conjugates. Let s look at f t H t f s / s. So, for a 2 nd order system: Undrdamd Sysms Undrdamd Sysms nd Ordr Sysms Ouu modld wih a nd ordr ODE: d y dy a a1 a0 y b f If a 0 0, hn: whr: a d y a1 dy b d y dy y f y f a a a 0 0 0 is h naural riod of oscillaion. is h daming facor.

More information

A Comparison Among Homotopy Perturbation Method And The Decomposition Method With The Variational Iteration Method For Dispersive Equation

A Comparison Among Homotopy Perturbation Method And The Decomposition Method With The Variational Iteration Method For Dispersive Equation Inernaional Jornal of Basic & Applied Sciences IJBAS-IJENS Vol:9 No: A Comparison Among Homoopy Perrbaion Mehod And The Decomposiion Mehod Wih The Variaional Ieraion Mehod For Dispersive Eqaion Hasan BULUT*

More information

3.4 Repeated Roots; Reduction of Order

3.4 Repeated Roots; Reduction of Order 3.4 Rpd Roos; Rducion of Ordr Rcll our nd ordr linr homognous ODE b c 0 whr, b nd c r consns. Assuming n xponnil soluion lds o chrcrisic quion: r r br c 0 Qudric formul or fcoring ilds wo soluions, r &

More information

Exact solitary-wave Special Solutions for the Nonlinear Dispersive K(m,n) Equations by Means of the Homotopy Analysis Method

Exact solitary-wave Special Solutions for the Nonlinear Dispersive K(m,n) Equations by Means of the Homotopy Analysis Method Available a hp://pva.ed/aa Appl. Appl. Mah. ISSN: 93-9466 Special Isse No. (Ags ) pp. 8 93 Applicaions Applied Maheaics: An Inernaional Jornal (AAM) Eac soliary-wave Special Solions for he Nonlinear Dispersive

More information

European and American options with a single payment of dividends. (About formula Roll, Geske & Whaley) Mark Ioffe. Abstract

European and American options with a single payment of dividends. (About formula Roll, Geske & Whaley) Mark Ioffe. Abstract 866 Uni Naions Plaza i 566 Nw Yo NY 7 Phon: + 3 355 Fa: + 4 668 info@gach.com www.gach.com Eoan an Amican oions wih a singl amn of ivins Abo fomla Roll Gs & Whal Ma Ioff Absac Th aicl ovis a ivaion of

More information

Ministry of Education and Science of Ukraine National Technical University Ukraine "Igor Sikorsky Kiev Polytechnic Institute"

Ministry of Education and Science of Ukraine National Technical University Ukraine Igor Sikorsky Kiev Polytechnic Institute Minisry of Educaion and Scinc of Ukrain Naional Tchnical Univrsiy Ukrain "Igor Sikorsky Kiv Polychnic Insiu" OPERATION CALCULATION Didacic marial for a modal rfrnc work on mahmaical analysis for sudns

More information

General Article Application of differential equation in L-R and C-R circuit analysis by classical method. Abstract

General Article Application of differential equation in L-R and C-R circuit analysis by classical method. Abstract Applicaion of Diffrnial... Gnral Aricl Applicaion of diffrnial uaion in - and C- circui analysis by classical mhod. ajndra Prasad gmi curr, Dparmn of Mahmaics, P.N. Campus, Pokhara Email: rajndraprasadrgmi@yahoo.com

More information

Riemann Function and Methods of Group Analysis

Riemann Function and Methods of Group Analysis American Research Jornal of Mahemaics Original Aricle ISSN 378-74X Volme Isse 3 5 Riemann Fncion and Mehods of Grop Analsis Akimov Andre Chernov Igor Abdllina Rfina 3 4533 Serliamak Rssia Lenina sree 47A

More information

Double Slits in Space and Time

Double Slits in Space and Time Doubl Slis in Sac an Tim Gorg Jons As has bn ror rcnly in h mia, a am l by Grhar Paulus has monsra an inrsing chniqu for ionizing argon aoms by using ulra-shor lasr ulss. Each lasr uls is ffcivly on an

More information

Computers and Mathematics with Applications

Computers and Mathematics with Applications Compers and Mahemaics wih Applicaions 59 (00) 80 809 Conens liss available a ScienceDirec Compers and Mahemaics wih Applicaions jornal homepage: www.elsevier.com/locae/camwa Solving fracional bondary vale

More information

Stability Solution of the Nonlinear Schrödinger Equation

Stability Solution of the Nonlinear Schrödinger Equation nrnaional Jornal of Morn Nonlinar Thory an Alicaion, 3,, -9 h://oiorg/36/imna35 Pblish Onlin Jn 3 (h://irorg/ornal/imna) abiliy olion of h Nonlinar chröingr Eqaion Mahi Ab Elm M-Ali Darmn of Mahmaics,

