SOLUTION OF THE HYPERBOLIC KEPLER EQUATION BY ADOMIAN S ASYMPTOTIC DECOMPOSITION METHOD

Size: px
Start display at page:

Download "SOLUTION OF THE HYPERBOLIC KEPLER EQUATION BY ADOMIAN S ASYMPTOTIC DECOMPOSITION METHOD"

Transcription

1 Romaia Rports i Physics 70, XYZ (08) SOLUTION OF THE HYPERBOLIC KEPLER EQUATION BY ADOMIAN S ASYMPTOTIC DECOMPOSITION METHOD ABDULRAHMAN F ALJOHANI, RANDOLPH RACH, ESSAM EL-ZAHAR,4, ABDUL-MAJID WAZWAZ 5, ABDELHALIM EBAID,* Dpartmt of Mathmatics, Faculty of Scic, Uivrsity of Tabuk, POBox 74, Tabuk 749, Kigdom of Saudi Arabia Th Gorg Adomia Ctr for Applid Mathmatics, 6 South Mapl Strt, Hartford, Michiga , USA Dpartmt of Mathmatics, Faculty of Scics ad Humaitis, Pric Sattam Bi Abdulaziz Uivrsity, Alkharj, 94, Kigdom of Saudi Arabia 4 Dpartmt of Basic Egirig Scic, Faculty of Egirig, Shbi El-Kom, 5, Mofia Uivrsity, Egypt 5 Dpartmt of Mathmatics, Sait Xavir Uivrsity, Chicago, IL 60655, USA * Corrspodig author, abaid@utdusa Rcivd Octobr 6, 07 Abstract Th hyprbolic Kplr quatio is of practical itrst i astroomy It is oft usd to dscrib th cctric aomaly of a comt of xtrasolar origi i its hyprbolic trajctory past th Su Efficit dtrmiatio of th radial distac ad/or th Cartsia coordiats of th comt rquirs accurat calculatio of th cctric aomaly, hc th d for a covit, robust mthod to solv Kplr s quatio of hyprbolic typ I this papr, th Adomia s asymptotic dcompositio mthod is proposd to solv this quatio Our calculatios hav dmostratd a rapid rat of covrgc of th squc of th obtaid approximat solutios, which ar displayd i svral graphs Also, w hav show i this papr that oly a fw trms of th Adomia dcompositio sris ar sufficit to achiv xtrmly accurat umrical rsults v for much highr valus tha thos i th litratur for th ma aomaly ad th cctricity of th orbit Th mai charactristic of th obtaid approximat solutios is that thy ar all odd fuctios i th ma aomaly, which w hav illustratd through graphs I additio, it is foud that th absolut rmaidr rror usig oly thr compots of Adomia s solutio dcrass across a spcifid domai ad approachs zro as th cctric aomaly tds to ifiity Morovr, th absolut rmaidr rror dcrass by icrasig th umbr of compots of th Adomia dcompositio sris Fially, th currt aalysis may b th first to mak a ffctiv applicatio of th Adomia s asymptotic dcompositio mthod i astroomical physics Ky words: Adomia s asymptotic dcompositio mthod; Adomia polyomials; hyprbolic Kplr s quatio; sris solutio INTRODUCTION I clstial mchaics, Kplr s quatios of lliptical ad hyprbolic typs play importat rols Efficit dtrmiatio of th accurat positio of a objct (a plat, comt or a astroid) wh orbitig th Su rquirs solvig ithr of ths

2 Articl o A F Aljohai, R Rach, E El-Zahar, A-M Wazwaz, A Ebaid quatios with a solutio mthod of high accuracy I our solar systm, som comts of xtrasolar origi follow hyprbolic trajctoris past th Su Such comts tr th solar systm comig from th Oort cloud ad itrstllar spac ad may xit th solar systm through hyprbolic trajctoris I astroomy, th origial orbits of such comts may chag from lliptical to hyprbolic, spcially, wh takig ito accout th possibl gravitatioal attractio of th plats of substatial mass, g, Jupitr I this papr, Kplr s quatio of hyprbolic typ is cosidrd i th stadard form [], sih( H ( t) ) H ( t) = M ( t), <, 0 M <, () μ whr H is dfid as th cctric aomaly, M ( t) = ( t τ ) is th ma a aomaly, a is th smi-major axis, is th cctricity of th orbit, μ = GM is th gravitatioal paramtr of th ctral body of mass M, whr G is th uivrsal gravitatioal costat ad τ is th tim of passag through th closst poit of approach to th focus Th polar quatio of a hyprbola with its focus at th origi may b writt as a( ) r = () + cos f This agl f is giv i trms of H through th followig rlatioship [], f + H ta = ta () I additio, at a istat t, th ( x, y) coordiats of a objct i th stadard fram of rfrc (whr th ctral body is at th origi ad th x -axis poits towards th priapsis) ar giv i trms of H by x = a( cosh H ), (4) (5) y = a sih H So, i ordr to calculat th radial distac r ad th tru aomaly f of a comt wh orbitig th Su at a spcifid tim t, th hyprbolic Kplr quatio () is first solvd for H at that tim t ad th Eqs () ad () ar applid As show by Eq (), th hyprbolic Kplr quatio is a trascdtal quatio that has o xact closd-form aalytic solutio Although may authors [ 0] hav dvisd various umrical ad aalytical solutios for Kplr s quatio of lliptical typ, littl ffort has b dvotd to ivstigat th hyprbolic form of this quatio [ 4] Sarchig for a w accurat but simpl aalytical solutio for th hyprbolic Kplr quatio is still of maifst practical itrst I ordr to cotribut to a improvd solutio of this problm, th authors bliv that th

3 Solutio of th hyprbolic Kplr quatio by Adomia s dcompositio mthod Articl o Th Adomia s dcompositio mthod (ADM) ca b ffctivly applid to solv th hyprbolic form of this quatio Th ADM is a systmatic aalytic approximatio mthod for solvig algbraic ad trascdtal quatios, matrix quatios, oliar itgral quatios, ad oliar diffrtial quatios icludig both oliar iitial valu problms ad oliar boudary valu problms v for irrgular boudary cotours It has b widly implmtd to solv a larg umbr of frotir problms i th applid scics ad girig ad ca b also xtdd to covr may scitific modls [5 4] It xprsss th solutio i th form of a ifiit sris Udr physically appropriat coditios, this sris oft rapidly covrgs ad hc a fw trms of Adomia s mthod ar sufficit to obtai accurat umrical rsults for th ivstigatd problm I this cas, th squc of approximat solutios by Adomia s mthod covrgs to a crtai curv or fuctio For xampl, th ADM has b applid by Ebaid [] to solv th Thomas-Frmi quatio that has o xact solutio I that papr, h showd gomtrically that th squc of th approximat solutios covrgs to a crtai curv, which may v b th xact solutio for that problm Th objctiv of this papr is to aalyz th hyprbolic Kplr quatio by usig th ADM W show that th Adomia s dcompositio sris solutio to th currt problm closly coicids with thos i th litratur for all valus of th ma aomaly paramtr M [0, ) ad for all valus of th cctricity of th orbit usig oly a fw of Adomia s solutio compots I additio, it will b show i this papr that th squc of th Adomia s dcompositio approximat solutios covrgs rapidly i a much widr rag tha thos cosidrd i th litratur for th paramtrs M ad APPLICATION OF ADOMIAN S ASYMPTOTIC DECOMPOSITION METHOD Th Adomia s asymptotic dcompositio mthod (AADM) is applid i this Sctio to calculat a squc of approximat aalytic solutios for th hyprbolic Kplr quatio W rwrit Eq () i th caoical form as M ( t) sih( H ( t) ) = + H ( t) (6) Th sris of th Adomia polyomials ad th Adomia dcompositio sris ar ( H t ) A t A t A ( H t H t ) sih () = (), ()= (),, (), =0 =0 Ht ()= H() t 0 (7)

