FUNDAMENTALS ON ALGEBRA MATRICES AND DETERMINANTS

Size: px
Start display at page:

Download "FUNDAMENTALS ON ALGEBRA MATRICES AND DETERMINANTS"

Transcription

1 Dol Bgyoko (0 FUNDAMENTALS ON ALGEBRA MATRICES AND DETERMINANTS Introducton Expressons of the form P(x o + x + x + + n x n re clled polynomls The coeffcents o,, n re ndependent of x nd the exponents 0,,, n re zero or postve ntegers The hghest nteger exponent n the expresson of P(x s clled the degree of the polynoml P(x The vrle x represents complex or rel numer In the cse of complex vrles, z s often used nsted of x Terms of the type n x n re monomls P(x x hs degree equl to Q(x s polynoml of degree 0 A(x + x - 7x 6 s polynoml of degree 6 f(x x + x / s not polynoml ( / s non nteger exponent, nor The Fundmentl Theorem of Alger (FTA Defnton: the roots or the zeros of polynoml re the vlues of the vrle x for whch the polynoml s equl to zero Let P(x - x, x s the root of ths polynoml Let P(x x -, x - nd x re the roots of ths polynoml Numercl methods re used to fnd the roots of polynomls of degrees greter thn See Numercl Recpes suroutne lrry for smple progrms for clcultng the roots or zeroes of polynoml The Fundmentl Theorem of Alger (FTA: A polynoml of degree n hs exctly n roots (These roots my e rel or complex nd some of them my e equl! The mthemtcl proof of ths theorem cn e found n pproprte lger textooks We prove t n Physcs 4 usng propertes of functons of complex vrle Once ts roots re known, gven polynoml cn e wrtten s product (fctorzton of polynoml If P(x x -, the roots x, x - Then P(x cn e wrtten s P(x (x x (x x (x -(x + Fctor Theorem: f x 0 s root for P(x of degree n, then P(x cn e wrtten s the product of polynoml Q(x of degree (n- nd (x-x 0 : P(x(x-x 0 Q(x Algerc equtons

2 Dol Bgyoko (0 Algerc equtons nclude those resultng from equtng polynomls x x + 9x 5 0 s n lgerc equton 0x - x 4 5 0x x s lso n lgerc equton Theses equtons do not nvolve dervtves or ntegrls Fundmentls on Mtrces Defnton of Mtrx: A mtrx s rectngulr (or squre rry of numers or functons tht re clled mtrx elements A s rectngulr mtrx B 4 s squre mtrx In generl, A column( column(4 Lne or row Let n e the numer of lnes or rows (horzontl n mtrx A nd m tht of column ( vertcl; then A s typcl n x m mtrx Row mtrx: B ( 4 s x 4 row mtrx; x n mtrces re row mtrces

3 Dol Bgyoko (0 Column mtrx: C s x column mtrx; m x mtrces re column mtrces 6 Squre mtrx: mtrx wth the sme numer of rows s of columns s squre mtrx n x n mtrces re squre Element of mtrx: Element s n row nd n column zero or null mtrces re those for whch ll the elements re zero A 0,, 0 Unt mtrx: A unt mtrx, whch s lwys squre for our purposes, s one n whch s zero for nd s for Hence,, δ, I, I 0 0, nd 0 0 I 0 0 re ll unt mtrces 0 0 If A s unt mtrx, then,, δ Kronecker Delt or Kronecker symol : δ 0 for nd δ for So, δ δ δ δ whle δ δ δ δ δ Dgonl elements: The dgonl elements of squre mtrx A re the elements for whch the row nd the column ndces re equl The dgonl elements re nd Dgonl mtrx: A mtrx D s dgonl or s n ts dgonl form f nd only f for ll elements d, d c+ δ, where the c + re numers lso known s the egenvlues of the mtrx

4 Dol Bgyoko (0 0 0 D 0 0 hs egenvlues of, -, nd 0 0 Trce of squre mtrx: The trce of squre mtrx s the sum of ts dgonl elements Tr(D l+ (- + 0 Tr(A + for A Trnspose of mtrx: The trnspose of mtrx A s mtrx noted A T or A ~ The trnspose A T T of A s such tht,,, The rows of A re the correspondng columns of A T 4 7 T Let A 4 5 6, then A Note well tht the dgonl elements of A nd of A T re the sme : Tr(A Tr(A T Also note tht the nth column of A T s the nth row (or lne of A Trnsposes of mtrces re wdely used n computtons, quntum mechncs, nd trnsformtons Is the trnspose of row mtrx column mtrx? NOTATION: Mtrx A s lso noted ( A ( : Note well tht, wthout the prentheses, refers to specfc mtrx element ε k s the Lev-Cvt symol or densty ε k f,, k, re ll dfferent nd n the order of - f,, k re ll dfferent nd NOT n the order 0 f ny two ndces re equl (, k, or k Even numers of permuttons of -- n tht order gve : ε ε ε ; Odd numers of permutton gve -: ε ε ε The sgn of ε k s chnged y ny sngle permutton of consecutve ndces: ε ε ε ε k k, k k 4

5 Dol Bgyoko (0 Note tht n even numer of permuttons does not chnge the sgn A permutton of two ndces tht re not consecutve my represent n even or n odd numer of permuttons of consecutve ndces, dependng on how mny ndces re etween the two eng permuted! Determnnts of Mtrces Let A, the determnnt of A, noted A det A If A, then det(a Note the rs- for determnnts- nd prentheses for mtrces det A + + ( ( ( ( ( ( The ove determnnt ws clculted (developed usng the frst row Theorem: A determnnt cn e evluted long ny row or ny column Ths theorem s extremely useful n the prctcl evluton of determnnts From t, t redly follows tht det(a det(a T A useful defnton follows from the ove expresson of det (A By defnton, the cofctor of the element of mtrx s the expresson tht s multpled y when det(a s developed long row or column tht ncludes From the ove expresson of det(a, the cofctor of s ( ( s ( + ( 4 Opertons on Mtrces + nd tht of Equlty: Two mtrces A nd B re equl f nd only f,, Ths defnton hs trvl consequences: n m n nd n (m ± n mtrces cnnot e equl; two squre mtrces of dfferent dmenson (m m nd n n wth m n cnnot e equl 5

