DESIGN AND FINITE ELEMENT MODE ANALYSIS OF NONCIRCULAR GEAR

Size: px
Start display at page:

Download "DESIGN AND FINITE ELEMENT MODE ANALYSIS OF NONCIRCULAR GEAR"

Transcription

1 DESIGN AND FINITE ELEMENT MODE ANALYSIS OF NONCIRCULAR GEAR Cho Li 1, Ki Cheg 2, Dtog Qi 1, Cicho Zhu 1, Hu Qiu 3, Xiohu R 1 1. The Stte Key Lbortory o Mechicl Trsmissio, Chogqig Uiversity, Chi 2. School o Egieerig d Desig, Bruel Uiversity, UK 3. Deprtmet o Mechicl Egieerig, Kyushu Sgyo Uiversity, Jp Abstrct The ocirculr ger trsmissio is importt brch o the ger trsmissio, it is chrcterized by its compct structure, good dymic equilibrtio d other dvtges, d c be used i the utomobile, egieerig mchie, ship, mchie tool, vitio d spcelight ield etc. Studyig o the dymics eture o ocirculr ger trsmissio c improve the bility to crry lods o, reduce the vibrtio d oise o, icrese the lie o the ocirculr ger trsmissio mchie, provides guidce or the desig o the ocirculr ger, d hs sigiict theories d prcticl meigs. I this pper, the ger trsmissio techique is used to studied the desig method o the ocirculr ger, which cotis distributio o teeth o the pitch curve, desigs o the tooth tip curve d the tooth root curve, desig o the tooth proile curve, the ger system dymics priciple is itroduced to estblish dymics model or the ocirculr ger; bsic theory o iite elemet d mode lysis method re pplied, iite elemet model or the ocirculr ger is estblished, turl vibrtio chrcteristic o the ocirculr ger is studied. Ad the ovl ger is tke s exmple, the mthemtics sotwre MthCAD, the 3D modelig sotwre UG d the iite elemet sotwre ABAQUS re used to relize precise 3D model o the ovl ger. The iite elemet method is used, the turl vibrtio chrcteristic o the ovl ger is studied, the mi vibrtio types d turl requecies o the ovl ger d tht o the equivlet cylidricl gers re lyzed d compred, the coclusios received relect the dymics perormce o the ovl ger, d solid oudtio is lid or dymics reserch d egieerig pplictio o the ovl ger trsmissio. Keywords: Nocirculr ger, Fiite elemet method, Nturl requecy, Nturl vibrtio shpe. 73

2 1. Itroductio The ocirculr ger is importt brch o ger trsmissio, c be used to trsmit movemet d power betwee two itersectt xes, is chrcterized by its compct structure, good dymic equilibrtio d other dvtges, d c be pplied i utomobile, egieerig mchie, ship, mchie tool, vitio d spce light ield etc. The curretly, the studyig work o ocirculr ger cocetrtes o geometry modelig, kiemtics, mchiig etc, while tht o dymics is much less. Studyig o the dymics eture o the ocirculr ger trsmissio c improve the bility to crry lods o reduce the vibrtio d oise, icrese the lie o the ocirculr ger trsmissio mchie, provides guidce or the desig o the ocirculr ger, d there re sigiict theories d prcticl meigs. 2. Desig o the Nocirculr Ger The pitch curve o the ocirculr ger is ocirculr, which mkes the desig o the ocirculr ger diicult. The keys o the ocirculr ger desig re to determie the positio o the pitch curve o ech tooth, the tooth tip curve, the tooth root curve d the tooth proile curve o the ocirculr ger First, it give poit o the pitch curve s begiig poit. The determie the positios or let d right tooth proile o ech tooth by clcultig rc legth ccordig to pitch distce d spirl thickess [1]. 2.1 The Tooth Tip Curve d Tooth Root Curve The tooth tip curve d the tooth root curve o the ocirculr ger re orml equl-distce curves o the pitch curve, the orml distces betwee them d the pitch curve re the tooth ddedum d the tooth root height respectively[1], the show i Fig. 1. From Fig. 1 the tooth tip curve ormul c be writte s. 2 2 r = r + h + 2rh si µ (1) Where: r Tooth tip curve rdius, r Pitch curve rdius, h Tooth ddedum, µ Agle betwee tgetil directio d rdil directio o poit (P) o pitch curve. r µ = rct (2) dr dϕ h cos µ θ = ϕ rcsi (3) r Where: θ Polr gle o tooth tip curve, ϕ Polr gle o pitch curve. The tooth root curve ormul c be writte s. 74

3 Where: r Tooth root curve rdius, Where: θ Polr gle o tooth root curve. 2.2 The Tooth Proile Curve 2 2 r = r + h + 2rh si µ (4) h Tooth dededum. h cos µ θ = ϕ + rcsi (5) r The tooth proile curve o the cylidricl ger is ivolute o the bsic circle, d c be settled ccordig to the bsic circle. The tooth proile curve o the ocirculr ger is computed rom evolute o tooth proile, d the proile curve o ech tooth is dieret[2]. The tooth proile curve o the ocirculr ger c be derived rom pitch curve ormul by lytic method s show i Fig Pitch curve, 2 Root curvem, 3 Tip curve. 1 Pitch curve, 2 Let tooth proile, 3 Right tooth proile. Fig. 1. Tip curve d root curve Fig. 2. Tooth proile curve From Fig. 2 the right tooth proile curve ormul o the ocirculr ger c be writte s x r cosϕ cos( ϕ + µ + α ) r yr r si ϕ si( ϕ + µ + α ) (6) Where: xr X coordites vlue o right tooth proile, yr Y coordites o right tooth proile, α Pressure gle o tool, Distce rom itersectio poit betwee pitch curve d orml o tooth proile to tooth proile log orml directio o tooth proile. Let tooth proile curve ormul o the ocirculr ger c be writte s. x r cosϕ ± cos( ϕ + µ α ) y l l r siϕ ± si( ϕ + µ α ) (7) Where: x X l coordites o let tooth proile, y Y l coordites o let tooth proile. From the ger meshig theory. = cosα (8) S Where: S Arc legth o the pitch rom poit () to itersectio poit ( ) betwee the pitch curve d the tooth proile curve. The tooth proile curve o the ocirculr ger c be relized by two methods: 1) The progrmmig, which is diicult to commo desiger. 2) The equivlet method, which use the ivolute o the equivlet cylidricl ger to substitute the tooth proile curve o the ocirculr ger, d mke the model imprecise. All these 75

4 mke the lysis o the ocirculr ger diicult. This pper ims t this problem, tkes the ovl ger s exmple, uses the tooth proile curve ormul, combies mthemtic sotwre MthCAD, sotwre UG d iite elemet sotwre ABAQUS, d relizes the precise model o the ovl ger. 2.3 Ovl Ger Modelig The pitch curve ormul o the ovl ger c be writte s. r (1 k ) /(1 k cos( ϕ)) 2 = (9) Where: = 2, k Eccetricity, Rdius o log xis. The pitch curve o the ovl ger is symmetricl with the X-xis d Y-xis o crtesi coordite. For the desig coveiece, the tooth umber Z = 4 C + 2 (C is positive iteger), d the sectios t log d short xes should be tooth d lveolus respectively. The desig steps o ovl ger modelig re show i Fig. 3. The prmeters o the ovl ger i this pper: The tooth umber Z = 22, modulus m = 5mm, eccetricity e =.1, tooth ddedum h = 5mm, tooth height h = mm, tooth width B = 25mm, rdius (legth hl xles) 54. mm =. The two ovl gers re sme. = 728, ier rdius r i 25mm Give desig prmeters: tooth umber z, modulus m, eccetricity k, d solve rdius. Determie the polr gles o the itersectio poits o the pitch curve d the tooth proile curves. Use MthCAD d the tooth proile curve ormul to product coordite dt o key poits o the tooth proile curves. Import the poit dt ito UG, obti the tooth proile curve by ittig with cube splie, obti the ple sketch o the ovl ger by rc legth, corer, trim, d mirror uctio, sve the ple sketch s IGS ile, import ito ABAQUS. The get the 3D model o the ovl ger by extrude uctio, show i Fig. 4. Fig. 3. Desig o the ovl ger modelig 3. Fiite Elemet Model o the Ovl Ger The ABAQUS is oe o the most dvced lrge-scle geerl iite elemet sotwre i the world, d hs powerul uctio i big stri, olier (geometry, mteril d boudry), viscoelstic, dymic stress, d cotct problem ields etc [3]. 76