4 Articl o A F Aljohai, R Rach, E El-Zahar, A-M Wazwaz, A Ebaid 4 Upo substitutio of Eq (7) ito Eq (6), w obtai M ( t) A ( t) = + H ( t) (8) =0 =0 Accordigly, th followig algorithm ca b stablishd usig th Adomia rcursio schm, M ( t) A 0( t) =, A + ( t) = H, 0 (9) Th Adomia polyomials for th hyprbolic si oliarity wr dfid by Adomia ad Rach i 98 [] as d = sih m A λ H ( t) m (0)! dλ m= 0 λ=0 Applyig this formula, th first svral Adomia polyomials for th hyprbolic si oliarity ar A 0 = sih( H 0 ), A = H cosh( H 0 ), A = H cosh( H 0 ) + H sih( H0 ),! A H cosh 0 0 +! ( H ) + H H sih( H ) H cosh( ), = H0 () Hc A A A A = H 0 = H = H 4 = H,,,, ()

5 5 Solutio of th hyprbolic Kplr quatio by Adomia s dcompositio mthod Articl o ad so o Combiig () ad (), w obtai M sih( H 0 ) =, H cosh( H0 ) = H0, H cosh( H0 ) + H sih( H0 ) = H,! H cosh H 0 + HH sih H0 + H cosh H 0 = H! Thrfor = M H, 0 sih M sih H =, + M H ( ) ( ) ( ) M M ( + M )sih M + M sih =, ( + M ) M M 6( + M ) sih 9 M + M sih ( M ) sih M H =, 5/ 6( + M ) () (4) Th ADM givs th -trm approximat aalytic solutio Φ (t) for th hyprbolic Kplr quatio as Accordigly, w calculat M Φ ()= t, + sih + M i=0 Φ ( t) = H i ( t) (5)

6 Articl o A F Aljohai, R Rach, E El-Zahar, A-M Wazwaz, A Ebaid 6 M M M Φ M + M ( + M ) ()= t sih, / sih (6) + M M M Φ ()= t / sih / + M ( + M ) ( + M ) M ( M ) M sih 5/ sih 6( + M ) I a subsqut Sctio, w will show that th squc of th approximat solutios i (6) for th hyprbolic Kplr quatio is covrgt i a widr rag tha thos rportd i th litratur for M ad I additio, th accuracy of th prst umrical rsults will b validatd by calculatig th absolut rmaidr rror RE + ( t) dfid by RE + ( t) = sih( Φ + ( t) ) Φ+ ( t) M, 0, (7) by usig th -trm approximat solutio to stimat th cctric aomaly H Morovr, th advatag ad th ffctivss of th prst low-ordr approximat aalytic solutios for th hyprbolic Kplr quatio ovr svral xistig mthods i th litratur will b provd for crtai highr valus of th paramtrs M ad DISCUSSION I th prvious Sctio, Adomia s asymptotic dcompositio mthod has b applid to obtai th approximat solutios of th hyprbolic Kplr quatio Such approximat solutios ar applid i this discussio to obtai svral plots Lt us bgi by graphically dmostratig th covrgc of th prst approximat solutios I Fig, th approximat solutios Φ ( t), Φ 5 ( t), ad Φ7 ( t) ar plottd for = 5 vrsus th ma aomaly M A rapid covrgc is obsrvd i this figur usig oly a fw trms of th Adomia asymptotic solutios

7 7 Solutio of th hyprbolic Kplr quatio by Adomia s dcompositio mthod Articl o Figur : Covrgc of th approximat solutios vrsus M at = 5 Th mai rsult hr is that th rat of covrgc is icrasd for highr valus of M, whr at M 4 th thr-trm approximat solutio Φ ( t) of Adomia s asymptotic dcompositio mthod is sufficit to provid a rmarkably accurat solutio, whil at th lowr valus of M i th domai [0,4) a highrordr approximat solutio such as Φ (t) for 5 is rquird to achiv a similarly high accuracy I additio, ths approximat solutios ar all odd fuctios i th ma aomaly M which has b show i Fig for a slctd highr valu of th cctricity paramtr = 05

8 Articl o A F Aljohai, R Rach, E El-Zahar, A-M Wazwaz, A Ebaid 8 Figur : Th odd proprty of th approximat solutios vrsus M at = 05 I a widr rag of M [0,00], it has b also show from Fig that th approximat solutios Φ ( ), Φ ( ), ad Φ ( ) covrg to a crtai t 5 t curv/fuctio Bsids, th odd proprty is also show i Fig 4 for a furthr widr rag M [ 00,00] Morovr, Fig 5 ad Fig 6 also dmostrat th rapid rat of covrgc of Adomia s squc of aalytic approximat solutios vrsus th cctricity paramtr i th domai [5,55] at th lowst ad th highst valus of M, which was cosidrd by Sharaf t al [], rspctivly It is radily appart from ths figurs that Adomia s solutios also covrg, v at th highst cosidrd valu, M = Th aformtiod discussio corroborats th ffctivss of Adomia s asymptotic dcompositio mthod i quickly ad accuratly solvig th hyprbolic Kplr quatio 7 t

9 9 Solutio of th hyprbolic Kplr quatio by Adomia s dcompositio mthod Articl o Figur : Covrgc of th approximat solutios vrsus M at = 5 i a widr rag Figur 4: Th odd proprty of th approximat solutios vrsus M at = 05 i a widr rag

10 Articl o A F Aljohai, R Rach, E El-Zahar, A-M Wazwaz, A Ebaid 0 Figur 5: Covrgc of th approximat solutios vrsus at M = 58 Figur 6: Covrgc of th approximat solutios vrsus at M = 75005