6 Dol Bgyoko (0 Addton: Addton s defned etween mtrces s follows: C A + B,, C + Ths defnton mples tht only m n mtrces cn e dded n the ordnry sense of ddton For squre mtrces, the numer of rows or of columns s clled the dmenson of the mtrces Only squre mtrces of equl dmensons cn e dded A B C ( + 0 C ( (0 + (0 + ( + ( ( + ( + (7 + 5 Multplcton of Mtrces The product of two mtrces A nd B s mtrx C such tht C k kk, where k to N C s otned y multplyng, term y term, the elements n lne of A y the elements n column of B Exmple: A B c AB c c c ( ( + + ( ( + + Notes: For the product of mtrces to e defned, the numer of columns of the frst mtrx must e equl to the numer of rows of the second mtrx Tke some smple mtrces to see tht n generl AB BA: the multplcton of mtrces s not commuttve The neutrl element, for mtrx multplcton, s unt mtrx I n ; for mtrces, 6

7 Dol Bgyoko (0 I 0 0 ; for x mtrces I Prove tht the set of n n mtrces consttutes n Aeln group when endowed wth the nry operton of ddton s defned ove (Do not confuse provng wth verfyng n prtculr cse Provng estlshes the vercty of proposton for ll cses! 6 Inverse of Mtrx By defnton, the nverse of mtrx A s mtrx noted A - such tht AA - A - A I, where I s the unt mtrx Fnd n your textook nd lern some methods of clcultng the nverse of mtrx See, for nstnce, pge If the nverse of squre mtrx exsts, then one of the wys to clculte t s s follows A T C det A where C s mtrx whose elements re the cofctors of elements of A: c cofctor of A mtrx whose determnnt s zero s sngulr mtrx nd t does not hve n nverse WARNING: For lrge mtrces, 0x0, 00x00, etc, the clculton of the nverse s done usng computer It s extremely mportnt to rememer, however, tht smll or tny round-off errors n the clculton of the nverse of mtrx led to huge errors n the fnl result Consequently, these clculton must e done usng s hgh precson s possle f one s to vod spurous results for the nverse (hgh precson mens tht every clculton s done y crryng s mny decml plces s possle 7 Drect Product of Two ( Mtrces By defnton, the drect product of two mtrces A nd B s mtrx D otned y multplyng every element of A y mtrx B Note: f s memer, to multply or dvde mtrx y mens to multply or dvde every element of the mtrx y Followng the ove defnton of the drect product, we get, for exmple, 7

8 Dol Bgyoko (0 A B nd A B Trvlly enough, the drect product of two mtrces s 4 4 mtrx The drect product of mtrces does not stsfy closure property, e, the drect product of two mtrces s not mtrx Note: The symol, etween two mtrces, sgnfes drect product nd not smple multplcton or product, unless otherwse ndcted explctly Some textooks use to further vod confuson Let us thnk t nd note tht someone who does not know thng out the drect product my nterpret to men smple product! Applcton: The drect product s extensvely used n some res of quntum mechncs (the theory of the moton nd propertes of electrons nd other prtcles whle they re nsde toms, molecules, solds, nd lquds Ordnry opertons on mtrces (ddton, multplcton, trnsposton, nverse clculton, etc re extensvely used n most res of most scence nd engneerng dscplnes, nd n socl scences 8

9 Dol Bgyoko (0 8 Specl Mtrces Before defnng some key specl mtrces, we recll some sc notons nd nottons: I s unt mtrx, I δ * * A or A s the complex conugte of A,, or s the complex conugte of (The complex conugte of complex numer s otned y chngng the sgn of the pure mgnry numer or throughout ( to - nd - to ~ ' A T T or A or A s the trnspose of A,, (lnes or rows of A ecome the correspondng columns of A T B s the Hermtn conugte of A T B ( ~ * A A * A B s the dont or dugte of A B Trnspose of the mtrx formed y cofctors of elements of A The dugte of A s often noted Ad (A or  The nverse of A s A - Ad( A A det( A A generl complex numer z + where nd nd re rel numers If z + 0, then z s rel (e, s rel numer If z 0 +, 0, then z s complex numer often clled "pure" mgnry numer For 0 nd 0, z s generl complex numer 7 Tle of Specl Mtrces A s rel *, s rel numer (e, A s complex t lest one element of A tht s complex (e, such * tht A s symmetrc A A T or, A s skew-symmetrc or A -A T, nt-symmetrc (Note: then the re zero nd the trce s zero! A s orthogonl A T A - or AA T A T A I, the unt mtrx U s untry UU U U I (or U U - H s Hermtn H H T* or h h *,, (the egenvlues of Hermtn mtrx re rel numers 9