More information

The radiation effect on the unsteady MHD convection flow through a nonuniform horizontal channel

The radiation effect on the unsteady MHD convection flow through a nonuniform horizontal channel Availabl onlin a www.plagiarsarchlibrar.com Plagia Rsarch Librar Advancs in Applid Scinc Rsarch :-8 ISSN: 976-86 CODEN USA: AASRFC h radiaion ffc on h nsad MHD convcion flow hrogh a nonniform horizonal

More information

REPETITION before the exam PART 2, Transform Methods. Laplace transforms: τ dτ. L1. Derive the formulas : L2. Find the Laplace transform F(s) if.

REPETITION before the exam PART 2, Transform Methods. Laplace transforms: τ dτ. L1. Derive the formulas : L2. Find the Laplace transform F(s) if. Tranform Mhod and Calculu of Svral Variabl H7, p Lcurr: Armin Halilovic KTH, Campu Haning E-mail: armin@dkh, wwwdkh/armin REPETITION bfor h am PART, Tranform Mhod Laplac ranform: L Driv h formula : a L[

More information

Lecture 1: Numerical Integration The Trapezoidal and Simpson s Rule

Lecture 1: Numerical Integration The Trapezoidal and Simpson s Rule Lcur : Numrical ngraion Th Trapzoidal and Simpson s Rul A problm Th probabiliy of a normally disribud (man µ and sandard dviaion σ ) vn occurring bwn h valus a and b is B A P( a x b) d () π whr a µ b -

More information

Lecture 4: Laplace Transforms

Lecture 4: Laplace Transforms Lur 4: Lapla Transforms Lapla and rlad ransformaions an b usd o solv diffrnial quaion and o rdu priodi nois in signals and imags. Basially, hy onvr h drivaiv opraions ino mulipliaion, diffrnial quaions

More information

An Indian Journal FULL PAPER. Trade Science Inc. A stage-structured model of a single-species with density-dependent and birth pulses ABSTRACT

An Indian Journal FULL PAPER. Trade Science Inc. A stage-structured model of a single-species with density-dependent and birth pulses ABSTRACT [Typ x] [Typ x] [Typ x] ISSN : 974-7435 Volum 1 Issu 24 BioTchnology 214 An Indian Journal FULL PAPE BTAIJ, 1(24), 214 [15197-1521] A sag-srucurd modl of a singl-spcis wih dnsiy-dpndn and birh pulss LI

More information

Asymptotic Solutions of Fifth Order Critically Damped Nonlinear Systems with Pair Wise Equal Eigenvalues and another is Distinct

Asymptotic Solutions of Fifth Order Critically Damped Nonlinear Systems with Pair Wise Equal Eigenvalues and another is Distinct Qus Journals Journal of Rsarch in Applid Mahmaics Volum ~ Issu (5 pp: -5 ISSN(Onlin : 94-74 ISSN (Prin:94-75 www.usjournals.org Rsarch Papr Asympoic Soluions of Fifh Ordr Criically Dampd Nonlinar Sysms

More information

Boyce/DiPrima 9 th ed, Ch 7.8: Repeated Eigenvalues

Boyce/DiPrima 9 th ed, Ch 7.8: Repeated Eigenvalues Boy/DiPrima 9 h d Ch 7.8: Rpad Eignvalus Elmnary Diffrnial Equaions and Boundary Valu Problms 9 h diion by William E. Boy and Rihard C. DiPrima 9 by John Wily & Sons In. W onsidr again a homognous sysm

More information

Summary Chapter Van der Waals-London Interaction: [1]

Summary Chapter Van der Waals-London Interaction: [1] Smmar hapr 3 In hapr 3 sdid h inracion of aoms in a solid. W larnd ha h inracion consiss of a rplling and an aracing rm. W can ndrsand h cohsi nrg, h mling poin, blk modls from h inracion nrg. W discssd

More information

MEM 355 Performance Enhancement of Dynamical Systems A First Control Problem - Cruise Control

MEM 355 Performance Enhancement of Dynamical Systems A First Control Problem - Cruise Control MEM 355 Prformanc Enhancmn of Dynamical Sysms A Firs Conrol Problm - Cruis Conrol Harry G. Kwany Darmn of Mchanical Enginring & Mchanics Drxl Univrsiy Cruis Conrol ( ) mv = F mg sinθ cv v +.2v= u 9.8θ

More information

Wave Equation (2 Week)

Wave Equation (2 Week) Rfrnc Wav quaion ( Wk 6.5 Tim-armonic filds 7. Ovrviw 7. Plan Wavs in Losslss Mdia 7.3 Plan Wavs in Loss Mdia 7.5 Flow of lcromagnic Powr and h Poning Vcor 7.6 Normal Incidnc of Plan Wavs a Plan Boundaris