11 Solutio of th hyprbolic Kplr quatio by Adomia s dcompositio mthod Articl o Th ffctivss ad fficicy of th currt lowr-ordr approximat solutios ar umrically validatd i Figs 7-8 I ths figurs, th corrspodig absolut rmaidr rrors RE, RE5, ad RE7 ar displayd at two slctd valus of th cctricity = 5 ad = 00 for two slctd domais of th ma aomaly M [0,00] i Fig 7 ad M [0,0000] i Fig 8 W coclud from figurs 7-8 that th absolut rmaidr rror RE usig oly thr compots of Adomia s asymptotic dcompositio mthod dcrass ad approachs zro as M tds to ifiity Howvr, th maximum valu of th absolut rmaidr rror RE is about 0 radias i th rgio M (0,) ad it is about 008 radias M (,6) as i Fig 7 ad th it dcrass with icrasig M th absolut rmaidr rror dcrass with icrasig th cctricity For xampl, th maximum valu of th absolut rmaidr rror RE is about radias as i Fig 8 wh = 00 th absolut rmaidr rror dcrass by icrasig th umbr of compots as illustratd by th curvs of RE ad RE i Figs Figur 7: Th absolut rmaidr rror vrsus M at = 5

12 Articl o A F Aljohai, R Rach, E El-Zahar, A-M Wazwaz, A Ebaid Figur 8: Th absolut rmaidr rror vrsus M at = 00 Figur 9: Th absolut rmaidr rror vrsus at M = 500

13 Solutio of th hyprbolic Kplr quatio by Adomia s dcompositio mthod Articl o Figur 0: Th absolut rmaidr rror vrsus at M = For a furthr validatio of th currt umrical rsults, two additioal plots ar displayd i Figs 9-0 for th absolut rmaidr rrors RE, RE5 ad RE7 vrsus th cctricity i th domai [5,00] for M = 500 ad M = 75000, rspctivly Th rsults plottd i ths two figurs rval that th approximat solutio usig oly thr trms of th asymptotic Adomia s sris is also accurat as M at all cosidrd valus of th cctricity paramtr Morovr, th absolut rmaidr rrors RE5 ad RE7 approach zro v at ths highr valus of th ma aomaly ad th cctricity This, of cours, provs th svral rmarkabl advatags of th Adomia s asymptotic dcompositio mthod ovr th xistig mthods i th litratur Fially, th authors of th prst papr rcommd th currt approach as th most ffctiv aalytical tchiqu to solv th hyprbolic Kplr quatio 4 CONCLUSION I this papr, Kplr s quatio for hyprbloic orbits has b aalytically solvd by usig th Adomia s asymptotic dcompositio mthod (AADM) Th odd proprty of th obtaid approximat solutios has b dmostratd through a sris of graphs Also, w hav show that oly a fw trms of th AADM ar sufficit to obtai xtrmly accurat umrical rsults v at highr valus tha

14 Articl o A F Aljohai, R Rach, E El-Zahar, A-M Wazwaz, A Ebaid 4 thos i th litratur for th ma aomaly ad th cctricity paramtrs I compariso to th mthods rportd i th litratur, th prst approach is ot oly ffctiv but also vry simpl i tchiqu Morovr, th advatags of th currt rsults for th cctric aomaly ar valid i ay spcifid domai Bsids, vry small absolut rmaidr rrors hav b achivd usig oly a fw trms of th Adomia s asymptotic dcompositio sris Th ffctivss provd i this papr for Adomia s asymptotic mthod to quickly ad asily solv th hyprbolic Kplr quatio may b advatagously xtdd to othr problms i physics ad girig REFERENCES FR Moulto, A Itroductio to Clstial Mchaics, d rvisd ditio, Dovr, Nw York, 970 NI Ioakimids ad KE Papadakis, Clstial Mchaics ad Dyamical Astroomy 5 (4), 05 6 (985) NM Swrdlow, J for History of Astroomy, 9 4 (000) 4 L Stumpf, Chaotic Clstial Mchaics ad Dyamical Astroomy 74, (999) 5 M Palacios, J Comput Appl Math 8, 5 46 (00) 6 P Colwll, Amrica Mathmatical Mothly 99(), 45 48(99) 7 P Colwll, Solvig Kplr s quatio ovr thr cturis, Willma-Bll Ed, Richmod, 99 8 K Boubakr, Amrica Mathmatical Mothly, Apiro 7 (), (00) 9 Rza Esmalzadh ad Hossi Ghadiri, It J Computr Applicatios 89(7), 8(04) 0 Curila Mirca ad Curila Sori, Aall Uivrsitatii di Orada, Fascicula Protc tia Mdiului, Vol XXII, 9 4 (04) M Avdao, V Marti-Molia, ad J Ortigas-Galido, arxiv:50064v [physicsclass-ph], (0 Fb 05) T Fukushima, Clstial Mchaics ad Dyamical Astroomy 68, 7(997) MA Sharaf, MA Baajh, ad AA Alshaary, J Astrophys Astr 8, 9 6 (007) 4 A Alshary ad A Ebaid, Acta Astroautica 40, 7 (07) 5 G Adomia ad R Rach, J Math Aal Applic 05, 4 66 (985) 6 G Adomia ad R Rach, J Math Aal Applic (), 6 40(985) 7 G Adomia ad R Rach, Kybrts 5 (), 7(986) 8 AM Wazwaz, Rom J Phys 6, (06) 9 AM Wazwaz t al, Rom Rp Phys 69, 0 (07) 0 Y Zhag, D Balau, ad X J Yag, Proc Romaia Acad A 7, 0 6 (06) AH Bhrawy t al, Proc Romaia Acad A 8, 7 4 (07) G Adomia, R Rach, J Math Aal Applic 9 (), 9 46 (98) I A Cristscu, Rom Rp Phys 68, (06) 4 RM Hafz t al, Rom Rp Phys 68, 7 (06) 5 L Bougoffa, Rom J Phys 6, 0 (07) 6 AM Wazwaz, Rom J Phys 60, 56 7 (05) 7 AM Wazwaz t al, Rom Rp Phys 69, 0 (07) 8 K Parad, H Yousfi, ad M Dlkhosh, Rom J Phys 6, 04 (07) 9 A Ebaid, Z Naturforschug A 66, 4 46 (0) 0 JS Dua ad R Rach, Appl Math Comput 8, (0) A Ebaid, J Comput Appl Math 5, (0) AM Wazwaz, R Rach, ad JS Dua, Appl Math Comput 9, (0)

15 5 Solutio of th hyprbolic Kplr quatio by Adomia s dcompositio mthod Articl o EH Ali, A Ebaid, ad R Rach, Comput Math Applic 6, (0) 4 I A Cristscu, Rom Rp Phys 68, (06) 5 C Chu, A Ebaid, M L, ad E Aly, ANZIAM Joural 5, 4 (0) 6 A Ebaid, MD Aljoufi, ad A-M Wazwaz, Appl Math Ltt 46, 7 (05) 7 HO Bakodah t al, Rom Rp Phys 70, XYZ (08) 8 AA Gabr ad A Ebaid, Rom Rp Phys 70, XYZ (08) 9 H Lblod, H Triki, ad D Mihalach, Phys Rv A 85, 0586 (0) 40 D Mihalach, Rom J Phys 59, 95 (04) 4 D Mihalach, Proc Romaia Acad A 6, 6 69 (05) 4 D Mihalach, Rom Rp Phys 69, 40 (07)

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

On the approximation of the constant of Napier

On the approximation of the constant of Napier Stud. Uiv. Babş-Bolyai Math. 560, No., 609 64 O th approximatio of th costat of Napir Adri Vrscu Abstract. Startig from som oldr idas of [] ad [6], w show w facts cocrig th approximatio of th costat of

