Exact 3-D Solution for System with Rectangular Fin, Part 1

Size: px
Start display at page:

Download "Exact 3-D Solution for System with Rectangular Fin, Part 1"

Transcription

1 th WSEAS Int. Conf. on APPLIED MATHEMATICS Cro Egpt Deceer Exct 3-D Soluton for Sste th Rectngulr Fn Prt MARGARITA BUIKE ANDRIS BUIKIS Insttute of Mthetcs nd Coputer Scence Unverst of Ltv Rn ulv. 9 Rg LV459 LATVIA lz.lv/scentsts/uks.ht Astrct: - In ths pper e construct severl exct nltcl three-densonl solutons for the dstruton of the teperture feld n the ll th rectngulr fn. We ssue tht the het trnsfer process n the ll nd the fn s sttonr. These exct solutons re otned the Green functon ethod n the for of the nd knd Fredhol ntegrl equton. The generlze trdtonl stteents n severl senses e.g. e consder 3-D stteent dfferent oundr condtons nd the het exchnge tke plce t non-hoogeneous envronentl teperture. Ke-Words: - sted-stte three-densonl het exchnge rectngulr fn non-hoogeneous envronent exct nltcl solutons. Introducton Sstes th extended surfces (fns spnes) re relted to refrgertors rdtors engnes nd odern electroncs (PC) etc. Usull ther thetcl odelng s relzed one densonl sted-stte ssuptons []-[5]. In our prevous ppers e hve constructed vrous to densonl nltcl pproxte [6] [] nd exct [] solutons. In ths pper e concentrte our ttenton on one eleent of fn ssel the hole sste (sseled nto rrs of fns) ll e consdered n the second pper. Such stteent essentll generlzes the prole consdered erler n lterture e.g. n pper []. In these to prts of our pper e otn severl ne exct nltcl solutons the Green functon ethod [3]-[6]. L B h ( B R) l B R B R k hb ( R) h ( B R) k k nd tepertures: W B R Mthetcl Forulton of 3-D Prole In ths prt e ll consder full thetcl three-densonl forulton of sted-stte prole for one eleent of sste th rectngulr fn (ths one eleent s depcted th drker color n ttched fgure). Ths thetcl forulton s essentll roder s n our ppers [6]-[]. We ll use follong densonless rguents preters: x z Δ x z B R B R B R B R V ( x z) T V( x z) T T V ( x z) T V ( x z) T T

2 th WSEAS Int. Conf. on APPLIED MATHEMATICS Cro Egpt Deceer Θ ( x z ) T Θ ( xz ) T T Θ ( z ) T Θ ( z ). T T We hve ntroduced follong densonl therl nd geoetrcl preters: k( k ) - het conductvt coeffcent for the fn (ll) h( h ) - het exchnge coeffcent for the fn (ll) B fn dth (thckness) L fn length Δ - thckness of the ll W lls dth (length) R dstnce eteen to fns (fn spcng). Further Θ ( z ) s the surroundng (envronent) teperture on the left (hot) sde (the het source sde) of the ll Θ ( x z )- the surroundng teperture on the rght (cold - the het snk sde) of the ll nd the fn. Fnll V ( x z) ( V ( x z) ) re the densonl tepertures n the fn (ll) here T ( T ) re ntegrl verged envronent tepertures over pproprte edges: W ( ) Δ L W W B T B R L W [ dz Θ( Δ z) d Δ B R W ( ) dx Θ ( x B z) dz dz Θ( Δ L z) d] T W B R d Θ ( z) dz. B R The one eleent of the ll (se) s plced n the don { x [ ] [ ] z [ ] }. The rectngulr fn n densonless rguents occupes the don { x [ l] [ ] z [ ] }. We descre the densonless teperture feld functon V ( x z ) ( V ( x z ) ) n the ll (fn). The fulfll the Lplce equtons: V V V V V V. At frst e consder the three densonl stteent th gven het fluxes fro the flnk surfces (edges) nd fro the top nd the otto edges: B Q ( x ) Q ( x ) 3 z z Q ( x ) Q ( x ). 3 z z () Such tpe of oundr condtons (BC) llos us to ke the exct reducng of ths three-densonl prole to to-densonl prole for Posson equton conservtve vergng ethod [7]- []. Let us ntroduce follong ntegrl verge vlues: Θ V ( x ) V ( x z) dz ϑ ( ) ( z) dz V( x ) V( x z) dz ϑ( x ) Θ( x z) dz. () It rens to relze the ntegrton of n equton usge of the oth BC () (correspondng one pr) nd e otn: V V Q ( x ) V V ( ). Qx (3) Here Q( x ) ( Q3( x ) Q( x ) ) Qx ( ) ( Q3( x ) Q( x )). We dd to n prtl dfferentl equtons (3) needed BC s follo: [ ϑ( ) V] x () (4) [ V ϑ( x ) ] ( ) x (5) Q( x) (6) Q ( x). (7)

3 th WSEAS Int. Conf. on APPLIED MATHEMATICS Cro Egpt Deceer We llo the terl of the fn to e dfferent fro the lls terl. It ens e ust forulte the conugtons condtons on the surfce eteen the ll nd the fn. We ssue the s del therl contct - there s no contct resstnce: V V x x (8). x x (9) We hve follong BC for the fn: [ V ϑ( x ) ] x l [ ] () Q ( x) () [ V ϑ( x ) ] x [ l].() We ssue tht ll condtons hch ensure exstence nd unqueness of clssc soluton of the prole (3)-() e.g. contnut of envronent tepertures consstenc condtons on the sdes of edges etc. re fulflled. Let s enton tht lost ll of the uthors neglgle the het trnsfer trough flnk surfce z (s ell s fro edge z ). We ssue gven (prescred) het fluxes on oth. 3 Exct Soluton of -D Prole 3. Soluton of the Splfed Prole We ould lke to expln the n de of soluton for the -D cse of perodcl sste th constnt densonless envronentl tepertures ϑ ( Θ T ) nd ϑ ( Θ T ). We neglect ddtonll the het fluxes fro flnk edges. In ths prtculr cse e hve follong n equtons for the teperture U ( ) x of the ll respectvel teperture U( x ) of the fn: U U { x [ ] [ ]} (3) U U { x [ l] [ ] }. (4) The BC (6) (7) nd () re ssued to e hoogeneous: U U U. (5) Insted of BC (4) (5) () nd () e hve: U ( U) x x () (6) U ( ) x x (7) U x l [ ] (8) U x [ l]. (9) The conugtons condtons on the lne eteen the ll nd the fn re stll stndng n the for (8) (9) for the functons U( x ) nd U ( ) x. The lner conton of the equtons (8) (9) together th BC (7) llo us rerte the s follong BC on the rght hnd sde of the ll: U x x F( ) () here U U F ( x ) () < x [ l]. On the ssupton tht the functon F ( x ) s gven e cn represent soluton for the ll n ver ell knon for the Green functon: U( x ) G( x υ) () F ( υ ) G ( x υ ). Tkng n the ccount forul () e rerte the soluton for the ll s follo: U ( x ) G ( x υ) U U G ( x υ ) d υ. ζ ζ (3) The expresson of the Green functon n () (3) hs the for (see e.g. [5]): x G ( x ζ ) G n( υ) G ( x ζυ ) (4) n ( πn) μ