More information

PFC Predictive Functional Control

PFC Predictive Functional Control PFC Prdiciv Funcional Conrol Prof. Car d Prada D. of Sm Enginring and Auomaic Conrol Univri of Valladolid, Sain rada@auom.uva. Oulin A iml a oibl Moivaion PFC main ida An inroducor xaml Moivaion Prdiciv

More information

Transfer function and the Laplace transformation

Transfer function and the Laplace transformation Lab No PH-35 Porland Sa Univriy A. La Roa Tranfr funcion and h Laplac ranformaion. INTRODUTION. THE LAPLAE TRANSFORMATION L 3. TRANSFER FUNTIONS 4. ELETRIAL SYSTEMS Analyi of h hr baic paiv lmn R, and

More information

Decline Curves. Exponential decline (constant fractional decline) Harmonic decline, and Hyperbolic decline.

Decline Curves. Exponential decline (constant fractional decline) Harmonic decline, and Hyperbolic decline. Dlin Curvs Dlin Curvs ha lo flow ra vs. im ar h mos ommon ools for forasing roduion and monioring wll rforman in h fild. Ths urvs uikly show by grahi mans whih wlls or filds ar roduing as xd or undr roduing.

More information

Differential Equations

Differential Equations UNIT I Diffrntial Equations.0 INTRODUCTION W li in a world of intrrlatd changing ntitis. Th locit of a falling bod changs with distanc, th position of th arth changs with tim, th ara of a circl changs

More information

First Lecture of Machine Learning. Hung-yi Lee

First Lecture of Machine Learning. Hung-yi Lee Firs Lcur of Machin Larning Hung-yi L Larning o say ys/no Binary Classificaion Larning o say ys/no Sam filring Is an -mail sam or no? Rcommndaion sysms rcommnd h roduc o h cusomr or no? Malwar dcion Is

More information

AR(1) Process. The first-order autoregressive process, AR(1) is. where e t is WN(0, σ 2 )

AR(1) Process. The first-order autoregressive process, AR(1) is. where e t is WN(0, σ 2 ) AR() Procss Th firs-ordr auorgrssiv procss, AR() is whr is WN(0, σ ) Condiional Man and Varianc of AR() Condiional man: Condiional varianc: ) ( ) ( Ω Ω E E ) var( ) ) ( var( ) var( σ Ω Ω Ω Ω E Auocovarianc

More information

Homotopy perturbation technique

Homotopy perturbation technique Comput. Mthods Appl. Mch. Engrg. 178 (1999) 257±262 www.lsvir.com/locat/cma Homotopy prturbation tchniqu Ji-Huan H 1 Shanghai Univrsity, Shanghai Institut of Applid Mathmatics and Mchanics, Shanghai 272,

More information

TMMI37, vt2, Lecture 8; Introductory 2-dimensional elastostatics; cont.

TMMI37, vt2, Lecture 8; Introductory 2-dimensional elastostatics; cont. Lctr 8; ntrodctor 2-dimnsional lastostatics; cont. (modifid 23--3) ntrodctor 2-dimnsional lastostatics; cont. W will now contin or std of 2-dim. lastostatics, and focs on a somwhat mor adancd lmnt thn

More information

On the numerical simulation of population dynamics with density-dependent migrations and the Allee effects

On the numerical simulation of population dynamics with density-dependent migrations and the Allee effects 7 Inernaional Symposim on Nonlinear Dynamics (7 ISND) IOP Pblishing Jornal of Physics: Conference Series 96 (8) 8 doi:88/74-6596/96//8 On he nmerical simlaion of poplaion dynamics wih densiy-dependen migraions

More information

Logistic equation of Human population growth (generalization to the case of reactive environment).

Logistic equation of Human population growth (generalization to the case of reactive environment). Logisic quaion of Human populaion growh gnralizaion o h cas of raciv nvironmn. Srg V. Ershkov Insiu for Tim aur Exploraions M.V. Lomonosov's Moscow Sa Univrsi Lninski gor - Moscow 999 ussia -mail: srgj-rshkov@andx.ru

More information

Charging of capacitor through inductor and resistor

Charging of capacitor through inductor and resistor cur 4&: R circui harging of capacior hrough inducor and rsisor us considr a capacior of capacianc is conncd o a D sourc of.m.f. E hrough a rsisr of rsisanc R, an inducor of inducanc and a y K in sris.

