On the Frame Properties of System of Exponents with Piecewise Continuous Phase

Size: px
Start display at page:

Download "On the Frame Properties of System of Exponents with Piecewise Continuous Phase"

Transcription

1 Alid Mahmaics h://dxdoiorg/436/am3456 Publishd Oli May 3 (h://wwwscirorg/joural/am) O h Fram Proris of Sysm of Exos wih Picwis Coiuous Phas Sad Mohammadali Farahai Tofig Isa ajafov Isiu of Mahmaics ad Mchaics of ASA Bau Azrbaija ahchiva Sa Uivrsiy ahchiva Azrbaija sadzfarahai@gmailcom ofi-cfov@mailru Rcivd Jauary 4 3; rvisd Aril 3 3; accd Aril 3 Coyrigh 3 Sad Mohammadali Farahai Tofig Isa ajafov This is a o accss aricl disribud udr h Craiv Commos Aribuio Lics which rmis ursricd us disribuio ad rroducio i ay mdium rovidd h origial wor is rorly cid ABSTRACT A doubl sysm of xos wih icwis coiuous comlx-valud cofficis ar cosidrd Udr dfii codiios o h cofficis h fram rory of his sysm i Lbsgu sacs of fucios is ivsigad Such sysms aris i h scral roblms for discoiuous diffrial oraors Kywords: Sysm of Exos; Fram Prory; Prurbaio Iroducio Cosidr h followig sysm of xos i () Z C is a suc of comlx umbrs Z ar igrs Sysms () ar modl os whil sudyig scral roris of diffrial oraors Udr suiabl choic of h boudd variaio fucio o h sgm aa hy ar igfucios of firs du ordr diffrial oraor Du wih a igral d codiio of h form u d a a For his raso may mahmaicias aald o sudy of basis roris of h sysms form () i diffr sacs of fucios If h oraor D is cosidrd i h Lbsgu sac L a a h is aural domai of dfiiio is h Sobolv sac W a a i h sac cosisig of absoluly coiuous o a a fucios whos drivaivs blog o L a a ad h rlaio du Du u () d holds a o all h sgm aa Aarly h firs rsuls for basis roris of h sysms of h form () i h sacs L L C a a blog o h famous mahmaicias Paly P- Wir [] ad Lviso [] I sul his dircio was dvlod i h ivsigaios of may mahmaicias For mor daild iformaio s h moograhs of R Youg [3] A M Sdlsii [4] Ch Hil [5] O Chriss [6] (ad also h ars [7-9]) ad hir rfrcs Thr is also h survy ar [] May roblms of mchaics ad mahmaical hysics rduc o discoiuous diffrial oraors i o h cas wh h domai of dfiiio of a diffrial oraor is o cocd I should b od ha h sysms of h form i (3) Z as has h rrsaio sig (4) aris as ig fucios of aroria diffrial oraors whil solvig may roblms of mchaics ad mahmaical hysics by h mhod of saraio of variabls Th followig sysm is a rivial xaml of h cas udr cosidraio si s cos L J J I is obvious ha s ar h ig fucios of h followig scral roblm Coyrigh 3 SciRs

2 S M FARAHAI T I AJAFOV 849 wih a scrum i boudary codiios u u J J uu u u u u Cocrig hs issus s also h ars [-4] Aohr rmarabl xaml is cosidrd i V A Ili s ar [5] Hr h cosidrs a mixd roblm wih cojugaio codiios a h ir oi x l wih rsc o h wav uaio u axu x x x l T wih codiios xx ux x ul a u x u ux u x x u u x ux x x a x x ax a x x l a a (wav vlociy i mdium) ad (mdium dsiy) ar osiiv cosas a ar Youg moduls wih addiioal codiio of ualiy of assag im of wav h sgms x ad x l : x l x a a Th comlss i L of h sysm of igfucios of a ordiary diffrial oraor ha corrsods o his roblm is sablishd i h ar [6] Th clos class of roblms was arlir cosidrd i h ar [7] Ths xamls vry clarly dmosra xdicy of sudy of fram roris of h sysms form (3) Th rs ar is dvod o ivsigaio of fram rory of sysm (3) i L L Prviously som rsuls of his ar wr aoucd wihou roof i [8] This wor is srucurd as follows I Scio w rs dful iformaio ad facs from h horis of bass ad clos bass ha will b usd o obai our mai rsuls This scio also coais h mai assumios abou h fucios ad which aar i formula (4) I Scio 3 w sa mai rsuls o h basiciy of h rurbd sysm of xos (3) i Lbsgu sacs L cssary Iformaio ad Mai Assumios I sul w will d h followig oio ad facs from h hory of bass ad frams W will us h sadard oaio will b h s of all osiiv igrs; will ma hr xis(s) ; will ma i follows ; will ma if ad oly if ;! will ma hr xiss uiu ; K R or K C will sad for h s of ral or comlx umbrs rscivly; is Krocrs symbol Th Baach sac will b calld a B-sac X is a sac cojuga o sac X By LM w do h liar sa of h s M X ad M will sad for h closur of M Dfiiio Sysm x X is said o b a ba- sis for X if x X! Dfiiio Sysm x l i X if K : x x X is said o b com- L x X I is calld miimal i X if x L x Dfiiio 3 Sysm x X is calld -li- arly idd i B -sac X if from ax imlis a I holds h followig Lmma L X b a B-sac wih h basis x ad F : X X b a Frdholm oraor Th h followig roris of h sysm y Fx i X ar uival: is coml; ) y ) y 3) y 4) y is miimal; is -liarly idd; a basis isomorhic o x W will d h followig oios Dfiiio 4 Th sysms x ad y i a B-sac X wih h orm ar said o b -clos if x y Dfiiio 5 Th miimal sysm x X i a B-sac X wih cojugad x X is said o b a x X : xx l l is a -sysm if for ordiary sac of sucs a of scalars wih h orm a a l I h cas of basiciy such a sysm will b calld a -basis Th followig lmma is also valid Lmma L X b a B-sac wih -basis x ad h sysm y X b -clos o i: Coyrigh 3 SciRs

3 85 S M FARAHAI T I AJAFOV Th h xrssio Fx x xy g- ras a Frdholm oraor i X x X is a sysm cojugad o x O ca s hs or ohr facs i h moograhs [39] ad also i h a rs [7-] W will d h followig Kri-Milma-Ruma s Thorm [] Thorm KMR X b a B-sac wih h orm ad wih h ormd basis x x X b a sysm biorhogoal o i If h sysm y X saisfis h codiio x y su x h i for rhic o ms a basis isomo x for X Whil obaiig h basic rsul w will us h fol- lowig asily rovabl lmma Lmma 3 L X b a B-sac wih h basis x ad x X b a sysm biorhogoal o x Th sysm y X diffr from x by a fiily may lms i y x Th if d x y h sysm y is o miimal i X Proof So X b a B-sac wih h basis x ad y X diffr from x by fiily ma y l ms i y x Exad y by his basis y y a x y (5) a x L A firs assum ha Th i is o bvious ha a As a rsul i follows from xrssio (5) ha y blogs o h c losur of h liar sa x ad so h sys m y is o miimal Cosidr h cas i y a x a x y y a x a x y (6) aa aa I is obvious ha if a a for or h h sysm y is o miimal Ohrwis xcludig x i (6) w hav: a y a y x a y a y a y ay a y ay a y ay I dircly follows from hs rlaios ha y y blogs o h closur of liar sa of h rmaiig lms y i is o mii- y Coyrigh 3 SciRs y mal i X Cosuly for h sysm y dos form a basis This rasoig is a o a arbirary v ry asily ڤ Bfor rocdig h mai rsuls w acc h followig basic assumios cocrig h fucios of ad ) is a icwis-holdr fucio o r : r r ar is discoiuiy ois of firs id; Do h jums of h fucio a h ois r r by : L h codiio ) Z r b fulfilld 3) Th fucios hav h followig asymoic rlaios O (7) 3 Basic Rsuls A firs w cosidr h sysm of xos i Z (8) sig Z For h basiciy of sysm (8) i L h rsuls of h ar [3] will b usd Rrs sysm (8) i h form i i i i ; Z (9) ( Z ar o-gaiv igrs) L h codiio ) b r fulfilld Fidig i Z from h followig i- ualiis : assum i i i i r () r () Basd o Thorm of h ar [3] w ca dircly coclud h followig Sam L h codiios ) ) b fu lfilld for h fucio Suos ha Th sysm (9) forms a basis for L (for = a Risz ba- sis) if ad oly if i holds h iualiy W will us h followig sam obaiig from h rsuls of h ar [4] Sam If sysm (9) forms a basis for L

