A Spatial Version of the Theorem of the Angle of Circumference

Size: px
Start display at page:

Download "A Spatial Version of the Theorem of the Angle of Circumference"

Transcription

1 This is a pr-print o a contribution publishd in In L. Cocchiarlla (d): ICGG Procdings o th 18th Intrnational Conrnc on Gomtr and Graphics, 40th Annivrsar, Milan/Ital 2018, pp , publishd b Springr Intrnational Publishing AG 2019 (ISBN ). Th inal authnticatd vrsion is availabl onlin at A Spatial Vrsion o th Thorm o th Angl o Circumrnc Gorg Glasr 1, Boris Odhnal 1, and Hllmuth Stachl 2 1 Univrsit o Applid Arts Vinna, Vinna, Austria gorg.glasr@uni-ak.ac.at, boris.odhnal@uni-ak.ac.at, 2 TU Win, Vinna, Austria stachl@dmg.tuwin.ac.at Abstract. W tr a gnraliation o th thorm o th angl o circumrnc to a vrsion in thr-dimnsional Euclidan spac and ask or pairs (ε, ϕ) o plans passing through two (dirnt skw) straight lins ε and ϕ such that th angl α nclosd b ε and ϕ is constant. It turns out that th st o all such intrsction lins is a quartic ruld surac with bing its doubl curv. W shall stud th surac and its proprtis togthr with crtain spcial apparancs showing up or spcial valus o som shap paramtrs such as th slop o and (with rspct to a id plan) or th angl α. Kwords: ruld surac, angl o circumrnc, quartic ruld surac, Thaloid, isoptic surac 1 Introduction Th thorm o th angl o circumrnc stats that a straight lin sgmnt (boundd b two points E and F) in th Euclidan plan is sn at a constant angl α rom an point o a pair o circular arcs passing through E and F. Espciall, i th visual angl α is a right angl, th pair o circls bcoms on circl with diamtr EF, usuall rrrd to as th Thals circl. It would b natural to gnrali th thorm o th angl o circumrnc in Euclidan thr-spac b asking or all points that s a straight lin sgmnt boundd b two points E and F undr a constant angl α. Th locus o all such points is an algbraic surac o dgr our. It is obvious that th lattr surac has a rotational smmtr - th ais o th rotation coincids with th straight lin [E,F] - and this isoptic surac can b obtaind b rotating th pair o circular arcs through E and F, and is thror, a torus, s Fig. 1. Isoptic curvs o sphrical conics ar also wll-known, s [1]. In this contribution, w tr a lin gomtric gnraliation. W ask or th st o all intrsction lins r o plans rom two pncils. Th lins r can b considrd as on-dimnsional sing a pair o straight lins undr a constant angl. In Sction 2, w shall driv th quation o th ruld surac carring all th lins that s a pair (,) o (skw) straight lins undr constant angl. From

2 2 Gorg Glasr t al. E α α F Fig. 1. A possibl gnraliation o th thorm o th angl o circumrnc in thrdimnsional Euclidan spac. th quation o w can driv som proprtis o th surac which shall b th contnts o Sction 3. Finall, in Sction 4 w look at spcial cass o th ruld surac that appar i ithr th as and rach a spcial rlativ position or i th angl α attains spcial valus or i vn both is th cas. 2 Equation o th ruld surac It is avorabl to rprsnt points in Euclidan thr-spac R 3 b Cartsian coordinats (,,). It mans no rstriction to assum that th as and o th two pncils o plans ar givn b d 0 d 0 = 0 +t 1, = 0 +u 1 (1) 0 k 0 k paramtridbralparamtrst,u R.Hrand inth ollowing, = 2d R is th distanc btwn th straight lins, and k R is thir slop with rspct to th plan = 0, s Fig. 2. Sinc g = (0,1,k) and h = (0,1, k) ar th dirctions o th lins and, th normals o th plans ε and ϕ ar linar combinations o g 1 = (0, k,1), g 2 = (1,0,0) or h 1 = (0,k,1), h 2 = g 2, rspctivl. With λ,µ R w lt n ε = g 1 +λg 2, n ϕ = h 1 +µh 2. (2) Now, w can writ down th condition <)(ε,ϕ) = <)(n ε,n ϕ ) = α b valuating n ε,n ϕ 2 = A 2 n ε,n ε n ϕ,n ϕ

3 A spatial vrsion o th thorm o th angl o circumrnc 3 k d 1 k d 1 Fig.2. Choic o a Cartsian coordinat sstm and th maning o d and k. whr u,v dnots th canonical scalar product o two vctors u,v R 3 and A := cosα. This givs (1 k 2 +λµ) 2 = A 2 (1+k 2 +λ 2 )(1+k 2 +µ 2 ). (3) Th plans rom ithr pncil hav normal vctors givn in (2), and thus, th hav th quations ε : λ k + = dλ, (4) ϕ : µ+k + = dµ. Soar,both λandµcanvarrlinr,andthus,th plansεandϕintrsctin th lins o a hprbolic linar lin congrunc with as and, paramtrid b r(t,λ,µ) = d k k µ µk +t 2k µ λ k(λ+µ) (5) whr t R is th paramtr on th lins in th congrunc. Th ruld surac w ar aiming at is prcisl that subst o th congrunc (5) whr λ and µ ar subjct to (3). Th quation o th ruld surac in trms o Cartsian coordinats is obtaind rom th paramtriation (5) b liminating all paramtrs t, λ, µ: Assum r = (r,r,r ). Thn, w liminat t rom r, r, and r b computing th rsultants r 1 := rs( r, r,t), r 2 := rs( r, r,t). In th nt stp, w liminat λ rom both, r 1 and r 2 using (3) which rsults in two urthr polnomials r 1 R[,,µ] and r 2 R[,,µ]. It would mak no dirnc i w liminat µ irst. Finall, th rsultant o r 1 and r 2 with rspct