More information

Predictive time optimal algorithm for a third-order dynamical system with delay

Predictive time optimal algorithm for a third-order dynamical system with delay Jornal of Phsics: Confrnc Sris PAPER OPEN ACCESS Prdiciv im opimal algorihm for a hird-ordr dnamical ssm wih dla To ci his aricl: G A Pikina 7 J Phs: Conf Sr 89 78 iw h aricl onlin for pdas and nhancmns

More information

Spring 2006 Process Dynamics, Operations, and Control Lesson 2: Mathematics Review

Spring 2006 Process Dynamics, Operations, and Control Lesson 2: Mathematics Review Spring 6 Procss Dynamics, Opraions, and Conrol.45 Lsson : Mahmaics Rviw. conx and dircion Imagin a sysm ha varis in im; w migh plo is oupu vs. im. A plo migh imply an quaion, and h quaion is usually an

More information

2.1. Differential Equations and Solutions #3, 4, 17, 20, 24, 35

2.1. Differential Equations and Solutions #3, 4, 17, 20, 24, 35 MATH 5 PS # Summr 00.. Diffrnial Equaions and Soluions PS.# Show ha ()C #, 4, 7, 0, 4, 5 ( / ) is a gnral soluion of h diffrnial quaion. Us a compur or calculaor o skch h soluions for h givn valus of h

More information

A STUDY OF MINDLIN PLATE FINITE ELEMENTS

A STUDY OF MINDLIN PLATE FINITE ELEMENTS Th 4h Inrnaional Confrnc Copaional Mchanics and Viral Enginring COMEC - OCTOBER Brasov Roania A STUY OF MINLIN LATE FINITE ELEMENTS Ada osa Hadan Ahd Af Alqaain Univrsi TRANSILVANIA Brasov ROMANIA adadosa@ahooco

More information

BSWithJump Model And Pricing Of Quanto CDS With FX Devaluation Risk

BSWithJump Model And Pricing Of Quanto CDS With FX Devaluation Risk MPRA Mnich Prsonal RPEc Archiv BSWihmp Mol An Pricing Of Qano CDS Wih FX Dvalaion Risk Rachi EL-Mohammai Bank Of Amrical Mrrill Lynch Ocobr 9 Onlin a hps:mpra.b.ni-mnchn.478 MPRA Papr No. 478, pos 8. Novmbr

More information

Chapter 12 Introduction To The Laplace Transform

Chapter 12 Introduction To The Laplace Transform Chapr Inroducion To Th aplac Tranorm Diniion o h aplac Tranorm - Th Sp & Impul uncion aplac Tranorm o pciic uncion 5 Opraional Tranorm Applying h aplac Tranorm 7 Invr Tranorm o Raional uncion 8 Pol and

More information

S.Y. B.Sc. (IT) : Sem. III. Applied Mathematics. Q.1 Attempt the following (any THREE) [15]

S.Y. B.Sc. (IT) : Sem. III. Applied Mathematics. Q.1 Attempt the following (any THREE) [15] S.Y. B.Sc. (IT) : Sm. III Applid Mahmaics Tim : ½ Hrs.] Prlim Qusion Papr Soluion [Marks : 75 Q. Amp h following (an THREE) 3 6 Q.(a) Rduc h mari o normal form and find is rank whr A 3 3 5 3 3 3 6 Ans.:

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

ME 321: FLUID MECHANICS-I

ME 321: FLUID MECHANICS-I 8/7/18 ME 31: FLUID MECHANICS-I Dr. A.B.M. Toiqe Hasan Proessor Dearmen o Mechanical Engineering Bangladesh Uniersi o Engineering & Technolog BUET, Dhaka Lecre-13 8/7/18 Dierenial Analsis o Flid Moion

More information

Problem 2. Describe the following signals in terms of elementary functions (δ, u,r, ) and compute. x(t+2) x(2-t) RT_1[x] -3-2 = 1 2 = 1

Problem 2. Describe the following signals in terms of elementary functions (δ, u,r, ) and compute. x(t+2) x(2-t) RT_1[x] -3-2 = 1 2 = 1 EEE 03, HW NAME: SOLUTIONS Problm. Considr h signal whos graph is shown blow. Skch h following signals:, -, RT [], whr R dnos h rflcion opraion and T 0 dnos shif dlay opraion by 0. - RT_[] - -3 - Problm.

More information

Voltage v(z) ~ E(z)D. We can actually get to this wave behavior by using circuit theory, w/o going into details of the EM fields!