4 th WSEAS Int. Conf. on APPLIED MATHEMATICS Cro Egpt Deceer x ϕ( x) ϕ( ζ) G ( x ζ ) ϕ G n ( υ) cos nπ ( υ) cos nπ ( υ). We hve for the frst one-densonl Green functon n (4) the follong expresson for the egenfunctons: ϕ( x) cos( μx) sn( μx) ϕ μ μ ( ) ( ). μ μ μ ( ) μ Here μ re the roots of the trnscendentl equton: μ ( ) tg( μ ). μ Unfortuntel the representton () s unusle s soluton for the ll ecuse of unknon functon F ( x ).e. teperture n the fn U( x ). Tht s h e ll p ttenton to the soluton for the fn no. In the se s for () e cn rerte the conugtons condtons n the for of BC on the left sde of the rectngulr fn: U F( ). (5) x Here the rght hnd sde functon of BC (5) hs the for: U F( x ) U (6) x [ ] [ ]. Then slr s for the ll e cn represent soluton for the fn n follong for: U( x ) F( η ) G( x η ) dη. (7) ( x) φ Here Gx ( ξη ) G ( x ξ ) G ( η) G ( x ) G ( x) ( ) λ κ φ ( x) φ ( ξ) ( x ξ ) G ( ) ψ ( η) ( η) ψ ( x ) φ( x) cos λ sn λ ( x ) λ l φ λ λ ψ ( η) ( ) ( ) cos κ η cos κ η ψ. κ Here λ ( κ ) re the roots of the trnscendentl equtons: λ tn( λl) tn( κ ). λ κ Usng notton () nd representton (7) e cn es otn the follong equton: F ( x ) F( η) Γ( x η) dη (8) Γ ( x ξ η) Gx ( ξ η). Fro () e otn edtel slr representton for the F( ) : F( ) ( υ) Γ (9) F ( υ ) Γ ( υ ). Here e hve ntroduced notton slr to the second equton of the forul (8): Γ ( x ζ υ) G( x ζ υ). (3) No e susttute the representton (9) n the rght hnd sde of forul (8) nd e otn follong second knd Fredhol ntegrl equton regrdng the functon F ( ) : F ( ) ϒ ( ) K( υ) F ( υ). (3) Here e hve ntroduced follong shorter denontons:

5 th WSEAS Int. Conf. on APPLIED MATHEMATICS Cro Egpt Deceer K( υ) Γ ( ηυ ) Γ( η ) dη ϒ ( ) Γ( η) dη Γ ( η υ). (3) When solved ntegrl equton (3) e edtel cn otn the teperture feld n the ll fro the representton (). In ts turn the representton (7) gves the teperture feld n the fn. B the n ll our ppers [6]-[] e restrct ourselves th hoogeneous oundr condtons (5) (7)-(9). 3. Soluton of the Generl Prole (3)-(9) Here no ll e consdered generl cse of non-hoogeneous envronentl teperture: dfferentl equtons (3) th oundr condtons (4)-(). The soluton for the ll nsted of () hs for: V( x ) Ψ ( x ) (33) F ( υ ) G ( x υ ). Here the knon ters re oned together: Ψ ( x ) Q ( ζ ) G ( x ζ) dζ Q ( ζ) G ( x ζ) dζ ϑ ( υ) G ( x υ) ϑ( υ) G ( x υ) dζ Q ( ζ υ) G ( x ζ υ). (34) In the slr for e cn represent soluton for the fn. It looks s follo: V( x ) Ψ( x ) F( η ) G( x η ) dη. The knon functon Ψ ( x ) hs the for: l Ψ ( x ) Q( ξ ) Gx ( ξ) dξ (35) ϑ ( l η) G( x l η) dη l ϑ( ξ Gx ) ( ξ d ) ξ l dξ Q( ξ η) G( x ξ η) dη. (36) We otn nsted of forule (8) nd (9) follong representtons: F( x ) Ψ ( x ) F ( υ) Γ ( x υ) F ( ) Ψ ( ) F( η) Γ( η) dη. (37) We hve ntroduced follong nottons n (37): Ψ ( x ) Ψ( x ) Ψ ( x ) Ψ( x ). We otn follong non-hoogeneous Fredhol ntegrl equton of nd knd n the se s equton (3) n su-secton 3.: F ( ) Φ ( ) K( υ) F ( υ). (38) Here Φ ( ) Ψ ( ) Ψ ( η ) Γ( η ) dη. Ths Fredhol ntegrl equton of nd knd hs contnuous kernel nd t hs unque soluton see e.g. []. Agn hen solved ntegrl equton (38) e cn otn edtel fro (33) the teperture feld n the ll. Then frst forul (37) llos fndng the conton F( x ). In ts turn forul (35) gves the teperture feld n the fn. We fnsh ths prt of our pper th the follong to rerks. Frstl the lst prole (th non-hoogeneous envronent tepertures) nd ts soluton llo conugtng teperture feld th hdrodnc (oton of flud or gs eteen to fns nd long the left edge of the ll). Secondl f e hd 3 rd tpe

6 th WSEAS Int. Conf. on APPLIED MATHEMATICS Cro Egpt Deceer BC nsted of the BC () e ould hve hd full three-densonl prole. 4 Conclusons We hve constructed severl exct three densonl nltcl solutons for one eleent of perodcl sste th rectngulr fn here the ll nd the fn consst of terls hch hve dfferent therl propertes. These solutons re n the for of Fredhol ntegrl equton of nd knd nd hs contnuous kernel. The re spler then the one otned n our pper []. The llo pssng over fro proles for ndvdul fns to proles for fns rrs hch ll e consdered n the prt of ths pper. Acknoledgeents: Reserch s supported Unverst of Ltv (proect Y-ZP9-) nd Councl of Scences of Ltv (grnt 5.55). References: [] Kern D.Q Krus A.D. Extended Surfce Het Trnsfer. McGr-Hll Book Copn. 97. [] Krus A.D. Anlss nd Evluton of Extended Surfce Therl Sstes. Hesphere Pulshng Corporton 98. [3] Mnzoor M. Het Flo through Extended Surfce Het Exchngers. Sprnger-Verlg: Berln nd Ne York 984. [4] Wood A.S. Tuphole G.E. Bhtt M.I.H. Heggs P.J. Perfornce ndctors for sted-stte het trnsfer through fn sseles Trns. ASME Journl of Het Trnsfer pp [5] Wood A.S. Tuphole G.E. Bhtt M.I.H. Heggs P.J. Sted-stte het trnsfer through extended plne surfces Int. Coun. n Het nd Mss Trnsfer No. 995 pp [6] Buks A. To-densonl soluton for het trnsfer n regulr fn ssel. Ltvn Journl of Phscs nd Techncl Scences No pp [7] Buks A. Buke M. Approxte nltcl to-densonl soluton for longtudnl fn of rectngulr profle. Act Unverstts Ltvenss vol pp [8] Buks A. Buke M. Closed to-densonl soluton for het trnsfer n perodcl sste th fn. Proceedngs of the Ltvn Acde of Scences. Secton B Vol.5 Nr pp. 8-. [9] Buke M. Sulton of sted-stte het process for the rectngulr fn-contnng sste Mthetcl Modellng nd Anlss 999 vol. 4 pp [] Mlk M.Y. Wood A.S. Buks A. An pproxte nltcl soluton to flr conugte het trnsfer prole Interntonl ournl of Pure nd Appled Mthetcs Vol. Nr. 4 pp [] Buks A. Buke M. Gusenov S. Anltcl to-densonl solutons for het trnsfer n sste th rectngulr fn. Advnced Coputtonl Methods n Het Trnsfer VIII. WIT press 4 pp [] Lehtnen A. Krvnen R. Anltcl threedensonl soluton for het snk teperture Proceedngs of IMECE p. [3] Crsl H.S. Jeger C.J. Conducton of Het n Solds. Oxford Clrendon Press 959. [4] Őzşk M. Nect. Boundr Vlue Proles of Het Conducton. Dover Pulctons Inc. Mneol Ne York 989. [5] Polnn A.D. Hndook of Lner Prtl Dfferentl Equtons for Engneers nd Scentsts. Chpn&Hll/CRC. (Russn edton ) [6] Stkgold I. Boundr Vlue Proles of Mthetcl Phscs Vol.. SIAM Phldelph. [7] Buks A. Aufgenstellung und Loesung ener Klsse von Proleen der thetschen Phsk t nchtklssschen Zustzedngungen. Rostock. Mth. Kolloq pp (In Gern) [8] Buks A. Proles of thetcl phscs th dscontnuous coeffcents nd ther pplctons. Rg p. (In Russn unpulshed ook) [9] Buks A. Conservtve vergng s n pproxte ethod for soluton of soe drect nd nverse het trnsfer proles. Advnced Coputtonl Methods n Het Trnsfer IX. WIT Press 6. p [] Vlus R. Buks A. Conservtve vergng ethod for prtl dfferentl equtons th dscontnuous coeffcents. WSEAS Trnsctons on Het nd Mss Trnsfer. Vol. Issue 4 6 p [] Guenther R.B. Lee J.W. Prtl Dfferentl Equtons of Mthetcl Phscs nd Integrl Equtons. Dover Pulctons Inc. Ne York 996.