4 4 Gorg Glasr t al. to µ contains a non-trivial actor which is th quation o. (Th trivial actors o th lattr rsultant ar dtctd b substituting (5) and vriing that th do not vanish.) So, w obtain th ollowing quation o : σ 1 σ 2 ( 2 d 2 ) 2 B 2 ( 2 k 2 2 ) σ 3 (d 2 2 +k )+2σ 4 (d 2 k )+ 8A 2 dk(1+k 2 ) = 0 (6) with th abbrviations σ 1,2 := A k 2 ±k 2 +A 1, σ 3,4 := A 2 k 2 k 2 +A 2 ±1, and B 2 = 1 A 2 (or B = sinα). Summariing, w can stat: Thorm 1. Th isoptic ruld surac as th st o intrsction lins r o plans ε, ϕ rom two pncils with as, and <)(ε,ϕ) = α = const. is th algbraic ruld surac with th quation (6) and is, in gnral, o dgr our. Fig. 3 shows an ampl o a ruld surac togthr with th as and o th pncils o plans. In th cas A = 0 which is quivalnt to α = π 2, thr ists a gnration o b mans o a projctiv mapping κ rom th pncil o plans about to th pncil o plans about. Th projctivit κ assigns to ach plan ε (through ) prcisl on plan ϕ (through ) such that ε ϕ. Thus, th lins ε κ(ε) orm a rgulus, i.., on amil o straight lins on a (rgular) ruld quadric. Insrting A = 0 into (6) rturns th quation o th rgular ruld quadric which is in an cas a hprboloid (with multiplicit two): ((1 k 2 ) 2 k d 2 (k 2 1)) 2 = 0 (7) an ampl o which is shown in Fig Proprtis o From th construction o it is clar that th lins and ar part o th surac. Morovr, th union o ths lins is th doubl curv o. Hnc, is o Sturm tp 1, c. [2]. Sinc is o Sturm tp 1, it is lliptic. Each plan ε in th pncil about intrscts along with multiplicit 2. Sinc ach such plan ε contains at last on gnrator, th rmaining part o ε has to b a straight lin s too. Th lin s is a urthr gnrator o. A similar statmnt can b mad about th plans ϕ through. Th tangnt plans o mt along (planar) cubic curvs which ar ithr rational or lliptic, s Fig. 5. Th quartic ruld surac carris no rgular conic: An plan ε through a pair o intrscting gnrators g 1, g 2 shars on

5 A spatial vrsion o th thorm o th angl o circumrnc 5 ϕ r ε Fig.3. Th quartic isoptic ruld surac o a pair o skw straight lins and. o th as, sa, with. Thror, th rmaining part o ε \ {,g 1,g 2 } has to b a straight lin l and l is a singular conic, c. [2]. I w prorm th projctiv closur o th Euclidan thr-spac, thn w can look s intrsction with th idal plan, s Fig. 6. Th idal points E and F o th straight lins and ar th onl doubl points o th lliptic quartic. An quation o can obtaind rom (6) b rmoving all trms o dgr thr and lss: : (σ 1 σ k 2 σ σ 4 2 ) 2 B 2 (k ) 2 = 0. (8) Thn, w intrprt : : as homognous coordinats o points in th plan at ininit and not that in s quation d dos not show up. 4 Spcial cass W can pct cptional apparancs o th quartic ruld surac i w choos spcial valus or A, d, or k. Although all ths valus ar originall assumd to b ral and spciall A 1, w nd not rstrictd ourslvs to ral valus. In th ollowing, w shall discuss som o ths spcial choics that lad to somtims unpctd suracs which, vntuall, ar thn no longr ruld suracs with ral rulings.

6 6 Gorg Glasr t al. Fig.4. A on-shtd hprboloid appars i A = 0, d,k R, c. (7). 4.1 On-shtd hprboloids. Intrscting lins and. In th vr bginning, w mad th natural assumption 2d = 0, i.., th lins and ar skw. I w allow d = 0, thn (6) simpliis to (8) which coms as no surpris, sinc (8) is indpndnt o d. Thror, (8) can also b viwd as th quation o a quartic con Γ manating rom (0,0,0). Obviousl, and ar gnrators with multiplicit two. Th con Γ is th asmptotic con o an ampl o which is displad in Fig. 7. Furthr, i k = 0 (togthr with d = 0 this actuall mans = ), thn Γ dgnratsandbcomsthpairoisotropicplans = 0with multiplicit two. I w allow A = 0, th con Γ bcoms th quadratic con (k 2 1) 2 +k = 0 (9) with multiplicit two. Th quadratic con (9) is a normal con (c. [1, p ]) and it is th asmptotic con o th doubl hprboloid (7) bing th spcial orm o i A = 0. An intrsting cas occurs i k = ±i (bsids d = 0), i.., th as and o th pncils o plans ar isotropic lins. In this cas, splits into two singular quadrics: 2 2 +(1 A) 2 +(1 A) 2 = 0, 2 2 +(1+A) 2 +(1+A) 2 (10) = 0.

7 A spatial vrsion o th thorm o th angl o circumrnc 7 τ c r Fig.5. Th quartic ruld surac carris a two-paramtr amil o cubic curvs which com as th intrsction o with its tangnt plans. Hr: τ = r c whr r τ is a ruling, τ is a tangnt plan through r, and c is th cubic curv. Y E Z F X Fig.6. Th intrsction o with th plan at ininit is an lliptic quartic curv with th two doubl points E and F which ar th idal points o s doubl curv.

8 8 Gorg Glasr t al. Fig.7. Intrscting lins and produc a quartic con which is also th asmptotic con o th gnric (non-dgnrat) quartic ruld surac. On o ths bcoms a plan with multiplicit two i ithr A = +1 or A = 1 whil th othr on bcoms an isotropic con = 0. Th cas A < 1 turns both o th quadrics into cons without an ral points bsids th common vrt (0,0,0). A > 1 corrsponds to purl imaginar angls α i ln(a+ A 2 1) (mod 2π). Nvrthlss, insrting A > 1 into (10) maks ithr th irst or th scond quadric a con with ral points whil th othr still has onl on ral point, naml th vrt (0,0,0). Paralll lins and. Th cas o paralllas and is clarlan trusion o th planar igur o th thorm o th angl o circumrnc. Thus, th ruld surac (6) will split into two clindrs 1 and 2 o rvolution rctd on thos circular arcs in th [,]-plan which ar th locus o all points sing th lin sgmnt EF (with E,F = (±d,0,0)) undr constant angl α (c. Fig. 8). From (6) w ind th quation o th dgnrat quartic b rplacing k with 1/K and subsquntl stting K = 0. (Othrwis, w would hav to st k =.) This rsults in th pctd pair o clindrs o rvolution 1,2 : ± 2dA 1 A 2 d2 = 0.