4 S M FARAHAI T I AJAFOV 85 h i is isomorhic o h classic sysm of i xos Z So l sysm (8) form a basis for L Do by L a sysm biorhogoal o i L Z f L a d b is biorhogoal cofficis by f Z sysm (8) i f f d Z is comlx cojugaio Th followig horm ca b dircly coclud d from Sam Thorm L sysm (8) forms a basis for L Th hr hold: ) L ad f L Th f l ad Z f m f Z l is fulfilld m is a cosa id d of f is a ordiary orm i L ) L ad h suc of umbrs a Z blog o l Th f L such ha f a Z morovr f M f M is a cosa Z l idd of f Z ow sudy h basiciy of sysm (3) i L W hav i i i M! c! c is a cosa idd of Th las iualiy follows from (7) Cosidr h diffr cass ) L W hav i i c Assum ha all h codiios of Sam ar fulfilld Th sysm (8) forms a basis for L Thus by Sam i forms a -basis for L i his cas L b a sysm biorhogoal o i Cosidr h Z oraor F : L L : i () Ff f f L f f d Z By Lmma oraor () is Frdholm i L I is asy o s ha i i F Z Th h sam of Lmma is valid fo r sysm (3) ) L I is clar ha Cosuly for f L i is valid f c f c dd s o ly o Assum ha all h codi- ios of Sam ar fulfilld Cosuly sysm (8) forms a basis for L I is clar ha f L ad Th from Thorm w obai ha f l Z f ar h orhogoal coffiz cis of f by sysm (8) From h sam ho rm w obai: f m f M f f L Z l h cosa M is idd of f Thus sysm (8) forms a -basis i L I is asy o s ha sysms (3) ad (8) -clos i L Cosidr oraor () Furhr w bhav similarly o cas I Hc h validiy of h followig horm is rovd Thorm L asymoic Formula (4) hold h fucio saisfy h codiios ) ) ad for h fucio h rlaios (7) b valid Assum ha i holds max ; mi is dfid from xrssios () () Th h followig roris for sysm (3) i L ar uival: ) Coml; ) Miimal; 3) -liarly idd; i 4) Forms a basis isomorhic o I sul w will cosidr a cas wh I his cas i is obvious ha i holds Z i i L all h codiios of Thorm b fulfilld Th h i sysm forms a basis for L Do by Z Z L a sysm biorhogoal o i Assum su I is clar ha : i i Cosidr h fucios Thus i holds i i Th as i follows from Thorm KMR h sysm i Z forms a basis isomorhic o i Z for Coyrigh 3 SciRs

5 85 S M FARAHAI T I AJAFOV L Sysm (3) ad h basis i diffr by a fiily may lms By do a biorhogoz al sysm o his basis Cosidr Z i i i a a (3) : I is obvious ha i i a d Z Do by h followig drmia I is clar ha if i lms d a ij i j (4) i h xasio (3) h may b rlacd by h l- i ms i Th h sysm Z forms a basis for L sic f L has h xasio f f i Hc i dircly follows ha if h f L has a xasio by s ysm (3) i i is com l i L Cosidr h oraor Ff f i W hav i i Ff f f i i f f I T f i I : L L is a idiy oraor ad T is a oraor grad by h scod summad Frdholm rory F i L follows from fii-dimsioaliy of h o raor T I is clar ha i i Z F Th from Lmma w obai h basiciy of sysm (3) i L Covrsly if sysm (3) forms a basis for L h as i follo ws from Lmma 3 Thus w sablishd ha udr accd codiios sysm (3) forms a basis for L if h drmia drmid by xrssio (4) is o zro Thus w rovd h followig Thorm 3 L all h codiios of Thorm b fulfilld Th drmia is drmid by xrssio (4) Sysm (3) forms a basis for L if ad oly if ow cosidr h cas wh L for xaml I his cas as i follows from Thorm of h ar [3] h sysm forms a basis for i i Z (5) L Cosidr h sysm i (6) Z L is a fucio L h codiios ) ) b fulfilld for sysm (3) ad max ; Th i is asy o s ha sysm (6) ad basis (5) ar -clos i L is drmid by h formula Cosuly sysm (3) is o coml i L Th rmaiig cass wh ar rovd i h similar way Cosidr a cas wh for xaml I h is cas agai as i follows from Thorm of h ar [3] h sysm i (7) forms a basis for L If h codiios ) ) ar fulfilld i h basis (7) ad h sysm ar -clos i L Cosuly sysm (3) is o miimal i L Th rmaiig cass wh ar rovd similarly Thrfor w obai h followig fial rsul for h basiciy of sysm (3) i L Thorm 4 L asymoic formula (4) hold h fucios ad saisfy h codiios ) ) 3) Th variabl b drmid from rlaios () () ad l max ; Th for sysm (3) is o miimal i L ; for i is o coml i L For ris of sysm (3) i ) Coml; ) Miimal; 3) -liarly idd; ba orhic o 5) h followig ro- L ar uival: i 4) Forms a sis isom ; Z is drmid by xrssio Coyrigh 3 SciRs