Exact 3-D Solution for System with Rectangular Fins, Part 2

Exact 3-D Solution for System with Rectangular Fins, Part 2 1th WSEAS Int. Conf. on APPLIED MATHEMATICS Caro Egypt Deceber 9-31 7 7 Exact 3-D Soluton for Syste th Rectangular Fns Part ANDRIS BUIKIS MARGARITA BUIKE Insttute of Matheatcs and Coputer Scence Unversty

More information

LOCAL FRACTIONAL LAPLACE SERIES EXPANSION METHOD FOR DIFFUSION EQUATION ARISING IN FRACTAL HEAT TRANSFER

LOCAL FRACTIONAL LAPLACE SERIES EXPANSION METHOD FOR DIFFUSION EQUATION ARISING IN FRACTAL HEAT TRANSFER Yn, S.-P.: Locl Frctonl Lplce Seres Expnson Method for Dffuson THERMAL SCIENCE, Yer 25, Vol. 9, Suppl., pp. S3-S35 S3 LOCAL FRACTIONAL LAPLACE SERIES EXPANSION METHOD FOR DIFFUSION EQUATION ARISING IN

More information

4. Eccentric axial loading, cross-section core

4. Eccentric axial loading, cross-section core . Eccentrc xl lodng, cross-secton core Introducton We re strtng to consder more generl cse when the xl force nd bxl bendng ct smultneousl n the cross-secton of the br. B vrtue of Snt-Vennt s prncple we

More information

? plate in A G in

? plate in A G in Proble (0 ponts): The plstc block shon s bonded to rgd support nd to vertcl plte to hch 0 kp lod P s ppled. Knong tht for the plstc used G = 50 ks, deterne the deflecton of the plte. Gven: G 50 ks, P 0

More information

International Journal of Pure and Applied Sciences and Technology

International Journal of Pure and Applied Sciences and Technology Int. J. Pure Appl. Sc. Technol., () (), pp. 44-49 Interntonl Journl of Pure nd Appled Scences nd Technolog ISSN 9-67 Avlle onlne t www.jopst.n Reserch Pper Numercl Soluton for Non-Lner Fredholm Integrl

More information

Numerical Solution of Freholm-Volterra Integral Equations by Using Scaling Function Interpolation Method

Numerical Solution of Freholm-Volterra Integral Equations by Using Scaling Function Interpolation Method Aled Mthetcs 3 4 4-9 htt://ddoorg/436/34a3 Pulshed Onlne Jnury 3 (htt://wwwscrorg/ournl/) uercl Soluton of Frehol-Volterr Integrl Equtons y Usng Sclng Functon Interolton Method Yousef Al-Jrrh En-Bng Ln

More information

CENTROID (AĞIRLIK MERKEZİ )

CENTROID (AĞIRLIK MERKEZİ ) CENTOD (ĞLK MEKEZİ ) centrod s geometrcl concept rsng from prllel forces. Tus, onl prllel forces possess centrod. Centrod s tougt of s te pont were te wole wegt of pscl od or sstem of prtcles s lumped.

More information

LAPLACE TRANSFORM SOLUTION OF THE PROBLEM OF TIME-FRACTIONAL HEAT CONDUCTION IN A TWO-LAYERED SLAB

LAPLACE TRANSFORM SOLUTION OF THE PROBLEM OF TIME-FRACTIONAL HEAT CONDUCTION IN A TWO-LAYERED SLAB Journl of Appled Mthemtcs nd Computtonl Mechncs 5, 4(4), 5-3 www.mcm.pcz.pl p-issn 99-9965 DOI:.75/jmcm.5.4. e-issn 353-588 LAPLACE TRANSFORM SOLUTION OF THE PROBLEM OF TIME-FRACTIONAL HEAT CONDUCTION

More information

Integral Transforms and Dual Integral Equations to Solve Heat Equation with Mixed Conditions

Integral Transforms and Dual Integral Equations to Solve Heat Equation with Mixed Conditions Int J Open Probles Copt Math, Vol 7, No 4, Deceber 214 ISSN 1998-6262; Copyrght ICSS Publcaton, 214 www-csrsorg Integral Transfors and Dual Integral Equatons to Solve Heat Equaton wth Mxed Condtons Naser

More information

Lecture 3 Camera Models 2 & Camera Calibration. Professor Silvio Savarese Computational Vision and Geometry Lab

Lecture 3 Camera Models 2 & Camera Calibration. Professor Silvio Savarese Computational Vision and Geometry Lab Lecture Cer Models Cer Clbrton rofessor Slvo Svrese Coputtonl Vson nd Geoetry Lb Slvo Svrese Lecture - Jn 7 th, 8 Lecture Cer Models Cer Clbrton Recp of cer odels Cer clbrton proble Cer clbrton wth rdl

More information

Solubilities and Thermodynamic Properties of SO 2 in Ionic

Solubilities and Thermodynamic Properties of SO 2 in Ionic Solubltes nd Therodync Propertes of SO n Ionc Lquds Men Jn, Yucu Hou, b Weze Wu, *, Shuhng Ren nd Shdong Tn, L Xo, nd Zhgng Le Stte Key Lbortory of Checl Resource Engneerng, Beng Unversty of Checl Technology,

More information

Machine Learning. Support Vector Machines. Le Song. CSE6740/CS7641/ISYE6740, Fall Lecture 8, Sept. 13, 2012 Based on slides from Eric Xing, CMU

Machine Learning. Support Vector Machines. Le Song. CSE6740/CS7641/ISYE6740, Fall Lecture 8, Sept. 13, 2012 Based on slides from Eric Xing, CMU Mchne Lernng CSE6740/CS764/ISYE6740 Fll 0 Support Vector Mchnes Le Song Lecture 8 Sept. 3 0 Bsed on sldes fro Erc Xng CMU Redng: Chp. 6&7 C.B ook Outlne Mu rgn clssfcton Constrned optzton Lgrngn dult Kernel