5 11 2 I this pper, the mteril o the ovl ger is 45 steel, Youg s modulus E = 2. 1 N / mm, Poisso s 3 3 rtio µ =. 3, d Desity ρ = kg / m. Crete mteril steel uder mteril module, crete the ovl ger sectio, set mteril steel s property o the ovl ger sectio, d ppoit to sectio o the ovl ger. The boudry coditio o iite elemet model or the ovl ger c be set ccordig to the ctul workig coditio. I the meshig process o the ovl gers, itererece it is pplied betwee iside surce d xis with splie, the itererece it betwee xis d the ger c be cosidered s rigid coectio i the iite elemet model, d the iluece o splie is eglected. The tolerce o this simpliictio is smll to dymic study. I order to relect the ctul coditio o ger meshig correctly, the ier surce o the ovl ger is restricted, d displcemets log X xis, Y xis, Z xis d rottios roud with X d Y xis re restricted. I the ABAQUS, the 3D solid uit oly hs three displcemet reedoms. I order to restrict rottio reedom o the ovl ger s ier surce, couplig must be dded to couple the ier surce to poit o the ceter rottig xis o the ovl ger, d reedoms o the ovl ger s ier surce c be restricted by settig the reerece poit s reedoms. The boudry coditio o the ovl ger c be pplied to iitil step. The mode is determied by turl property o the ger system, d it is irrespective with outer lods, so it is eedless to set the lod boudry coditio or the ovl ger. I course o the meshig, distortio should be reduced rthest, s or the problem tht the grids distorts bdly, smll sized lier reduced itegrtio uit c be used, or the 3D problem, hexhedro uit should be pplied utmost, which c get better result with lower cst, the result received orm tetrhedro uit is imprecise, so lrge umbers o uits must be pplied to get better result, which mkes computig cost icrese gretly. Accordig to the priciple bove, swept meshig techique is pplied i the this model, C3D8R uit (8 odes hexhedro reduced itegrtio uit) is used, d 196 uits d odes re received. The iite elemet model o the ovl ger completed is show i Fig. 5. Fig. 4. The 3D model o the ovl ger Fig. 5. The iite elemet model o the ovl ger 4. Clcultig the Nturl Mode d Nturl The methods o clcultig the turl mode d turl requecy. Accordig to the mechicl system dymics theory d the iite elemet theory, the movemet dieretil equtio o the multi-reedom system c be writte s[4]. [ M ]{ u } + [ C ]{ u } + [ K ]{ u} = { p (t )} Where [ M ] Mss mtrix, { u } Accelertio mtrix, [ ] [ K Stiess ] mtrix, { u} Displcemet mtrix, { p(t) } (1) C Dmpig mtrix, { } Outer lod mtrix. u Velocity mtrix, 77

6 Whe the dmpig orce is eglected d the system is ree o lod, the movemet dieretil equtio o udmped ree vibrtio system c be writte s[4]. ([ ] ω 2 [ M ]){ φ} = K (11) Where ω Frequecies o system, { φ } Eigevector o system. The LANCZOS method d the subspce itertive method re provided to clculte eigevlue. Whe the system hs my reedoms d pletiul chrcteristic modes re requested, it is much quicker by pplyig the LANCZOS method, while ew chrcteristic modes (< 2) re requested, it is much quicker by usig subspce itertive method. I this pper, the LANCZOS method is pplied. 5. Alyticl Result The structure vibrtio c be expressed s lier combitio o ech order turl vibrtio shpe, while lower order vibrtio shpe hs big iluece o structure vibrtio, d ply decisive role i structure s dymic chrcter. First 5 to 1 orders re eeded oly whe mode lysis. I order to expli the dymic chrcter o the ovl ger cotrstively, the iite elemet models o equivlet cylidricl gers ( degree, 3 degree, 6 degree, 9 degree) re estblished, d the turl vibrtios d turl requecies re clculted d lyzed. The 1st, 2d, 3rd, 5th, 7th, 1th mode vibrtio shpes re show i Fig. 6 () ~ (), d the vibrtio shpes d turl requecies re show i Tble 1. The Tble 1 d Fig. 7 show tht the turl requecies o the ovl ger lie betwee the correspodig order s turl requecies o the big sectio ( degree) d tht o the smll sectio (9 degree), they re bigger th tht o the big sectio d smller th tht o the smll sectio. The turl requecy icreses with the order icreses. The vibrtio shpes o the ovl ger re sme with tht o equivlet cylidricl ger, but the orders rise re dieret. Compred with the cylidricl ger, the requecies to ech order o the ovl ger is dieret obviously, while the requecies to ech order o the cylidricl ger my be sme or similr. The reso is tht the cylidricl ger is symmetricl with the rottig ceter bsolutely, while the ovl ger is symmetricl with the rottig ceter icompletely. The Tble 1 d Fig. 6 show tht the 3rd, 4th d 6th mode vibrtio shpes re sme, the 5th d 9th mode vibrtio shpes re sme, d the 7th d 8th mode vibrtio shpes re sme. The mi diereces lie i tht the vibrtio directios o ech tooth re dieret. The Fig. 8 shows tht the turl requecies to ech order o the equivlet cylidricl ger icrese while the polr gle o the ovl ger icreses d the pitch curve rdius decrese. The compred with cylidricl ger, the distce mog the mplitudes o ech tooth to ech mode o the ovl ger is quite big. For exmple, or the 2d SZ mode, the mplitude o the tooth bout the big sectio ( degree) is quite big, while the tooth bout the smll sectio does t vibrte bsiclly. 78

7 The Fig. 6 d Tble 1 show tht the mi vibrtio shpes o the ovl ger is the DZ mode d YZ mode, while rdil vibrtio is quite smll. So the DZ mode d YZ mode is the vibrtio shpe which is most possible to rouse resoce o the ovl ger. I desig o the ovl ger trsmissio system, the turl vibrtio shpes d turl requecies should be cosidered dequtely, the workig requecy should keeps wy rom the turl requecies to void resoce. Tble 1: Nturl requecies d vibrtio shpes o the ovl ger d the equivlet gers Model Order Ovl ger Type DZ1 SZ DZ2 DZ2 YZ DZ2 DZ3 DZ3 YZ DZ Type DZ1 DZ1 SZ DZ2 DZ2 DZ3 DZ3 YZ YZ DZ Type DZ1 DZ1 SZ DZ2 DZ2 DZ3 DZ3 YZ YZ DZ Type DZ1 DZ1 SZ DZ2 DZ2 DZ3 DZ3 YZ YZ DZ Type SZ DZ1 DZ1 DZ2 DZ2 YZ YZ DZ3 DZ3 DZ3 DZ1 1st olio vibrtio,dz2 2d olio vibrtio,sz Bevel vibrtio,dz3 3rd olio vibrtio,dz4 4th olio vibrtio,yz Circle vibrtio () 1st mode vibrtio (b) 2d mode vibrtio (c) 3rd mode vibrtio shpe shpe shpe Fig. 6. (d) 5th mode vibrtio (e) 7th mode vibrtio () 1th mode vibrtio shpe shpe shpe Mode vibrtio shpes o the ovl ger 3 Ovl deg 9 deg 25 (F/Hz) Order Fig. 7. Reltio o requecies betwee the ovl ger d equivlet ger 79