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

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

STIRLING'S 1 FORMULA AND ITS APPLICATION

STIRLING'S 1 FORMULA AND ITS APPLICATION MAT-KOL (Baja Luka) XXIV ()(08) 57-64 http://wwwimviblorg/dmbl/dmblhtm DOI: 075/МК80057A ISSN 0354-6969 (o) ISSN 986-588 (o) STIRLING'S FORMULA AND ITS APPLICATION Šfkt Arslaagić Sarajvo B&H Abstract:

More information

1985 AP Calculus BC: Section I

1985 AP Calculus BC: Section I 985 AP Calculus BC: Sctio I 9 Miuts No Calculator Nots: () I this amiatio, l dots th atural logarithm of (that is, logarithm to th bas ). () Ulss othrwis spcifid, th domai of a fuctio f is assumd to b

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

MONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx

MONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx MONTGOMERY COLLEGE Dpartmt of Mathmatics Rockvill Campus MATH 8 - REVIEW PROBLEMS. Stat whthr ach of th followig ca b itgratd by partial fractios (PF), itgratio by parts (PI), u-substitutio (U), or o of

More information

Statistics 3858 : Likelihood Ratio for Exponential Distribution

Statistics 3858 : Likelihood Ratio for Exponential Distribution Statistics 3858 : Liklihood Ratio for Expotial Distributio I ths two xampl th rjctio rjctio rgio is of th form {x : 2 log (Λ(x)) > c} for a appropriat costat c. For a siz α tst, usig Thorm 9.5A w obtai

More information

2.29 Numerical Fluid Mechanics Spring 2015 Lecture 12

2.29 Numerical Fluid Mechanics Spring 2015 Lecture 12 REVIEW Lctur 11: Numrical Fluid Mchaics Sprig 2015 Lctur 12 Fiit Diffrcs basd Polyomial approximatios Obtai polyomial (i gral u-qually spacd), th diffrtiat as dd Nwto s itrpolatig polyomial formulas Triagular

More information

Option 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges.

Option 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges. Optio Chaptr Ercis. Covrgs to Covrgs to Covrgs to Divrgs Covrgs to Covrgs to Divrgs 8 Divrgs Covrgs to Covrgs to Divrgs Covrgs to Covrgs to Covrgs to Covrgs to 8 Proof Covrgs to π l 8 l a b Divrgt π Divrgt

More information

H2 Mathematics Arithmetic & Geometric Series ( )

H2 Mathematics Arithmetic & Geometric Series ( ) H Mathmatics Arithmtic & Gomtric Sris (08 09) Basic Mastry Qustios Arithmtic Progrssio ad Sris. Th rth trm of a squc is 4r 7. (i) Stat th first four trms ad th 0th trm. (ii) Show that th squc is a arithmtic

More information

An Introduction to Asymptotic Expansions

An Introduction to Asymptotic Expansions A Itroductio to Asmptotic Expasios R. Shaar Subramaia Asmptotic xpasios ar usd i aalsis to dscrib th bhavior of a fuctio i a limitig situatio. Wh a fuctio ( x, dpds o a small paramtr, ad th solutio of

More information

Chapter 11.00C Physical Problem for Fast Fourier Transform Civil Engineering

Chapter 11.00C Physical Problem for Fast Fourier Transform Civil Engineering haptr. Physical Problm for Fast Fourir Trasform ivil Egirig Itroductio I this chaptr, applicatios of FFT algorithms [-5] for solvig ral-lif problms such as computig th dyamical (displacmt rspos [6-7] of

More information

Review Exercises. 1. Evaluate using the definition of the definite integral as a Riemann Sum. Does the answer represent an area? 2

Review Exercises. 1. Evaluate using the definition of the definite integral as a Riemann Sum. Does the answer represent an area? 2 MATHEMATIS --RE Itgral alculus Marti Huard Witr 9 Rviw Erciss. Evaluat usig th dfiitio of th dfiit itgral as a Rima Sum. Dos th aswr rprst a ara? a ( d b ( d c ( ( d d ( d. Fid f ( usig th Fudamtal Thorm

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

An Introduction to Asymptotic Expansions

An Introduction to Asymptotic Expansions A Itroductio to Asmptotic Expasios R. Shaar Subramaia Dpartmt o Chmical ad Biomolcular Egirig Clarso Uivrsit Asmptotic xpasios ar usd i aalsis to dscrib th bhavior o a uctio i a limitig situatio. Wh a

More information

Restricted Factorial And A Remark On The Reduced Residue Classes

Restricted Factorial And A Remark On The Reduced Residue Classes Applid Mathmatics E-Nots, 162016, 244-250 c ISSN 1607-2510 Availabl fr at mirror sits of http://www.math.thu.du.tw/ am/ Rstrictd Factorial Ad A Rmark O Th Rducd Rsidu Classs Mhdi Hassai Rcivd 26 March

More information

NET/JRF, GATE, IIT JAM, JEST, TIFR

NET/JRF, GATE, IIT JAM, JEST, TIFR Istitut for NET/JRF, GATE, IIT JAM, JEST, TIFR ad GRE i PHYSICAL SCIENCES Mathmatical Physics JEST-6 Q. Giv th coditio φ, th solutio of th quatio ψ φ φ is giv by k. kφ kφ lφ kφ lφ (a) ψ (b) ψ kφ (c) ψ

More information

New Sixteenth-Order Derivative-Free Methods for Solving Nonlinear Equations

New Sixteenth-Order Derivative-Free Methods for Solving Nonlinear Equations Amrica Joural o Computatioal ad Applid Mathmatics 0 (: -8 DOI: 0.59/j.ajcam.000.08 Nw Sixtth-Ordr Drivativ-Fr Mthods or Solvig Noliar Equatios R. Thukral Padé Rsarch Ctr 9 Daswood Hill Lds Wst Yorkshir

More information

A Solution of Kepler s Equation

A Solution of Kepler s Equation Itratioal Joural of Astroomy ad Astrohysics, 4, 4, 68-698 Publishd Oli Dcmbr 4 i SciRs. htt://www.scir.org/joural/ijaa htt://dx.doi.org/.46/ijaa.4.446 A Solutio of Klr s Equatio Joh N. Tokis Tchological

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

COLLECTION OF SUPPLEMENTARY PROBLEMS CALCULUS II

COLLECTION OF SUPPLEMENTARY PROBLEMS CALCULUS II COLLECTION OF SUPPLEMENTARY PROBLEMS I. CHAPTER 6 --- Trscdtl Fuctios CALCULUS II A. FROM CALCULUS BY J. STEWART:. ( How is th umbr dfid? ( Wht is pproimt vlu for? (c ) Sktch th grph of th turl potil fuctios.