More information

NUMERICAL MODELLING OF A CILIUM USING AN INTEGRAL EQUATION

NUMERICAL MODELLING OF A CILIUM USING AN INTEGRAL EQUATION NUEICAL ODELLING OF A CILIU USING AN INTEGAL EQUATION IHAI EBICAN, DANIEL IOAN Key words: Cl, Numercl nlyss, Electromgnetc feld, gnetton. The pper presents fst nd ccurte method to model the mgnetc behvour

More information

Jens Siebel (University of Applied Sciences Kaiserslautern) An Interactive Introduction to Complex Numbers

Jens Siebel (University of Applied Sciences Kaiserslautern) An Interactive Introduction to Complex Numbers Jens Sebel (Unversty of Appled Scences Kserslutern) An Interctve Introducton to Complex Numbers 1. Introducton We know tht some polynoml equtons do not hve ny solutons on R/. Exmple 1.1: Solve x + 1= for

More information

The areolar strain concept applied to elasticity

The areolar strain concept applied to elasticity Computtonl Methods nd Epermentl Mesurements XIII 579 The reolr strn concept ppled to elstct I. D. Kotchergenko Insttuto Mltr de Engenhr, Ro de Jnero, Brl Astrct In contrst to the ooks tht strt th solutons

More information

Fitting a Polynomial to Heat Capacity as a Function of Temperature for Ag. Mathematical Background Document

Fitting a Polynomial to Heat Capacity as a Function of Temperature for Ag. Mathematical Background Document Fttng Polynol to Het Cpcty s Functon of Teperture for Ag. thetcl Bckground Docuent by Theres Jul Zelnsk Deprtent of Chestry, edcl Technology, nd Physcs onouth Unversty West ong Brnch, J 7764-898 tzelns@onouth.edu

More information

Effects of polarization on the reflected wave

Effects of polarization on the reflected wave Lecture Notes. L Ros PPLIED OPTICS Effects of polrzton on the reflected wve Ref: The Feynmn Lectures on Physcs, Vol-I, Secton 33-6 Plne of ncdence Z Plne of nterfce Fg. 1 Y Y r 1 Glss r 1 Glss Fg. Reflecton

More information

7.2 Volume. A cross section is the shape we get when cutting straight through an object.

7.2 Volume. A cross section is the shape we get when cutting straight through an object. 7. Volume Let s revew the volume of smple sold, cylnder frst. Cylnder s volume=se re heght. As llustrted n Fgure (). Fgure ( nd (c) re specl cylnders. Fgure () s rght crculr cylnder. Fgure (c) s ox. A

More information

THE COMBINED SHEPARD ABEL GONCHAROV UNIVARIATE OPERATOR

THE COMBINED SHEPARD ABEL GONCHAROV UNIVARIATE OPERATOR REVUE D ANALYSE NUMÉRIQUE ET DE THÉORIE DE L APPROXIMATION Tome 32, N o 1, 2003, pp 11 20 THE COMBINED SHEPARD ABEL GONCHAROV UNIVARIATE OPERATOR TEODORA CĂTINAŞ Abstrct We extend the Sheprd opertor by

More information

Lecture 36. Finite Element Methods

Lecture 36. Finite Element Methods CE 60: Numercl Methods Lecture 36 Fnte Element Methods Course Coordntor: Dr. Suresh A. Krth, Assocte Professor, Deprtment of Cvl Engneerng, IIT Guwht. In the lst clss, we dscussed on the ppromte methods

More information

NON-HOMOGENEOUS COMPOSITE BEAMS: ANALYTIC FORMULATION AND SOLUTION

NON-HOMOGENEOUS COMPOSITE BEAMS: ANALYTIC FORMULATION AND SOLUTION TH NTERNATONAL CONGRESS O THE AERONAUTCAL SCENCES NON-HOMOGENEOUS COMPOSTE BEAMS: ANALYTC ORMULATON AND SOLUTON M Greshten V Rovens M r (eershvl nd O Rnd Technon srel nsttute of Technolog cult of Aerospce

More information

The Number of Rows which Equal Certain Row

The Number of Rows which Equal Certain Row Interntonl Journl of Algebr, Vol 5, 011, no 30, 1481-1488 he Number of Rows whch Equl Certn Row Ahmd Hbl Deprtment of mthemtcs Fcult of Scences Dmscus unverst Dmscus, Sr hblhmd1@gmlcom Abstrct Let be X

More information

APPROXIMATE SOLUTION OF HIGHER ORDER LINEAR DIFFERENTIAL EQUATIONS BY MEANS OF A NEW RATIONAL CHEBYSHEV COLLOCATION METHOD

APPROXIMATE SOLUTION OF HIGHER ORDER LINEAR DIFFERENTIAL EQUATIONS BY MEANS OF A NEW RATIONAL CHEBYSHEV COLLOCATION METHOD thetcl nd oputtonl Applctons ol. 5 o. pp. 5-56. Assocton for Scentfc eserch APPOXIAE SOLUIO OF HIGHE ODE LIEA DIFFEEIAL EQUAIOS BY EAS OF A EW AIOAL HEBYSHE OLLOAIO EHOD Slh Ylçınbş * esrn Özso ehet Sezer

More information

DCDM BUSINESS SCHOOL NUMERICAL METHODS (COS 233-8) Solutions to Assignment 3. x f(x)

DCDM BUSINESS SCHOOL NUMERICAL METHODS (COS 233-8) Solutions to Assignment 3. x f(x) DCDM BUSINESS SCHOOL NUMEICAL METHODS (COS -8) Solutons to Assgnment Queston Consder the followng dt: 5 f() 8 7 5 () Set up dfference tble through fourth dfferences. (b) Wht s the mnmum degree tht n nterpoltng

More information

TWO INTERFACIAL COLLINEAR GRIFFITH CRACKS IN THERMO-ELASTIC COMPOSITE MEDIA

TWO INTERFACIAL COLLINEAR GRIFFITH CRACKS IN THERMO-ELASTIC COMPOSITE MEDIA THERMAL SCIENCE: Yer 8, Vol., No. B, pp. 43-433 43 TWO INTERFACIAL COLLINEAR GRIFFITH CRACKS IN THERMO-ELASTIC COMPOSITE MEDIA y Prshnt Kumr MISHRA nd Sur DAS * Deprtment of Mthemtcl Scences, Indn Insttute

More information

ORDINARY DIFFERENTIAL EQUATIONS

ORDINARY DIFFERENTIAL EQUATIONS 6 ORDINARY DIFFERENTIAL EQUATIONS Introducton Runge-Kutt Metods Mult-step Metods Sstem o Equtons Boundr Vlue Problems Crcterstc Vlue Problems Cpter 6 Ordnr Derentl Equtons / 6. Introducton In mn engneerng

More information

Chemical Reaction Engineering

Chemical Reaction Engineering Lecture 20 hemcl Recton Engneerng (RE) s the feld tht studes the rtes nd mechnsms of chemcl rectons nd the desgn of the rectors n whch they tke plce. Lst Lecture Energy Blnce Fundmentls F E F E + Q! 0

More information

Katholieke Universiteit Leuven Department of Computer Science

Katholieke Universiteit Leuven Department of Computer Science Updte Rules for Weghted Non-negtve FH*G Fctorzton Peter Peers Phlp Dutré Report CW 440, Aprl 006 Ktholeke Unverstet Leuven Deprtment of Computer Scence Celestjnenln 00A B-3001 Heverlee (Belgum) Updte Rules