6 S M FARAHAI T I AJAFOV 853 (4) Idd uiv alc of roris )-4) follows dircly from Lmma Euivalc of codiios 4) ad 5) is rovd 4 Coclusios Taig io a ccou h obaid rsuls w ca summariz his wor as follows Prurbd sysm of xos h has of which may has diffr asymoic bhavior i diffr ars of h basic irval is sudid i his wor I should b od ha i s robably h firs im h roblm of basiciy is co sidrd for such a sysm Udr crai codiios o h fucios dfiig h has w rov ha his sysm may hav a fii dfc i L Morovr i ihr forms a basis for L or i is o coml ad o miimal i L 5 Acowldgms Th auhors xrss hir ds graiud o Profssor B T Bilalov for his aio ad valuabl guidac o his aricl Aalysis Iogi aui i Thii Srmaya Mamaia i Prilozhiya Tmaichsi Obzory Vol [] L H Lars Iral Wavs Icid uo a Kif Edg Barrir D Sa Rsarch Vol 6 o [] S A Gabov ad P A Kruisii O Lars s osaioary Problm Zhural Vychislil oi Mamaii i Mamaichsoi Fizii Vol 7 o [3] P A Kruisii Small o-saioary Vibraios of Vrical Plas i a Chal wih a Sraifid Fluid USSR Comuaioal Mahmaics ad Mahmaical Physics Vol 8 o [4] E I Moisv ad Abbasi Basis Prory of Eigfucios of h Gralizd Gasdyamic Problm of Fral wih a olocal Oddss Codiio ad wih h Discoiuiy of h Gradi of Soluio Diffrial Euaios Vol 45 o [5] V A Ili Mixd Problm Dscribig h Damig Procss of a Bar Cosisig of Two Scios of Diffr Dsiy ad Elasiciy Providd ha h Tim of Wav s Passag i Each of Ths Scios Coicid Trudi Isiua Mamaii i Mhaii Uro RA Vol [6] I S Lomov o-smooh Eigfucios i Problms of Mahmaical Physics Diffrial Euaios Vol 47 REFERECES o [] R Paly ad Wir F ourir Trasforms i h Com- [7] L M Lujia Rgulariy of Scral Problms wih Adlx Domai Amrica Mahmaical Sociy Provi- diioal Codiios a h Ir Pois Mamaichsdc 934 i Zami Vol 49 o Ga ad Dsiy Thorms Amrica [8] B T Bilalov ad S M Farahai O Prurbd Bass of [] Lviso Mahmaical Sociy Providc 94 Exoial Fucios wih Comlx Cofficis Tras- [3] [4] R M Youg A Iroducio o o-harmoic Fourir Sris Srigr Brli A M Sdlsii Classs of Aalyic Fourir Trasforacios of AS of Azrbaija Vol 56 o [9] I Sigr Bass i Baach Sacs I Srigr Brli maios ad Exoial Aroximaios Fizmali doi:7/ Moscow 5 [] I T Hochbrg ad A S Marus O Sabiliy of Bass [5] Ch Hil A Basis Thory Primr Srigr Brli of Baach ad Hilbr Sacs Izvsiya Aadmii au 534 doi:7/ Moldavsoj SSR o [6] O Chriss A Iroducio o Frams ad Risz [] B T Bilalov ad T R Muradov O Euival Bass bass Srigr Brli 3 44 i Baach Sacs Uraiia Mahmaical Joural Vol [7] D L Russll O Exoial Bass for h Sobolv 59 o Sacs Ovr a Irval Joural of Mahmaical Aadoi:7/s lysis ad Alica ios Vol 87 o [] B T Bilalov Bass from Exos Cosis ad Sis doi:6/-47x(8)94- Big Eig Fucios of Diffrial Oraors Diffrial Euaios Vol 39 o [8] X H ad H Volmr Risz Bass of Soluios of Surm-Liovill Euaios Joural of Fourir Aalysis ad Alicaios Vol 7 o doi:7/bf585 [9] H Milos Ivrs Scral Problms ad Closd Exoial Sysms Aals of Mahmaics Vol 6 o doi:47/aals56885 [] A M Sdlsii oharmoic Aalysis Fucioal [3] B T Bilalov Basiciy of Som Sysms of Exos Cosis ad Sis Diffrial Euaios Vol o 99-6 [4] B T Bilalov O Isomorhism of Two Bass Fudamalaya i Priladaya Mamaia Vol o Coyrigh 3 SciRs

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

Response of LTI Systems to Complex Exponentials

Response of LTI Systems to Complex Exponentials 3 Fourir sris coiuous-im Rspos of LI Sysms o Complx Expoials Ouli Cosidr a LI sysm wih h ui impuls rspos Suppos h ipu sigal is a complx xpoial s x s is a complx umbr, xz zis a complx umbr h or h h w will

More information

What Is the Difference between Gamma and Gaussian Distributions?

What Is the Difference between Gamma and Gaussian Distributions? Applid Mahmaics,,, 85-89 hp://ddoiorg/6/am Publishd Oli Fbruary (hp://wwwscirporg/joural/am) Wha Is h Diffrc bw Gamma ad Gaussia Disribuios? iao-li Hu chool of Elcrical Egirig ad Compur cic, Uivrsiy of

More information

1973 AP Calculus BC: Section I

1973 AP Calculus BC: Section I 97 AP Calculus BC: Scio I 9 Mius No Calculaor No: I his amiaio, l dos h aural logarihm of (ha is, logarihm o h bas ).. If f ( ) =, h f ( ) = ( ). ( ) + d = 7 6. If f( ) = +, h h s of valus for which f

More information

Part B: Transform Methods. Professor E. Ambikairajah UNSW, Australia

Part B: Transform Methods. Professor E. Ambikairajah UNSW, Australia Par B: rasform Mhods Profssor E. Ambikairaah UNSW, Ausralia Chapr : Fourir Rprsaio of Sigal. Fourir Sris. Fourir rasform.3 Ivrs Fourir rasform.4 Propris.4. Frqucy Shif.4. im Shif.4.3 Scalig.4.4 Diffriaio

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

The Development of Suitable and Well-founded Numerical Methods to Solve Systems of Integro- Differential Equations,

The Development of Suitable and Well-founded Numerical Methods to Solve Systems of Integro- Differential Equations, Shiraz Uivrsiy of Tchology From h SlcdWorks of Habibolla Laifizadh Th Dvlopm of Suiabl ad Wll-foudd Numrical Mhods o Solv Sysms of Igro- Diffrial Equaios, Habibolla Laifizadh, Shiraz Uivrsiy of Tchology

More information

UNIT III STANDARD DISTRIBUTIONS

UNIT III STANDARD DISTRIBUTIONS UNIT III STANDARD DISTRIBUTIONS Biomial, Poisso, Normal, Gomric, Uiform, Eoial, Gamma disribuios ad hir roris. Prard by Dr. V. Valliammal Ngaiv biomial disribuios Prard by Dr.A.R.VIJAYALAKSHMI Sadard Disribuios

More information

2 Dirac delta function, modeling of impulse processes. 3 Sine integral function. Exponential integral function

2 Dirac delta function, modeling of impulse processes. 3 Sine integral function. Exponential integral function Chapr VII Spcial Fucios Ocobr 7, 7 479 CHAPTER VII SPECIAL FUNCTIONS Cos: Havisid sp fucio, filr fucio Dirac dla fucio, modlig of impuls procsss 3 Si igral fucio 4 Error fucio 5 Gamma fucio E Epoial igral

More information

Continous system: differential equations

Continous system: differential equations /6/008 Coious sysm: diffrial quaios Drmiisic modls drivaivs isad of (+)-( r( compar ( + ) R( + r ( (0) ( R ( 0 ) ( Dcid wha hav a ffc o h sysm Drmi whhr h paramrs ar posiiv or gaiv, i.. giv growh or rducio

More information

Ring of Large Number Mutually Coupled Oscillators Periodic Solutions

Ring of Large Number Mutually Coupled Oscillators Periodic Solutions Iraioal Joural of horical ad Mahmaical Physics 4, 4(6: 5-9 DOI: 59/jijmp446 Rig of arg Numbr Muually Coupld Oscillaors Priodic Soluios Vasil G Aglov,*, Dafika z Aglova Dparm Nam of Mahmaics, Uivrsiy of

More information

ON H-TRICHOTOMY IN BANACH SPACES

ON H-TRICHOTOMY IN BANACH SPACES CODRUTA STOICA IHAIL EGA O H-TRICHOTOY I BAACH SPACES Absrac: I his papr w mphasiz h oio of skw-oluio smiflows cosidrd a gralizaio of smigroups oluio opraors ad skw-produc smiflows which aris i h sabiliy