More information

Iterative Methods of Order Four for Solving Nonlinear Equations

Iterative Methods of Order Four for Solving Nonlinear Equations Itrativ Mods of Ordr Four for Solvig Noliar Equatios V.B. Kumar,Vatti, Shouri Domii ad Mouia,V Dpartmt of Egirig Mamatis, Formr Studt of Chmial Egirig Adhra Uivrsity Collg of Egirig A, Adhra Uivrsity Visakhapatam

More information

Bipolar Junction Transistors

Bipolar Junction Transistors ipolar Juctio Trasistors ipolar juctio trasistors (JT) ar activ 3-trmial dvics with aras of applicatios: amplifirs, switch tc. high-powr circuits high-spd logic circuits for high-spd computrs. JT structur:

More information

A Propagating Wave Packet Group Velocity Dispersion

A Propagating Wave Packet Group Velocity Dispersion Lctur 8 Phys 375 A Propagating Wav Packt Group Vlocity Disprsion Ovrviw and Motivation: In th last lctur w lookd at a localizd solution t) to th 1D fr-particl Schrödingr quation (SE) that corrsponds to

More information

A Simple Proof that e is Irrational

A Simple Proof that e is Irrational Two of th most bautiful ad sigificat umbrs i mathmatics ar π ad. π (approximatly qual to 3.459) rprsts th ratio of th circumfrc of a circl to its diamtr. (approximatly qual to.788) is th bas of th atural

More information

Triple Play: From De Morgan to Stirling To Euler to Maclaurin to Stirling

Triple Play: From De Morgan to Stirling To Euler to Maclaurin to Stirling Tripl Play: From D Morga to Stirlig To Eulr to Maclauri to Stirlig Augustus D Morga (186-1871) was a sigificat Victoria Mathmaticia who mad cotributios to Mathmatics History, Mathmatical Rcratios, Mathmatical

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

APPENDIX: STATISTICAL TOOLS

APPENDIX: STATISTICAL TOOLS I. Nots o radom samplig Why do you d to sampl radomly? APPENDI: STATISTICAL TOOLS I ordr to masur som valu o a populatio of orgaisms, you usually caot masur all orgaisms, so you sampl a subst of th populatio.

More information

Calculus & analytic geometry

Calculus & analytic geometry Calculus & aalytic gomtry B Sc MATHEMATICS Admissio owards IV SEMESTER CORE COURSE UNIVERSITY OF CALICUT SCHOOL OF DISTANCE EDUCATION CALICUT UNIVERSITYPO, MALAPPURAM, KERALA, INDIA 67 65 5 School of Distac

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

Normal Form for Systems with Linear Part N 3(n)

Normal Form for Systems with Linear Part N 3(n) Applid Mathmatics 64-647 http://dxdoiorg/46/am7 Publishd Oli ovmbr (http://wwwscirporg/joural/am) ormal Form or Systms with Liar Part () Grac Gachigua * David Maloza Johaa Sigy Dpartmt o Mathmatics Collg

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

International Journal of Advanced and Applied Sciences

International Journal of Advanced and Applied Sciences Itratioal Joural of Advacd ad Applid Scics x(x) xxxx Pags: xx xx Cotts lists availabl at Scic Gat Itratioal Joural of Advacd ad Applid Scics Joural hompag: http://wwwscic gatcom/ijaashtml Symmtric Fuctios

More information

CDS 101: Lecture 5.1 Reachability and State Space Feedback

CDS 101: Lecture 5.1 Reachability and State Space Feedback CDS, Lctur 5. CDS : Lctur 5. Rachability ad Stat Spac Fdback Richard M. Murray 7 Octobr 3 Goals: Di rachability o a cotrol systm Giv tsts or rachability o liar systms ad apply to ampls Dscrib th dsig o

More information

The Interplay between l-max, l-min, p-max and p-min Stable Distributions

The Interplay between l-max, l-min, p-max and p-min Stable Distributions DOI: 0.545/mjis.05.4006 Th Itrplay btw lma lmi pma ad pmi Stabl Distributios S Ravi ad TS Mavitha Dpartmt of Studis i Statistics Uivrsity of Mysor Maasagagotri Mysuru 570006 Idia. Email:ravi@statistics.uimysor.ac.i

More information

CDS 101: Lecture 5.1 Reachability and State Space Feedback

CDS 101: Lecture 5.1 Reachability and State Space Feedback CDS, Lctur 5. CDS : Lctur 5. Rachability ad Stat Spac Fdback Richard M. Murray ad Hido Mabuchi 5 Octobr 4 Goals: Di rachability o a cotrol systm Giv tsts or rachability o liar systms ad apply to ampls

More information

Available online at Energy Procedia 4 (2011) Energy Procedia 00 (2010) GHGT-10

Available online at   Energy Procedia 4 (2011) Energy Procedia 00 (2010) GHGT-10 Availabl oli at www.scicdirct.com Ergy Procdia 4 (01 170 177 Ergy Procdia 00 (010) 000 000 Ergy Procdia www.lsvir.com/locat/procdia www.lsvir.com/locat/xxx GHGT-10 Exprimtal Studis of CO ad CH 4 Diffusio

More information

+ x. x 2x. 12. dx. 24. dx + 1)

+ x. x 2x. 12. dx. 24. dx + 1) INTEGRATION of FUNCTION of ONE VARIABLE INDEFINITE INTEGRAL Fidig th idfiit itgrals Rductio to basic itgrals, usig th rul f ( ) f ( ) d =... ( ). ( )d. d. d ( ). d. d. d 7. d 8. d 9. d. d. d. d 9. d 9.

More information

NEW VERSION OF SZEGED INDEX AND ITS COMPUTATION FOR SOME NANOTUBES

NEW VERSION OF SZEGED INDEX AND ITS COMPUTATION FOR SOME NANOTUBES Digst Joural of Naomatrials ad Biostructurs Vol 4, No, March 009, p 67-76 NEW VERSION OF SZEGED INDEX AND ITS COMPUTATION FOR SOME NANOTUBES A IRANMANESH a*, O KHORMALI b, I NAJAFI KHALILSARAEE c, B SOLEIMANI

More information

Probability & Statistics,

Probability & Statistics, Probability & Statistics, BITS Pilai K K Birla Goa Campus Dr. Jajati Kshari Sahoo Dpartmt of Mathmatics BITS Pilai, K K Birla Goa Campus Poisso Distributio Poisso Distributio: A radom variabl X is said

More information

Euler s Method for Solving Initial Value Problems in Ordinary Differential Equations.

Euler s Method for Solving Initial Value Problems in Ordinary Differential Equations. Eulr s Mthod for Solvig Iitial Valu Problms i Ordiar Diffrtial Equatios. Suda Fadugba, M.Sc. * ; Bosd Ogurid, Ph.D. ; ad Tao Okulola, M.Sc. 3 Dpartmt of Mathmatical ad Phsical Scics, Af Babalola Uivrsit,

More information

ln x = n e = 20 (nearest integer)

ln x = n e = 20 (nearest integer) H JC Prlim Solutios 6 a + b y a + b / / dy a b 3/ d dy a b at, d Giv quatio of ormal at is y dy ad y wh. d a b () (,) is o th curv a+ b () y.9958 Qustio Solvig () ad (), w hav a, b. Qustio d.77 d d d.77

More information

Worksheet: Taylor Series, Lagrange Error Bound ilearnmath.net

Worksheet: Taylor Series, Lagrange Error Bound ilearnmath.net Taylor s Thorm & Lagrag Error Bouds Actual Error This is th ral amout o rror, ot th rror boud (worst cas scario). It is th dirc btw th actual () ad th polyomial. Stps:. Plug -valu ito () to gt a valu.