More information

Math 497C Sep 17, Curves and Surfaces Fall 2004, PSU

Math 497C Sep 17, Curves and Surfaces Fall 2004, PSU Mth 497C Sep 17, 004 1 Curves nd Surfces Fll 004, PSU Lecture Notes 3 1.8 The generl defnton of curvture; Fox-Mlnor s Theorem Let α: [, b] R n be curve nd P = {t 0,...,t n } be prtton of [, b], then the

More information

Chemical Reaction Engineering

Chemical Reaction Engineering Lecture 20 hemcl Recton Engneerng (RE) s the feld tht studes the rtes nd mechnsms of chemcl rectons nd the desgn of the rectors n whch they tke plce. Lst Lecture Energy Blnce Fundmentls F 0 E 0 F E Q W

More information

Two Coefficients of the Dyson Product

Two Coefficients of the Dyson Product Two Coeffcents of the Dyson Product rxv:07.460v mth.co 7 Nov 007 Lun Lv, Guoce Xn, nd Yue Zhou 3,,3 Center for Combntorcs, LPMC TJKLC Nnk Unversty, Tnjn 30007, P.R. Chn lvlun@cfc.nnk.edu.cn gn@nnk.edu.cn

More information

Rank One Update And the Google Matrix by Al Bernstein Signal Science, LLC

Rank One Update And the Google Matrix by Al Bernstein Signal Science, LLC Introducton Rnk One Updte And the Google Mtrx y Al Bernsten Sgnl Scence, LLC www.sgnlscence.net here re two dfferent wys to perform mtrx multplctons. he frst uses dot product formulton nd the second uses

More information

STATISTICAL MECHANICS OF THE INVERSE ISING MODEL

STATISTICAL MECHANICS OF THE INVERSE ISING MODEL STATISTICAL MECHANICS OF THE INVESE ISING MODEL Muro Cro Supervsors: rof. Mchele Cselle rof. ccrdo Zecchn uly 2009 INTODUCTION SUMMAY OF THE ESENTATION Defnton of the drect nd nverse prole Approton ethods

More information

Decomposition of Boolean Function Sets for Boolean Neural Networks

Decomposition of Boolean Function Sets for Boolean Neural Networks Decomposton of Boolen Functon Sets for Boolen Neurl Netorks Romn Kohut,, Bernd Stenbch Freberg Unverst of Mnng nd Technolog Insttute of Computer Scence Freberg (Schs), Germn Outlne Introducton Boolen Neuron

More information

Numbers Related to Bernoulli-Goss Numbers

Numbers Related to Bernoulli-Goss Numbers ursh Journl of Anlyss n Nuber heory, 4, Vol., No., -8 Avlble onlne t htt://ubs.sceub.co/tnt///4 Scence n Eucton Publshng OI:.69/tnt---4 Nubers Relte to Bernoull-Goss Nubers Mohe Oul ouh Benough * érteent

More information

Chapter Newton-Raphson Method of Solving a Nonlinear Equation

Chapter Newton-Raphson Method of Solving a Nonlinear Equation Chpter.4 Newton-Rphson Method of Solvng Nonlner Equton After redng ths chpter, you should be ble to:. derve the Newton-Rphson method formul,. develop the lgorthm of the Newton-Rphson method,. use the Newton-Rphson

More information

Quantum Particle Motion in Physical Space

Quantum Particle Motion in Physical Space Adv. Studes Theor. Phys., Vol. 8, 014, no. 1, 7-34 HIKARI Ltd, www.-hkar.co http://dx.do.org/10.1988/astp.014.311136 Quantu Partcle Moton n Physcal Space A. Yu. Saarn Dept. of Physcs, Saara State Techncal

More information

Statistics and Probability Letters

Statistics and Probability Letters Sttstcs nd Probblty Letters 79 (2009) 105 111 Contents lsts vlble t ScenceDrect Sttstcs nd Probblty Letters journl homepge: www.elsever.com/locte/stpro Lmtng behvour of movng verge processes under ϕ-mxng

More information

Research Article On the Upper Bounds of Eigenvalues for a Class of Systems of Ordinary Differential Equations with Higher Order

Research Article On the Upper Bounds of Eigenvalues for a Class of Systems of Ordinary Differential Equations with Higher Order Hndw Publshng Corporton Interntonl Journl of Dfferentl Equtons Volume 0, Artcle ID 7703, pges do:055/0/7703 Reserch Artcle On the Upper Bounds of Egenvlues for Clss of Systems of Ordnry Dfferentl Equtons

More information

Lecture 4: Piecewise Cubic Interpolation

Lecture 4: Piecewise Cubic Interpolation Lecture notes on Vrtonl nd Approxmte Methods n Appled Mthemtcs - A Perce UBC Lecture 4: Pecewse Cubc Interpolton Compled 6 August 7 In ths lecture we consder pecewse cubc nterpolton n whch cubc polynoml

More information

Electrochemical Thermodynamics. Interfaces and Energy Conversion

Electrochemical Thermodynamics. Interfaces and Energy Conversion CHE465/865, 2006-3, Lecture 6, 18 th Sep., 2006 Electrochemcl Thermodynmcs Interfces nd Energy Converson Where does the energy contrbuton F zϕ dn come from? Frst lw of thermodynmcs (conservton of energy):

More information

DETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM

DETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM Ganj, Z. Z., et al.: Determnaton of Temperature Dstrbuton for S111 DETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM by Davood Domr GANJI

More information

1 Matrix representations of canonical matrices

1 Matrix representations of canonical matrices 1 Matrx representatons of canoncal matrces 2-d rotaton around the orgn: ( ) cos θ sn θ R 0 = sn θ cos θ 3-d rotaton around the x-axs: R x = 1 0 0 0 cos θ sn θ 0 sn θ cos θ 3-d rotaton around the y-axs:

More information

A new Approach for Solving Linear Ordinary Differential Equations

A new Approach for Solving Linear Ordinary Differential Equations , ISSN 974-57X (Onlne), ISSN 974-5718 (Prnt), Vol. ; Issue No. 1; Year 14, Copyrght 13-14 by CESER PUBLICATIONS A new Approach for Solvng Lnear Ordnary Dfferental Equatons Fawz Abdelwahd Department of

More information

Lectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix

Lectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix Lectures - Week 4 Matrx norms, Condtonng, Vector Spaces, Lnear Independence, Spannng sets and Bass, Null space and Range of a Matrx Matrx Norms Now we turn to assocatng a number to each matrx. We could

More information

Second degree generalized gauss-seidel iteration method for solving linear system of equations. ABSTRACT

Second degree generalized gauss-seidel iteration method for solving linear system of equations. ABSTRACT Ethiop. J. Sci. & Technol. 7( 5-, 0 5 Second degree generlized guss-seidel itertion ethod for solving liner syste of equtions Tesfye Keede Bhir Dr University, College of Science, Deprtent of Mthetics tk_ke@yhoo.co

More information

90 S.S. Drgomr nd (t b)du(t) =u()(b ) u(t)dt: If we dd the bove two equltes, we get (.) u()(b ) u(t)dt = p(; t)du(t) where p(; t) := for ll ; t [; b]:

90 S.S. Drgomr nd (t b)du(t) =u()(b ) u(t)dt: If we dd the bove two equltes, we get (.) u()(b ) u(t)dt = p(; t)du(t) where p(; t) := for ll ; t [; b]: RGMIA Reserch Report Collecton, Vol., No. 1, 1999 http://sc.vu.edu.u/οrgm ON THE OSTROWSKI INTEGRAL INEQUALITY FOR LIPSCHITZIAN MAPPINGS AND APPLICATIONS S.S. Drgomr Abstrct. A generlzton of Ostrowsk's

More information

Lecture 8: Camera Calibration

Lecture 8: Camera Calibration Lecture 8: Cer Clbrton rofessor Fe-Fe L Stnford Vson Lb Fe-Fe L 9-Oct- Wht we wll lern tody? Revew cer preters Affne cer odel (roble Set (Q4)) Cer clbrton Vnshng ponts nd lnes (roble Set (Q)) Redng: [F]

More information

Some circular summation formulas for theta functions

Some circular summation formulas for theta functions Ci et l. Boundr Vlue Prolems 013, 013:59 R E S E A R C H Open Access Some circulr summtion formuls for thet functions Yi Ci, Si Chen nd Qiu-Ming Luo * * Correspondence: luomth007@163.com Deprtment of Mthemtics,

More information

OXFORD H i g h e r E d u c a t i o n Oxford University Press, All rights reserved.