More information

Poisson Arrival Process

Poisson Arrival Process 1 Poisso Arrival Procss Arrivals occur i) i a mmorylss mar ii) [ o arrival durig Δ ] = λδ + ( Δ ) P o [ o arrival durig Δ ] = 1 λδ + ( Δ ) P o P j arrivals durig Δ = o Δ for j = 2,3, ( ) o Δ whr lim =

More information

Mixing time with Coupling

Mixing time with Coupling Mixig im wih Couplig Jihui Li Mig Zhg Saisics Dparm May 7 Goal Iroducio o boudig h mixig im for MCMC wih couplig ad pah couplig Prsig a simpl xampl o illusra h basic ida Noaio M is a Markov chai o fii

More information

Fourier Series: main points

Fourier Series: main points BIOEN 3 Lcur 6 Fourir rasforms Novmbr 9, Fourir Sris: mai pois Ifii sum of sis, cosis, or boh + a a cos( + b si( All frqucis ar igr mulipls of a fudamal frqucy, o F.S. ca rprs ay priodic fucio ha w ca

More information

( A) ( B) ( C) ( D) ( E)

( A) ( B) ( C) ( D) ( E) d Smsr Fial Exam Worksh x 5x.( NC)If f ( ) d + 7, h 4 f ( ) d is 9x + x 5 6 ( B) ( C) 0 7 ( E) divrg +. (NC) Th ifii sris ak has h parial sum S ( ) for. k Wha is h sum of h sris a? ( B) 0 ( C) ( E) divrgs

More information

Mathematical Preliminaries for Transforms, Subbands, and Wavelets

Mathematical Preliminaries for Transforms, Subbands, and Wavelets Mahmaical Prlimiaris for rasforms, Subbads, ad Wavls C.M. Liu Prcpual Sigal Procssig Lab Collg of Compur Scic Naioal Chiao-ug Uivrsiy hp://www.csi.cu.du.w/~cmliu/courss/comprssio/ Offic: EC538 (03)5731877

More information

Poisson Arrival Process

Poisson Arrival Process Poisso Arrival Procss Arrivals occur i) i a mmylss mar ii) [ o arrival durig Δ ] = λδ + ( Δ ) P o [ o arrival durig Δ ] = λδ + ( Δ ) P o P j arrivals durig Δ = o Δ f j = 2,3, o Δ whr lim =. Δ Δ C C 2 C

More information

ECEN620: Network Theory Broadband Circuit Design Fall 2014

ECEN620: Network Theory Broadband Circuit Design Fall 2014 ECE60: work Thory Broadbad Circui Dig Fall 04 Lcur 6: PLL Trai Bhavior Sam Palrmo Aalog & Mixd-Sigal Cr Txa A&M Uivriy Aoucm, Agda, & Rfrc HW i du oday by 5PM PLL Trackig Rpo Pha Dcor Modl PLL Hold Rag

More information

Modeling of the CML FD noise-to-jitter conversion as an LPTV process

Modeling of the CML FD noise-to-jitter conversion as an LPTV process Modlig of h CML FD ois-o-ir covrsio as a LPV procss Marko Alksic. Rvisio hisory Vrsio Da Comms. //4 Firs vrsio mrgd wo docums. Cyclosaioary Nois ad Applicaio o CML Frqucy Dividr Jir/Phas Nois Aalysis fil

More information

Fourier Techniques Chapters 2 & 3, Part I

Fourier Techniques Chapters 2 & 3, Part I Fourir chiqus Chaprs & 3, Par I Dr. Yu Q. Shi Dp o Elcrical & Compur Egirig Nw Jrsy Isiu o chology Email: shi@i.du usd or h cours: , 4 h Ediio, Lahi ad Dog, Oord

More information

MA6451-PROBABILITY AND RANDOM PROCESSES

MA6451-PROBABILITY AND RANDOM PROCESSES MA645-PROBABILITY AND RANDOM PROCESSES UNIT I RANDOM VARIABLES Dr. V. Valliammal Darm of Alid Mahmaics Sri Vkaswara Collg of Egirig Radom variabl Radom Variabls A ral variabl whos valu is drmid by h oucom

More information

1.7 Vector Calculus 2 - Integration

1.7 Vector Calculus 2 - Integration cio.7.7 cor alculus - Igraio.7. Ordiary Igrals o a cor A vcor ca b igrad i h ordiary way o roduc aohr vcor or aml 5 5 d 6.7. Li Igrals Discussd hr is h oio o a dii igral ivolvig a vcor ucio ha gras a scalar.

More information

From Fourier Series towards Fourier Transform

From Fourier Series towards Fourier Transform From Fourir Sris owards Fourir rasform D D d D, d wh lim Dparm of Elcrical ad Compur Eiri D, d wh lim L s Cosidr a fucio G d W ca xprss D i rms of Gw D G Dparm of Elcrical ad Compur Eiri D G G 3 Dparm

More information

Thomas J. Osler. 1. INTRODUCTION. This paper gives another proof for the remarkable simple

Thomas J. Osler. 1. INTRODUCTION. This paper gives another proof for the remarkable simple 5/24/5 A PROOF OF THE CONTINUED FRACTION EXPANSION OF / Thomas J Oslr INTRODUCTION This ar givs aothr roof for th rmarkabl siml cotiud fractio = 3 5 / Hr is ay ositiv umbr W us th otatio x= [ a; a, a2,

More information

(A) 1 (B) 1 + (sin 1) (C) 1 (sin 1) (D) (sin 1) 1 (C) and g be the inverse of f. Then the value of g'(0) is. (C) a. dx (a > 0) is

(A) 1 (B) 1 + (sin 1) (C) 1 (sin 1) (D) (sin 1) 1 (C) and g be the inverse of f. Then the value of g'(0) is. (C) a. dx (a > 0) is [STRAIGHT OBJECTIVE TYPE] l Q. Th vlu of h dfii igrl, cos d is + (si ) (si ) (si ) Q. Th vlu of h dfii igrl si d whr [, ] cos cos Q. Vlu of h dfii igrl ( si Q. L f () = d ( ) cos 7 ( ) )d d g b h ivrs

More information

Some Applications of the Poisson Process

Some Applications of the Poisson Process Applid Maaics, 24, 5, 3-37 Publishd Oli Novbr 24 i SciRs. hp://www.scirp.org/oural/a hp://dx.doi.org/.4236/a.24.59288 So Applicaios of Poisso Procss Kug-Ku s Dpar of Maaics, Ka Uivrsiy, Uio, USA Eail:

More information

EEE 303: Signals and Linear Systems

EEE 303: Signals and Linear Systems 33: Sigls d Lir Sysms Orhogoliy bw wo sigls L us pproim fucio f () by fucio () ovr irvl : f ( ) = c( ); h rror i pproimio is, () = f() c () h rgy of rror sigl ovr h irvl [, ] is, { }{ } = f () c () d =

More information

Chapter 11 INTEGRAL EQUATIONS

Chapter 11 INTEGRAL EQUATIONS hapr INTERAL EQUATIONS hapr INTERAL EUATIONS Dcmbr 4, 8 hapr Igral Eqaios. Normd Vcor Spacs. Eclidia vcor spac. Vcor spac o coios cios ( ). Vcor Spac L ( ) 4. achy-byaowsi iqaliy 5. iowsi iqaliy. Liar

More information

Infinite Continued Fraction (CF) representations. of the exponential integral function, Bessel functions and Lommel polynomials