10 Dol Bgyoko (0 Plese see numercl nlyss ooks (Numercl Recpes s n the Physcs Redng Room for mny other specl mtrces Assgnment: Prove tht the set of m x m mtrces, for m fxed, n whch the nry operton of ddton s defned s done ove, consttutes n Aeln group The opposte of mtrx A s -A, such tht A + (-A (-A +A 0 mtrx Sutrcton s smply prt of the operton of ddton To sutrct mtrx A s to dd ts opposte The opposte of mtrx A s A: A + (-A mtrx If A, -A, nd A + (-A ϕ DIAGONALIZATION OF A MATRIX Equtons of the form A re egenvlue equtons, Lmd, multplyng, s numer A s mtrx In generl, nd re t lest un-column mtrces The generl form of egenvlue equtons s: 0 0 [mtrx (or opertor] [functon ] [numer] [functon ] If A s mtrx, then lso s mtrx such tht the multplcton of the two mtrces s possle So, f A s mtrx, then could e mtrx s shown n exmples dscussed elsewhere [See your textook for detls nd llustrtons] To solve the ove egenvlue equton s the sme s to dgonlze mtrx A There re severl wys for dgonlzng mtrx The one we must know follows (see the textook for others One dgonlzes mtrx A y settng the determnnt of ( A I equl to zero nd y solvng the resultng equton: (for nxn mtrces, ths determnnt wll e polynoml of degree n! A I 0 The soluton of ths equton re the egenvlues of A 0

11 Dol Bgyoko ( Then clculte the determnnt of ths lst mtrx; t s polynoml of degree Hence, ccordng to the fundmentl theorem of lger, ths polynoml hs roots (An n n mtrx, y vrtue of the FTA, wll hve n egenvlues Let us dgonlze the followng mtrx (e, solve the followng egenvlue equton To solve ths egenvlue equton s to dgonlze the mtrx ( 0 or ( 4 0 Hence, ( 4 0 nd ( ± or + nd Consequently, nd For ech egenvlue of the mtrx there corresponds n egenfuncton Wth the ove egenvlues, let us fnd the correspondng egenfunctons We fnd y solvng the equton A where A nd re gven ove ( ( ( So, + 0 nd + 0 A soluton of ths system of two equtons wth two unknowns s We cn tke tht constnt to e Hence, We cn verfy tht Proceedng smlrly, we fnd elow the egenfuncton correspondng to A Set Then, A ecomes:

12 Dol Bgyoko (0 A Ths leds to nd or Therefore, stsfes ths system of equton The rtrry vlue cn e set to e equl to Consequently, We esly verfy tht For ech egenvlue of mtrx, there s n egenfuncton [These egenfunctons re column mtrces n our exmple ove] A ; or s sd to e normlzed when ts squre mgntude s ( * + Ths squre mgntude s not nd hence s not normlzed To normlze, let us defne new functon tht s dvded y the squre-root of ts squre-mgntude of : Set φ Ths new functon, φ, s the normlzed egenfuncton correspondng to It s esly verfed tht * φ φ Hence, φ s normlzed Proceedng smlrly, we cn fnd the normlzed the egenfuncton correspondng to

13 Dol Bgyoko (0 Some key ponts: Dgonlzton tkes mtrx nd trnsforms t nto ts dgonl form Mtrx Dgonlzton, see the textook, cn e ccomplshed usng untry trnsformtons! Theorem- the dgonlzton process does not chnge the trce of mtrx 0 A 0 Tr( A Tr( dgonla Egenvlues of mtrces re fundmentl physcl propertes If the mtrx s tht of the moment of nert, the egenvlues wll e the moments of nert for rottons round the prncpl xes! In sc quntum mechncs, the egenvlues resultng from the Schrödnger equton represent energes of prtcles Crtclly Importnt Pont Aout Mtrx Inverson nd Dgonlzton (Need for hgh precson rthmetc n mtrx nverson or dgonlzton For most mtrces, the clculton of the nverse s done usng computer The sme s true for the dgonlzton of mtrces These two opertons, however, s extremely senstve to errors: Specfclly, smll roundng errors n the nverson of mtrx cn led to huge errors n the nverse mtrx So, mtrx nverson, when performed usng computer, must e done usng doule, qudruple, or hgher precson In computer progrmmng rgon, sngle precson rthmetc crres dgts up to the sxth decml plce whle doule precson rthmetc crres dgts up to the th decml plce When workng on mportnt ssues (medcl reserch, trectory of spcecrft, energes levels of quntum prtcles, etc one MUST PAY EXTREME ATTENTION TO GUARANTEE THAT NO SPURIOUS RESULTS ARE OBTAINED BY CARELESSNESS (flure to utlze hgh precson rthmetc, e, doule, qudruple, etc, precson In quntum mechncs, you wll encounter egenfunctons of the followng type, whch cn not e normlzed utlzng the ove process In such cse, utlze the method of ntegrton to normlze (r Thus, nsert the egenfuncton, (r, nd ts complex conugte nto the followng equton: r ( r e, * ψ ( r ψ ( r dv N, where N represents the vlue of the ntegrl If N, then the functon s normlzed; however f N, you must construct new functon, dvded y the squre-root of the vlue of the ntegrl, N ψ ( r φ ( r, whch s N

14 Dol Bgyoko (0 4 SYSTEM OF ALGEBRIAC EQUATIONS As prevously mentoned n Secton, lgerc equtons do not nvolve dervtves or ntegrls, nd the system cn hve the followng form: x + y + z c x + y + z c x + y + z c It s mportnt to note tht you must lwys plce the system n queston nto the ove cnoncl form A system of lgerc equtons cn e homogeneous or nhomogeneous A System of Homogeneous Algerc Equtons The system s homogeneous f, nd only f, every term n the equtons whch, does not contn vrle, s zero Thus, c,c, nd c s gven ove must e zero A System of Inhomogeneous Algerc Equtons An lgerc equton s nhomogeneous f you hve term tht does not contn vrle nd s not zero Note tht only one equton needs to e nhomogeneous for the system to e nhomogeneous THEOREMS (A system of homogeneous lgerc equtons hs non-trvl solutons f nd only f the determnnt of the mtrx of the coeffcents s zero 0, If the mtrx s not equl to zero, then non-trvl soluton does not exst (A system of nhomogeneous lgerc equtons hs non-trvl solutons f nd only f the determnnt of the mtrx of the coeffcents s dfferent from zero 0 4