OXFORD H i g h e r E d u c a t i o n Oxford University Press, All rights reserved. Renshw: Mths for Econoics nswers to dditionl exercises Exercise.. Given: nd B 5 Find: () + B + B 7 8 (b) (c) (d) (e) B B B + B T B (where 8 B 6 B 6 8 B + B T denotes the trnspose of ) T 8 B 5 (f) (g) B

More information

Sequences of Intuitionistic Fuzzy Soft G-Modules

Sequences of Intuitionistic Fuzzy Soft G-Modules Interntonl Mthemtcl Forum, Vol 13, 2018, no 12, 537-546 HIKARI Ltd, wwwm-hkrcom https://doorg/1012988/mf201881058 Sequences of Intutonstc Fuzzy Soft G-Modules Velyev Kemle nd Huseynov Afq Bku Stte Unversty,

More information

INTRODUCTION TO COMPLEX NUMBERS

INTRODUCTION TO COMPLEX NUMBERS INTRODUCTION TO COMPLEX NUMBERS The numers -4, -3, -, -1, 0, 1,, 3, 4 represent the negtve nd postve rel numers termed ntegers. As one frst lerns n mddle school they cn e thought of s unt dstnce spced

More information

Study of Trapezoidal Fuzzy Linear System of Equations S. M. Bargir 1, *, M. S. Bapat 2, J. D. Yadav 3 1

Study of Trapezoidal Fuzzy Linear System of Equations S. M. Bargir 1, *, M. S. Bapat 2, J. D. Yadav 3 1 mercn Interntonl Journl of Reserch n cence Technology Engneerng & Mthemtcs vlble onlne t http://wwwsrnet IN (Prnt: 38-349 IN (Onlne: 38-3580 IN (CD-ROM: 38-369 IJRTEM s refereed ndexed peer-revewed multdscplnry

More information

Applied Statistics Qualifier Examination

Applied Statistics Qualifier Examination Appled Sttstcs Qulfer Exmnton Qul_june_8 Fll 8 Instructons: () The exmnton contns 4 Questons. You re to nswer 3 out of 4 of them. () You my use ny books nd clss notes tht you mght fnd helpful n solvng

More information

Applied Mathematics Letters

Applied Mathematics Letters Appled Matheatcs Letters 2 (2) 46 5 Contents lsts avalable at ScenceDrect Appled Matheatcs Letters journal hoepage: wwwelseverco/locate/al Calculaton of coeffcents of a cardnal B-splne Gradr V Mlovanovć

More information

Approximate Large Deflection Analysis of Thin Rectangular Plates under Distributed Lateral Line Load

Approximate Large Deflection Analysis of Thin Rectangular Plates under Distributed Lateral Line Load Second Interntionl Conference on Advnces in Engineering nd Technolog Approite Lrge eflection Anlsis of Thin Rectngulr Pltes under istriuted Lterl Line Lod Alln Okodi, Y N. Zir, Jckson A. Mkli Grdute Student,

More information

THE SMOOTH INDENTATION OF A CYLINDRICAL INDENTOR AND ANGLE-PLY LAMINATES

THE SMOOTH INDENTATION OF A CYLINDRICAL INDENTOR AND ANGLE-PLY LAMINATES THE SMOOTH INDENTATION OF A CYLINDRICAL INDENTOR AND ANGLE-PLY LAMINATES W. C. Lao Department of Cvl Engneerng, Feng Cha Unverst 00 Wen Hwa Rd, Tachung, Tawan SUMMARY: The ndentaton etween clndrcal ndentor

More information

Introduction to Numerical Integration Part II

Introduction to Numerical Integration Part II Introducton to umercl Integrton Prt II CS 75/Mth 75 Brn T. Smth, UM, CS Dept. Sprng, 998 4/9/998 qud_ Intro to Gussn Qudrture s eore, the generl tretment chnges the ntegrton prolem to ndng the ntegrl w

More information

Haddow s Experiment:

Haddow s Experiment: schemtc drwng of Hddow's expermentl set-up movng pston non-contctng moton sensor bems of sprng steel poston vres to djust frequences blocks of sold steel shker Hddow s Experment: terr frm Theoretcl nd

More information

Analysis and Experimental Verification of the Strength of Telescopic Booms for Construction Machinery

Analysis and Experimental Verification of the Strength of Telescopic Booms for Construction Machinery ZHE CUI et l: ANALYSIS AND EXPERIMENTAL VERIFICATION OF THE STRENGTH OF TELESCOPIC Anlss nd Eperentl Verfcton of the Strength of Telescopc Boos for Constructon Mchner Zhe CUI, Wengung JIANG*, Le CHENG

More information

Chemistry 163B Absolute Entropies and Entropy of Mixing

Chemistry 163B Absolute Entropies and Entropy of Mixing Chemstry 163 Wnter 1 Hndouts for hrd Lw nd Entropy of Mxng (del gs, dstngushle molecules) PPENDIX : H f, G f, U S (no Δ, no su f ) Chemstry 163 solute Entropes nd Entropy of Mxng Hº f Gº f Sº 1 hrd Lw

More information

Outline. Review Quadrilateral Equation. Review Linear φ i Quadrilateral. Review x and y Derivatives. Review φ Derivatives

Outline. Review Quadrilateral Equation. Review Linear φ i Quadrilateral. Review x and y Derivatives. Review φ Derivatives E 5 Engneerng nlss ore on Fnte Eleents n ore on Fnte Eleents n Two Densons Two Densons Lrr Cretto echncl Engneerng 5 Senr n Engneerng nlss prl 7-9 9 Otlne Revew lst lectre Qrtc ss nctons n two ensons orer

More information

COMPLEX NUMBERS AND QUADRATIC EQUATIONS

COMPLEX NUMBERS AND QUADRATIC EQUATIONS COMPLEX NUMBERS AND QUADRATIC EQUATIONS INTRODUCTION We know that x 0 for all x R e the square of a real number (whether postve, negatve or ero) s non-negatve Hence the equatons x, x, x + 7 0 etc are not

More information

Constructing Free Energy Approximations and GBP Algorithms

Constructing Free Energy Approximations and GBP Algorithms 3710 Advnced Topcs n A ecture 15 Brnslv Kveton kveton@cs.ptt.edu 5802 ennott qure onstructng Free Energy Approxtons nd BP Algorths ontent Why? Belef propgton (BP) Fctor grphs egon-sed free energy pproxtons

More information

6. Chemical Potential and the Grand Partition Function

6. Chemical Potential and the Grand Partition Function 6. Chemcl Potentl nd the Grnd Prtton Functon ome Mth Fcts (see ppendx E for detls) If F() s n nlytc functon of stte vrles nd such tht df d pd then t follows: F F p lso snce F p F we cn conclude: p In other

More information

Elastic Collisions. Definition: two point masses on which no external forces act collide without losing any energy.