Voltage v(z) ~ E(z)D. We can actually get to this wave behavior by using circuit theory, w/o going into details of the EM fields! Considr a pair of wirs idal wirs ngh >, say, infinily long olag along a cabl can vary! D olag v( E(D W can acually g o his wav bhavior by using circui hory, w/o going ino dails of h EM filds! Thr

More information

EXERCISE - 01 CHECK YOUR GRASP

EXERCISE - 01 CHECK YOUR GRASP DIFFERENTIAL EQUATION EXERCISE - CHECK YOUR GRASP 7. m hn D() m m, D () m m. hn givn D () m m D D D + m m m m m m + m m m m + ( m ) (m ) (m ) (m + ) m,, Hnc numbr of valus of mn will b. n ( ) + c sinc

More information

Stability and Hopf bifurcation for Kaldor-Kalecki model of business cycles with two time delays Xiao-hong Wang 1, Yan-hui Zhai 2, Ka Long 3

Stability and Hopf bifurcation for Kaldor-Kalecki model of business cycles with two time delays Xiao-hong Wang 1, Yan-hui Zhai 2, Ka Long 3 Sabiliy and Hopf bifrcaion for aldor-alcki modl of bsinss cycls wih wo im dlays Xiao-hong Wang an-hi Zhai a Long 3 School of Scinc Tianjin Polychnic Univrsiy Tianjin Absrac Paprs invsiga a aldor-alcki

More information

82A Engineering Mathematics

82A Engineering Mathematics Class Nos 5: Sod Ordr Diffrial Eqaio No Homoos 8A Eiri Mahmais Sod Ordr Liar Diffrial Eqaios Homoos & No Homoos v q Homoos No-homoos q ar iv oios fios o h o irval I Sod Ordr Liar Diffrial Eqaios Homoos

More information

Applied Statistics and Probability for Engineers, 6 th edition October 17, 2016

Applied Statistics and Probability for Engineers, 6 th edition October 17, 2016 Applid Saisics and robabiliy for Enginrs, 6 h diion Ocobr 7, 6 CHATER Scion - -. a d. 679.. b. d. 88 c d d d. 987 d. 98 f d.. Thn, = ln. =. g d.. Thn, = ln.9 =.. -7. a., by symmry. b.. d...6. 7.. c...

More information

, u denotes uxt (,) and u. mean first partial derivatives of u with respect to x and t, respectively. Equation (1.1) can be simply written as

, u denotes uxt (,) and u. mean first partial derivatives of u with respect to x and t, respectively. Equation (1.1) can be simply written as Proceedings of he rd IMT-GT Regional Conference on Mahemaics Saisics and Applicaions Universii Sains Malaysia ANALYSIS ON () + () () = G( ( ) ()) Jessada Tanhanch School of Mahemaics Insie of Science Sranaree

More information

Effect of Chemical Reaction on MHD Free Convection Flow past a Vertical Plate with Variable Temperature and Variable Concentration

Effect of Chemical Reaction on MHD Free Convection Flow past a Vertical Plate with Variable Temperature and Variable Concentration Inrnaional Jornal of inific & Eninrin sarch Volm Iss 9 Spmr- ISSN 9-558 Effc of Chmical acion on HD Fr Convcion Flo pas a Vrical Pla ih Varial mprar and Varial Concnraion Bhan Ch. No dra Kr. Das dra K.

More information

A THREE COMPARTMENT MATHEMATICAL MODEL OF LIVER

A THREE COMPARTMENT MATHEMATICAL MODEL OF LIVER A THREE COPARTENT ATHEATICAL ODEL OF LIVER V. An N. Ch. Paabhi Ramacharyulu Faculy of ahmaics, R D collgs, Hanamonda, Warangal, India Dparmn of ahmaics, Naional Insiu of Tchnology, Warangal, India E-ail:

More information

Why Laplace transforms?

Why Laplace transforms? MAE4 Linar ircui Why Lalac ranform? Firordr R cc v v v KVL S R inananou for ach Subiu lmn rlaion v S Ordinary diffrnial quaion in rm of caacior volag Lalac ranform Solv Invr LT V u, v Ri, i A R V A _ v

More information

DE Dr. M. Sakalli

DE Dr. M. Sakalli DE-0 Dr. M. Sakalli DE 55 M. Sakalli a n n 0 a Lh.: an Linar g Equaions Hr if g 0 homognous non-homognous ohrwis driving b a forc. You know h quaions blow alrad. A linar firs ordr ODE has h gnral form

More information

Let s look again at the first order linear differential equation we are attempting to solve, in its standard form:

Let s look again at the first order linear differential equation we are attempting to solve, in its standard form: Th Ingraing Facor Mhod In h prvious xampls of simpl firs ordr ODEs, w found h soluions by algbraically spara h dpndn variabl- and h indpndn variabl- rms, and wri h wo sids of a givn quaion as drivaivs,

More information

( ) ( ) + = ( ) + ( )

( ) ( ) + = ( ) + ( ) Mah 0 Homwork S 6 Soluions 0 oins. ( ps I ll lav i o you vrify ha h omplimnary soluion is : y ( os( sin ( Th guss for h pariular soluion and is drivaivs ar, +. ( os( sin ( ( os( ( sin ( Y ( D 6B os( +