9 A spatial vrsion o th thorm o th angl o circumrnc 9 Fig.8. A pair o clindrs o rvolution as th isoptic ruld surac o paralll lins and. In ordr to ind ral suracs i, th valus or A ar rstrictd to A 0. Th Thaloid = d 2 (clindr orvolution)throughand cannot b obtaind dirctl rom th clindrs quations, sinc thn A = 1. Othr quadrics. Th as and o th pncils o plans can b chosn as isotropic lins. Thror, w lt k = i. (Th choic k = i producs th sam rsult.) Again, w ind that(6) dgnrats and splits into quadratic polnomials: Q 1 : 2 2 +(1 A) 2 +(1 A) 2 = 2d 2, Q 2 : 2 2 +(1+A) 2 +(1+A) 2 = 2d 2. (11) Th cas d = 0 was discussd arlir, so w hav d 0 in th ollowing. Indpndnt o th choic o A and rgardlss o th rgularit, both quadrics Q 1 and Q 2 hav th -as or thir common ais o rvolution. In th vr spcial cas A = ±1, th pair o quadrics (11) contains prcisl th singular quadric 2 d 2 = ( d)(+d) = 0 (a pair o (ral) paralll plans) and th Euclidan sphr = d 2 with radius d cntrd at (0,0,0) touching th plans at (±d,0,0). I A > 1, th pair (Q 1,Q 2 ) o quadrics consists o a two-shtd hprboloid o rvolution and an llipsoid o rvolution. Finall, w obtain two llipsoids o rvolution i A < 1. Th ollowing tabl summaris th spcial and dgnrat cass o dpnding on spcial choics o A, k, d.

10 10 Gorg Glasr t al. A = 0 k = 0 k = i k = (d ) 2 = 0 (2d ) 2 = 0 (d ) 2 = 0 right clindr, µ = 2 llipsoid, µ = 2 right clindr, µ = 2 d = 0 d = 0 d = 0 ( ) 2 = 0 ( ) 2 = 0 ( ) 2 = 0 compl. conj. plans, con, no ral compl. conj. plans, µ = 2 point (0,0,0), µ = 2 µ = 2 d = i d = i d = i ( ) 2 = 0 ( ) 2 = 0 ( ) 2 = 0 right clindr, llipsoid, right clindr, no ral points, µ = 2 no ral point, µ = 2 no ral point, µ = 2 A = 1 k = 0 k = i k = 2 = 0 ( 2 d 2 )(d )=0 2 = 0 plan, µ = 2 sphr tangnt plans plan, µ = 2 d = 0 d = 0 d = 0 2 ( )=0 mpt st ral doubl plan mpt st isotropic con d = i d = i d = i 2 = 0 ( 2 +1)( ) 2 =0 2 = 0 plan, µ = 2 sphr, no ral point plan, µ = 2 compl. tang. plans Tabl 1. Spcial shaps o causd b A = 0,1, α = 0, π, d = 0, k = 0,,i; 2 th intgr µ dnots th multiplicitis o th componnts. Rrncs 1. G. Glasr, H. Stachl, B. Odhnal: Th Univrs o Conics. From th ancint Grks to 21 st cntur dvlopmnts. Springr-Spktrum, Springr-Vrlag, Hidlbrg, E. Müllr: Vorlsungn übr Darstllnd Gomtri. III. Band: Konstruktiv Bhandlung dr Rgllächn. Dutick, Lipig und Win, H. Wilitnr: Spill Ebn Kurv. Sammlung Schubrt LVI, G.J. Göschn sch Vrlagshandlung, Lipig, 1908.

Section 11.6: Directional Derivatives and the Gradient Vector

Section 11.6: Directional Derivatives and the Gradient Vector Sction.6: Dirctional Drivativs and th Gradint Vctor Practic HW rom Stwart Ttbook not to hand in p. 778 # -4 p. 799 # 4-5 7 9 9 35 37 odd Th Dirctional Drivativ Rcall that a b Slop o th tangnt lin to th

More information

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the Copyright itutcom 005 Fr download & print from wwwitutcom Do not rproduc by othr mans Functions and graphs Powr functions Th graph of n y, for n Q (st of rational numbrs) y is a straight lin through th

More information

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values Dnamic Macroconomic Thor Prof. Thomas Lux Bifurcation Thor Bifurcation: qualitativ chang in th natur of th solution occurs if a paramtr passs through a critical point bifurcation or branch valu. Local

More information

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013 18.782 Introduction to Arithmtic Gomtry Fall 2013 Lctur #20 11/14/2013 20.1 Dgr thorm for morphisms of curvs Lt us rstat th thorm givn at th nd of th last lctur, which w will now prov. Thorm 20.1. Lt φ:

More information

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

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

More information

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim.

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim. MTH rviw part b Lucian Mitroiu Th LOG and EXP functions Th ponntial function p : R, dfind as Proprtis: lim > lim p Eponntial function Y 8 6 - -8-6 - - X Th natural logarithm function ln in US- log: function

More information

u 3 = u 3 (x 1, x 2, x 3 )

u 3 = u 3 (x 1, x 2, x 3 ) Lctur 23: Curvilinar Coordinats (RHB 8.0 It is oftn convnint to work with variabls othr than th Cartsian coordinats x i ( = x, y, z. For xampl in Lctur 5 w mt sphrical polar and cylindrical polar coordinats.

More information

First derivative analysis

First derivative analysis Robrto s Nots on Dirntial Calculus Chaptr 8: Graphical analysis Sction First drivativ analysis What you nd to know alrady: How to us drivativs to idntiy th critical valus o a unction and its trm points

More information

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero.

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero. SETION 6. 57 6. Evaluation of Dfinit Intgrals Exampl 6.6 W hav usd dfinit intgrals to valuat contour intgrals. It may com as a surpris to larn that contour intgrals and rsidus can b usd to valuat crtain

More information

Text: WMM, Chapter 5. Sections , ,

Text: WMM, Chapter 5. Sections , , Lcturs 6 - Continuous Probabilit Distributions Tt: WMM, Chaptr 5. Sctions 6.-6.4, 6.6-6.8, 7.-7. In th prvious sction, w introduc som of th common probabilit distribution functions (PDFs) for discrt sampl

More information

DIFFERENTIAL EQUATION

DIFFERENTIAL EQUATION MD DIFFERENTIAL EQUATION Sllabus : Ordinar diffrntial quations, thir ordr and dgr. Formation of diffrntial quations. Solution of diffrntial quations b th mthod of sparation of variabls, solution of homognous

More information

Thomas Whitham Sixth Form

Thomas Whitham Sixth Form Thomas Whitham Sith Form Pur Mathmatics Unit C Algbra Trigonomtr Gomtr Calculus Vctor gomtr Pag Algbra Molus functions graphs, quations an inqualitis Graph of f () Draw f () an rflct an part of th curv

More information

Division of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):.