Elastic Collisions. Definition: two point masses on which no external forces act collide without losing any energy. Elastc Collsons Defnton: to pont asses on hch no external forces act collde thout losng any energy v Prerequstes: θ θ collsons n one denson conservaton of oentu and energy occurs frequently n everyday

More information

Physics for Scientists and Engineers I

Physics for Scientists and Engineers I Phscs for Scentsts nd Engneers I PHY 48, Secton 4 Dr. Betr Roldán Cuen Unverst of Centrl Flord, Phscs Deprtment, Orlndo, FL Chpter - Introducton I. Generl II. Interntonl Sstem of Unts III. Converson of

More information

Math Fall 2006 Sample problems for the final exam: Solutions

Math Fall 2006 Sample problems for the final exam: Solutions Mth 42-5 Fll 26 Smple problems for the finl exm: Solutions Any problem my be ltered or replced by different one! Some possibly useful informtion Prsevl s equlity for the complex form of the Fourier series

More information

ADVANCEMENT OF THE CLOSELY COUPLED PROBES POTENTIAL DROP TECHNIQUE FOR NDE OF SURFACE CRACKS

ADVANCEMENT OF THE CLOSELY COUPLED PROBES POTENTIAL DROP TECHNIQUE FOR NDE OF SURFACE CRACKS ADVANCEMENT OF THE CLOSELY COUPLED PROBES POTENTIAL DROP TECHNIQUE FOR NDE OF SURFACE CRACKS F. Tkeo 1 nd M. Sk 1 Hchinohe Ntionl College of Technology, Hchinohe, Jpn; Tohoku University, Sendi, Jpn Abstrct:

More information

UNIVERSITY OF IOANNINA DEPARTMENT OF ECONOMICS. M.Sc. in Economics MICROECONOMIC THEORY I. Problem Set II

UNIVERSITY OF IOANNINA DEPARTMENT OF ECONOMICS. M.Sc. in Economics MICROECONOMIC THEORY I. Problem Set II Mcroeconomc Theory I UNIVERSITY OF IOANNINA DEPARTMENT OF ECONOMICS MSc n Economcs MICROECONOMIC THEORY I Techng: A Lptns (Note: The number of ndctes exercse s dffculty level) ()True or flse? If V( y )

More information

Geometric Correction or Georeferencing

Geometric Correction or Georeferencing Geoetrc Correcton or Georeferencng GEOREFERENCING: fro ge to p Coordntes on erth: (λ, φ) ge: (, ) p: (, ) rel nteger Trnsfortons (nvolvng deforton): erth-to-ge: χ erth-to-p: ψ (crtogrphc proecton) ge-to-p:

More information

Inelastic electron tunneling through a vibrational modulated barrier in STM

Inelastic electron tunneling through a vibrational modulated barrier in STM Romnn Reports n Physcs, olume 55, Numer 4, P. 47 58, 3 Inelstc electron tunnelng through vrtonl modulted rrer n SM P. udu culty of Physcs, Unversty of uchrest, PO ox MG, Mgurele, Romn strct: Usng mny ody

More information

Rectangular group congruences on an epigroup

Rectangular group congruences on an epigroup cholrs Journl of Engineering nd Technology (JET) ch J Eng Tech, 015; 3(9):73-736 cholrs Acdemic nd cientific Pulisher (An Interntionl Pulisher for Acdemic nd cientific Resources) wwwsspulishercom IN 31-435X

More information

A Brief Note on Quasi Static Thermal Stresses In A Thin Rectangular Plate With Internal Heat Generation

A Brief Note on Quasi Static Thermal Stresses In A Thin Rectangular Plate With Internal Heat Generation Americn Journl of Engineering Reserch (AJER) 13 Americn Journl of Engineering Reserch (AJER) e-issn : 3-847 p-issn : 3-936 Volume-, Issue-1, pp-388-393 www.jer.org Reserch Pper Open Access A Brief Note

More information

8.3 THE TRIGONOMETRIC FUNCTIONS. skipped 8.4 THE ALGEBRAIC COMPLETENESS OF THE COMPLEX FIELD. skipped 8.5 FOURIER SERIES

8.3 THE TRIGONOMETRIC FUNCTIONS. skipped 8.4 THE ALGEBRAIC COMPLETENESS OF THE COMPLEX FIELD. skipped 8.5 FOURIER SERIES 8.5 FOURIER SERIES 0 8.3 THE TRIGONOMETRIC FUNCTIONS skipped 8.4 THE ALGEBRAIC COMPLETENESS OF THE COMPLEX FIELD skipped 8.5 FOURIER SERIES 8.9 Orthogonl Functions, Orthonorl: Let { n }, n, 2, 3,...,besequence

More information

Lecture 12: Discrete Laplacian

Lecture 12: Discrete Laplacian Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly

More information

GAUSS ELIMINATION. Consider the following system of algebraic linear equations

GAUSS ELIMINATION. Consider the following system of algebraic linear equations Numercl Anlyss for Engneers Germn Jordnn Unversty GAUSS ELIMINATION Consder the followng system of lgebrc lner equtons To solve the bove system usng clsscl methods, equton () s subtrcted from equton ()

More information

The Schur-Cohn Algorithm

The Schur-Cohn Algorithm Modelng, Estmton nd Otml Flterng n Sgnl Processng Mohmed Njm Coyrght 8, ISTE Ltd. Aendx F The Schur-Cohn Algorthm In ths endx, our m s to resent the Schur-Cohn lgorthm [] whch s often used s crteron for

More information

EXAMPLES of THEORETICAL PROBLEMS in the COURSE MMV031 HEAT TRANSFER, version 2017

EXAMPLES of THEORETICAL PROBLEMS in the COURSE MMV031 HEAT TRANSFER, version 2017 EXAMPLES of THEORETICAL PROBLEMS n the COURSE MMV03 HEAT TRANSFER, verson 207 a) What s eant by sotropc ateral? b) What s eant by hoogeneous ateral? 2 Defne the theral dffusvty and gve the unts for the

More information

13 Design of Revetments, Seawalls and Bulkheads Forces & Earth Pressures

13 Design of Revetments, Seawalls and Bulkheads Forces & Earth Pressures 13 Desgn of Revetments, Sewlls nd Bulkheds Forces & Erth ressures Ref: Shore rotecton Mnul, USACE, 1984 EM 1110--1614, Desgn of Revetments, Sewlls nd Bulkheds, USACE, 1995 Brekwters, Jettes, Bulkheds nd

More information

M344 - ADVANCED ENGINEERING MATHEMATICS

M344 - ADVANCED ENGINEERING MATHEMATICS M3 - ADVANCED ENGINEERING MATHEMATICS Lecture 18: Lplce s Eqution, Anltic nd Numericl Solution Our emple of n elliptic prtil differentil eqution is Lplce s eqution, lso clled the Diffusion Eqution. If

More information

THE BERNOULLI PERIODIC FUNCTIONS. 1. Definitions

THE BERNOULLI PERIODIC FUNCTIONS. 1. Definitions THE BERNOULLI PERIODIC FUNCTIONS MIGUEL A. LERMA Abstrct. We study slightly modified versions of the Bernoulli periodic functions with nicer structurl properties, nd use them to give very simple proof