More information

Chapter 3 Linear Equations of Higher Order (Page # 144)

Chapter 3 Linear Equations of Higher Order (Page # 144) Ma Modr Dirial Equaios Lcur wk 4 Jul 4-8 Dr Firozzama Darm o Mahmaics ad Saisics Arizoa Sa Uivrsi This wk s lcur will covr har ad har 4 Scios 4 har Liar Equaios o Highr Ordr Pag # 44 Scio Iroducio: Scod

More information

A Direct Method for Solving Nonlinear PDEs and. New Exact Solutions for Some Examples

A Direct Method for Solving Nonlinear PDEs and. New Exact Solutions for Some Examples In. J. Conemp. Mah. Sciences, Vol. 6, 011, no. 46, 83-90 A Direc Mehod for Solving Nonlinear PDEs and New Eac Solions for Some Eamples Ameina S. Nseir Jordan Universiy of Science and Technology Deparmen

More information

Applied Mathematics Letters. Oscillation results for fourth-order nonlinear dynamic equations

Applied Mathematics Letters. Oscillation results for fourth-order nonlinear dynamic equations Applied Mahemaics Leers 5 (0) 058 065 Conens liss available a SciVerse ScienceDirec Applied Mahemaics Leers jornal homepage: www.elsevier.com/locae/aml Oscillaion resls for forh-order nonlinear dynamic

More information

7.4 QUANTUM MECHANICAL TREATMENT OF FLUCTUATIONS *

7.4 QUANTUM MECHANICAL TREATMENT OF FLUCTUATIONS * Andri Tokmakoff, MIT Dparmn of Chmisry, 5/19/5 7-11 7.4 QUANTUM MECANICAL TREATMENT OF FLUCTUATIONS * Inroducion and Prviw Now h origin of frquncy flucuaions is inracions of our molcul (or mor approprialy

More information

TIME-SPACE DEPENDENT FRACTIONAL VISCOELASTIC MHD FLUID FLOW AND HEAT TRANSFER OVER ACCELERATING PLATE WITH SLIP BOUNDARY

TIME-SPACE DEPENDENT FRACTIONAL VISCOELASTIC MHD FLUID FLOW AND HEAT TRANSFER OVER ACCELERATING PLATE WITH SLIP BOUNDARY HERMAL SCIENCE: Year 7, Vol., No. A, pp. 7-7 IME-SPACE DEPENDEN FRACIONAL VISCOELASIC MHD FLUID FLOW AND HEA RANSFER OVER ACCELERAING PLAE WIH SLIP BOUNDARY b Shenging CHEN a, Liancn ZHENG a*, Chnri LI

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

1. Inverse Matrix 4[(3 7) (02)] 1[(0 7) (3 2)] Recall that the inverse of A is equal to:

1. Inverse Matrix 4[(3 7) (02)] 1[(0 7) (3 2)] Recall that the inverse of A is equal to: Rfrncs Brnank, B. and I. Mihov (1998). Masuring monary policy, Quarrly Journal of Economics CXIII, 315-34. Blanchard, O. R. Proi (00). An mpirical characrizaion of h dynamic ffcs of changs in govrnmn spnding

More information

surface of a dielectric-metal interface. It is commonly used today for discovering the ways in

surface of a dielectric-metal interface. It is commonly used today for discovering the ways in Surfac plasmon rsonanc is snsitiv mchanism for obsrving slight changs nar th surfac of a dilctric-mtal intrfac. It is commonl usd toda for discovring th was in which protins intract with thir nvironmnt,

More information

C From Faraday's Law, the induced voltage is, C The effect of electromagnetic induction in the coil itself is called selfinduction.

C From Faraday's Law, the induced voltage is, C The effect of electromagnetic induction in the coil itself is called selfinduction. Inducors and Inducanc C For inducors, v() is proporional o h ra of chang of i(). Inducanc (con d) C Th proporionaliy consan is h inducanc, L, wih unis of Hnris. 1 Hnry = 1 Wb / A or 1 V sc / A. C L dpnds

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

Relay Feedback Based Time Domain Modeling of Linear 3-by-3 MIMO System

Relay Feedback Based Time Domain Modeling of Linear 3-by-3 MIMO System Amrican Jornal of Sysms Scinc 0; (): 7- OI: 0.593/j.ajss.000.0 Rlay Fdback Basd im omain Modlin of Linar 3-by-3 MIMO Sysm Sjaha V, Rams C. Panda * armn of Chmical Eninrin, CLRI (CSIR), Adyar, Chnnai, 60000,