Division of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):. Division of Mchanics Lund Univrsity MULTIBODY DYNMICS Examination 7033 Nam (writ in block lttrs):. Id.-numbr: Writtn xamination with fiv tasks. Plas chck that all tasks ar includd. clan copy of th solutions

More information

2008 AP Calculus BC Multiple Choice Exam

2008 AP Calculus BC Multiple Choice Exam 008 AP Multipl Choic Eam Nam 008 AP Calculus BC Multipl Choic Eam Sction No Calculator Activ AP Calculus 008 BC Multipl Choic. At tim t 0, a particl moving in th -plan is th acclration vctor of th particl

More information

That is, we start with a general matrix: And end with a simpler matrix:

That is, we start with a general matrix: And end with a simpler matrix: DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss

More information

3 Finite Element Parametric Geometry

3 Finite Element Parametric Geometry 3 Finit Elmnt Paramtric Gomtry 3. Introduction Th intgral of a matrix is th matrix containing th intgral of ach and vry on of its original componnts. Practical finit lmnt analysis rquirs intgrating matrics,

More information

Note If the candidate believes that e x = 0 solves to x = 0 or gives an extra solution of x = 0, then withhold the final accuracy mark.

Note If the candidate believes that e x = 0 solves to x = 0 or gives an extra solution of x = 0, then withhold the final accuracy mark. . (a) Eithr y = or ( 0, ) (b) Whn =, y = ( 0 + ) = 0 = 0 ( + ) = 0 ( )( ) = 0 Eithr = (for possibly abov) or = A 3. Not If th candidat blivs that = 0 solvs to = 0 or givs an tra solution of = 0, thn withhold

More information

LINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM

LINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM Elctronic Journal of Diffrntial Equations, Vol. 2003(2003), No. 92, pp. 1 6. ISSN: 1072-6691. URL: http://jd.math.swt.du or http://jd.math.unt.du ftp jd.math.swt.du (login: ftp) LINEAR DELAY DIFFERENTIAL

More information

Sectrix Curves on the Sphere

Sectrix Curves on the Sphere riginal scintific papr Accptd 22. 2. 205. LÁSZLÓ NÉMETH Sctri Curvs on th Sphr Sctri Curvs on th Sphr ABSTRACT In this papr w introduc a class of curvs drivd from a gomtrical construction. Ths planar curvs

More information

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 0 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat th

More information

MATHEMATICS PAPER IB COORDINATE GEOMETRY(2D &3D) AND CALCULUS. Note: This question paper consists of three sections A,B and C.

MATHEMATICS PAPER IB COORDINATE GEOMETRY(2D &3D) AND CALCULUS. Note: This question paper consists of three sections A,B and C. MATHEMATICS PAPER IB COORDINATE GEOMETRY(D &D) AND CALCULUS. TIME : hrs Ma. Marks.75 Not: This qustion papr consists of thr sctions A,B and C. SECTION A VERY SHORT ANSWER TYPE QUESTIONS. 0X =0.If th portion

More information

Thomas Whitham Sixth Form

Thomas Whitham Sixth Form Thomas Whitham Sith Form Pur Mathmatics Cor rvision gui Pag Algbra Moulus functions graphs, quations an inqualitis Graph of f () Draw f () an rflct an part of th curv blow th ais in th ais. f () f () f

More information

Objective Mathematics

Objective Mathematics x. Lt 'P' b a point on th curv y and tangnt x drawn at P to th curv has gratst slop in magnitud, thn point 'P' is,, (0, 0),. Th quation of common tangnt to th curvs y = 6 x x and xy = x + is : x y = 8

More information

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation.

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation. Lur 7 Fourir Transforms and th Wav Euation Ovrviw and Motivation: W first discuss a fw faturs of th Fourir transform (FT), and thn w solv th initial-valu problm for th wav uation using th Fourir transform

More information

1973 AP Calculus AB: Section I

1973 AP Calculus AB: Section I 97 AP Calculus AB: Sction I 9 Minuts No Calculator Not: In this amination, ln dnots th natural logarithm of (that is, logarithm to th bas ).. ( ) d= + C 6 + C + C + C + C. If f ( ) = + + + and ( ), g=

More information

MAXIMA-MINIMA EXERCISE - 01 CHECK YOUR GRASP

MAXIMA-MINIMA EXERCISE - 01 CHECK YOUR GRASP EXERCISE - MAXIMA-MINIMA CHECK YOUR GRASP. f() 5 () 75 f'() 5. () 75 75.() 7. 5 + 5. () 7 {} 5 () 7 ( ) 5. f() 9a + a +, a > f'() 6 8a + a 6( a + a ) 6( a) ( a) p a, q a a a + + a a a (rjctd) or a a 6.

More information

Mapping properties of the elliptic maximal function

Mapping properties of the elliptic maximal function Rv. Mat. Ibroamricana 19 (2003), 221 234 Mapping proprtis of th lliptic maximal function M. Burak Erdoğan Abstract W prov that th lliptic maximal function maps th Sobolv spac W 4,η (R 2 )intol 4 (R 2 )

More information

4. Money cannot be neutral in the short-run the neutrality of money is exclusively a medium run phenomenon.

4. Money cannot be neutral in the short-run the neutrality of money is exclusively a medium run phenomenon. PART I TRUE/FALSE/UNCERTAIN (5 points ach) 1. Lik xpansionary montary policy, xpansionary fiscal policy rturns output in th mdium run to its natural lvl, and incrass prics. Thrfor, fiscal policy is also

More information

Introduction to Condensed Matter Physics

Introduction to Condensed Matter Physics Introduction to Condnsd Mattr Physics pcific hat M.P. Vaughan Ovrviw Ovrviw of spcific hat Hat capacity Dulong-Ptit Law Einstin modl Dby modl h Hat Capacity Hat capacity h hat capacity of a systm hld at

More information

Systems of Equations

Systems of Equations CHAPTER 4 Sstms of Equations 4. Solving Sstms of Linar Equations in Two Variabls 4. Solving Sstms of Linar Equations in Thr Variabls 4. Sstms of Linar Equations and Problm Solving Intgratd Rviw Sstms of

More information

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 07 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat

More information

Partial Derivatives: Suppose that z = f(x, y) is a function of two variables.