8 st 3rd 4th 6th 8th 1th (F/Hz) Pitch curev rdis (R/cm) Fig. 8. Reltio betwee requecies d rdius 6. Coclusio I this pper, the desig method o the ocirculr ger is studied by usig ger trsmissio techique, the mthemtics sotwre MthCAD, the 3D solid modelig sotwre d the iite elemet sotwre re combied to relize precise model o the ovl ger, d solid oudtio is lid or lysis o the ovl ger. The ger system dymics priciple is itroduced to estblish dymics model or the ocirculr ger. The bsic theory o iite elemet d mode lysis method re pplied, the iite elemet model or the ocirculr ger is estblished, d turl vibrtio chrcteristic o the ocirculr ger is studied. The iite elemet method is used, the turl vibrtio chrcteristic o the ovl ger is studied, the mi vibrtio shpes d turl requecies o the ovl ger d tht o the equivlet cylidricl gers re lyzed d compred, the coclusios received relect the dymics perormce o the ovl ger, d solid oudtio is lid or dymics reserch d egieerig pplictio o the ovl ger. Ackowledgemet The uthors wish to ckowledge the ssistce d support o the Ntiol Sciece d Techology Plig Key Project o Chi (No. 26BAF1B7-1). Reereces [1] Wu Xutg, Nocirculr Ger d Vrible Rtio Trsmissio, Beijig: Mchiery Idustry Press, Chi, pp. 52~53, [2] Li Fusheg, Desig o Nocirculr Ger d Specil Ger, Beijig: Mchiery Idustry Press, Chi, pp. 57~59, [3] Zhug Qu, Accidece Guide or ABAQUS Fiite Elemet Sotwre, Beijig: Tsighu Uiversity Press, Chi, pp. 49~8, [4] Li Rug, Dymics o Ger System, Beijig: Sciece Press, Chi, pp. 69~96,

BC Calculus Review Sheet

BC Calculus Review Sheet BC Clculus Review Sheet Whe you see the words. 1. Fid the re of the ubouded regio represeted by the itegrl (sometimes 1 f ( ) clled horizotl improper itegrl). This is wht you thik of doig.... Fid the re

More information

sin m a d F m d F m h F dy a dy a D h m h m, D a D a c1cosh c3cos 0

sin m a d F m d F m h F dy a dy a D h m h m, D a D a c1cosh c3cos 0 Q1. The free vibrtio of the plte is give by By ssumig h w w D t, si cos w W x y t B t Substitutig the deflectio ito the goverig equtio yields For the plte give, the mode shpe W hs the form h D W W W si

More information

HIGHER SCHOOL CERTIFICATE EXAMINATION MATHEMATICS 3 UNIT (ADDITIONAL) AND 3/4 UNIT (COMMON) Time allowed Two hours (Plus 5 minutes reading time)

HIGHER SCHOOL CERTIFICATE EXAMINATION MATHEMATICS 3 UNIT (ADDITIONAL) AND 3/4 UNIT (COMMON) Time allowed Two hours (Plus 5 minutes reading time) HIGHER SCHOOL CERTIFICATE EXAMINATION 999 MATHEMATICS 3 UNIT (ADDITIONAL) AND 3/ UNIT (COMMON) Time llowed Two hours (Plus 5 miutes redig time) DIRECTIONS TO CANDIDATES Attempt ALL questios. ALL questios

More information

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

DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS. Assoc. Prof. Dr. Burak Kelleci. Spring 2018 DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS Assoc. Prof. Dr. Bur Kelleci Sprig 8 OUTLINE The Z-Trsform The Regio of covergece for the Z-trsform The Iverse Z-Trsform Geometric

More information

Students must always use correct mathematical notation, not calculator notation. the set of positive integers and zero, {0,1, 2, 3,...

Students must always use correct mathematical notation, not calculator notation. the set of positive integers and zero, {0,1, 2, 3,... Appedices Of the vrious ottios i use, the IB hs chose to dopt system of ottio bsed o the recommedtios of the Itertiol Orgiztio for Stdrdiztio (ISO). This ottio is used i the emitio ppers for this course

More information

Particle in a Box. and the state function is. In this case, the Hermitian operator. The b.c. restrict us to 0 x a. x A sin for 0 x a, and 0 otherwise

Particle in a Box. and the state function is. In this case, the Hermitian operator. The b.c. restrict us to 0 x a. x A sin for 0 x a, and 0 otherwise Prticle i Box We must hve me where = 1,,3 Solvig for E, π h E = = where = 1,,3, m 8m d the stte fuctio is x A si for 0 x, d 0 otherwise x ˆ d KE V. m dx I this cse, the Hermiti opertor 0iside the box The

More information

Module 4. Signal Representation and Baseband Processing. Version 2 ECE IIT, Kharagpur

Module 4. Signal Representation and Baseband Processing. Version 2 ECE IIT, Kharagpur Module 4 Sigl Represettio d Bsed Processig Versio ECE IIT, Khrgpur Lesso 5 Orthogolity Versio ECE IIT, Khrgpur Ater redig this lesso, you will ler out Bsic cocept o orthogolity d orthoormlity; Strum -

More information

b a 2 ((g(x))2 (f(x)) 2 dx

b a 2 ((g(x))2 (f(x)) 2 dx Clc II Fll 005 MATH Nme: T3 Istructios: Write swers to problems o seprte pper. You my NOT use clcultors or y electroic devices or otes of y kid. Ech st rred problem is extr credit d ech is worth 5 poits.

More information

Prior distributions. July 29, 2002

Prior distributions. July 29, 2002 Prior distributios Aledre Tchourbov PKI 357, UNOmh, South 67th St. Omh, NE 688-694, USA Phoe: 4554-64 E-mil: tchourb@cse.ul.edu July 9, Abstrct This documet itroduces prior distributios for the purposes

More information

Here and further the following reduction of record is applied.

Here and further the following reduction of record is applied. MODL OF SRSSD-SRAIND SA OF MULILAYR MASSS WIH RGARD FOR NON-IDAL CONAC OF LAYRS V.G.Piskuov, A.V.Mrchuk We cosider lyered desig i rectgulr crtesi system o coordites. o xes o coordites x, y, there corresod

More information

SOLUTION OF DIFFERENTIAL EQUATION FOR THE EULER-BERNOULLI BEAM

SOLUTION OF DIFFERENTIAL EQUATION FOR THE EULER-BERNOULLI BEAM Jourl of Applied Mthemtics d Computtiol Mechics () 57-6 SOUION O DIERENIA EQUAION OR HE EUER-ERNOUI EAM Izbel Zmorsk Istitute of Mthemtics Czestochow Uiversit of echolog Częstochow Pold izbel.zmorsk@im.pcz.pl

More information

INTEGRATION TECHNIQUES (TRIG, LOG, EXP FUNCTIONS)

INTEGRATION TECHNIQUES (TRIG, LOG, EXP FUNCTIONS) Mthemtics Revisio Guides Itegrtig Trig, Log d Ep Fuctios Pge of MK HOME TUITION Mthemtics Revisio Guides Level: AS / A Level AQA : C Edecel: C OCR: C OCR MEI: C INTEGRATION TECHNIQUES (TRIG, LOG, EXP FUNCTIONS)

More information

Fig. 1. I a. V ag I c. I n. V cg. Z n Z Y. I b. V bg

Fig. 1. I a. V ag I c. I n. V cg. Z n Z Y. I b. V bg ymmetricl Compoets equece impedces Although the followig focuses o lods, the results pply eqully well to lies, or lies d lods. Red these otes together with sectios.6 d.9 of text. Cosider the -coected lced