More information

Advanced Control Systems Problem Sheet for Part B: Multivariable Systems

Advanced Control Systems Problem Sheet for Part B: Multivariable Systems 436-45 Advanced Conrol Ssems Problem Shee for Par B: Mlivariable Ssems Qesion B 998 Given a lan o be conrolled, which is described b a sae-sace model A B C Oline he rocess b which o wold design a discree

More information

Construction of Analytical Solutions to Fractional Differential Equations Using Homotopy Analysis Method

Construction of Analytical Solutions to Fractional Differential Equations Using Homotopy Analysis Method IAENG Inernaional Journal of Applied Mahemaics, 0:, IJAM_0 01 Consrucion of Analical Soluions o Fracional Differenial Equaions Using Homoop Analsis Mehod Ahmad El-Ajou 1, Zaid Odiba *, Shaher Momani 3,

More information

Estimation of Mean Time between Failures in Two Unit Parallel Repairable System

Estimation of Mean Time between Failures in Two Unit Parallel Repairable System Inrnaional Journal on Rcn Innovaion rnd in Comuing Communicaion ISSN: -869 Volum: Iu: 6 Eimaion of Man im bwn Failur in wo Uni Paralll Rairabl Sym Sma Sahu V.K. Paha Kamal Mha hih Namdo 4 ian Profor D.

More information

Centre for Computational Finance and Economic Agents WP Working Paper Series. Hengxu Wang, John G. O Hara, Nick Constantinou

Centre for Computational Finance and Economic Agents WP Working Paper Series. Hengxu Wang, John G. O Hara, Nick Constantinou Cenre for Compaional Finance and Economic Agens WP67-13 Working Paper Series Hengx Wang, John G. O Hara, Nick Consanino A pah-independen approach o inegraed variance nder he CEV model 13 www.ccfea.ne A

More information

International Conference on Energy and Environmental Protection (ICEEP 2016)

International Conference on Energy and Environmental Protection (ICEEP 2016) Inrnaional Confrnc on Enrgy and Environmnal Procion (ICEEP 6) Discussion abou diffrnial quaion of diffusion y in h Submarin Inducd Polarizaion Elcrical Proscing Wang Yuanshng,a Yan LinBo,b, LU Guiying,,c

More information

Research Article The Intrinsic Structure and Properties of Laplace-Typed Integral Transforms

Research Article The Intrinsic Structure and Properties of Laplace-Typed Integral Transforms Hindawi Mahemaical Problems in Engineering Volme 217, Aricle ID 1762729, 8 pages hps://doi.org/1.1155/217/1762729 Research Aricle The Inrinsic Srcre and Properies of Laplace-Typed Inegral Transforms Hwajoon

More information

DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS. Assoc. Prof. Dr. Burak Kelleci. Spring 2018

DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS. Assoc. Prof. Dr. Burak Kelleci. Spring 2018 DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS Aoc. Prof. Dr. Burak Kllci Spring 08 OUTLINE Th Laplac Tranform Rgion of convrgnc for Laplac ranform Invr Laplac ranform Gomric valuaion

More information

Laplace Transforms recap for ccts

Laplace Transforms recap for ccts Lalac Tranform rca for cc Wha h big ida?. Loo a iniial condiion ron of cc du o caacior volag and inducor currn a im Mh or nodal analyi wih -domain imdanc rianc or admianc conducanc Soluion of ODE drivn

More information

Introduction to Bayesian Estimation. McGill COMP 765 Sept 12 th, 2017

Introduction to Bayesian Estimation. McGill COMP 765 Sept 12 th, 2017 Inrodcion o Baesian Esimaion McGill COM 765 Sep 2 h 207 Where am I? or firs core problem Las class: We can model a robo s moions and he world as spaial qaniies These are no perfec and herefore i is p o

More information

On General Solutions of First-Order Nonlinear Matrix and Scalar Ordinary Differential Equations

On General Solutions of First-Order Nonlinear Matrix and Scalar Ordinary Differential Equations saartvlos mcnirbata rovnuli akadmiis moamb 3 #2 29 BULLTN OF TH ORN NTONL DMY OF SNS vol 3 no 2 29 Mahmaics On nral Soluions of Firs-Ordr Nonlinar Mari and Scalar Ordinary Diffrnial uaions uram L Kharaishvili

More information

Math 3301 Homework Set 6 Solutions 10 Points. = +. The guess for the particular P ( ) ( ) ( ) ( ) ( ) ( ) ( ) cos 2 t : 4D= 2

Math 3301 Homework Set 6 Solutions 10 Points. = +. The guess for the particular P ( ) ( ) ( ) ( ) ( ) ( ) ( ) cos 2 t : 4D= 2 Mah 0 Homwork S 6 Soluions 0 oins. ( ps) I ll lav i o you o vrify ha y os sin = +. Th guss for h pariular soluion and is drivaivs is blow. Noi ha w ndd o add s ono h las wo rms sin hos ar xaly h omplimnary