Partial Derivatives: Suppose that z = f(x, y) is a function of two variables. Chaptr Functions o Two Variabls Applid Calculus 61 Sction : Calculus o Functions o Two Variabls Now that ou hav som amiliarit with unctions o two variabls it s tim to start appling calculus to hlp us solv

More information

Self-Adjointness and Its Relationship to Quantum Mechanics. Ronald I. Frank 2016

Self-Adjointness and Its Relationship to Quantum Mechanics. Ronald I. Frank 2016 Ronald I. Frank 06 Adjoint https://n.wikipdia.org/wiki/adjoint In gnral thr is an oprator and a procss that dfin its adjoint *. It is thn slf-adjoint if *. Innr product spac https://n.wikipdia.org/wiki/innr_product_spac

More information

On Certain Conditions for Generating Production Functions - II

On Certain Conditions for Generating Production Functions - II J o u r n a l o A c c o u n t i n g a n d M a n a g m n t J A M v o l 7, n o ( 0 7 ) On Crtain Conditions or Gnrating Production Functions - II Catalin Anglo Ioan, Gina Ioan Abstract: Th articl is th scond

More information

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002 3.4 Forc Analysis of Linkas An undrstandin of forc analysis of linkas is rquird to: Dtrmin th raction forcs on pins, tc. as a consqunc of a spcifid motion (don t undrstimat th sinificanc of dynamic or

More information

The Equitable Dominating Graph

The Equitable Dominating Graph Intrnational Journal of Enginring Rsarch and Tchnology. ISSN 0974-3154 Volum 8, Numbr 1 (015), pp. 35-4 Intrnational Rsarch Publication Hous http://www.irphous.com Th Equitabl Dominating Graph P.N. Vinay

More information

cycle that does not cross any edges (including its own), then it has at least

cycle that does not cross any edges (including its own), then it has at least W prov th following thorm: Thorm If a K n is drawn in th plan in such a way that it has a hamiltonian cycl that dos not cross any dgs (including its own, thn it has at last n ( 4 48 π + O(n crossings Th

More information

From Elimination to Belief Propagation

From Elimination to Belief Propagation School of omputr Scinc Th lif Propagation (Sum-Product lgorithm Probabilistic Graphical Modls (10-708 Lctur 5, Sp 31, 2007 Rcptor Kinas Rcptor Kinas Kinas X 5 ric Xing Gn G T X 6 X 7 Gn H X 8 Rading: J-hap

More information

On spanning trees and cycles of multicolored point sets with few intersections

On spanning trees and cycles of multicolored point sets with few intersections On spanning trs and cycls of multicolord point sts with fw intrsctions M. Kano, C. Mrino, and J. Urrutia April, 00 Abstract Lt P 1,..., P k b a collction of disjoint point sts in R in gnral position. W

More information

Differential Equations

Differential Equations UNIT I Diffrntial Equations.0 INTRODUCTION W li in a world of intrrlatd changing ntitis. Th locit of a falling bod changs with distanc, th position of th arth changs with tim, th ara of a circl changs

More information

1 General boundary conditions in diffusion

1 General boundary conditions in diffusion Gnral boundary conditions in diffusion Πρόβλημα 4.8 : Δίνεται μονοδιάτατη πλάκα πάχους, που το ένα άκρο της κρατιέται ε θερμοκραία T t και το άλλο ε θερμοκραία T 2 t. Αν η αρχική θερμοκραία της πλάκας

More information

Chapter 1. Chapter 10. Chapter 2. Chapter 11. Chapter 3. Chapter 12. Chapter 4. Chapter 13. Chapter 5. Chapter 14. Chapter 6. Chapter 7.

Chapter 1. Chapter 10. Chapter 2. Chapter 11. Chapter 3. Chapter 12. Chapter 4. Chapter 13. Chapter 5. Chapter 14. Chapter 6. Chapter 7. Chaptr Binomial Epansion Chaptr 0 Furthr Probability Chaptr Limits and Drivativs Chaptr Discrt Random Variabls Chaptr Diffrntiation Chaptr Discrt Probability Distributions Chaptr Applications of Diffrntiation

More information

surface of a dielectric-metal interface. It is commonly used today for discovering the ways in

surface of a dielectric-metal interface. It is commonly used today for discovering the ways in Surfac plasmon rsonanc is snsitiv mchanism for obsrving slight changs nar th surfac of a dilctric-mtal intrfac. It is commonl usd toda for discovring th was in which protins intract with thir nvironmnt,

More information

MATHEMATICS PAPER IIB COORDINATE GEOMETRY AND CALCULUS. Note: This question paper consists of three sections A, B and C.

MATHEMATICS PAPER IIB COORDINATE GEOMETRY AND CALCULUS. Note: This question paper consists of three sections A, B and C. MATHEMATICS PAPER IIB COORDINATE GEOMETRY AND CALCULUS. Tim: 3hrs Ma. Marks.75 Not: This qustion papr consists of thr sctions A, B and C. SECTION -A Vry Short Answr Typ Qustions. 0 X = 0. Find th condition

More information

Answers & Solutions. for MHT CET-2018 Paper-I (Mathematics) Instruction for Candidates

Answers & Solutions. for MHT CET-2018 Paper-I (Mathematics) Instruction for Candidates DATE : /5/8 Qustion Booklt Vrsion Rgd. Offic : Aakash Towr, 8, Pusa Road, Nw Dlhi-5 Ph.: -75 Fa : -77 Tim : Hour Min. Total Marks : Answrs & Solutions for MHT CET-8 Papr-I (Mathmatics) Instruction for

More information

Exercise 1. Sketch the graph of the following function. (x 2

Exercise 1. Sketch the graph of the following function. (x 2 Writtn tst: Fbruary 9th, 06 Exrcis. Sktch th graph of th following function fx = x + x, spcifying: domain, possibl asymptots, monotonicity, continuity, local and global maxima or minima, and non-drivability

More information

4037 ADDITIONAL MATHEMATICS

4037 ADDITIONAL MATHEMATICS CAMBRIDGE INTERNATIONAL EXAMINATIONS GCE Ordinary Lvl MARK SCHEME for th Octobr/Novmbr 0 sris 40 ADDITIONAL MATHEMATICS 40/ Papr, maimum raw mark 80 This mark schm is publishd as an aid to tachrs and candidats,

More information

MATHEMATICS (B) 2 log (D) ( 1) = where z =

MATHEMATICS (B) 2 log (D) ( 1) = where z = MATHEMATICS SECTION- I STRAIGHT OBJECTIVE TYPE This sction contains 9 multipl choic qustions numbrd to 9. Each qustion has choic (A), (B), (C) and (D), out of which ONLY-ONE is corrct. Lt I d + +, J +