More information

Statistics for Financial Engineering Session 1: Linear Algebra Review March 18 th, 2006

Statistics for Financial Engineering Session 1: Linear Algebra Review March 18 th, 2006 Sttistics for Ficil Egieerig Sessio : Lier Algebr Review rch 8 th, 6 Topics Itroductio to trices trix opertios Determits d Crmer s rule Eigevlues d Eigevectors Quiz The cotet of Sessio my be fmilir to

More information

Frequency-domain Characteristics of Discrete-time LTI Systems

Frequency-domain Characteristics of Discrete-time LTI Systems requecy-domi Chrcteristics of Discrete-time LTI Systems Prof. Siripog Potisuk LTI System descriptio Previous bsis fuctio: uit smple or DT impulse The iput sequece is represeted s lier combitio of shifted

More information

1. (25 points) Use the limit definition of the definite integral and the sum formulas to compute. [1 x + x2

1. (25 points) Use the limit definition of the definite integral and the sum formulas to compute. [1 x + x2 Mth 3, Clculus II Fil Exm Solutios. (5 poits) Use the limit defiitio of the defiite itegrl d the sum formuls to compute 3 x + x. Check your swer by usig the Fudmetl Theorem of Clculus. Solutio: The limit

More information

Vectors. Vectors in Plane ( 2

Vectors. Vectors in Plane ( 2 Vectors Vectors i Ple ( ) The ide bout vector is to represet directiol force Tht mes tht every vector should hve two compoets directio (directiol slope) d mgitude (the legth) I the ple we preset vector

More information

Variational Iteration Method for Solving Volterra and Fredholm Integral Equations of the Second Kind

Variational Iteration Method for Solving Volterra and Fredholm Integral Equations of the Second Kind Ge. Mth. Notes, Vol. 2, No. 1, Jury 211, pp. 143-148 ISSN 2219-7184; Copyright ICSRS Publictio, 211 www.i-csrs.org Avilble free olie t http://www.gem.i Vritiol Itertio Method for Solvig Volterr d Fredholm

More information

Taylor Polynomials. The Tangent Line. (a, f (a)) and has the same slope as the curve y = f (x) at that point. It is the best

Taylor Polynomials. The Tangent Line. (a, f (a)) and has the same slope as the curve y = f (x) at that point. It is the best Tylor Polyomils Let f () = e d let p() = 1 + + 1 + 1 6 3 Without usig clcultor, evlute f (1) d p(1) Ok, I m still witig With little effort it is possible to evlute p(1) = 1 + 1 + 1 (144) + 6 1 (178) =

More information

National Quali cations AHEXEMPLAR PAPER ONLY

National Quali cations AHEXEMPLAR PAPER ONLY Ntiol Quli ctios AHEXEMPLAR PAPER ONLY EP/AH/0 Mthemtics Dte Not pplicble Durtio hours Totl mrks 00 Attempt ALL questios. You my use clcultor. Full credit will be give oly to solutios which coti pproprite

More information

PROGRESSIONS AND SERIES

PROGRESSIONS AND SERIES PROGRESSIONS AND SERIES A sequece is lso clled progressio. We ow study three importt types of sequeces: () The Arithmetic Progressio, () The Geometric Progressio, () The Hrmoic Progressio. Arithmetic Progressio.

More information

Chapter 25 Sturm-Liouville problem (II)

Chapter 25 Sturm-Liouville problem (II) Chpter 5 Sturm-Liouville problem (II Speer: Lug-Sheg Chie Reerece: [] Veerle Ledou, Study o Specil Algorithms or solvig Sturm-Liouville d Schrodiger Equtios. [] 王信華教授, chpter 8, lecture ote o Ordiry Dieretil

More information

INFINITE SERIES. ,... having infinite number of terms is called infinite sequence and its indicated sum, i.e., a 1

INFINITE SERIES. ,... having infinite number of terms is called infinite sequence and its indicated sum, i.e., a 1 Appedix A.. Itroductio As discussed i the Chpter 9 o Sequeces d Series, sequece,,...,,... hvig ifiite umber of terms is clled ifiite sequece d its idicted sum, i.e., + + +... + +... is clled ifite series

More information

S(x)along the bar (shear force diagram) by cutting the bar at x and imposing force_y equilibrium.

S(x)along the bar (shear force diagram) by cutting the bar at x and imposing force_y equilibrium. mmetric leder Bems i Bedig Lodig Coditios o ech ectio () pplied -Forces & z-omets The resultts t sectio re: the bedig momet () d z re sectio smmetr es the sher force () [ for sleder bems stresses d deformtio

More information

Schrödinger Equation Via Laplace-Beltrami Operator

Schrödinger Equation Via Laplace-Beltrami Operator IOSR Jourl of Mthemtics (IOSR-JM) e-issn: 78-578, p-issn: 39-765X. Volume 3, Issue 6 Ver. III (Nov. - Dec. 7), PP 9-95 www.iosrjourls.org Schrödiger Equtio Vi Lplce-Beltrmi Opertor Esi İ Eskitşçioğlu,

More information

5.1 - Areas and Distances

5.1 - Areas and Distances Mth 3B Midterm Review Writte by Victori Kl vtkl@mth.ucsb.edu SH 63u Office Hours: R 9:5 - :5m The midterm will cover the sectios for which you hve received homework d feedbck Sectios.9-6.5 i your book.

More information

334 MATHS SERIES DSE MATHS PREVIEW VERSION B SAMPLE TEST & FULL SOLUTION

334 MATHS SERIES DSE MATHS PREVIEW VERSION B SAMPLE TEST & FULL SOLUTION MATHS SERIES DSE MATHS PREVIEW VERSION B SAMPLE TEST & FULL SOLUTION TEST SAMPLE TEST III - P APER Questio Distributio INSTRUCTIONS:. Attempt ALL questios.. Uless otherwise specified, ll worig must be

More information

Convergence rates of approximate sums of Riemann integrals

Convergence rates of approximate sums of Riemann integrals Jourl of Approximtio Theory 6 (9 477 49 www.elsevier.com/locte/jt Covergece rtes of pproximte sums of Riem itegrls Hiroyuki Tski Grdute School of Pure d Applied Sciece, Uiversity of Tsukub, Tsukub Ibrki

More information

BC Calculus Path to a Five Problems

BC Calculus Path to a Five Problems BC Clculus Pth to Five Problems # Topic Completed U -Substitutio Rule Itegrtio by Prts 3 Prtil Frctios 4 Improper Itegrls 5 Arc Legth 6 Euler s Method 7 Logistic Growth 8 Vectors & Prmetrics 9 Polr Grphig

More information

Pre-Calculus - Chapter 3 Sections Notes

Pre-Calculus - Chapter 3 Sections Notes Pre-Clculus - Chpter 3 Sectios 3.1-3.4- Notes Properties o Epoets (Review) 1. ( )( ) = + 2. ( ) =, (c) = 3. 0 = 1 4. - = 1/( ) 5. 6. c Epoetil Fuctios (Sectio 3.1) Deiitio o Epoetil Fuctios The uctio deied

More information

Qn Suggested Solution Marking Scheme 1 y. G1 Shape with at least 2 [2]

Qn Suggested Solution Marking Scheme 1 y. G1 Shape with at least 2 [2] Mrkig Scheme for HCI 8 Prelim Pper Q Suggested Solutio Mrkig Scheme y G Shpe with t lest [] fetures correct y = f'( ) G ll fetures correct SR: The mimum poit could be i the first or secod qudrt. -itercept