More information

Solving a System of Nonlinear Functional Equations Using Revised New Iterative Method

Solving a System of Nonlinear Functional Equations Using Revised New Iterative Method Solving a Sysem of Nonlinear Funcional Equaions Using Revised New Ieraive Mehod Sachin Bhalekar and Varsha Dafardar-Gejji Absrac In he presen paper, we presen a modificaion of he New Ieraive Mehod (NIM

More information

RESPONSE OF DUFFING OSCILLATOR UNDER NARROW-BAND RANDOM EXCITATION

RESPONSE OF DUFFING OSCILLATOR UNDER NARROW-BAND RANDOM EXCITATION Th rd Intrnational Confrnc on Comutational Mchanics and Virtual Enginring COMEC 9 9 OCTOBER 9, Brasov, Romania RESPONSE O DUING OSCILLATOR UNDER NARROW-BAND RANDOM EXCITATION Ptr STAN, Mtallurgical High

More information

Method of Moment Area Equations

Method of Moment Area Equations Noe proided b JRR Page-1 Noe proided b JRR Page- Inrodcion ehod of omen rea qaions Perform deformaion analsis of flere-dominaed srcres eams Frames asic ssmpions (on.) No aial deformaion (aiall rigid members)

More information

H is equal to the surface current J S

H is equal to the surface current J S Chapr 6 Rflcion and Transmission of Wavs 6.1 Boundary Condiions A h boundary of wo diffrn mdium, lcromagnic fild hav o saisfy physical condiion, which is drmind by Maxwll s quaion. This is h boundary condiion

More information

Modified Variational Iteration Method for the Solution of nonlinear Partial Differential Equations

Modified Variational Iteration Method for the Solution of nonlinear Partial Differential Equations Iraioal Joral of Sciific & Egirig Rsarch Volm Iss Oc- ISSN 9-558 Modifid Variaioal Iraio Mhod for h Solio of oliar Parial Diffrial Eqaios Olayiwola M O Akipl F O Gbolagad A W Absrac-Th Variaioal Iraio

More information

LaPlace Transform in Circuit Analysis

LaPlace Transform in Circuit Analysis LaPlac Tranform in Circui Analyi Obciv: Calcula h Laplac ranform of common funcion uing h dfiniion and h Laplac ranform abl Laplac-ranform a circui, including componn wih non-zro iniial condiion. Analyz

More information

CSE 245: Computer Aided Circuit Simulation and Verification

CSE 245: Computer Aided Circuit Simulation and Verification CSE 45: Compur Aidd Circui Simulaion and Vrificaion Fall 4, Sp 8 Lcur : Dynamic Linar Sysm Oulin Tim Domain Analysis Sa Equaions RLC Nwork Analysis by Taylor Expansion Impuls Rspons in im domain Frquncy

More information

Phys463.nb Conductivity. Another equivalent definition of the Fermi velocity is

Phys463.nb Conductivity. Another equivalent definition of the Fermi velocity is 39 Anohr quival dfiniion of h Fri vlociy is pf vf (6.4) If h rgy is a quadraic funcion of k H k L, hs wo dfiniions ar idical. If is NOT a quadraic funcion of k (which could happ as will b discussd in h

More information

Mathematical Theory and Modeling ISSN (Paper) ISSN (Online) Vol.2, No.4, 2012

Mathematical Theory and Modeling ISSN (Paper) ISSN (Online) Vol.2, No.4, 2012 Soluion of Telegraph quaion by Modified of Double Sumudu Transform "lzaki Transform" Tarig. M. lzaki * man M. A. Hilal. Mahemaics Deparmen, Faculy of Sciences and Ars-Alkamil, King Abdulaziz Uniersiy,

More information

Instructors Solution for Assignment 3 Chapter 3: Time Domain Analysis of LTIC Systems

Instructors Solution for Assignment 3 Chapter 3: Time Domain Analysis of LTIC Systems Inrucor Soluion for Aignmn Chapr : Tim Domain Anali of LTIC Sm Problm i a 8 x x wih x u,, an Zro-inpu rpon of h m: Th characriic quaion of h LTIC m i i 8, which ha roo a ± j Th zro-inpu rpon i givn b zi

More information

Numerical Solution and Exponential Decay to Von Kármán System with Frictional Damping

Numerical Solution and Exponential Decay to Von Kármán System with Frictional Damping Appl. Mah. Inf. Sci. 8, No. 4, 575-58 (4) 575 Applied Mahemaics & Informaion Sciences An Inernaional Jornal hp://d.doi.org/.785/amis/84 Nmerical Solion and Eponenial Deca o Von Kármán Ssem wih Fricional

More information