15 Dol Bgyoko (0 5 CRAMER METHOD (INHOMOGENEOUS ALGEBRAIC EQUATIONS The Crmer Method s utlzed to solve system of nhomogenous lgerc equtons, e, c,c, nd c re not ll equl to zero (e, t lest one s non-zero Let system of nhomogeneous, lgerc equtons e gven s follows: x + y + z c x + y + z c x + y + z c Let c, c, nd c Let C e the mtrx whose elements re the coeffcents s shown elow C If the determnnt of C s not equl to zero, then one clcultes C x, C y, nd C z s follows you replce ech respectve column of the mtrx y c,c, nd c to fnd the determnnt of ech mtrx Exmple: C x, det (C x? to clculte; C y, det (C y? to clculte; nd C z, det (C z? to clculte Then, y the Crmer Method (lso clled Crmer rule, we hve x det ( c x, y det ( c det ( c y, nd z det ( c det ( c z det ( c 5

16 Dol Bgyoko (0 6 THEOREMS ON LIMITS OF POLYNOMIALS THEOREMS ( A polynoml s functon of ny vrle such s x, t, or n goes to the term wth the hghest exponent when the vrle x, t, or n, goes to nfnty ( As such, the lmt of the polynoml s the term wth the hghest exponent when the vrle goes to nfnty ( Exmple: P(t t + t 7 9t 8-9t 8 when t ( A polynoml s functon of ny vrle such s x, t, or n goes to the term wth the lowest (smllest exponent when the vrle x, t, or n, goes to zero As such, the lmt of the polynoml s the term wth the smllest exponent when the vrle s gong to zero Exmple: P(t t + t 7 9t 8 t when t 0 Applctons of the Theorem ( ove to the study of the convergence of nfnte seres n 5n4 + 9n5 9n5 9 U ( n n, for n So ths seres does not even meet + 5 5n n n 5n the necessry condton for convergence (s we wll see n the next lesson Hence, t dverges 6

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

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

COMPLEX NUMBERS INDEX

COMPLEX NUMBERS INDEX COMPLEX NUMBERS INDEX. The hstory of the complex numers;. The mgnry unt I ;. The Algerc form;. The Guss plne; 5. The trgonometrc form;. The exponentl form; 7. The pplctons of the complex numers. School

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

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

COMPLEX NUMBER & QUADRATIC EQUATION

COMPLEX NUMBER & QUADRATIC EQUATION MCQ COMPLEX NUMBER & QUADRATIC EQUATION Syllus : Comple numers s ordered prs of rels, Representton of comple numers n the form + nd ther representton n plne, Argnd dgrm, lger of comple numers, modulus

More information

6 Roots of Equations: Open Methods

6 Roots of Equations: Open Methods HK Km Slghtly modfed 3//9, /8/6 Frstly wrtten t Mrch 5 6 Roots of Equtons: Open Methods Smple Fed-Pont Iterton Newton-Rphson Secnt Methods MATLAB Functon: fzero Polynomls Cse Study: Ppe Frcton Brcketng

More information

Review of linear algebra. Nuno Vasconcelos UCSD

Review of linear algebra. Nuno Vasconcelos UCSD Revew of lner lgebr Nuno Vsconcelos UCSD Vector spces Defnton: vector spce s set H where ddton nd sclr multplcton re defned nd stsf: ) +( + ) (+ )+ 5) λ H 2) + + H 6) 3) H, + 7) λ(λ ) (λλ ) 4) H, - + 8)

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

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

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

Quiz: Experimental Physics Lab-I

Quiz: Experimental Physics Lab-I Mxmum Mrks: 18 Totl tme llowed: 35 mn Quz: Expermentl Physcs Lb-I Nme: Roll no: Attempt ll questons. 1. In n experment, bll of mss 100 g s dropped from heght of 65 cm nto the snd contner, the mpct s clled

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

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

FINITE NEUTROSOPHIC COMPLEX NUMBERS. W. B. Vasantha Kandasamy Florentin Smarandache

FINITE NEUTROSOPHIC COMPLEX NUMBERS. W. B. Vasantha Kandasamy Florentin Smarandache INITE NEUTROSOPHIC COMPLEX NUMBERS W. B. Vsnth Kndsmy lorentn Smrndche ZIP PUBLISHING Oho 11 Ths book cn be ordered from: Zp Publshng 1313 Chespeke Ave. Columbus, Oho 31, USA Toll ree: (61) 85-71 E-ml:

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

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

Vectors and Tensors. R. Shankar Subramanian. R. Aris, Vectors, Tensors, and the Equations of Fluid Mechanics, Prentice Hall (1962).

Vectors and Tensors. R. Shankar Subramanian. R. Aris, Vectors, Tensors, and the Equations of Fluid Mechanics, Prentice Hall (1962). 005 Vectors nd Tensors R. Shnkr Subrmnn Good Sources R. rs, Vectors, Tensors, nd the Equtons of Flud Mechncs, Prentce Hll (96). nd ppendces n () R. B. Brd, W. E. Stewrt, nd E. N. Lghtfoot, Trnsport Phenomen,

More information

Proof that if Voting is Perfect in One Dimension, then the First. Eigenvector Extracted from the Double-Centered Transformed

Proof that if Voting is Perfect in One Dimension, then the First. Eigenvector Extracted from the Double-Centered Transformed Proof tht f Votng s Perfect n One Dmenson, then the Frst Egenvector Extrcted from the Doule-Centered Trnsformed Agreement Score Mtrx hs the Sme Rn Orderng s the True Dt Keth T Poole Unversty of Houston

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

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

Multiple view geometry

Multiple view geometry EECS 442 Computer vson Multple vew geometry Perspectve Structure from Moton - Perspectve structure from moton prolem - mgutes - lgerc methods - Fctorzton methods - Bundle djustment - Self-clrton Redng:

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

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

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

Principle Component Analysis

Principle Component Analysis Prncple Component Anlyss Jng Go SUNY Bufflo Why Dmensonlty Reducton? We hve too mny dmensons o reson bout or obtn nsghts from o vsulze oo much nose n the dt Need to reduce them to smller set of fctors

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

ESCI 342 Atmospheric Dynamics I Lesson 1 Vectors and Vector Calculus

ESCI 342 Atmospheric Dynamics I Lesson 1 Vectors and Vector Calculus ESI 34 tmospherc Dnmcs I Lesson 1 Vectors nd Vector lculus Reference: Schum s Outlne Seres: Mthemtcl Hndbook of Formuls nd Tbles Suggested Redng: Mrtn Secton 1 OORDINTE SYSTEMS n orthonorml coordnte sstem

More information

ψ ij has the eigenvalue

ψ ij has the eigenvalue Moller Plesset Perturbton Theory In Moller-Plesset (MP) perturbton theory one tes the unperturbed Hmltonn for n tom or molecule s the sum of the one prtcle Foc opertors H F() where the egenfunctons 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

INTRODUCTORY NUMERICAL ANALYSIS

INTRODUCTORY NUMERICAL ANALYSIS ITRODUCTORY UMERICL LYSIS Lecture otes y Mrce ndrecut Unversl Pulshers/UPUBLISHCOM Prlnd FL US Introductory umercl nlyss: Lecture otes Copyrght Mrce ndrecut ll rghts reserved ISB: 877 Unversl Pulshers/uPUBLISHcom

More information

VECTORS AND TENSORS IV.1.1. INTRODUCTION

VECTORS AND TENSORS IV.1.1. INTRODUCTION Chpter IV Vector nd Tensor Anlyss IV. Vectors nd Tensors Septemer 5, 08 05 IV. VECTORS AND TENSORS IV... INTRODUCTION In mthemtcs nd mechncs, we he to operte wth qunttes whch requre dfferent mthemtcl ojects

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

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

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

Chapter 2 Introduction to Algebra. Dr. Chih-Peng Li ( 李 )

Chapter 2 Introduction to Algebra. Dr. Chih-Peng Li ( 李 ) Chpter Introducton to Algebr Dr. Chh-Peng L 李 Outlne Groups Felds Bnry Feld Arthetc Constructon of Glos Feld Bsc Propertes of Glos Feld Coputtons Usng Glos Feld Arthetc Vector Spces Groups 3 Let G be set

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

Section 3.6 Complex Zeros

Section 3.6 Complex Zeros 04 Chapter Secton 6 Comple Zeros When fndng the zeros of polynomals, at some pont you're faced wth the problem Whle there are clearly no real numbers that are solutons to ths equaton, leavng thngs there

More information

Variable time amplitude amplification and quantum algorithms for linear algebra. Andris Ambainis University of Latvia

Variable time amplitude amplification and quantum algorithms for linear algebra. Andris Ambainis University of Latvia Vrble tme mpltude mplfcton nd quntum lgorthms for lner lgebr Andrs Ambns Unversty of Ltv Tlk outlne. ew verson of mpltude mplfcton;. Quntum lgorthm for testng f A s sngulr; 3. Quntum lgorthm for solvng

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

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

Many-Body Calculations of the Isotope Shift

Many-Body Calculations of the Isotope Shift Mny-Body Clcultons of the Isotope Shft W. R. Johnson Mrch 11, 1 1 Introducton Atomc energy levels re commonly evluted ssumng tht the nucler mss s nfnte. In ths report, we consder correctons to tomc levels

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

H-matrix theory and applications

H-matrix theory and applications MtTrd 205, Combr H-mtrx theory nd pplctons Mj Nedovć Unversty of Nov d, erb jont work wth Ljljn Cvetkovć Contents! H-mtrces nd DD-property Benefts from H-subclsses! Brekng the DD Addtve nd multplctve condtons

More information

2.12 Pull Back, Push Forward and Lie Time Derivatives

2.12 Pull Back, Push Forward and Lie Time Derivatives Secton 2.2 2.2 Pull Bck Push Forwrd nd e me Dertes hs secton s n the mn concerned wth the follown ssue: n oserer ttched to fxed sy Crtesn coordnte system wll see mterl moe nd deform oer tme nd wll osere

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

Department of Mechanical Engineering, University of Bath. Mathematics ME Problem sheet 11 Least Squares Fitting of data

Department of Mechanical Engineering, University of Bath. Mathematics ME Problem sheet 11 Least Squares Fitting of data Deprtment of Mechncl Engneerng, Unversty of Bth Mthemtcs ME10305 Prolem sheet 11 Lest Squres Fttng of dt NOTE: If you re gettng just lttle t concerned y the length of these questons, then do hve look t

More information

Chapter 3 MATRIX. In this chapter: 3.1 MATRIX NOTATION AND TERMINOLOGY

Chapter 3 MATRIX. In this chapter: 3.1 MATRIX NOTATION AND TERMINOLOGY Chpter 3 MTRIX In this chpter: Definition nd terms Specil Mtrices Mtrix Opertion: Trnspose, Equlity, Sum, Difference, Sclr Multipliction, Mtrix Multipliction, Determinnt, Inverse ppliction of Mtrix in

More information

Section 8.3 Polar Form of Complex Numbers

Section 8.3 Polar Form of Complex Numbers 80 Chapter 8 Secton 8 Polar Form of Complex Numbers From prevous classes, you may have encountered magnary numbers the square roots of negatve numbers and, more generally, complex numbers whch are the

More information

How do we solve these things, especially when they get complicated? How do we know when a system has a solution, and when is it unique?