More information

Exact Solutions for a Class of Nonlinear Singular Two-Point Boundary Value Problems: The Decomposition Method

Exact Solutions for a Class of Nonlinear Singular Two-Point Boundary Value Problems: The Decomposition Method Exact Solutios for a Class of Noliear Sigular Two-Poit Boudary Value Problems: The Decompositio Method Abd Elhalim Ebaid Departmet of Mathematics, Faculty of Sciece, Tabuk Uiversity, P O Box 741, Tabuki

More information

Modified Decomposition Method by Adomian and. Rach for Solving Nonlinear Volterra Integro- Differential Equations

Modified Decomposition Method by Adomian and. Rach for Solving Nonlinear Volterra Integro- Differential Equations Noliear Aalysis ad Differetial Equatios, Vol. 5, 27, o. 4, 57-7 HIKARI Ltd, www.m-hikari.com https://doi.org/.2988/ade.27.62 Modified Decompositio Method by Adomia ad Rach for Solvig Noliear Volterra Itegro-

More information

SOME IDENTITIES FOR THE GENERALIZED POLY-GENOCCHI POLYNOMIALS WITH THE PARAMETERS A, B AND C

SOME IDENTITIES FOR THE GENERALIZED POLY-GENOCCHI POLYNOMIALS WITH THE PARAMETERS A, B AND C Joural of Mathatical Aalysis ISSN: 2217-3412, URL: www.ilirias.co/ja Volu 8 Issu 1 2017, Pags 156-163 SOME IDENTITIES FOR THE GENERALIZED POLY-GENOCCHI POLYNOMIALS WITH THE PARAMETERS A, B AND C BURAK

More information

Digital Signal Processing, Fall 2006

Digital Signal Processing, Fall 2006 Digital Sigal Procssig, Fall 6 Lctur 9: Th Discrt Fourir Trasfor Zhg-Hua Ta Dpartt of Elctroic Systs Aalborg Uivrsity, Dar zt@o.aau.d Digital Sigal Procssig, I, Zhg-Hua Ta, 6 Cours at a glac MM Discrt-ti

More information

A semi-analytical approach for stress concentration of cantilever beams with circular holes under bending

A semi-analytical approach for stress concentration of cantilever beams with circular holes under bending A smi-aaltical approach for strss coctratio of catilvr bams with circular hols udr bdig 梁 力 Po-Yua Ch ad Jg-Tzog Ch Graduat Studt, Dpartmt of Harbor ad ivr Egirig Distiguishd Profssor, Dpartmt of Harbor

More information

Chapter 4 - The Fourier Series

Chapter 4 - The Fourier Series M. J. Robrts - 8/8/4 Chaptr 4 - Th Fourir Sris Slctd Solutios (I this solutio maual, th symbol,, is usd for priodic covolutio bcaus th prfrrd symbol which appars i th txt is ot i th fot slctio of th word

More information

Mixed Mode Oscillations as a Mechanism for Pseudo-Plateau Bursting

Mixed Mode Oscillations as a Mechanism for Pseudo-Plateau Bursting Mixd Mod Oscillatios as a Mchaism for Psudo-Platau Burstig Richard Brtram Dpartmt of Mathmatics Florida Stat Uivrsity Tallahass, FL Collaborators ad Support Thodor Vo Marti Wchslbrgr Joël Tabak Uivrsity

More information

Numerov-Cooley Method : 1-D Schr. Eq. Last time: Rydberg, Klein, Rees Method and Long-Range Model G(v), B(v) rotation-vibration constants.

Numerov-Cooley Method : 1-D Schr. Eq. Last time: Rydberg, Klein, Rees Method and Long-Range Model G(v), B(v) rotation-vibration constants. Numrov-Cooly Mthod : 1-D Schr. Eq. Last tim: Rydbrg, Kli, Rs Mthod ad Log-Rag Modl G(v), B(v) rotatio-vibratio costats 9-1 V J (x) pottial rgy curv x = R R Ev,J, v,j, all cocivabl xprimts wp( x, t) = ai

More information

Lectures 9 IIR Systems: First Order System

Lectures 9 IIR Systems: First Order System EE3054 Sigals ad Systms Lcturs 9 IIR Systms: First Ordr Systm Yao Wag Polytchic Uivrsity Som slids icludd ar xtractd from lctur prstatios prpard by McCllla ad Schafr Lics Ifo for SPFirst Slids This work

More information

Global Chaos Synchronization of the Hyperchaotic Qi Systems by Sliding Mode Control

Global Chaos Synchronization of the Hyperchaotic Qi Systems by Sliding Mode Control Dr. V. Sudarapadia t al. / Itratioal Joural o Computr Scic ad Egirig (IJCSE) Global Chaos Sychroizatio of th Hyprchaotic Qi Systms by Slidig Mod Cotrol Dr. V. Sudarapadia Profssor, Rsarch ad Dvlopmt Ctr

More information

Journal of Modern Applied Statistical Methods

Journal of Modern Applied Statistical Methods Joural of Modr Applid Statistical Mthods Volum Issu Articl 6 --03 O Som Proprtis of a Htrogous Trasfr Fuctio Ivolvig Symmtric Saturatd Liar (SATLINS) with Hyprbolic Tagt (TANH) Trasfr Fuctios Christophr

More information

EFFECT OF P-NORMS ON THE ACCURACY ORDER OF NUMERICAL SOLUTION ERRORS IN CFD

EFFECT OF P-NORMS ON THE ACCURACY ORDER OF NUMERICAL SOLUTION ERRORS IN CFD rocdigs of NIT 00 opyright 00 by ABM 3 th Brazilia ogrss of Thrmal Scics ad girig Dcmbr 05-0, 00, brladia, MG, Brazil T O -NORMS ON TH ARAY ORDR O NMRIAL SOLTION RRORS IN D arlos Hriqu Marchi, marchi@ufpr.br

More information

2617 Mark Scheme June 2005 Mark Scheme 2617 June 2005

2617 Mark Scheme June 2005 Mark Scheme 2617 June 2005 Mark Schm 67 Ju 5 GENERAL INSTRUCTIONS Marks i th mark schm ar plicitly dsigatd as M, A, B, E or G. M marks ("mthod" ar for a attmpt to us a corrct mthod (ot mrly for statig th mthod. A marks ("accuracy"

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

Ordinary Differential Equations

Ordinary Differential Equations Basi Nomlatur MAE 0 all 005 Egirig Aalsis Ltur Nots o: Ordiar Diffrtial Equatios Author: Profssor Albrt Y. Tog Tpist: Sakurako Takahashi Cosidr a gral O. D. E. with t as th idpdt variabl, ad th dpdt variabl.