More information

CHAPTER 1. Introductory Concepts Elements of Vector Analysis Newton s Laws Units The basis of Newtonian Mechanics D Alembert s Principle

CHAPTER 1. Introductory Concepts Elements of Vector Analysis Newton s Laws Units The basis of Newtonian Mechanics D Alembert s Principle CHPTER 1 Introductory Concpts Elmnts of Vctor nalysis Nwton s Laws Units Th basis of Nwtonian Mchanics D lmbrt s Principl 1 Scinc of Mchanics: It is concrnd with th motion of matrial bodis. odis hav diffrnt

More information

Direct Approach for Discrete Systems One-Dimensional Elements

Direct Approach for Discrete Systems One-Dimensional Elements CONTINUUM & FINITE ELEMENT METHOD Dirct Approach or Discrt Systms On-Dimnsional Elmnts Pro. Song Jin Par Mchanical Enginring, POSTECH Dirct Approach or Discrt Systms Dirct approach has th ollowing aturs:

More information

Content Skills Assessments Lessons. Identify, classify, and apply properties of negative and positive angles.

Content Skills Assessments Lessons. Identify, classify, and apply properties of negative and positive angles. Tachr: CORE TRIGONOMETRY Yar: 2012-13 Cours: TRIGONOMETRY Month: All Months S p t m b r Angls Essntial Qustions Can I idntify draw ngativ positiv angls in stard position? Do I hav a working knowldg of

More information

Electromagnetic scattering. Graduate Course Electrical Engineering (Communications) 1 st Semester, Sharif University of Technology

Electromagnetic scattering. Graduate Course Electrical Engineering (Communications) 1 st Semester, Sharif University of Technology Elctromagntic scattring Graduat Cours Elctrical Enginring (Communications) 1 st Smstr, 1388-1389 Sharif Univrsity of Tchnology Contnts of lctur 8 Contnts of lctur 8: Scattring from small dilctric objcts

More information

Curl, Divergence, Gradient, and Laplacian in Cylindrical and Spherical Coordinate Systems

Curl, Divergence, Gradient, and Laplacian in Cylindrical and Spherical Coordinate Systems A P P E N D I X B Curl, Divrgnc, Gradint, and Laplacian in Cylindrical and Sphrical Coordinat Systms 788 In Chaptr 3, w introducd th curl, divrgnc, gradint, and Laplacian and drivd th xprssions or thm

More information

CLONES IN 3-CONNECTED FRAME MATROIDS

CLONES IN 3-CONNECTED FRAME MATROIDS CLONES IN 3-CONNECTED FRAME MATROIDS JAKAYLA ROBBINS, DANIEL SLILATY, AND XIANGQIAN ZHOU Abstract. W dtrmin th structur o clonal classs o 3-connctd ram matroids in trms o th structur o biasd graphs. Robbins

More information

1 Isoparametric Concept

1 Isoparametric Concept UNIVERSITY OF CALIFORNIA BERKELEY Dpartmnt of Civil Enginring Spring 06 Structural Enginring, Mchanics and Matrials Profssor: S. Govindj Nots on D isoparamtric lmnts Isoparamtric Concpt Th isoparamtric

More information

Types of Transfer Functions. Types of Transfer Functions. Types of Transfer Functions. Ideal Filters. Ideal Filters

Types of Transfer Functions. Types of Transfer Functions. Types of Transfer Functions. Ideal Filters. Ideal Filters Typs of Transfr Typs of Transfr x[n] X( LTI h[n] H( y[n] Y( y [ n] h[ k] x[ n k] k Y ( H ( X ( Th tim-domain classification of an LTI digital transfr function is basd on th lngth of its impuls rspons h[n]:

More information

Triaxial coordinate systems and their geometrical interpretation

Triaxial coordinate systems and their geometrical interpretation Triaial coordinat sstms and thir gomtrical intrprtation G. Panou, R. Korakitis, D. Dlikaraoglou Dpartmnt of Surving Enginring, ational Tchnical Univrsit of Athns, Zografou Campus, 5780 Athns, Grc Abstract:

More information

Linear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let

Linear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let It is impossibl to dsign an IIR transfr function with an xact linar-phas It is always possibl to dsign an FIR transfr function with an xact linar-phas rspons W now dvlop th forms of th linarphas FIR transfr

More information

Figure 1: Closed surface, surface with boundary, or not a surface?

Figure 1: Closed surface, surface with boundary, or not a surface? QUESTION 1 (10 marks) Two o th topological spacs shown in Figur 1 ar closd suracs, two ar suracs with boundary, and two ar not suracs. Dtrmin which is which. You ar not rquird to justiy your answr, but,

More information

ENJOY MATHEMATICS WITH SUHAAG SIR

ENJOY MATHEMATICS WITH SUHAAG SIR R-, OPPOSITE RAILWAY TRACK, ZONE-, M. P. NAGAR, BHOPAL :(0755) 00 000, 80 5 888 IIT-JEE, AIEEE (WITH TH, TH 0 TH, TH & DROPPERS ) www.tkoclasss.com Pag: SOLUTION OF IITJEE 0; PAPER ; BHARAT MAIN SABSE

More information

SCHUR S THEOREM REU SUMMER 2005

SCHUR S THEOREM REU SUMMER 2005 SCHUR S THEOREM REU SUMMER 2005 1. Combinatorial aroach Prhas th first rsult in th subjct blongs to I. Schur and dats back to 1916. On of his motivation was to study th local vrsion of th famous quation

More information

SOME PARAMETERS ON EQUITABLE COLORING OF PRISM AND CIRCULANT GRAPH.