How do we solve these things, especially when they get complicated? How do we know when a system has a solution, and when is it unique? XII. LINEAR ALGEBRA: SOLVING SYSTEMS OF EQUATIONS Tody we re going to tlk out solving systems of liner equtions. These re prolems tht give couple of equtions with couple of unknowns, like: 6= x + x 7=

More information

Online Appendix to. Mandating Behavioral Conformity in Social Groups with Conformist Members

Online Appendix to. Mandating Behavioral Conformity in Social Groups with Conformist Members Onlne Appendx to Mndtng Behvorl Conformty n Socl Groups wth Conformst Members Peter Grzl Andrze Bnk (Correspondng uthor) Deprtment of Economcs, The Wllms School, Wshngton nd Lee Unversty, Lexngton, 4450

More information

Bridging the gap: GCSE AS Level

Bridging the gap: GCSE AS Level Bridging the gp: GCSE AS Level CONTENTS Chpter Removing rckets pge Chpter Liner equtions Chpter Simultneous equtions 8 Chpter Fctors 0 Chpter Chnge the suject of the formul Chpter 6 Solving qudrtic equtions

More information

Formulas for the Determinant

Formulas for the Determinant page 224 224 CHAPTER 3 Determnants e t te t e 2t 38 A = e t 2te t e 2t e t te t 2e 2t 39 If 123 A = 345, 456 compute the matrx product A adj(a) What can you conclude about det(a)? For Problems 40 43, use

More information

Chapter 5 Supplemental Text Material R S T. ij i j ij ijk

Chapter 5 Supplemental Text Material R S T. ij i j ij ijk Chpter 5 Supplementl Text Mterl 5-. Expected Men Squres n the Two-fctor Fctorl Consder the two-fctor fxed effects model y = µ + τ + β + ( τβ) + ε k R S T =,,, =,,, k =,,, n gven s Equton (5-) n the textook.

More information

Farey Fractions. Rickard Fernström. U.U.D.M. Project Report 2017:24. Department of Mathematics Uppsala University

Farey Fractions. Rickard Fernström. U.U.D.M. Project Report 2017:24. Department of Mathematics Uppsala University U.U.D.M. Project Report 07:4 Frey Frctions Rickrd Fernström Exmensrete i mtemtik, 5 hp Hledre: Andres Strömergsson Exmintor: Jörgen Östensson Juni 07 Deprtment of Mthemtics Uppsl University Frey Frctions

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

More metrics on cartesian products

More metrics on cartesian products More metrcs on cartesan products If (X, d ) are metrc spaces for 1 n, then n Secton II4 of the lecture notes we defned three metrcs on X whose underlyng topologes are the product topology The purpose of

More information

Foundations of Arithmetic

Foundations of Arithmetic Foundatons of Arthmetc Notaton We shall denote the sum and product of numbers n the usual notaton as a 2 + a 2 + a 3 + + a = a, a 1 a 2 a 3 a = a The notaton a b means a dvdes b,.e. ac = b where c s an

More information

CISE 301: Numerical Methods Lecture 5, Topic 4 Least Squares, Curve Fitting

CISE 301: Numerical Methods Lecture 5, Topic 4 Least Squares, Curve Fitting CISE 3: umercl Methods Lecture 5 Topc 4 Lest Squres Curve Fttng Dr. Amr Khouh Term Red Chpter 7 of the tetoo c Khouh CISE3_Topc4_Lest Squre Motvton Gven set of epermentl dt 3 5. 5.9 6.3 The reltonshp etween

More information

Chapter 1: Fundamentals

Chapter 1: Fundamentals Chpter 1: Fundmentls 1.1 Rel Numbers Types of Rel Numbers: Nturl Numbers: {1, 2, 3,...}; These re the counting numbers. Integers: {... 3, 2, 1, 0, 1, 2, 3,...}; These re ll the nturl numbers, their negtives,

More information

Physics 121 Sample Common Exam 2 Rev2 NOTE: ANSWERS ARE ON PAGE 7. Instructions:

Physics 121 Sample Common Exam 2 Rev2 NOTE: ANSWERS ARE ON PAGE 7. Instructions: Physcs 121 Smple Common Exm 2 Rev2 NOTE: ANSWERS ARE ON PAGE 7 Nme (Prnt): 4 Dgt ID: Secton: Instructons: Answer ll 27 multple choce questons. You my need to do some clculton. Answer ech queston on the

More information

INTRODUCTION TO LINEAR ALGEBRA

INTRODUCTION TO LINEAR ALGEBRA ME Applied Mthemtics for Mechnicl Engineers INTRODUCTION TO INEAR AGEBRA Mtrices nd Vectors Prof. Dr. Bülent E. Pltin Spring Sections & / ME Applied Mthemtics for Mechnicl Engineers INTRODUCTION TO INEAR

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

Strong Gravity and the BKL Conjecture

Strong Gravity and the BKL Conjecture Introducton Strong Grvty nd the BKL Conecture Dvd Slon Penn Stte October 16, 2007 Dvd Slon Strong Grvty nd the BKL Conecture Introducton Outlne The BKL Conecture Ashtekr Vrbles Ksner Sngulrty 1 Introducton

More information

Inner Product. Euclidean Space. Orthonormal Basis. Orthogonal

Inner Product. Euclidean Space. Orthonormal Basis. Orthogonal Inner Product Defnton 1 () A Eucldean space s a fnte-dmensonal vector space over the reals R, wth an nner product,. Defnton 2 (Inner Product) An nner product, on a real vector space X s a symmetrc, blnear,

More information

SUMMER KNOWHOW STUDY AND LEARNING CENTRE

SUMMER KNOWHOW STUDY AND LEARNING CENTRE SUMMER KNOWHOW STUDY AND LEARNING CENTRE Indices & Logrithms 2 Contents Indices.2 Frctionl Indices.4 Logrithms 6 Exponentil equtions. Simplifying Surds 13 Opertions on Surds..16 Scientific Nottion..18