Infinite Continued Fraction (CF) representations. of the exponential integral function, Bessel functions and Lommel polynomials Ifii Coiu Fraio CF rraio of h oial igral fuio l fuio a Lol olyoial Coiu Fraio CF rraio a orhogoal olyoial I hi io w rall h rlaio bw ifi rurry rlaio of olyoial orroig orhogoaliy a aroria ifii oiu fraio

More information

Web-appendix 1: macro to calculate the range of ( ρ, for which R is positive definite

Web-appendix 1: macro to calculate the range of ( ρ, for which R is positive definite Wb-basd Supplmary Marials for Sampl siz cosidraios for GEE aalyss of hr-lvl clusr radomizd rials by Sv Trsra, Big Lu, oh S. Prissr, Tho va Achrbrg, ad Gorg F. Borm Wb-appdix : macro o calcula h rag of

More information

Gauge Theories. Elementary Particle Physics Strong Interaction Fenomenology. Diego Bettoni Academic year

Gauge Theories. Elementary Particle Physics Strong Interaction Fenomenology. Diego Bettoni Academic year Gau Thors Elmary Parcl Physcs Sro Iraco Fomoloy o Bo cadmc yar - Gau Ivarac Gau Ivarac Whr do Laraas or Hamloas com from? How do w kow ha a cra raco should dscrb a acual hyscal sysm? Why s h lcromac raco

More information

Practice papers A and B, produced by Edexcel in 2009, with mark schemes. Practice Paper A. 5 cosh x 2 sinh x = 11,

Practice papers A and B, produced by Edexcel in 2009, with mark schemes. Practice Paper A. 5 cosh x 2 sinh x = 11, Prai paprs A ad B, produd by Edl i 9, wih mark shms Prai Papr A. Fid h valus of for whih 5 osh sih =, givig your aswrs as aural logarihms. (Toal 6 marks) k. A = k, whr k is a ral osa. 9 (a) Fid valus of

More information

ELECTROMAGNETIC COMPATIBILITY HANDBOOK 1. Chapter 12: Spectra of Periodic and Aperiodic Signals

ELECTROMAGNETIC COMPATIBILITY HANDBOOK 1. Chapter 12: Spectra of Periodic and Aperiodic Signals ELECTOMAGNETIC COMPATIBILITY HANDBOOK Chapr : Spcra of Priodic ad Apriodic Sigals. Drmi whhr ach of h followig fucios ar priodic. If hy ar priodic, provid hir fudamal frqucy ad priod. a) x 4cos( 5 ) si(

More information

Boyce/DiPrima 9 th ed, Ch 7.9: Nonhomogeneous Linear Systems

Boyce/DiPrima 9 th ed, Ch 7.9: Nonhomogeneous Linear Systems BoDiPrima 9 h d Ch 7.9: Nohomogou Liar Sm Elmar Diffrial Equaio ad Boudar Valu Prolm 9 h diio William E. Bo ad Rihard C. DiPrima 9 Joh Wil & So I. Th gral hor of a ohomogou m of quaio g g aralll ha of

More information

Advanced Engineering Mathematics, K.A. Stroud, Dexter J. Booth Engineering Mathematics, H.K. Dass Higher Engineering Mathematics, Dr. B.S.

Advanced Engineering Mathematics, K.A. Stroud, Dexter J. Booth Engineering Mathematics, H.K. Dass Higher Engineering Mathematics, Dr. B.S. Rfrc: (i) (ii) (iii) Advcd Egirig Mhmic, K.A. Sroud, Dxr J. Booh Egirig Mhmic, H.K. D Highr Egirig Mhmic, Dr. B.S. Grwl Th mhod of m Thi coi of h followig xm wih h giv coribuio o h ol. () Mid-rm xm : 3%

More information

MAT3700. Tutorial Letter 201/2/2016. Mathematics III (Engineering) Semester 2. Department of Mathematical sciences MAT3700/201/2/2016

MAT3700. Tutorial Letter 201/2/2016. Mathematics III (Engineering) Semester 2. Department of Mathematical sciences MAT3700/201/2/2016 MAT3700/0//06 Tuorial Lr 0//06 Mahmaics III (Egirig) MAT3700 Smsr Dparm of Mahmaical scics This uorial lr coais soluios ad aswrs o assigms. BARCODE CONTENTS Pag SOLUTIONS ASSIGNMENT... 3 SOLUTIONS ASSIGNMENT...

More information

Chapter Five. More Dimensions. is simply the set of all ordered n-tuples of real numbers x = ( x 1

Chapter Five. More Dimensions. is simply the set of all ordered n-tuples of real numbers x = ( x 1 Chatr Fiv Mor Dimsios 51 Th Sac R W ar ow rard to mov o to sacs of dimsio gratr tha thr Ths sacs ar a straightforward gralizatio of our Euclida sac of thr dimsios Lt b a ositiv itgr Th -dimsioal Euclida

More information

Testing Goodness-of-Fit in Autoregressive Fractionally Integrated Moving- Average Models with Conditional Hetroscedastic Errors of Unknown form

Testing Goodness-of-Fit in Autoregressive Fractionally Integrated Moving- Average Models with Conditional Hetroscedastic Errors of Unknown form Rsarch Joural of Rc Scics ISSN 77-5 Vol. (5, 9-4, May ( Rs.J.Rc Sci. Tsig Goodss-of-Fi i Auorgrssiv Fracioally Igrad Movig- Avrag Modls wih Codiioal roscdasic Errors of Uow form Absrac Ali Amad, Salahuddi

More information

Controllability and Observability of Matrix Differential Algebraic Equations

Controllability and Observability of Matrix Differential Algebraic Equations NERNAONAL JOURNAL OF CRCUS, SYSEMS AND SGNAL PROCESSNG Corollabiliy ad Obsrvabiliy of Marix Diffrial Algbrai Equaios Ya Wu Absra Corollabiliy ad obsrvabiliy of a lass of marix Diffrial Algbrai Equaio (DAEs)

More information

Approximation of Functions Belonging to. Lipschitz Class by Triangular Matrix Method. of Fourier Series

Approximation of Functions Belonging to. Lipschitz Class by Triangular Matrix Method. of Fourier Series I Jorl of Mh Alysis, Vol 4, 2, o 2, 4-47 Approximio of Fcios Blogig o Lipschiz Clss by Triglr Mrix Mhod of Forir Sris Shym Ll Dprm of Mhmics Brs Hid Uivrsiy, Brs, Idi shym _ll@rdiffmilcom Biod Prsd Dhl

More information

ECE351: Signals and Systems I. Thinh Nguyen

ECE351: Signals and Systems I. Thinh Nguyen ECE35: Sigals ad Sysms I Thih Nguy FudamalsofSigalsadSysms x Fudamals of Sigals ad Sysms co. Fudamals of Sigals ad Sysms co. x x] Classificaio of sigals Classificaio of sigals co. x] x x] =xt s =x

More information

The geometry of surfaces contact

The geometry of surfaces contact Applid ad ompuaioal Mchaics (007 647-656 h gomry of surfacs coac J. Sigl a * J. Švíglr a a Faculy of Applid Scics UWB i Pils Uivrzií 0 00 Pils zch public civd 0 Spmbr 007; rcivd i rvisd form 0 Ocobr 007