SOME PARAMETERS ON EQUITABLE COLORING OF PRISM AND CIRCULANT GRAPH. SOME PARAMETERS ON EQUITABLE COLORING OF PRISM AND CIRCULANT GRAPH. K VASUDEVAN, K. SWATHY AND K. MANIKANDAN 1 Dpartmnt of Mathmatics, Prsidncy Collg, Chnnai-05, India. E-Mail:vasu k dvan@yahoo.com. 2,

More information

EEO 401 Digital Signal Processing Prof. Mark Fowler

EEO 401 Digital Signal Processing Prof. Mark Fowler EEO 401 Digital Signal Procssing Prof. Mark Fowlr Dtails of th ot St #19 Rading Assignmnt: Sct. 7.1.2, 7.1.3, & 7.2 of Proakis & Manolakis Dfinition of th So Givn signal data points x[n] for n = 0,, -1

More information

INTEGRATION BY PARTS

INTEGRATION BY PARTS Mathmatics Rvision Guids Intgration by Parts Pag of 7 MK HOME TUITION Mathmatics Rvision Guids Lvl: AS / A Lvl AQA : C Edcl: C OCR: C OCR MEI: C INTEGRATION BY PARTS Vrsion : Dat: --5 Eampls - 6 ar copyrightd

More information

Recall that by Theorems 10.3 and 10.4 together provide us the estimate o(n2 ), S(q) q 9, q=1

Recall that by Theorems 10.3 and 10.4 together provide us the estimate o(n2 ), S(q) q 9, q=1 Chaptr 11 Th singular sris Rcall that by Thorms 10 and 104 togthr provid us th stimat 9 4 n 2 111 Rn = SnΓ 2 + on2, whr th singular sris Sn was dfind in Chaptr 10 as Sn = q=1 Sq q 9, with Sq = 1 a q gcda,q=1

More information

Epipolar Geometry and the Fundamental Matrix

Epipolar Geometry and the Fundamental Matrix 9 Epipolar Gomtry and th Fundamntal Matrix Th pipolar gomtry is th intrinsic projctiv gomtry btwn two viws. It is indpndnt of scn structur, and only dpnds on th camras intrnal paramtrs and rlativ pos.

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 Corrctions and commnts ar wlcom Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix () A A k I + A + k!

More information

(Upside-Down o Direct Rotation) β - Numbers

(Upside-Down o Direct Rotation) β - Numbers Amrican Journal of Mathmatics and Statistics 014, 4(): 58-64 DOI: 10593/jajms0140400 (Upsid-Down o Dirct Rotation) β - Numbrs Ammar Sddiq Mahmood 1, Shukriyah Sabir Ali,* 1 Dpartmnt of Mathmatics, Collg

More information

COUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM

COUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM COUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM Jim Brown Dpartmnt of Mathmatical Scincs, Clmson Univrsity, Clmson, SC 9634, USA jimlb@g.clmson.du Robrt Cass Dpartmnt of Mathmatics,

More information

Math 102. Rumbos Spring Solutions to Assignment #8. Solution: The matrix, A, corresponding to the system in (1) is

Math 102. Rumbos Spring Solutions to Assignment #8. Solution: The matrix, A, corresponding to the system in (1) is Math 12. Rumbos Spring 218 1 Solutions to Assignmnt #8 1. Construct a fundamntal matrix for th systm { ẋ 2y ẏ x + y. (1 Solution: Th matrix, A, corrsponding to th systm in (1 is 2 A. (2 1 1 Th charactristic

More information

ν a (p e ) p e fpt(a) = lim

ν a (p e ) p e fpt(a) = lim THE F -PURE THRESHOLD OF AN ELLIPTIC CURVE BHARGAV BHATT ABSTRACT. W calculat th F -pur thrshold of th affin con on an lliptic curv in a fixd positiv charactristic p. Th mthod mployd is dformation-thortic,

More information

The Matrix Exponential

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

More information

GEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES. Eduard N. Klenov* Rostov-on-Don, Russia

GEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES. Eduard N. Klenov* Rostov-on-Don, Russia GEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES Eduard N. Klnov* Rostov-on-Don, Russia Th articl considrs phnomnal gomtry figurs bing th carrirs of valu spctra for th pairs of th rmaining additiv

More information

Differentiation of Exponential Functions

Differentiation of Exponential Functions Calculus Modul C Diffrntiation of Eponntial Functions Copyright This publication Th Northrn Albrta Institut of Tchnology 007. All Rights Rsrvd. LAST REVISED March, 009 Introduction to Diffrntiation of

More information

Week 3: Connected Subgraphs

Week 3: Connected Subgraphs Wk 3: Connctd Subgraphs Sptmbr 19, 2016 1 Connctd Graphs Path, Distanc: A path from a vrtx x to a vrtx y in a graph G is rfrrd to an xy-path. Lt X, Y V (G). An (X, Y )-path is an xy-path with x X and y

More information

10. Limits involving infinity

10. Limits involving infinity . Limits involving infinity It is known from th it ruls for fundamntal arithmtic oprations (+,-,, ) that if two functions hav finit its at a (finit or infinit) point, that is, thy ar convrgnt, th it of

More information

2F1120 Spektrala transformer för Media Solutions to Steiglitz, Chapter 1

2F1120 Spektrala transformer för Media Solutions to Steiglitz, Chapter 1 F110 Spktrala transformr för Mdia Solutions to Stiglitz, Chaptr 1 Prfac This documnt contains solutions to slctd problms from Kn Stiglitz s book: A Digital Signal Procssing Primr publishd by Addison-Wsly.

More information

Southern Taiwan University

Southern Taiwan University Chaptr Ordinar Diffrntial Equations of th First Ordr and First Dgr Gnral form:., d +, d 0.a. f,.b I. Sparabl Diffrntial quations Form: d + d 0 C d d E 9 + 4 0 Solution: 9d + 4d 0 9 + 4 C E + d Solution:

More information

International Journal of Scientific & Engineering Research, Volume 6, Issue 7, July ISSN

International Journal of Scientific & Engineering Research, Volume 6, Issue 7, July ISSN Intrnational Journal of Scintific & Enginring Rsarch, Volum 6, Issu 7, July-25 64 ISSN 2229-558 HARATERISTIS OF EDGE UTSET MATRIX OF PETERSON GRAPH WITH ALGEBRAI GRAPH THEORY Dr. G. Nirmala M. Murugan

More information

10. The Discrete-Time Fourier Transform (DTFT)

10. The Discrete-Time Fourier Transform (DTFT) Th Discrt-Tim Fourir Transform (DTFT Dfinition of th discrt-tim Fourir transform Th Fourir rprsntation of signals plays an important rol in both continuous and discrt signal procssing In this sction w

More information

Inference Methods for Stochastic Volatility Models

Inference Methods for Stochastic Volatility Models Intrnational Mathmatical Forum, Vol 8, 03, no 8, 369-375 Infrnc Mthods for Stochastic Volatility Modls Maddalna Cavicchioli Cá Foscari Univrsity of Vnic Advancd School of Economics Cannargio 3, Vnic, Italy