More information

Demand. Demand and Comparative Statics. Graphically. Marshallian Demand. ECON 370: Microeconomic Theory Summer 2004 Rice University Stanley Gilbert

Demand. Demand and Comparative Statics. Graphically. Marshallian Demand. ECON 370: Microeconomic Theory Summer 2004 Rice University Stanley Gilbert Demnd Demnd nd Comrtve Sttcs ECON 370: Mcroeconomc Theory Summer 004 Rce Unversty Stnley Glbert Usng the tools we hve develoed u to ths ont, we cn now determne demnd for n ndvdul consumer We seek demnd

More information

Introduction to Vapor/Liquid Equilibrium, part 2. Raoult s Law:

Introduction to Vapor/Liquid Equilibrium, part 2. Raoult s Law: CE304, Sprng 2004 Lecture 4 Introducton to Vapor/Lqud Equlbrum, part 2 Raoult s Law: The smplest model that allows us do VLE calculatons s obtaned when we assume that the vapor phase s an deal gas, and

More information

APPENDIX A Some Linear Algebra

APPENDIX A Some Linear Algebra APPENDIX A Some Lnear Algebra The collecton of m, n matrces A.1 Matrces a 1,1,..., a 1,n A = a m,1,..., a m,n wth real elements a,j s denoted by R m,n. If n = 1 then A s called a column vector. Smlarly,

More information

Matrix Eigenvalues and Eigenvectors September 13, 2017

Matrix Eigenvalues and Eigenvectors September 13, 2017 Mtri Eigenvlues nd Eigenvectors September, 7 Mtri Eigenvlues nd Eigenvectors Lrry Cretto Mechnicl Engineering 5A Seminr in Engineering Anlysis September, 7 Outline Review lst lecture Definition of eigenvlues

More information

Geometric Sequences. Geometric Sequence a sequence whose consecutive terms have a common ratio.

Geometric Sequences. Geometric Sequence a sequence whose consecutive terms have a common ratio. Geometric Sequences Geometric Sequence sequence whose consecutive terms hve common rtio. Geometric Sequence A sequence is geometric if the rtios of consecutive terms re the sme. 2 3 4... 2 3 The number

More information

Chapter Newton-Raphson Method of Solving a Nonlinear Equation

Chapter Newton-Raphson Method of Solving a Nonlinear Equation Chpter 0.04 Newton-Rphson Method o Solvng Nonlner Equton Ater redng ths chpter, you should be ble to:. derve the Newton-Rphson method ormul,. develop the lgorthm o the Newton-Rphson method,. use the Newton-Rphson

More information

Three hours UNIVERSITY OF MANCHESTER SCHOOL OF COMPUTER SCIENCE. Date: Wednesday 16th January 2013 Time: 09:45-12:45

Three hours UNIVERSITY OF MANCHESTER SCHOOL OF COMPUTER SCIENCE. Date: Wednesday 16th January 2013 Time: 09:45-12:45 Three hours UNIVERSITY OF MANHESTER SHOOL OF OMPUTER SIENE Prllel Progrms nd ther Performnce Dte: Wednesdy 16th Jnury 2013 Tme: 09:45-12:45 Plese nswer ny TWO Questons from the FOUR Questons provded. Ths

More information

Generalized Spectral Resolution & some of its applications

Generalized Spectral Resolution & some of its applications Generlzed Spectrl Resoluton & some of ts pplctons Nchols Wheeler, Reed College Physcs Deprtment 27 Aprl 29 Introducton Fmlrly, f the n n mtrx H s complex hermtn (or, more prtculrly, rel symmetrc or mgnry

More information

September 13 Homework Solutions

September 13 Homework Solutions College of Engineering nd Computer Science Mechnicl Engineering Deprtment Mechnicl Engineering 5A Seminr in Engineering Anlysis Fll Ticket: 5966 Instructor: Lrry Cretto Septemer Homework Solutions. Are

More information

Matrix Algebra. Matrix Addition, Scalar Multiplication and Transposition. Linear Algebra I 24

Matrix Algebra. Matrix Addition, Scalar Multiplication and Transposition. Linear Algebra I 24 Mtrix lger Mtrix ddition, Sclr Multipliction nd rnsposition Mtrix lger Section.. Mtrix ddition, Sclr Multipliction nd rnsposition rectngulr rry of numers is clled mtrix ( the plurl is mtrices ) nd the

More information

Designing Information Devices and Systems I Discussion 8B

Designing Information Devices and Systems I Discussion 8B Lst Updted: 2018-10-17 19:40 1 EECS 16A Fll 2018 Designing Informtion Devices nd Systems I Discussion 8B 1. Why Bother With Thévenin Anywy? () Find Thévenin eqiuvlent for the circuit shown elow. 2kΩ 5V

More information

Finite Fields and Their Applications

Finite Fields and Their Applications Fnte Felds nd Ther Applctons 18 (2012) 271 282 Contents lsts vlble t ScVerse ScenceDrect Fnte Felds nd Ther Applctons www.elsever.com/locte/ff Bnoml nd fctorl congruences for F q [t] Dnesh S. Thkur 1 Deprtment

More information

Chapter I Vector Analysis

Chapter I Vector Analysis . Chpte I Vecto nlss . Vecto lgeb j It s well-nown tht n vecto cn be wtten s Vectos obe the followng lgebc ules: scl s ) ( j v v cos ) ( e Commuttv ) ( ssoctve C C ) ( ) ( v j ) ( ) ( ) ( ) ( (v) he lw

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

Fall 2012 Analysis of Experimental Measurements B. Eisenstein/rev. S. Errede. with respect to λ. 1. χ λ χ λ ( ) λ, and thus:

Fall 2012 Analysis of Experimental Measurements B. Eisenstein/rev. S. Errede. with respect to λ. 1. χ λ χ λ ( ) λ, and thus: More on χ nd errors : uppose tht we re fttng for sngle -prmeter, mnmzng: If we epnd The vlue χ ( ( ( ; ( wth respect to. χ n Tlor seres n the vcnt of ts mnmum vlue χ ( mn χ χ χ χ + + + mn mnmzes χ, nd

More information

Polynomials and Division Theory

Polynomials and Division Theory Higher Checklist (Unit ) Higher Checklist (Unit ) Polynomils nd Division Theory Skill Achieved? Know tht polynomil (expression) is of the form: n x + n x n + n x n + + n x + x + 0 where the i R re the

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

MTH 146 Class 7 Notes

MTH 146 Class 7 Notes 7.7- Approxmte Itegrto Motvto: MTH 46 Clss 7 Notes I secto 7.5 we lered tht some defte tegrls, lke x e dx, cot e wrtte terms of elemetry fuctos. So, good questo to sk would e: How c oe clculte somethg

More information

p-adic Egyptian Fractions

p-adic Egyptian Fractions p-adic Egyptin Frctions Contents 1 Introduction 1 2 Trditionl Egyptin Frctions nd Greedy Algorithm 2 3 Set-up 3 4 p-greedy Algorithm 5 5 p-egyptin Trditionl 10 6 Conclusion 1 Introduction An Egyptin frction

More information

The area under the graph of f and above the x-axis between a and b is denoted by. f(x) dx. π O

The area under the graph of f and above the x-axis between a and b is denoted by. f(x) dx. π O 1 Section 5. The Definite Integrl Suppose tht function f is continuous nd positive over n intervl [, ]. y = f(x) x The re under the grph of f nd ove the x-xis etween nd is denoted y f(x) dx nd clled the

More information

Dennis Bricker, 2001 Dept of Industrial Engineering The University of Iowa. MDP: Taxi page 1

Dennis Bricker, 2001 Dept of Industrial Engineering The University of Iowa. MDP: Taxi page 1 Denns Brcker, 2001 Dept of Industrl Engneerng The Unversty of Iow MDP: Tx pge 1 A tx serves three djcent towns: A, B, nd C. Ech tme the tx dschrges pssenger, the drver must choose from three possble ctons:

More information

Zbus 1.0 Introduction The Zbus is the inverse of the Ybus, i.e., (1) Since we know that

Zbus 1.0 Introduction The Zbus is the inverse of the Ybus, i.e., (1) Since we know that us. Introducton he us s the nverse of the us,.e., () Snce we now tht nd therefore then I V () V I () V I (4) So us reltes the nodl current njectons to the nodl voltges, s seen n (4). In developng the power

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

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

p (i.e., the set of all nonnegative real numbers). Similarly, Z will denote the set of all

p (i.e., the set of all nonnegative real numbers). Similarly, Z will denote the set of all th Prelmnry E 689 Lecture Notes by B. Yo 0. Prelmnry Notton themtcl Prelmnres It s ssumed tht the reder s fmlr wth the noton of set nd ts elementry oertons, nd wth some bsc logc oertors, e.g. x A : x s

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

Section 7.1 Integration by Substitution

Section 7.1 Integration by Substitution Section 7. Integrtion by Substitution Evlute ech of the following integrls. Keep in mind tht using substitution my not work on some problems. For one of the definite integrls, it is not possible to find

More information

ECON 331 Lecture Notes: Ch 4 and Ch 5

ECON 331 Lecture Notes: Ch 4 and Ch 5 Mtrix Algebr ECON 33 Lecture Notes: Ch 4 nd Ch 5. Gives us shorthnd wy of writing lrge system of equtions.. Allows us to test for the existnce of solutions to simultneous systems. 3. Allows us to solve

More information

PART 1: VECTOR & TENSOR ANALYSIS

PART 1: VECTOR & TENSOR ANALYSIS PART : VECTOR & TENSOR ANALYSIS wth LINEAR ALGEBRA Obectves Introduce the concepts, theores, nd opertonl mplementton of vectors, nd more generlly tensors, n dvnced engneerng nlyss. The emphss s on geometrc

More information

2.4 Linear Inequalities and Interval Notation

2.4 Linear Inequalities and Interval Notation .4 Liner Inequlities nd Intervl Nottion We wnt to solve equtions tht hve n inequlity symol insted of n equl sign. There re four inequlity symols tht we will look t: Less thn , Less thn or

More information

Before we can begin Ch. 3 on Radicals, we need to be familiar with perfect squares, cubes, etc. Try and do as many as you can without a calculator!!!

Before we can begin Ch. 3 on Radicals, we need to be familiar with perfect squares, cubes, etc. Try and do as many as you can without a calculator!!! Nme: Algebr II Honors Pre-Chpter Homework Before we cn begin Ch on Rdicls, we need to be fmilir with perfect squres, cubes, etc Try nd do s mny s you cn without clcultor!!! n The nth root of n n Be ble

More information

The graphs of Rational Functions

The graphs of Rational Functions Lecture 4 5A: The its of Rtionl Functions s x nd s x + The grphs of Rtionl Functions The grphs of rtionl functions hve severl differences compred to power functions. One of the differences is the behvior

More information

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X Statstcs 1: Probablty Theory II 37 3 EPECTATION OF SEVERAL RANDOM VARIABLES As n Probablty Theory I, the nterest n most stuatons les not on the actual dstrbuton of a random vector, but rather on a number

More information

8.6 The Complex Number System

8.6 The Complex Number System 8.6 The Complex Number System Earler n the chapter, we mentoned that we cannot have a negatve under a square root, snce the square of any postve or negatve number s always postve. In ths secton we want

More information