More information

Chapter 7 INTEGRAL EQUATIONS

Chapter 7 INTEGRAL EQUATIONS hapr 7 INTERAL EQUATIONS hapr 7 INTERAL EUATIONS hapr 7 Igral Eqaios 7. Normd Vcor Spacs. Eclidia vcor spac. Vcor spac o coios cios ( ). Vcor Spac L ( ) 4. ach-baowsi iqali 5. iowsi iqali 7. Liar Opraors

More information

Chapter Taylor Theorem Revisited

Chapter Taylor Theorem Revisited Captr 0.07 Taylor Torm Rvisitd Atr radig tis captr, you sould b abl to. udrstad t basics o Taylor s torm,. writ trascdtal ad trigoomtric uctios as Taylor s polyomial,. us Taylor s torm to id t valus o

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

8. Queueing systems. Contents. Simple teletraffic model. Pure queueing system

8. Queueing systems. Contents. Simple teletraffic model. Pure queueing system 8. Quug sysms Cos 8. Quug sysms Rfrshr: Sml lraffc modl Quug dscl M/M/ srvr wag lacs Alcao o ack lvl modllg of daa raffc M/M/ srvrs wag lacs lc8. S-38.45 Iroduco o Tlraffc Thory Srg 5 8. Quug sysms 8.

More information

FIXED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE

FIXED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE Mohia & Samaa, Vol. 1, No. II, December, 016, pp 34-49. ORIGINAL RESEARCH ARTICLE OPEN ACCESS FIED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE 1 Mohia S. *, Samaa T. K. 1 Deparme of Mahemaics, Sudhir Memorial

More information

Adomian Decomposition Method for Dispersion. Phenomena Arising in Longitudinal Dispersion of. Miscible Fluid Flow through Porous Media

Adomian Decomposition Method for Dispersion. Phenomena Arising in Longitudinal Dispersion of. Miscible Fluid Flow through Porous Media dv. Thor. ppl. Mch. Vol. 3 o. 5 - domia Dcomposiio Mhod for Disprsio Phoma risig i ogiudial Disprsio of Miscibl Fluid Flow hrough Porous Mdia Ramakaa Mhr ad M.N. Mha Dparm of Mahmaics S.V. Naioal Isiu

More information

Control Systems. Transient and Steady State Response.

Control Systems. Transient and Steady State Response. Corol Sym Trai a Say Sa Ro chibum@oulch.ac.kr Ouli Tim Domai Aalyi orr ym Ui ro Ui ram ro Ui imul ro Chibum L -Soulch Corol Sym Tim Domai Aalyi Afr h mahmaical mol of h ym i obai, aalyi of ym rformac i.

More information

Linear Systems Analysis in the Time Domain

Linear Systems Analysis in the Time Domain Liar Sysms Aalysis i h Tim Domai Firs Ordr Sysms di vl = L, vr = Ri, d di L + Ri = () d R x= i, x& = x+ ( ) L L X() s I() s = = = U() s E() s Ls+ R R L s + R u () = () =, i() = L i () = R R Firs Ordr Sysms

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

Note 6 Frequency Response

Note 6 Frequency Response No 6 Frqucy Rpo Dparm of Mchaical Egirig, Uivriy Of Sakachwa, 57 Campu Driv, Sakaoo, S S7N 59, Caada Dparm of Mchaical Egirig, Uivriy Of Sakachwa, 57 Campu Driv, Sakaoo, S S7N 59, Caada. alyical Exprio

More information

Discrete Fourier Transform (DFT)

Discrete Fourier Transform (DFT) Discrt Fourir Trasorm DFT Major: All Egirig Majors Authors: Duc guy http://umricalmthods.g.us.du umrical Mthods or STEM udrgraduats 8/3/29 http://umricalmthods.g.us.du Discrt Fourir Trasorm Rcalld th xpotial

More information

Further Results on Pair Sum Graphs

Further Results on Pair Sum Graphs Applid Mathmatis, 0,, 67-75 http://dx.doi.org/0.46/am.0.04 Publishd Oli Marh 0 (http://www.sirp.org/joural/am) Furthr Rsults o Pair Sum Graphs Raja Poraj, Jyaraj Vijaya Xavir Parthipa, Rukhmoi Kala Dpartmt

More information

Comparison between Fourier and Corrected Fourier Series Methods

Comparison between Fourier and Corrected Fourier Series Methods Malaysia Joural of Mahemaical Scieces 7(): 73-8 (13) MALAYSIAN JOURNAL OF MATHEMATICAL SCIENCES Joural homepage: hp://eispem.upm.edu.my/oural Compariso bewee Fourier ad Correced Fourier Series Mehods 1

More information

Common Fixed Point Theorem in Intuitionistic Fuzzy Metric Space via Compatible Mappings of Type (K)

Common Fixed Point Theorem in Intuitionistic Fuzzy Metric Space via Compatible Mappings of Type (K) Ieraioal Joural of ahemaics Treds ad Techology (IJTT) Volume 35 umber 4- July 016 Commo Fixed Poi Theorem i Iuiioisic Fuzzy eric Sace via Comaible aigs of Tye (K) Dr. Ramaa Reddy Assisa Professor De. of

More information

15/03/1439. Lectures on Signals & systems Engineering

15/03/1439. Lectures on Signals & systems Engineering Lcturs o Sigals & syms Egirig Dsigd ad Prd by Dr. Ayma Elshawy Elsfy Dpt. of Syms & Computr Eg. Al-Azhar Uivrsity Email : aymalshawy@yahoo.com A sigal ca b rprd as a liar combiatio of basic sigals. Th

More information

LINEAR 2 nd ORDER DIFFERENTIAL EQUATIONS WITH CONSTANT COEFFICIENTS

LINEAR 2 nd ORDER DIFFERENTIAL EQUATIONS WITH CONSTANT COEFFICIENTS Diol Bgyoko (0) I.INTRODUCTION LINEAR d ORDER DIFFERENTIAL EQUATIONS WITH CONSTANT COEFFICIENTS I. Dfiiio All suh diffril quios s i h sdrd or oil form: y + y + y Q( x) dy d y wih y d y d dx dx whr,, d

More information

3.2. Derivation of Laplace Transforms of Simple Functions

3.2. Derivation of Laplace Transforms of Simple Functions 3. aplac Tarform 3. PE TRNSFORM wid rag of girig ym ar modld mahmaically by uig diffrial quaio. I gral, h diffrial quaio of h ordr ym i wri: d y( a d d d y( dy( a a y( f( (3. d Which i alo ow a a liar

More information

1. Solve by the method of undetermined coefficients and by the method of variation of parameters. (4)

1. Solve by the method of undetermined coefficients and by the method of variation of parameters. (4) 7 Differeial equaios Review Solve by he mehod of udeermied coefficies ad by he mehod of variaio of parameers (4) y y = si Soluio; we firs solve he homogeeous equaio (4) y y = 4 The correspodig characerisic

More information

) and furthermore all X. The definition of the term stationary requires that the distribution fulfills the condition:

) and furthermore all X. The definition of the term stationary requires that the distribution fulfills the condition: Assigm Thomas Aam, Spha Brumm, Haik Lor May 6 h, 3 8 h smsr, 357, 7544, 757 oblm For R b X a raom variabl havig ormal isribuio wih ma µ a variac σ (his is wri as ~ (,) X. by: R a. Is X ) a urhrmor all

More information

(Reference: sections in Silberberg 5 th ed.)