More information

FACULTY OF MATHEMATICAL STUDIES MATHEMATICS FOR PART I ENGINEERING. Lectures

FACULTY OF MATHEMATICAL STUDIES MATHEMATICS FOR PART I ENGINEERING. Lectures FACULTY OF MATHEMATICAL STUDIES MATHEMATICS FOR PART I ENGINEERING Lectures MODULE 0 FURTHER CALCULUS II. Sequeces d series. Rolle s theorem d me vlue theorems 3. Tlor s d Mcluri s theorems 4. L Hopitl

More information

2. Infinite Series 3. Power Series 4. Taylor Series 5. Review Questions and Exercises 6. Sequences and Series with Maple

2. Infinite Series 3. Power Series 4. Taylor Series 5. Review Questions and Exercises 6. Sequences and Series with Maple Chpter II CALCULUS II.4 Sequeces d Series II.4 SEQUENCES AND SERIES Objectives: After the completio of this sectio the studet - should recll the defiitios of the covergece of sequece, d some limits; -

More information

Using Quantum Mechanics in Simple Systems Chapter 15

Using Quantum Mechanics in Simple Systems Chapter 15 /16/17 Qutiztio rises whe the loctio of prticle (here electro) is cofied to dimesiolly smll regio of spce qutum cofiemet. Usig Qutum Mechics i Simple Systems Chpter 15 The simplest system tht c be cosidered

More information

Integral Operator Defined by k th Hadamard Product

Integral Operator Defined by k th Hadamard Product ITB Sci Vol 4 A No 35-5 35 Itegrl Opertor Deied by th Hdmrd Product Msli Drus & Rbh W Ibrhim School o Mthemticl Scieces Fculty o sciece d Techology Uiversiti Kebgs Mlysi Bgi 436 Selgor Drul Ehs Mlysi Emil:

More information

0 otherwise. sin( nx)sin( kx) 0 otherwise. cos( nx) sin( kx) dx 0 for all integers n, k.

0 otherwise. sin( nx)sin( kx) 0 otherwise. cos( nx) sin( kx) dx 0 for all integers n, k. . Computtio of Fourier Series I this sectio, we compute the Fourier coefficiets, f ( x) cos( x) b si( x) d b, i the Fourier series To do this, we eed the followig result o the orthogolity of the trigoometric

More information

Infinite Series Sequences: terms nth term Listing Terms of a Sequence 2 n recursively defined n+1 Pattern Recognition for Sequences Ex:

Infinite Series Sequences: terms nth term Listing Terms of a Sequence 2 n recursively defined n+1 Pattern Recognition for Sequences Ex: Ifiite Series Sequeces: A sequece i defied s fuctio whose domi is the set of positive itegers. Usully it s esier to deote sequece i subscript form rther th fuctio ottio.,, 3, re the terms of the sequece

More information

MA123, Chapter 9: Computing some integrals (pp )

MA123, Chapter 9: Computing some integrals (pp ) MA13, Chpter 9: Computig some itegrls (pp. 189-05) Dte: Chpter Gols: Uderstd how to use bsic summtio formuls to evlute more complex sums. Uderstd how to compute its of rtiol fuctios t ifiity. Uderstd how

More information

A GENERAL METHOD FOR SOLVING ORDINARY DIFFERENTIAL EQUATIONS: THE FROBENIUS (OR SERIES) METHOD

A GENERAL METHOD FOR SOLVING ORDINARY DIFFERENTIAL EQUATIONS: THE FROBENIUS (OR SERIES) METHOD Diol Bgoo () A GENERAL METHOD FOR SOLVING ORDINARY DIFFERENTIAL EQUATIONS: THE FROBENIUS (OR SERIES) METHOD I. Itroductio The first seprtio of vribles (see pplictios to Newto s equtios) is ver useful method

More information

Section 6.3: Geometric Sequences

Section 6.3: Geometric Sequences 40 Chpter 6 Sectio 6.: Geometric Sequeces My jobs offer ul cost-of-livig icrese to keep slries cosistet with ifltio. Suppose, for exmple, recet college grdute fids positio s sles mger erig ul slry of $6,000.

More information

Numerical Solutions of Fredholm Integral Equations Using Bernstein Polynomials

Numerical Solutions of Fredholm Integral Equations Using Bernstein Polynomials Numericl Solutios of Fredholm Itegrl Equtios Usig erstei Polyomils A. Shiri, M. S. Islm Istitute of Nturl Scieces, Uited Itertiol Uiversity, Dhk-, gldesh Deprtmet of Mthemtics, Uiversity of Dhk, Dhk-,

More information

F x = 2x λy 2 z 3 = 0 (1) F y = 2y λ2xyz 3 = 0 (2) F z = 2z λ3xy 2 z 2 = 0 (3) F λ = (xy 2 z 3 2) = 0. (4) 2z 3xy 2 z 2. 2x y 2 z 3 = 2y 2xyz 3 = ) 2

F x = 2x λy 2 z 3 = 0 (1) F y = 2y λ2xyz 3 = 0 (2) F z = 2z λ3xy 2 z 2 = 0 (3) F λ = (xy 2 z 3 2) = 0. (4) 2z 3xy 2 z 2. 2x y 2 z 3 = 2y 2xyz 3 = ) 2 0 微甲 07- 班期中考解答和評分標準 5%) Fid the poits o the surfce xy z = tht re closest to the origi d lso the shortest distce betwee the surfce d the origi Solutio Cosider the Lgrge fuctio F x, y, z, λ) = x + y + z

More information

FOURIER SERIES PART I: DEFINITIONS AND EXAMPLES. To a 2π-periodic function f(x) we will associate a trigonometric series. a n cos(nx) + b n sin(nx),

FOURIER SERIES PART I: DEFINITIONS AND EXAMPLES. To a 2π-periodic function f(x) we will associate a trigonometric series. a n cos(nx) + b n sin(nx), FOURIER SERIES PART I: DEFINITIONS AND EXAMPLES To -periodic fuctio f() we will ssocite trigoometric series + cos() + b si(), or i terms of the epoetil e i, series of the form c e i. Z For most of the

More information

Mathematics for Engineers Part II (ISE) Version 1.1/

Mathematics for Engineers Part II (ISE) Version 1.1/ Mthemtics or Egieers Prt II (ISE Versio /4-6- Curves i Prmetric descriptio o curves We exted the theory o derivtives d itegrls to uctios whose rge re vectors i isted o rel umers Deiitio : A curve C i is

More information

lecture 16: Introduction to Least Squares Approximation

lecture 16: Introduction to Least Squares Approximation 97 lecture 16: Itroductio to Lest Squres Approximtio.4 Lest squres pproximtio The miimx criterio is ituitive objective for pproximtig fuctio. However, i my cses it is more ppelig (for both computtio d

More information

Numbers (Part I) -- Solutions

Numbers (Part I) -- Solutions Ley College -- For AMATYC SML Mth Competitio Cochig Sessios v.., [/7/00] sme s /6/009 versio, with presettio improvemets Numbers Prt I) -- Solutios. The equtio b c 008 hs solutio i which, b, c re distict

More information

APPLICATION OF DIFFERENCE EQUATIONS TO CERTAIN TRIDIAGONAL MATRICES

APPLICATION OF DIFFERENCE EQUATIONS TO CERTAIN TRIDIAGONAL MATRICES Scietific Reserch of the Istitute of Mthetics d Coputer Sciece 3() 0, 5-0 APPLICATION OF DIFFERENCE EQUATIONS TO CERTAIN TRIDIAGONAL MATRICES Jolt Borows, Le Łcińs, Jowit Rychlews Istitute of Mthetics,