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

Washington State University

Washington State University he 3 Ktics ad Ractor Dsig Sprg, 00 Washgto Stat Uivrsity Dpartmt of hmical Egrg Richard L. Zollars Exam # You will hav o hour (60 muts) to complt this xam which cosists of four (4) problms. You may us

More information

ELECTRONIC APPENDIX TO: ELASTIC-PLASTIC CONTACT OF A ROUGH SURFACE WITH WEIERSTRASS PROFILE. Yan-Fei Gao and A. F. Bower

ELECTRONIC APPENDIX TO: ELASTIC-PLASTIC CONTACT OF A ROUGH SURFACE WITH WEIERSTRASS PROFILE. Yan-Fei Gao and A. F. Bower ELECTRONIC APPENDIX TO: ELASTIC-PLASTIC CONTACT OF A ROUGH SURFACE WITH WEIERSTRASS PROFILE Ya-Fi Gao ad A. F. Bowr Divisio of Egirig, Brow Uivrsity, Providc, RI 9, USA Appdix A: Approximat xprssios for

More information

UNIT 2: MATHEMATICAL ENVIRONMENT

UNIT 2: MATHEMATICAL ENVIRONMENT UNIT : MATHEMATICAL ENVIRONMENT. Itroductio This uit itroducs som basic mathmatical cocpts ad rlats thm to th otatio usd i th cours. Wh ou hav workd through this uit ou should: apprciat that a mathmatical

More information

LECTURE 13 Filling the bands. Occupancy of Available Energy Levels

LECTURE 13 Filling the bands. Occupancy of Available Energy Levels LUR 3 illig th bads Occupacy o Availabl rgy Lvls W hav dtrmid ad a dsity o stats. W also d a way o dtrmiig i a stat is illd or ot at a giv tmpratur. h distributio o th rgis o a larg umbr o particls ad

More information

A Strain-based Non-linear Elastic Model for Geomaterials

A Strain-based Non-linear Elastic Model for Geomaterials A Strai-basd No-liar Elastic Modl for Gomatrials ANDREW HEATH Dpartmt of Architctur ad Civil Egirig Uivrsity of Bath Bath, BA2 7AY UNITED KINGDOM A.Hath@bath.ac.uk http://www.bath.ac.uk/ac Abstract: -

More information

Difference -Analytical Method of The One-Dimensional Convection-Diffusion Equation

Difference -Analytical Method of The One-Dimensional Convection-Diffusion Equation Diffrnc -Analytical Mthod of Th On-Dimnsional Convction-Diffusion Equation Dalabav Umurdin Dpartmnt mathmatic modlling, Univrsity of orld Economy and Diplomacy, Uzbistan Abstract. An analytical diffrncing

More information

Technical Support Document Bias of the Minimum Statistic

Technical Support Document Bias of the Minimum Statistic Tchical Support Documt Bias o th Miimum Stattic Itroductio Th papr pla how to driv th bias o th miimum stattic i a radom sampl o siz rom dtributios with a shit paramtr (also kow as thrshold paramtr. Ths

More information

Empirical Study in Finite Correlation Coefficient in Two Phase Estimation

Empirical Study in Finite Correlation Coefficient in Two Phase Estimation M. Khoshvisa Griffith Uivrsity Griffith Busiss School Australia F. Kaymarm Massachustts Istitut of Tchology Dpartmt of Mchaical girig USA H. P. Sigh R. Sigh Vikram Uivrsity Dpartmt of Mathmatics ad Statistics

More information

A Review of Complex Arithmetic

A Review of Complex Arithmetic /0/005 Rviw of omplx Arithmti.do /9 A Rviw of omplx Arithmti A omplx valu has both a ral ad imagiary ompot: { } ad Im{ } a R b so that w a xprss this omplx valu as: whr. a + b Just as a ral valu a b xprssd

More information

Rational Approximation for the one-dimensional Bratu Equation

Rational Approximation for the one-dimensional Bratu Equation Intrnational Journal of Enginring & Tchnology IJET-IJES Vol:3 o:05 5 Rational Approximation for th on-dimnsional Bratu Equation Moustafa Aly Soliman Chmical Enginring Dpartmnt, Th British Univrsity in

More information

Performance Rating of the Type 1 Half Logistic Gompertz Distribution: An Analytical Approach

Performance Rating of the Type 1 Half Logistic Gompertz Distribution: An Analytical Approach Amrica Joural of Mathmatics ad Statistics 27, 7(3): 93-98 DOI:.5923/j.ajms.2773. Prformac Ratig of th Typ Half Logistic Gomprtz Distributio: A Aalytical Approach Ogud A. A. *, Osghal O. I., Audu A. T.

More information

Sundials and Linear Algebra

Sundials and Linear Algebra Sundials and Linar Algbra M. Scot Swan July 2, 25 Most txts on crating sundials ar dirctd towards thos who ar solly intrstd in making and using sundials and usually assums minimal mathmatical background.

More information

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

Part B: Transform Methods. Professor E. Ambikairajah UNSW, Australia Part B: Trasform Mthods Chaptr 3: Discrt-Tim Fourir Trasform (DTFT) 3. Discrt Tim Fourir Trasform (DTFT) 3. Proprtis of DTFT 3.3 Discrt Fourir Trasform (DFT) 3.4 Paddig with Zros ad frqucy Rsolutio 3.5

More information

Solid State Device Fundamentals

Solid State Device Fundamentals 8 Biasd - Juctio Solid Stat Dvic Fudamtals 8. Biasd - Juctio ENS 345 Lctur Cours by Aladr M. Zaitsv aladr.zaitsv@csi.cuy.du Tl: 718 98 81 4N101b Dartmt of Egirig Scic ad Physics Biasig uiolar smicoductor

More information

COMPUTING FOLRIER AND LAPLACE TRANSFORMS. Sven-Ake Gustafson. be a real-valued func'cion, defined for nonnegative arguments.

COMPUTING FOLRIER AND LAPLACE TRANSFORMS. Sven-Ake Gustafson. be a real-valued func'cion, defined for nonnegative arguments. 77 COMPUTNG FOLRER AND LAPLACE TRANSFORMS BY MEANS OF PmER SERES EVALU\TON Sv-Ak Gustafso 1. NOTATONS AND ASSUMPTONS Lt f b a ral-valud fuc'cio, dfid for ogativ argumts. W shall discuss som aspcts of th

More information

DTFT Properties. Example - Determine the DTFT Y ( e ) of n. Let. We can therefore write. From Table 3.1, the DTFT of x[n] is given by 1

DTFT Properties. Example - Determine the DTFT Y ( e ) of n. Let. We can therefore write. From Table 3.1, the DTFT of x[n] is given by 1 DTFT Proprtis Exampl - Dtrmi th DTFT Y of y α µ, α < Lt x α µ, α < W ca thrfor writ y x x From Tabl 3., th DTFT of x is giv by ω X ω α ω Copyright, S. K. Mitra Copyright, S. K. Mitra DTFT Proprtis DTFT

More information

How many neutrino species?

How many neutrino species? ow may utrio scis? Two mthods for dtrmii it lium abudac i uivrs At a collidr umbr of utrio scis Exasio of th uivrs is ovrd by th Fridma quatio R R 8G tot Kc R Whr: :ubblcostat G :Gravitatioal costat 6.