(Reference: sections in Silberberg 5 th ed.) ALE. Atomic Structur Nam HEM K. Marr Tam No. Sctio What is a atom? What is th structur of a atom? Th Modl th structur of a atom (Rfrc: sctios.4 -. i Silbrbrg 5 th d.) Th subatomic articls that chmists

More information

15. Numerical Methods

15. Numerical Methods S K Modal' 5. Numrical Mhod. Th quaio + 4 4 i o b olvd uig h Nwo-Rapho mhod. If i ak a h iiial approimaio of h oluio, h h approimaio uig hi mhod will b [EC: GATE-7].(a (a (b 4 Nwo-Rapho iraio chm i f(

More information

CS 688 Pattern Recognition. Linear Models for Classification

CS 688 Pattern Recognition. Linear Models for Classification //6 S 688 Pr Rcogiio Lir Modls for lssificio Ø Probbilisic griv modls Ø Probbilisic discrimiiv modls Probbilisic Griv Modls Ø W o ur o robbilisic roch o clssificio Ø W ll s ho modls ih lir dcisio boudris

More information

Chapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series

Chapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series Chatr Ifiit Sris Pag of Sctio F Itgral Tst Chatr : Ifiit Sris By th d of this sctio you will b abl to valuat imror itgrals tst a sris for covrgc by alyig th itgral tst aly th itgral tst to rov th -sris

More information

On the Hubbard-Stratonovich Transformation for Interacting Bosons

On the Hubbard-Stratonovich Transformation for Interacting Bosons O h ubbrd-sroovh Trsformo for Irg osos Mr R Zrbur ff Fbrury 8 8 ubbrd-sroovh for frmos: rmdr osos r dffr! Rdom mrs: hyrbol S rsformo md rgorous osus for rg bosos /8 Wyl grou symmry L : G GL V b rrso of

More information

Boyce/DiPrima/Meade 11 th ed, Ch 4.1: Higher Order Linear ODEs: General Theory

Boyce/DiPrima/Meade 11 th ed, Ch 4.1: Higher Order Linear ODEs: General Theory Bo/DiPima/Mad h d Ch.: High Od Lia ODEs: Gal Tho Elma Diffial Eqaios ad Boda Val Poblms h diio b William E. Bo Rihad C. DiPima ad Dog Mad 7 b Joh Wil & Sos I. A h od ODE has h gal fom d d P P P d d W assm

More information

Analysis of TE (Transverse Electric) Modes of Symmetric Slab Waveguide

Analysis of TE (Transverse Electric) Modes of Symmetric Slab Waveguide Adv. Sudis Thor. Phs., Vol. 6,, o. 7, 33-336 Aalsis of T (Trasvrs lcric Mods of Smmric Slab Wavguid arr Rama SPCTC (Spcrum Tcholog Rsarch Group Dparm of lcrical, lcroic ad Ssms girig Naioal Uivrsi of Malasia

More information

Review Topics from Chapter 3&4. Fourier Series Fourier Transform Linear Time Invariant (LTI) Systems Energy-Type Signals Power-Type Signals

Review Topics from Chapter 3&4. Fourier Series Fourier Transform Linear Time Invariant (LTI) Systems Energy-Type Signals Power-Type Signals Rviw opics from Chapr 3&4 Fourir Sris Fourir rasform Liar im Ivaria (LI) Sysms Ergy-yp Sigals Powr-yp Sigals Fourir Sris Rprsaio for Priodic Sigals Dfiiio: L h sigal () b a priodic sigal wih priod. ()

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

Overview. Review Elliptic and Parabolic. Review General and Hyperbolic. Review Multidimensional II. Review Multidimensional

Overview. Review Elliptic and Parabolic. Review General and Hyperbolic. Review Multidimensional II. Review Multidimensional Mlil idd variabls March 9 Mlidisioal Parial Dirial Eaios arr aro Mchaical Egirig 5B iar i Egirig Aalsis March 9 Ovrviw Rviw las class haracrisics ad classiicaio o arial dirial aios Probls i or ha wo idd

More information

DISTRIBUTION OF DIFFERENCE BETWEEN INVERSES OF CONSECUTIVE INTEGERS MODULO P

DISTRIBUTION OF DIFFERENCE BETWEEN INVERSES OF CONSECUTIVE INTEGERS MODULO P DISTRIBUTION OF DIFFERENCE BETWEEN INVERSES OF CONSECUTIVE INTEGERS MODULO P Tsz Ho Chan Dartmnt of Mathmatics, Cas Wstrn Rsrv Univrsity, Clvland, OH 4406, USA txc50@cwru.du Rcivd: /9/03, Rvisd: /9/04,

More information

A Generalization of Hermite Polynomials

A Generalization of Hermite Polynomials Ieraioal Mahemaical Forum, Vol. 8, 213, o. 15, 71-76 HIKARI Ld, www.m-hikari.com A Geeralizaio of Hermie Polyomials G. M. Habibullah Naioal College of Busiess Admiisraio & Ecoomics Gulberg-III, Lahore,

More information

PURE MATHEMATICS A-LEVEL PAPER 1

PURE MATHEMATICS A-LEVEL PAPER 1 -AL P MATH PAPER HONG KONG EXAMINATIONS AUTHORITY HONG KONG ADVANCED LEVEL EXAMINATION PURE MATHEMATICS A-LEVEL PAPER 8 am am ( hours) This papr must b aswrd i Eglish This papr cosists of Sctio A ad Sctio

More information

ISSN: [Bellale* et al., 6(1): January, 2017] Impact Factor: 4.116

ISSN: [Bellale* et al., 6(1): January, 2017] Impact Factor: 4.116 IESRT INTERNTIONL OURNL OF ENGINEERING SCIENCES & RESERCH TECHNOLOGY HYBRID FIED POINT THEOREM FOR NONLINER DIFFERENTIL EQUTIONS Sidhshwar Sagram Bllal*, Gash Babrwa Dapk * Dparm o Mahmaics, Daaad Scic

More information

Available online at J. Math. Comput. Sci. 4 (2014), No. 4, ISSN:

Available online at   J. Math. Comput. Sci. 4 (2014), No. 4, ISSN: Available olie a hp://sci.org J. Mah. Compu. Sci. 4 (2014), No. 4, 716-727 ISSN: 1927-5307 ON ITERATIVE TECHNIQUES FOR NUMERICAL SOLUTIONS OF LINEAR AND NONLINEAR DIFFERENTIAL EQUATIONS S.O. EDEKI *, A.A.