More information

Canonical Form and Separability of PPT States on Multiple Quantum Spaces

Canonical Form and Separability of PPT States on Multiple Quantum Spaces Coicl Form d Seprbility of PPT Sttes o Multiple Qutum Spces Xio-Hog Wg d Sho-Mig Fei, 2 rxiv:qut-ph/050445v 20 Apr 2005 Deprtmet of Mthemtics, Cpitl Norml Uiversity, Beijig, Chi 2 Istitute of Applied Mthemtics,

More information

Chapter 10: The Z-Transform Adapted from: Lecture notes from MIT, Binghamton University Dr. Hamid R. Rabiee Fall 2013

Chapter 10: The Z-Transform Adapted from: Lecture notes from MIT, Binghamton University Dr. Hamid R. Rabiee Fall 2013 Sigls & Systems Chpter 0: The Z-Trsform Adpted from: Lecture otes from MIT, Bighmto Uiversity Dr. Hmid R. Rbiee Fll 03 Lecture 5 Chpter 0 Lecture 6 Chpter 0 Outlie Itroductio to the -Trsform Properties

More information

PhysicsAndMathsTutor.com

PhysicsAndMathsTutor.com PhysicsAdMthsTutor.com PhysicsAdMthsTutor.com Jue 009 4. Give tht y rsih ( ), > 0, () fid d y d, givig your swer s simplified frctio. () Leve lk () Hece, or otherwise, fid 4 d, 4 [ ( )] givig your swer

More information

Fourier Series and Applications

Fourier Series and Applications 9/7/9 Fourier Series d Applictios Fuctios epsio is doe to uderstd the better i powers o etc. My iportt probles ivolvig prtil dieretil equtios c be solved provided give uctio c be epressed s iiite su o

More information

Definite Integral. The Left and Right Sums

Definite Integral. The Left and Right Sums Clculus Li Vs Defiite Itegrl. The Left d Right Sums The defiite itegrl rises from the questio of fidig the re betwee give curve d x-xis o itervl. The re uder curve c be esily clculted if the curve is give

More information

Circle Marker Based Distance Measurement Using a Single Camera

Circle Marker Based Distance Measurement Using a Single Camera Circle Mrker Bsed Distce Mesuremet Usig Sigle Cmer Yu-To Co, Ji-Mig Wg, Yu-Ku Su, d Xio-Jie Du Abstrct A ew distce mesuremet method with the use of sigle cmer d circle mrker is preseted. The distce mesuremet

More information

1 Section 8.1: Sequences. 2 Section 8.2: Innite Series. 1.1 Limit Rules. 1.2 Common Sequence Limits. 2.1 Denition. 2.

1 Section 8.1: Sequences. 2 Section 8.2: Innite Series. 1.1 Limit Rules. 1.2 Common Sequence Limits. 2.1 Denition. 2. Clculus II d Alytic Geometry Sectio 8.: Sequeces. Limit Rules Give coverget sequeces f g; fb g with lim = A; lim b = B. Sum Rule: lim( + b ) = A + B, Dierece Rule: lim( b ) = A B, roduct Rule: lim b =

More information

Closed Newton-Cotes Integration

Closed Newton-Cotes Integration Closed Newto-Cotes Itegrtio Jmes Keeslig This documet will discuss Newto-Cotes Itegrtio. Other methods of umericl itegrtio will be discussed i other posts. The other methods will iclude the Trpezoidl Rule,

More information

PEPERIKSAAN PERCUBAAN SPM TAHUN 2007 ADDITIONAL MATHEMATICS. Form Five. Paper 2. Two hours and thirty minutes

PEPERIKSAAN PERCUBAAN SPM TAHUN 2007 ADDITIONAL MATHEMATICS. Form Five. Paper 2. Two hours and thirty minutes SULIT 347/ 347/ Form Five Additiol Mthemtics Pper September 007 ½ hours PEPERIKSAAN PERCUBAAN SPM TAHUN 007 ADDITIONAL MATHEMATICS Form Five Pper Two hours d thirty miutes DO NOT OPEN THIS QUESTION PAPER

More information

Linear Algebra. Lecture 1 September 19, 2011

Linear Algebra. Lecture 1 September 19, 2011 Lier Algebr Lecture September 9, Outlie Course iformtio Motivtio Outlie of the course Wht is lier lgebr? Chpter. Systems of Lier Equtios. Solvig Lier Systems. Vectors d Mtrices Course iformtio Istructor:

More information

[Ismibayli*, 5(3): March, 2016] ISSN: (I2OR), Publication Impact Factor: 3.785

[Ismibayli*, 5(3): March, 2016] ISSN: (I2OR), Publication Impact Factor: 3.785 IJERT INTERNATIONAL JOURNAL OF ENGINEERING CIENCE & REEARCH TECHNOLOGY IMULATION OF ELECTROMAGNETIC FIELD FROM MICROWAVE RECTANGULAR WAVEGUIDE TO CIRCULAR IN TRANITION DEVICE E.G.Ismibyli, I.J.Islmov,

More information

POWER SERIES R. E. SHOWALTER

POWER SERIES R. E. SHOWALTER POWER SERIES R. E. SHOWALTER. sequeces We deote by lim = tht the limit of the sequece { } is the umber. By this we me tht for y ε > 0 there is iteger N such tht < ε for ll itegers N. This mkes precise

More information

A GENERALIZATION OF GAUSS THEOREM ON QUADRATIC FORMS

A GENERALIZATION OF GAUSS THEOREM ON QUADRATIC FORMS A GENERALIZATION OF GAU THEOREM ON QUADRATIC FORM Nicole I Brtu d Adi N Cret Deprtmet of Mth - Criov Uiversity, Romi ABTRACT A origil result cocerig the extesio of Guss s theorem from the theory of biry

More information

EXERCISE a a a 5. + a 15 NEETIIT.COM

EXERCISE a a a 5. + a 15 NEETIIT.COM - Dowlod our droid App. Sigle choice Type Questios EXERCISE -. The first term of A.P. of cosecutive iteger is p +. The sum of (p + ) terms of this series c be expressed s () (p + ) () (p + ) (p + ) ()

More information

Name: A2RCC Midterm Review Unit 1: Functions and Relations Know your parent functions!

Name: A2RCC Midterm Review Unit 1: Functions and Relations Know your parent functions! Nme: ARCC Midterm Review Uit 1: Fuctios d Reltios Kow your pret fuctios! 1. The ccompyig grph shows the mout of rdio-ctivity over time. Defiitio of fuctio. Defiitio of 1-1. Which digrm represets oe-to-oe

More information

f(bx) dx = f dx = dx l dx f(0) log b x a + l log b a 2ɛ log b a.

f(bx) dx = f dx = dx l dx f(0) log b x a + l log b a 2ɛ log b a. Eercise 5 For y < A < B, we hve B A f fb B d = = A B A f d f d For y ɛ >, there re N > δ >, such tht d The for y < A < δ d B > N, we hve ba f d f A bb f d l By ba A A B A bb ba fb d f d = ba < m{, b}δ

More information

Mathematics Extension 2

Mathematics Extension 2 05 Bored of Studies Tril Emitios Mthemtics Etesio Writte by Crrotsticks & Trebl Geerl Istructios Totl Mrks 00 Redig time 5 miutes. Workig time 3 hours. Write usig blck or blue pe. Blck pe is preferred.

More information

(1 q an+b ). n=0. n=0

(1 q an+b ). n=0. n=0 AN ELEMENTARY DERIVATION OF THE ASYMPTOTICS OF PARTITION FUNCTIONS Diel M Ke Abstrct Let S,b { + b : 0} where is iteger Let P,b deote the umber of prtitios of ito elemets of S,b I prticulr, we hve the

More information

is continuous at x 2 and g(x) 2. Oil spilled from a ruptured tanker spreads in a circle whose area increases at a

is continuous at x 2 and g(x) 2. Oil spilled from a ruptured tanker spreads in a circle whose area increases at a . Cosider two fuctios f () d g () defied o itervl I cotiig. f () is cotiuous t d g() is discotiuous t. Which of the followig is true bout fuctios f g d f g, the sum d the product of f d g, respectively?