More information

Convexity preserving interpolation by splines of arbitrary degree

Convexity preserving interpolation by splines of arbitrary degree Computer Scence Journal of Moldova, vol.18, no.1(52), 2010 Convexty preservng nterpolaton by splnes of arbtrary degree Igor Verlan Abstract In the present paper an algorthm of C 2 nterpolaton of dscrete

More information

Module 9: The Method of Green s Functions

Module 9: The Method of Green s Functions Module 9: The Method of Green s Functions The method of Green s functions is n importnt technique for solving oundry vlue nd, initil nd oundry vlue prolems for prtil differentil equtions. In this module,

More information

Work and Energy (Work Done by a Varying Force)

Work and Energy (Work Done by a Varying Force) Lecture 1 Chpter 7 Physcs I 3.5.14 ork nd Energy (ork Done y Vryng Force) Course weste: http://fculty.uml.edu/andry_dnylov/techng/physcsi Lecture Cpture: http://echo36.uml.edu/dnylov13/physcs1fll.html

More information

Activator-Inhibitor Model of a Dynamical System: Application to an Oscillating Chemical Reaction System

Activator-Inhibitor Model of a Dynamical System: Application to an Oscillating Chemical Reaction System Actvtor-Inhtor Model of Dynmcl System: Applcton to n Osclltng Chemcl Recton System C.G. Chrrth*P P,Denn BsuP P * Deprtment of Appled Mthemtcs Unversty of Clcutt 9, A. P. C. Rod, Kolt-79 # Deprtment of

More information

arxiv:gr-qc/ v1 14 Mar 2000

arxiv:gr-qc/ v1 14 Mar 2000 The binry blck-hole dynmics t the third post-newtonin order in the orbitl motion Piotr Jrnowski Institute of Theoreticl Physics, University of Bi lystok, Lipow 1, 15-2 Bi lystok, Polnd Gerhrd Schäfer Theoretisch-Physiklisches

More information

Electrical double layer: revisit based on boundary conditions

Electrical double layer: revisit based on boundary conditions Electrcal double layer: revst based on boundary condtons Jong U. Km Department of Electrcal and Computer Engneerng, Texas A&M Unversty College Staton, TX 77843-318, USA Abstract The electrcal double layer

More information

Supplemental document

Supplemental document Electronc Supplementary Materal (ESI) for Physcal Chemstry Chemcal Physcs. Ths journal s the Owner Socetes 01 Supplemental document Behnam Nkoobakht School of Chemstry, The Unversty of Sydney, Sydney,

More information

INTERPOLATION(1) ELM1222 Numerical Analysis. ELM1222 Numerical Analysis Dr Muharrem Mercimek

INTERPOLATION(1) ELM1222 Numerical Analysis. ELM1222 Numerical Analysis Dr Muharrem Mercimek ELM Numercl Anlss Dr Muhrrem Mercmek INTEPOLATION ELM Numercl Anlss Some of the contents re dopted from Lurene V. Fusett, Appled Numercl Anlss usng MATLAB. Prentce Hll Inc., 999 ELM Numercl Anlss Dr Muhrrem

More information

COMP 465: Data Mining More on PageRank

COMP 465: Data Mining More on PageRank COMP 465: Dt Mnng Moe on PgeRnk Sldes Adpted Fo: www.ds.og (Mnng Mssve Dtsets) Powe Iteton: Set = 1/ 1: = 2: = Goto 1 Exple: d 1/3 1/3 5/12 9/24 6/15 = 1/3 3/6 1/3 11/24 6/15 1/3 1/6 3/12 1/6 3/15 Iteton

More information

A Family of Multivariate Abel Series Distributions. of Order k

A Family of Multivariate Abel Series Distributions. of Order k Appled Mthemtcl Scences, Vol. 2, 2008, no. 45, 2239-2246 A Fmly of Multvrte Abel Seres Dstrbutons of Order k Rupk Gupt & Kshore K. Ds 2 Fculty of Scence & Technology, The Icf Unversty, Agrtl, Trpur, Ind

More information

On the Connectedness of the Solution Set for the Weak Vector Variational Inequality 1

On the Connectedness of the Solution Set for the Weak Vector Variational Inequality 1 Journal of Mathematcal Analyss and Alcatons 260, 15 2001 do:10.1006jmaa.2000.7389, avalable onlne at htt:.dealbrary.com on On the Connectedness of the Soluton Set for the Weak Vector Varatonal Inequalty

More information

r = cos θ + 1. dt ) dt. (1)

r = cos θ + 1. dt ) dt. (1) MTHE 7 Proble Set 5 Solutions (A Crdioid). Let C be the closed curve in R whose polr coordintes (r, θ) stisfy () Sketch the curve C. r = cos θ +. (b) Find pretriztion t (r(t), θ(t)), t [, b], of C in polr

More information

Summary: Method of Separation of Variables

Summary: Method of Separation of Variables Physics 246 Electricity nd Mgnetism I, Fll 26, Lecture 22 1 Summry: Method of Seprtion of Vribles 1. Seprtion of Vribles in Crtesin Coordintes 2. Fourier Series Suggested Reding: Griffiths: Chpter 3, Section

More information

Abhilasha Classes Class- XII Date: SOLUTION (Chap - 9,10,12) MM 50 Mob no

Abhilasha Classes Class- XII Date: SOLUTION (Chap - 9,10,12) MM 50 Mob no hlsh Clsses Clss- XII Dte: 0- - SOLUTION Chp - 9,0, MM 50 Mo no-996 If nd re poston vets of nd B respetvel, fnd the poston vet of pont C n B produed suh tht C B vet r C B = where = hs length nd dreton

More information

THE CHINESE REMAINDER THEOREM. We should thank the Chinese for their wonderful remainder theorem. Glenn Stevens

THE CHINESE REMAINDER THEOREM. We should thank the Chinese for their wonderful remainder theorem. Glenn Stevens THE CHINESE REMAINDER THEOREM KEITH CONRAD We should thank the Chnese for ther wonderful remander theorem. Glenn Stevens 1. Introducton The Chnese remander theorem says we can unquely solve any par of

More information

Existence and Uniqueness of Solution for a Fractional Order Integro-Differential Equation with Non-Local and Global Boundary Conditions

Existence and Uniqueness of Solution for a Fractional Order Integro-Differential Equation with Non-Local and Global Boundary Conditions Applied Mthetic 0 9-96 doi:0.436/.0.079 Pulihed Online Octoer 0 (http://www.scirp.org/journl/) Eitence nd Uniquene of Solution for Frctionl Order Integro-Differentil Eqution with Non-Locl nd Glol Boundry

More information

Physics 240: Worksheet 30 Name:

Physics 240: Worksheet 30 Name: (1) One mole of an deal monatomc gas doubles ts temperature and doubles ts volume. What s the change n entropy of the gas? () 1 kg of ce at 0 0 C melts to become water at 0 0 C. What s the change n entropy

More information

Denote the function derivatives f(x) in given points. x a b. Using relationships (1.2), polynomials (1.1) are written in the form

Denote the function derivatives f(x) in given points. x a b. Using relationships (1.2), polynomials (1.1) are written in the form SET OF METHODS FO SOUTION THE AUHY POBEM FO STIFF SYSTEMS OF ODINAY DIFFEENTIA EUATIONS AF atypov and YuV Nulchev Insttute of Theoretcal and Appled Mechancs SB AS 639 Novosbrs ussa Introducton A constructon

More information