More information

Spectral Synthesis in the Heisenberg Group

Spectral Synthesis in the Heisenberg Group Intrnational Journal of Mathmatical Analysis Vol. 13, 19, no. 1, 1-5 HIKARI Ltd, www.m-hikari.com https://doi.org/1.1988/ijma.19.81179 Spctral Synthsis in th Hisnbrg Group Yitzhak Wit Dpartmnt of Mathmatics,

More information

Pipe flow friction, small vs. big pipes

Pipe flow friction, small vs. big pipes Friction actor (t/0 t o pip) Friction small vs larg pips J. Chaurtt May 016 It is an intrsting act that riction is highr in small pips than largr pips or th sam vlocity o low and th sam lngth. Friction

More information

Derivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian

Derivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian Drivation of Elctron-Elctron Intraction Trms in th Multi-Elctron Hamiltonian Erica Smith Octobr 1, 010 1 Introduction Th Hamiltonian for a multi-lctron atom with n lctrons is drivd by Itoh (1965) by accounting

More information

Equidistribution and Weyl s criterion

Equidistribution and Weyl s criterion Euidistribution and Wyl s critrion by Brad Hannigan-Daly W introduc th ida of a sunc of numbrs bing uidistributd (mod ), and w stat and prov a thorm of Hrmann Wyl which charactrizs such suncs. W also discuss

More information

Function Spaces. a x 3. (Letting x = 1 =)) a(0) + b + c (1) = 0. Row reducing the matrix. b 1. e 4 3. e 9. >: (x = 1 =)) a(0) + b + c (1) = 0

Function Spaces. a x 3. (Letting x = 1 =)) a(0) + b + c (1) = 0. Row reducing the matrix. b 1. e 4 3. e 9. >: (x = 1 =)) a(0) + b + c (1) = 0 unction Spacs Prrquisit: Sction 4.7, Coordinatization n this sction, w apply th tchniqus of Chaptr 4 to vctor spacs whos lmnts ar functions. Th vctor spacs P n and P ar familiar xampls of such spacs. Othr

More information

perm4 A cnt 0 for for if A i 1 A i cnt cnt 1 cnt i j. j k. k l. i k. j l. i l

perm4 A cnt 0 for for if A i 1 A i cnt cnt 1 cnt i j. j k. k l. i k. j l. i l h 4D, 4th Rank, Antisytric nsor and th 4D Equivalnt to th Cross Product or Mor Fun with nsors!!! Richard R Shiffan Digital Graphics Assoc 8 Dunkirk Av LA, Ca 95 rrs@isidu his docunt dscribs th four dinsional

More information

PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS

PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS 1 Dharmndra

More information

Finding low cost TSP and 2-matching solutions using certain half integer subtour vertices

Finding low cost TSP and 2-matching solutions using certain half integer subtour vertices Finding low cost TSP and 2-matching solutions using crtain half intgr subtour vrtics Sylvia Boyd and Robrt Carr Novmbr 996 Introduction Givn th complt graph K n = (V, E) on n nods with dg costs c R E,

More information

Lenses & Prism Consider light entering a prism At the plane surface perpendicular light is unrefracted Moving from the glass to the slope side light

Lenses & Prism Consider light entering a prism At the plane surface perpendicular light is unrefracted Moving from the glass to the slope side light Lnss & Prism Considr light ntring a prism At th plan surac prpndicular light is unrractd Moving rom th glass to th slop sid light is bnt away rom th normal o th slop Using Snll's law n sin( ϕ ) = n sin(

More information

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers:

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers: APPM 6 Final 5 pts) Spring 4. 6 pts total) Th following parts ar not rlatd, justify your answrs: a) Considr th curv rprsntd by th paramtric quations, t and y t + for t. i) 6 pts) Writ down th corrsponding

More information

Title: Vibrational structure of electronic transition

Title: Vibrational structure of electronic transition Titl: Vibrational structur of lctronic transition Pag- Th band spctrum sn in th Ultra-Violt (UV) and visibl (VIS) rgions of th lctromagntic spctrum can not intrprtd as vibrational and rotational spctrum

More information

Search sequence databases 3 10/25/2016

Search sequence databases 3 10/25/2016 Sarch squnc databass 3 10/25/2016 Etrm valu distribution Ø Suppos X is a random variabl with probability dnsity function p(, w sampl a larg numbr S of indpndnt valus of X from this distribution for an

More information

5. B To determine all the holes and asymptotes of the equation: y = bdc dced f gbd

5. B To determine all the holes and asymptotes of the equation: y = bdc dced f gbd 1. First you chck th domain of g x. For this function, x cannot qual zro. Thn w find th D domain of f g x D 3; D 3 0; x Q x x 1 3, x 0 2. Any cosin graph is going to b symmtric with th y-axis as long as

More information

2.3 Matrix Formulation

2.3 Matrix Formulation 23 Matrix Formulation 43 A mor complicatd xampl ariss for a nonlinar systm of diffrntial quations Considr th following xampl Exampl 23 x y + x( x 2 y 2 y x + y( x 2 y 2 (233 Transforming to polar coordinats,

More information

7' The growth of yeast, a microscopic fungus used to make bread, in a test tube can be

7' The growth of yeast, a microscopic fungus used to make bread, in a test tube can be N Sction A: Pur Mathmatics 55 marks] / Th rgion R is boundd by th curv y, th -ais, and th lins = V - +7 and = m, whr m >. Find th volum gnratd whn R is rotatd through right angls about th -ais, laving

More information

1 Minimum Cut Problem

1 Minimum Cut Problem CS 6 Lctur 6 Min Cut and argr s Algorithm Scribs: Png Hui How (05), Virginia Dat: May 4, 06 Minimum Cut Problm Today, w introduc th minimum cut problm. This problm has many motivations, on of which coms

More information

Differential Equations

Differential Equations Prfac Hr ar m onlin nots for m diffrntial quations cours that I tach hr at Lamar Univrsit. Dspit th fact that ths ar m class nots, th should b accssibl to anon wanting to larn how to solv diffrntial quations

More information

EXST Regression Techniques Page 1

EXST Regression Techniques Page 1 EXST704 - Rgrssion Tchniqus Pag 1 Masurmnt rrors in X W hav assumd that all variation is in Y. Masurmnt rror in this variabl will not ffct th rsults, as long as thy ar uncorrlatd and unbiasd, sinc thy

More information

BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES

BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES DONALD M. DAVIS Abstract. If p is a prim (implicit in notation and n a positiv intgr, lt ν(n dnot th xponnt of p in n, and U(n n/p ν(n, th unit

More information