More information

Numerical Integration

Numerical Integration Numericl tegrtio Newto-Cotes Numericl tegrtio Scheme Replce complicted uctio or tulted dt with some pproimtig uctio tht is esy to itegrte d d 3-7 Roerto Muscedere The itegrtio o some uctios c e very esy

More information

Linear Programming. Preliminaries

Linear Programming. Preliminaries Lier Progrmmig Prelimiries Optimiztio ethods: 3L Objectives To itroduce lier progrmmig problems (LPP To discuss the stdrd d coicl form of LPP To discuss elemetry opertio for lier set of equtios Optimiztio

More information

Indices and Logarithms

Indices and Logarithms the Further Mthemtics etwork www.fmetwork.org.uk V 7 SUMMARY SHEET AS Core Idices d Logrithms The mi ides re AQA Ed MEI OCR Surds C C C C Lws of idices C C C C Zero, egtive d frctiol idices C C C C Bsic

More information

Algebra II, Chapter 7. Homework 12/5/2016. Harding Charter Prep Dr. Michael T. Lewchuk. Section 7.1 nth roots and Rational Exponents

Algebra II, Chapter 7. Homework 12/5/2016. Harding Charter Prep Dr. Michael T. Lewchuk. Section 7.1 nth roots and Rational Exponents Algebr II, Chpter 7 Hrdig Chrter Prep 06-07 Dr. Michel T. Lewchuk Test scores re vilble olie. I will ot discuss the test. st retke opportuit Sturd Dec. If ou hve ot tke the test, it is our resposibilit

More information

NUMERICAL RESEARCH ON THE EQUIVALENT TRANSFORMATION BETWEEN STRUCTURAL DYNAMIC ANALYSIS IN TIME-DOMAIN AND FREQUENCY DOMAIN

NUMERICAL RESEARCH ON THE EQUIVALENT TRANSFORMATION BETWEEN STRUCTURAL DYNAMIC ANALYSIS IN TIME-DOMAIN AND FREQUENCY DOMAIN he 4 th World Coferece o Erthquke Egieerig October -7, 8, Beijig, Chi NUMERICAL RESEARCH ON HE EQUIVALEN RANSFORMAION BEWEEN SRUCURAL DYNAMIC ANALYSIS IN IME-DOMAIN AND FREQUENCY DOMAIN Yuelig Jig,Jibo

More information

S. Socrate 2013 K. Qian

S. Socrate 2013 K. Qian S. Socrte 213 K. Qi odig Coditios o ech Sectio () pplied lodig oly log the is () of the br. The oly iterl resultt t y sectios is the il force N() Fid N()log the br (il force digrm) by cuttig the br t ech

More information

1.3 Continuous Functions and Riemann Sums

1.3 Continuous Functions and Riemann Sums mth riem sums, prt 0 Cotiuous Fuctios d Riem Sums I Exmple we sw tht lim Lower() = lim Upper() for the fuctio!! f (x) = + x o [0, ] This is o ccidet It is exmple of the followig theorem THEOREM Let f be

More information

General properties of definite integrals

General properties of definite integrals Roerto s Notes o Itegrl Clculus Chpter 4: Defiite itegrls d the FTC Sectio Geerl properties of defiite itegrls Wht you eed to kow lredy: Wht defiite Riem itegrl is. Wht you c ler here: Some key properties

More information

=> PARALLEL INTERCONNECTION. Basic Properties LTI Systems. The Commutative Property. Convolution. The Commutative Property. The Distributive Property

=> PARALLEL INTERCONNECTION. Basic Properties LTI Systems. The Commutative Property. Convolution. The Commutative Property. The Distributive Property Lier Time-Ivrit Bsic Properties LTI The Commuttive Property The Distributive Property The Associtive Property Ti -6.4 / Chpter Covolutio y ] x ] ] x ]* ] x ] ] y] y ( t ) + x( τ ) h( t τ ) dτ x( t) * h(

More information

Chapter 2 Infinite Series Page 1 of 9

Chapter 2 Infinite Series Page 1 of 9 Chpter Ifiite eries Pge of 9 Chpter : Ifiite eries ectio A Itroductio to Ifiite eries By the ed of this sectio you will be ble to uderstd wht is met by covergece d divergece of ifiite series recogise geometric

More information

Surface profiles with zero and finite adhesion force and adhesion instabilities

Surface profiles with zero and finite adhesion force and adhesion instabilities Surfce profiles with zero d fiite dhesio force d dhesio istbilities Vleti L. Popov Techische Uiversität Berli, Str. des 7. Jui 35, 063 Berli, Germy Abstrct. A simple but geerl lysis of the stbility of

More information

Riemann Integration. Chapter 1

Riemann Integration. Chapter 1 Mesure, Itegrtio & Rel Alysis. Prelimiry editio. 8 July 2018. 2018 Sheldo Axler 1 Chpter 1 Riem Itegrtio This chpter reviews Riem itegrtio. Riem itegrtio uses rectgles to pproximte res uder grphs. This

More information

Physics of Semiconductor Devices Vol.10

Physics of Semiconductor Devices Vol.10 10-1 Vector Spce Physics of Semicoductor Devices Vol.10 Lier Algebr for Vector Alysis To prove Crmer s rule which ws used without proof, we expli the vector lgebr tht ws explied ituitively i Vol. 9, by

More information

UNIVERSITY OF CALICUT SCHOOL OF DISTANCE EDUCATION. (2014 Admn. onwards) III Semester. B.Sc. Mathematics CORE COURSE CALCULUS AND ANALYTICAL GEOMETRY

UNIVERSITY OF CALICUT SCHOOL OF DISTANCE EDUCATION. (2014 Admn. onwards) III Semester. B.Sc. Mathematics CORE COURSE CALCULUS AND ANALYTICAL GEOMETRY UNIVERSITY OF CALICUT SCHOOL OF DISTANCE EDUCATION (0 Adm. owrds) III Semester B.Sc. Mthemtics CORE COURSE CALCULUS AND ANALYTICAL GEOMETRY Questio Bk & Aswer Key. l l () =... 0.00 b) 0 c). l d =... c

More information

THE NATIONAL UNIVERSITY OF IRELAND, CORK COLÁISTE NA hollscoile, CORCAIGH UNIVERSITY COLLEGE, CORK SUMMER EXAMINATION 2005 FIRST ENGINEERING

THE NATIONAL UNIVERSITY OF IRELAND, CORK COLÁISTE NA hollscoile, CORCAIGH UNIVERSITY COLLEGE, CORK SUMMER EXAMINATION 2005 FIRST ENGINEERING OLLSCOIL NA héireann, CORCAIGH THE NATIONAL UNIVERSITY OF IRELAND, CORK COLÁISTE NA hollscoile, CORCAIGH UNIVERSITY COLLEGE, CORK SUMMER EXAMINATION 2005 FIRST ENGINEERING MATHEMATICS MA008 Clculus d Lier

More information

f(x) is a function of x and it is defined on the set R of real numbers. If then f(x) is continuous at x=x 0, where x 0 R.

f(x) is a function of x and it is defined on the set R of real numbers. If then f(x) is continuous at x=x 0, where x 0 R. MATHEMATICAL PRELIMINARIES Limit Cotiuity Coverget squece Series Dieretible uctios Itegrble uctios Summtio deiitio o itegrl Me vlue theorem Me vlue theorem or itegrls Tylor's theorem Computer represettio

More information

Reduction of Higher Order Linear Ordinary Differential Equations into the Second Order and Integral Evaluation of Exact Solutions

Reduction of Higher Order Linear Ordinary Differential Equations into the Second Order and Integral Evaluation of Exact Solutions Mthemtic Aeter, Vol. 4, 04, o., 75-89 Reductio o Higher Order Lier Ordiry Dieretil Equtios ito the Secod Order d Itegrl Evlutio o Ect Solutios Guw Nugroho* Deprtmet o Egieerig Physics, Istitut Tekologi

More information

Chapter 7 Infinite Series

Chapter 7 Infinite Series MA Ifiite Series Asst.Prof.Dr.Supree Liswdi Chpter 7 Ifiite Series Sectio 7. Sequece A sequece c be thought of s list of umbers writte i defiite order:,,...,,... 2 The umber is clled the first term, 2

More information

National Quali cations SPECIMEN ONLY

National Quali cations SPECIMEN ONLY AH Ntiol Quli ctios SPECIMEN ONLY SQ/AH/0 Mthemtics Dte Not pplicble Durtio hours Totl mrks 00 Attempt ALL questios. You my use clcultor. Full credit will be give oly to solutios which coti pproprite workig.