More information

Discrete Fourier Transform. Nuno Vasconcelos UCSD

Discrete Fourier Transform. Nuno Vasconcelos UCSD Discrt Fourir Trasform uo Vascoclos UCSD Liar Shift Ivariat (LSI) systms o of th most importat cocpts i liar systms thory is that of a LSI systm Dfiitio: a systm T that maps [ ito y[ is LSI if ad oly if

More information

Chapter (8) Estimation and Confedence Intervals Examples

Chapter (8) Estimation and Confedence Intervals Examples Chaptr (8) Estimatio ad Cofdc Itrvals Exampls Typs of stimatio: i. Poit stimatio: Exampl (1): Cosidr th sampl obsrvatios, 17,3,5,1,18,6,16,10 8 X i i1 17 3 5 118 6 16 10 116 X 14.5 8 8 8 14.5 is a poit

More information

10. Joint Moments and Joint Characteristic Functions

10. Joint Moments and Joint Characteristic Functions 0 Joit Momts ad Joit Charactristic Fctios Followig sctio 6 i this sctio w shall itrodc varios paramtrs to compactly rprst th iformatio cotaid i th joit pdf of two rvs Giv two rvs ad ad a fctio g x y dfi

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

They must have different numbers of electrons orbiting their nuclei. They must have the same number of neutrons in their nuclei.

They must have different numbers of electrons orbiting their nuclei. They must have the same number of neutrons in their nuclei. 37 1 How may utros ar i a uclus of th uclid l? 20 37 54 2 crtai lmt has svral isotops. Which statmt about ths isotops is corrct? Thy must hav diffrt umbrs of lctros orbitig thir ucli. Thy must hav th sam

More information

Bayesian Test for Lifetime Performance Index of Exponential Distribution under Symmetric Entropy Loss Function

Bayesian Test for Lifetime Performance Index of Exponential Distribution under Symmetric Entropy Loss Function Mathmatics ttrs 08; 4(): 0-4 http://www.scicpublishiggroup.com/j/ml doi: 0.648/j.ml.08040.5 ISSN: 575-503X (Prit); ISSN: 575-5056 (Oli) aysia Tst for iftim Prformac Idx of Expotial Distributio udr Symmtric

More information

Problem Value Score Earned No/Wrong Rec -3 Total

Problem Value Score Earned No/Wrong Rec -3 Total GEORGIA INSTITUTE OF TECHNOLOGY SCHOOL of ELECTRICAL & COMPUTER ENGINEERING ECE6 Fall Quiz # Writt Eam Novmr, NAME: Solutio Kys GT Usram: LAST FIRST.g., gtiit Rcitatio Sctio: Circl t dat & tim w your Rcitatio

More information

Electronic Supplementary Information

Electronic Supplementary Information Elctroic Supplmtary Matrial (ESI) for Joural of Matrials Chmistry A. This joural is Th Royal Socity of Chmistry 2016 Elctroic Supplmtary Iformatio Photolctrochmical Watr Oxidatio usig a Bi 2 MoO 6 / MoO

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 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

Law of large numbers

Law of large numbers Law of larg umbrs Saya Mukhrj W rvisit th law of larg umbrs ad study i som dtail two typs of law of larg umbrs ( 0 = lim S ) p ε ε > 0, Wak law of larrg umbrs [ ] S = ω : lim = p, Strog law of larg umbrs

More information

Chapter 3 Fourier Series Representation of Periodic Signals

Chapter 3 Fourier Series Representation of Periodic Signals Chptr Fourir Sris Rprsttio of Priodic Sigls If ritrry sigl x(t or x[] is xprssd s lir comitio of som sic sigls th rspos of LI systm coms th sum of th idividul rsposs of thos sic sigls Such sic sigl must:

More information

Australian Journal of Basic and Applied Sciences, 4(9): , 2010 ISSN

Australian Journal of Basic and Applied Sciences, 4(9): , 2010 ISSN Australia Joural of Basic ad Applid Scics, 4(9): 4-43, ISSN 99-878 Th Caoical Product of th Diffrtial Equatio with O Turig Poit ad Sigular Poit A Dabbaghia, R Darzi, 3 ANaty ad 4 A Jodayr Akbarfa, Islaic

More information

DETECTION OF RELIABLE SOFTWARE USING SPRT ON TIME DOMAIN DATA

DETECTION OF RELIABLE SOFTWARE USING SPRT ON TIME DOMAIN DATA Itratioal Joural of Computr Scic, Egirig ad Applicatios (IJCSEA Vol., No.4, August DETECTION OF RELIABLE SOFTWARE USING SRT ON TIME DOMAIN DATA G.Krisha Moha ad Dr. Satya rasad Ravi Radr, Dpt. of Computr

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

Character sums over generalized Lehmer numbers

Character sums over generalized Lehmer numbers Ma t al. Joural of Iualitis ad Applicatios 206 206:270 DOI 0.86/s3660-06-23-y R E S E A R C H Op Accss Charactr sums ovr gralizd Lhmr umbrs Yuakui Ma, Hui Ch 2, Zhzh Qi 2 ad Tiapig Zhag 2* * Corrspodc:

More information

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA NE APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA Mirca I CÎRNU Ph Dp o Mathmatics III Faculty o Applid Scincs Univrsity Polithnica o Bucharst Cirnumirca @yahoocom Abstract In a rcnt papr [] 5 th indinit intgrals

More information

Chapter At each point (x, y) on the curve, y satisfies the condition

Chapter At each point (x, y) on the curve, y satisfies the condition Chaptr 6. At ach poit (, y) o th curv, y satisfis th coditio d y 6; th li y = 5 is tagt to th curv at th poit whr =. I Erciss -6, valuat th itgral ivolvig si ad cosi.. cos si. si 5 cos 5. si cos 5. cos

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

A Novel Approach to Recovering Depth from Defocus

A Novel Approach to Recovering Depth from Defocus Ssors & Trasducrs 03 by IFSA http://www.ssorsportal.com A Novl Approach to Rcovrig Dpth from Dfocus H Zhipa Liu Zhzhog Wu Qiufg ad Fu Lifag Collg of Egirig Northast Agricultural Uivrsity 50030 Harbi Chia

More information

Songklanakarin Journal of Science and Technology SJST belhocine

Songklanakarin Journal of Science and Technology SJST belhocine Exact solutio of boudary valu problm dscribig th covctiv hat trasfr i fully- dvlopd lamiar flow through a circular coduit Joural: Sogklaakari Joural of Scic ad Tchology Mauscript ID SJST-- Mauscript Typ:

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

Analysis of the power losses in the three-phase high-current busducts

Analysis of the power losses in the three-phase high-current busducts Computr Applicatios i Elctrical Egirig Vol. 3 5 Aalysis of th powr losss i th thr-phas high-currt busucts Tomasz Szczgiliak, Zygmut Piątk, Dariusz Kusiak Częstochowa Uivrsity of Tchology 4- Częstochowa,

More information