More information

Basic Results in Functional Analysis

Basic Results in Functional Analysis Preared by: F.. ewis Udaed: Suday, Augus 7, 4 Basic Resuls i Fucioal Aalysis f ( ): X Y is coiuous o X if X, (, ) z f( z) f( ) f ( ): X Y is uiformly coiuous o X if i is coiuous ad ( ) does o deed o. f

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

Time : 1 hr. Test Paper 08 Date 04/01/15 Batch - R Marks : 120

Time : 1 hr. Test Paper 08 Date 04/01/15 Batch - R Marks : 120 Tim : hr. Tst Papr 8 D 4//5 Bch - R Marks : SINGLE CORRECT CHOICE TYPE [4, ]. If th compl umbr z sisfis th coditio z 3, th th last valu of z is qual to : z (A) 5/3 (B) 8/3 (C) /3 (D) o of ths 5 4. Th itgral,

More information

Strictly as per the compliance and regulations of :

Strictly as per the compliance and regulations of : Global Joural of Scic Froir Rsarch Mahaics & Dcisio Scics Volu Issu Vrsio. Typ : Doubl lid Pr Rviwd Iraioal Rsarch Joural Publishr: Global Jourals Ic. US Oli ISSN: 9-66 & i ISSN: 975-5896 Oscillaory Fr

More information

Chapter 2 The Poisson Process

Chapter 2 The Poisson Process Chapr 2 Th oisso rocss 2. Expoial ad oisso disribuios 2... Th Birh Modl I scods, a oal of popl ar bor. Sarig a ay poi i im, wha is h waiig im for h firs birh? I milliscods, a oal of lpho calls arriv a

More information

Midterm exam 2, April 7, 2009 (solutions)

Midterm exam 2, April 7, 2009 (solutions) Univrsiy of Pnnsylvania Dparmn of Mahmaics Mah 26 Honors Calculus II Spring Smsr 29 Prof Grassi, TA Ashr Aul Midrm xam 2, April 7, 29 (soluions) 1 Wri a basis for h spac of pairs (u, v) of smooh funcions

More information

An Analytical Study on Fractional Partial Differential Equations by Laplace Transform Operator Method

An Analytical Study on Fractional Partial Differential Equations by Laplace Transform Operator Method Iraioal Joural o Applid Egirig Rsarch ISSN 973-456 Volum 3 Numbr (8 pp 545-549 Rsarch Idia Publicaios hp://wwwripublicaiocom A Aalical Sud o Fracioal Parial Dirial Euaios b aplac Trasorm Opraor Mhod SKElaga

More information

Intrinsic formulation for elastic line deformed on a surface by an external field in the pseudo-galilean space 3. Nevin Gürbüz

Intrinsic formulation for elastic line deformed on a surface by an external field in the pseudo-galilean space 3. Nevin Gürbüz risic formuaio for asic i form o a surfac by a xra fi i h psuo-aia spac Nvi ürbüz Eskişhir Osmaazi Uivrsiy Mahmaics a Compur Scics Dparm urbuz@ouur Absrac: his papr w riv irisic formuaio for asic i form

More information

Hadamard Exponential Hankel Matrix, Its Eigenvalues and Some Norms

Hadamard Exponential Hankel Matrix, Its Eigenvalues and Some Norms Math Sci Ltt Vol No 8-87 (0) adamard Exotial al Matrix, Its Eigvalus ad Som Norms İ ad M bula Mathmatical Scics Lttrs Itratioal Joural @ 0 NSP Natural Scics Publishig Cor Dartmt of Mathmatics, aculty of

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

Application of Fixed Point Theorem of Convex-power Operators to Nonlinear Volterra Type Integral Equations

Application of Fixed Point Theorem of Convex-power Operators to Nonlinear Volterra Type Integral Equations Ieraioal Mahemaical Forum, Vol 9, 4, o 9, 47-47 HIKRI Ld, wwwm-hikaricom h://dxdoiorg/988/imf4333 licaio of Fixed Poi Theorem of Covex-ower Oeraors o Noliear Volerra Tye Iegral Equaios Ya Chao-dog Huaiyi

More information

Outline. Overlook. Controllability measures. Observability measures. Infinite Gramians. MOR: Balanced truncation based on infinite Gramians

Outline. Overlook. Controllability measures. Observability measures. Infinite Gramians. MOR: Balanced truncation based on infinite Gramians Ouli Ovrlook Corollabiliy masurs Obsrvabiliy masurs Ifii Gramias MOR: alacd rucaio basd o ifii Gramias Ovrlook alacd rucaio: firs balacig h ruca. Giv a I sysm: / y u d d For covic of discussio w do h sysm

More information

EE415/515 Fundamentals of Semiconductor Devices Fall 2012

EE415/515 Fundamentals of Semiconductor Devices Fall 2012 3 EE4555 Fudmls of Smicoducor vics Fll cur 8: PN ucio iod hr 8 Forwrd & rvrs bis Moriy crrir diffusio Brrir lowrd blcd by iffusio rducd iffusio icrsd mioriy crrir drif rif hcd 3 EE 4555. E. Morris 3 3

More information

c. What is the average rate of change of f on the interval [, ]? Answer: d. What is a local minimum value of f? Answer: 5 e. On what interval(s) is f

c. What is the average rate of change of f on the interval [, ]? Answer: d. What is a local minimum value of f? Answer: 5 e. On what interval(s) is f Essential Skills Chapter f ( x + h) f ( x ). Simplifying the difference quotient Section. h f ( x + h) f ( x ) Example: For f ( x) = 4x 4 x, find and simplify completely. h Answer: 4 8x 4 h. Finding the

More information

Chapter4 Time Domain Analysis of Control System

Chapter4 Time Domain Analysis of Control System Chpr4 im Domi Alyi of Corol Sym Rouh biliy cririo Sdy rror ri rpo of h fir-ordr ym ri rpo of h cod-ordr ym im domi prformc pcificio h rliohip bw h prformc pcificio d ym prmr ri rpo of highr-ordr ym Dfiiio

More information

A L A BA M A L A W R E V IE W

A L A BA M A L A W R E V IE W A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N

More information

z 1+ 3 z = Π n =1 z f() z = n e - z = ( 1-z) e z e n z z 1- n = ( 1-z/2) 1+ 2n z e 2n e n -1 ( 1-z )/2 e 2n-1 1-2n -1 1 () z

z 1+ 3 z = Π n =1 z f() z = n e - z = ( 1-z) e z e n z z 1- n = ( 1-z/2) 1+ 2n z e 2n e n -1 ( 1-z )/2 e 2n-1 1-2n -1 1 () z Sris Expasio of Rciprocal of Gamma Fuctio. Fuctios with Itgrs as Roots Fuctio f with gativ itgrs as roots ca b dscribd as follows. f() Howvr, this ifiit product divrgs. That is, such a fuctio caot xist

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

C o r p o r a t e l i f e i n A n c i e n t I n d i a e x p r e s s e d i t s e l f

C o r p o r a t e l i f e i n A n c i e n t I n d i a e x p r e s s e d i t s e l f C H A P T E R I G E N E S I S A N D GROWTH OF G U IL D S C o r p o r a t e l i f e i n A n c i e n t I n d i a e x p r e s s e d i t s e l f i n a v a r i e t y o f f o r m s - s o c i a l, r e l i g i

More information

Folding of Hyperbolic Manifolds

Folding of Hyperbolic Manifolds It. J. Cotmp. Math. Scics, Vol. 7, 0, o. 6, 79-799 Foldig of Hyprbolic Maifolds H. I. Attiya Basic Scic Dpartmt, Collg of Idustrial Educatio BANE - SUEF Uivrsity, Egypt hala_attiya005@yahoo.com Abstract

More information

Modeling of Reductive Biodegradation of TCE to ETH. Adam Worsztynowicz, Dorota Rzychon, Sebastian Iwaszenko, Tomasz Siobowicz

Modeling of Reductive Biodegradation of TCE to ETH. Adam Worsztynowicz, Dorota Rzychon, Sebastian Iwaszenko, Tomasz Siobowicz Modlig of Rduciv Biodgradaio of o ETH Adam Worszyowicz, Doroa Rzycho, Sbasia Iwaszo, Tomasz Siobowicz Isiu for Ecology of Idusrial Aras Kossuha S., Kaowic, Polad l. (+-) 5, fax: (+-) 5 7 7 -mail: iu@iu.aowic.pl

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by D. Klain Vrsion 207.0.05 Corrctions and commnts ar wlcom. Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix A A k I + A + k!

More information