More information

Name of the Student:

Name of the Student: Egieerig Mthemtics 5 NAME OF THE SUBJECT : Mthemtics I SUBJECT CODE : MA65 MATERIAL NAME : Additiol Prolems MATERIAL CODE : HGAUM REGULATION : R UPDATED ON : M-Jue 5 (Sc the ove QR code for the direct

More information

Power Series Solutions to Generalized Abel Integral Equations

Power Series Solutions to Generalized Abel Integral Equations Itertiol Jourl of Mthemtics d Computtiol Sciece Vol., No. 5, 5, pp. 5-54 http://www.isciece.org/jourl/ijmcs Power Series Solutios to Geerlized Abel Itegrl Equtios Rufi Abdulli * Deprtmet of Physics d Mthemtics,

More information

Certain sufficient conditions on N, p n, q n k summability of orthogonal series

Certain sufficient conditions on N, p n, q n k summability of orthogonal series Avilble olie t www.tjs.com J. Nolier Sci. Appl. 7 014, 7 77 Reserch Article Certi sufficiet coditios o N, p, k summbility of orthogol series Xhevt Z. Krsiqi Deprtmet of Mthemtics d Iformtics, Fculty of

More information

Application: Volume. 6.1 Overture. Cylinders

Application: Volume. 6.1 Overture. Cylinders Applictio: Volume 6 Overture I this chpter we preset other pplictio of the defiite itegrl, this time to fid volumes of certi solids As importt s this prticulr pplictio is, more importt is to recogize ptter

More information

Autar Kaw Benjamin Rigsby. Transforming Numerical Methods Education for STEM Undergraduates

Autar Kaw Benjamin Rigsby.   Transforming Numerical Methods Education for STEM Undergraduates Autr Kw Bejmi Rigsby http://m.mthforcollege.com Trsformig Numericl Methods Eductio for STEM Udergrdutes http://m.mthforcollege.com . solve set of simulteous lier equtios usig Nïve Guss elimitio,. ler the

More information

Angle of incidence estimation for converted-waves

Angle of incidence estimation for converted-waves Agle of icidece estimtio for coverted-wves Crlos E. Nieto d Robert R. tewrt Agle of icidece estimtio ABTRACT Amplitude-versus-gle AA lysis represets li betwee te geologicl properties of roc iterfces d

More information

Graphing Review Part 3: Polynomials

Graphing Review Part 3: Polynomials Grphig Review Prt : Polomils Prbols Recll, tht the grph of f ( ) is prbol. It is eve fuctio, hece it is smmetric bout the bout the -is. This mes tht f ( ) f ( ). Its grph is show below. The poit ( 0,0)

More information

8.1 Arc Length. What is the length of a curve? How can we approximate it? We could do it following the pattern we ve used before

8.1 Arc Length. What is the length of a curve? How can we approximate it? We could do it following the pattern we ve used before 8.1 Arc Legth Wht is the legth of curve? How c we pproximte it? We could do it followig the ptter we ve used efore Use sequece of icresigly short segmets to pproximte the curve: As the segmets get smller

More information

Math 2414 Activity 17 (Due with Final Exam) Determine convergence or divergence of the following alternating series: a 3 5 2n 1 2n 1

Math 2414 Activity 17 (Due with Final Exam) Determine convergence or divergence of the following alternating series: a 3 5 2n 1 2n 1 Mth 44 Activity 7 (Due with Fil Exm) Determie covergece or divergece of the followig ltertig series: l 4 5 6 4 7 8 4 {Hit: Loo t 4 } {Hit: } 5 {Hit: AST or just chec out the prtil sums} {Hit: AST or just

More information

GRAPHING LINEAR EQUATIONS. Linear Equations. x l ( 3,1 ) _x-axis. Origin ( 0, 0 ) Slope = change in y change in x. Equation for l 1.

GRAPHING LINEAR EQUATIONS. Linear Equations. x l ( 3,1 ) _x-axis. Origin ( 0, 0 ) Slope = change in y change in x. Equation for l 1. GRAPHING LINEAR EQUATIONS Qudrt II Qudrt I ORDERED PAIR: The first umer i the ordered pir is the -coordite d the secod umer i the ordered pir is the y-coordite. (, ) Origi ( 0, 0 ) _-is Lier Equtios Qudrt

More information

Theorem 5.3 (Continued) The Fundamental Theorem of Calculus, Part 2: ab,, then. f x dx F x F b F a. a a. f x dx= f x x

Theorem 5.3 (Continued) The Fundamental Theorem of Calculus, Part 2: ab,, then. f x dx F x F b F a. a a. f x dx= f x x Chpter 6 Applictios Itegrtio Sectio 6. Regio Betwee Curves Recll: Theorem 5.3 (Cotiued) The Fudmetl Theorem of Clculus, Prt :,,, the If f is cotiuous t ever poit of [ ] d F is tiderivtive of f o [ ] (

More information

Linford 1. Kyle Linford. Math 211. Honors Project. Theorems to Analyze: Theorem 2.4 The Limit of a Function Involving a Radical (A4)

Linford 1. Kyle Linford. Math 211. Honors Project. Theorems to Analyze: Theorem 2.4 The Limit of a Function Involving a Radical (A4) Liford 1 Kyle Liford Mth 211 Hoors Project Theorems to Alyze: Theorem 2.4 The Limit of Fuctio Ivolvig Rdicl (A4) Theorem 2.8 The Squeeze Theorem (A5) Theorem 2.9 The Limit of Si(x)/x = 1 (p. 85) Theorem

More information

[ 20 ] 1. Inequality exists only between two real numbers (not complex numbers). 2. If a be any real number then one and only one of there hold.

[ 20 ] 1. Inequality exists only between two real numbers (not complex numbers). 2. If a be any real number then one and only one of there hold. [ 0 ]. Iequlity eists oly betwee two rel umbers (ot comple umbers).. If be y rel umber the oe d oly oe of there hold.. If, b 0 the b 0, b 0.. (i) b if b 0 (ii) (iii) (iv) b if b b if either b or b b if

More information

Double Sums of Binomial Coefficients

Double Sums of Binomial Coefficients Itertiol Mthemticl Forum, 3, 008, o. 3, 50-5 Double Sums of Biomil Coefficiets Athoy Sofo School of Computer Sciece d Mthemtics Victori Uiversity, PO Box 448 Melboure, VIC 800, Austrli thoy.sofo@vu.edu.u

More information

( a n ) converges or diverges.

( a n ) converges or diverges. Chpter Ifiite Series Pge of Sectio E Rtio Test Chpter : Ifiite Series By the ed of this sectio you will be ble to uderstd the proof of the rtio test test series for covergece by pplyig the rtio test pprecite

More information