Computational Geometry. Kirkpatrick-Seidel s Prune-and-Search Convex Hull Algorithm
|
|
- Annabel Washington
- 6 years ago
- Views:
Transcription
1 COSC 6114 Coutational Geoety Kikatick-Seidel Pune-and-Seach Convex Hull Algoith Intoduction Thi note concen the coutation of the convex hull of a given et P ={ 1, 2,..., n }of n oint in the lane. et h denote the ize of the convex hull, ie the nube of it vetice. The value h i not known befoehand, and it can ange anywhee fo a all contant to n. Wehave aleady een that any convex hull algoith euie at leat Ω(n lgn)tie in the wot cae, and have tudied a nube of algoith, uch a Gaha can algoith, whoe wot cae tie colexity i O(n lgn). If n wa the only eaue of oble ize, then thee algoith ae otial. Howeve, we alo know that the Javi ach algoith euie O(nh) tie. The latte can ange anywhee fo O(n) to O(n 2 )deending on the value of h. Ithee an algoith which i aytotically ueio to both Gaha can and Javi ach, fo all oible value of h? Below, we will decibe Kikatick and Seidel [KiS86] algoith that euie O(n lgh)tie. Kikatick-Seidel algoith alie a deign techniue known a the une-andeach ethod o Megiddo techniue. Niod Megiddo howed, eg, how thi techniue can be ued to olve fixed dienional linea oga in linea tie [Meg83, Meg84], and how tocoute the allet cicle that encloe a finite nube of given oint in the lane in linea tie [Meg89]. Dye [Dye84] indeendently dicoveed the ae techniue. Many othe alication of thi oweful algoith deign techniue aea in the liteatue. Edelbunne book [Ede87] alo give a bief decition of the ethod in ection 15.6 and how it alication, eg, to linea ogaing in chate 10, and to ha-andwich cut in ection Fance Yao in ection 6, chate 7 of van eeuwen book [van90] alo dicue thi techniue. The une-and-each techniue can be taced back to the fit linea tie edian finding algoith of Blu-Floyd-Patt-ivet- Tajan [BFP73]. The latte algoith find the edian (and in geneal, the k-th allet eleent) of a finite et of given nube in linea tie and i alo decibed in ection 10.3 of Coen-eieon-ivet [C91]. Kikatick-Seidel Algoith Conide the iniu and axiu x-coodinate of oint in P, denoted x in and x ax. Convex Hull of P can be be viewed a a ai of convex chain called the ue hull and the lowe hull of P (excluding the oible vetical edge at x in o x ax ). (See Fig. 1(a).) The algoith that coute the ue-hull of P i given below. The lowehull can be couted in a iila anne and i oitted fo futhe dicuion.
2 -2- ue hull vetical t edge lowe hull x in x ax (a) Fig. 1 (a) The ue and lowe hull, (b) The ue bidge. Algoith UeHull(P) 0. if P 2 then etun the obviou anwe 1. ele begin 2. Coute the edian x ed of x-coodinate of oint in P. 3. Patition P into two et and each of ize about n/2 aound the edian x ed. 4. Find the ue bidge of and,, and 5. { x() x() } 6. { x() x() } 7. UH UeHall( ) 8. UH UeHall( ) 9. etun the concatenated lit UH,, UH a the ue hull of P. 10. end (b) Analyi Thi i a divide-&-conue algoith. The key te i the coutation of the ue bidge in te 4 which i baed on the une-&-each techniue. (See Fig. 1(b).) In the next ection we will how that thi te can be done in O(n) tie. We alo know that te 2can be done in O(n) tie by the linea tie edian finding algoith. Hence, te 3-6 can be done in O(n) tie. Fo the uoe of analyzing algoith UeHall(P), let u aue the ue hull of P conit of h edge. Ou analyi will ue both aaete n (inut ize) and h (outut ize). et T (n, h) denote the wot-cae tie colexity of the algoith. Suoe UH and UH in te 7 and 8 conit of h 1 and h 2 edge, eectively. Since and, the two ecuive call in te 7 and 8 take tie T (n/2, h 1 ) and T (n/2, h 2 ) tie. (Note that h =1+ h 1 + h 2. Hence, h 2 = h 1 h 1.) Theefoe, the ecuence that decibe the wot-cae tie colexity of the algoith i T (n, h) = O(n) + ax { T ( n h1 2, h 1) + T ( n 2, h 1 h 1)} if h >2 O(n) if h 2
3 -3- Theoe: T (n, h) =O(n lg h). Poof: Suoe the two occuence of O(n) inthe above ecuence ae at ot cn, whee c i a uitably lage contant. We will how by induction on h that T (n, h) cn lg h fo all n and h 2. Fo the bae cae whee h = 2, T (n, h) cn cnlg2 =cn lg h. Fo the inductive cae, T (n, h) cn + ax { c n h1 2 lg h 1 + c n 2 lg (h 1 h 1)} = cn + c n 2 ax lg ( h 1 (h 1 h 1 )) h 1 cn + c n 2 lg ( h 2 h 2 ) = cn + c n 2 2 lg h 2 = cn lgh. Finding the Ue Bidge in inea Tie The oble i thi: we ae given acollection P of n oint in the lane, which i eaated into two non-ety ubet and by a known vetical line, with on the left and on the ight. We wih to find a line t aing though one oint fo each ubet, uch that none of the given oint lie above t. See Fig 1(b). In othe wod, we want the ue exteio coon tangent (the ue bidge) of the convex hull of and. If the convex hull of and wee known, the coon tangent could eaily be found in linea tie (ee the ege te in the divide-&-conue convex hull algoith dicued ealie in the coue). Howeve, couting the convex hull of Θ(n) oint cot Θ(n lgn)tie in the wot cae. Coutation of the ue bidge of and can be foulated a a 2-vaiable linea oga with n linea containt, and hence, can be olved in O(n) tie by Megiddo linea-ogaing algoith. The linea oga foulation i a follow. Suoe the euation of the (non-vetical) bidge line t i y = x + β. The two coefficient (the loe) and β (the y-inteet) ae the two unknown that we have to coute. Suoe the x-coodinate of the vetical eaato line between and i x = a. (See Fig. 1(b).) Then, the y-coodinate of the inteection of t and i y o = a + β. Clealy any line that i at o above evey oint of cannot inteect at a y-coodinate lowe than y o.thi give uthe deied 2-vaiable linea oga; find and β to: iniize ubject to: a + β x( i ) + β y( i ) fo all i. Intead of dicuing Megiddo olution of thi linea oga, we will dicu Kiktick-Seidel diect ethod. The key to thei algoith i a ile une-&-each citeion that in linea tie allow u to eliinate a good any of the oint that do not define the ue bidge.
4 -4- et u fix fo the oent ou attention on line of a aticula loe. Wecan coute in linea tie a uoting line of of loe. Suoe thi line i tangent to at oe oint. Wecan do the ae fo and obtain a uoting line of of loe tangent to at oe oint. Now if the line ha loe le than,then o ut the coon tangent t; iilaly, if ha loe geate than then o doe t; and if ha loe then t =. See Fig 2(a,b). (a) (b) Fig 2. (c) Now uoe the fit cae hold, o loe of t i le than. et, be any two oint of, uch that i to the left of and the line ha loe geate than. Then we can conclude that t cannot a though, becaue a line of loe le than though ut a below. See Fig 2(c). The econd cae, whee the loe of t i geate than, i entiely yetical: we can eliinate the econd ebe of any ai,, with to the left of, ifthe line ha loe le than. Thee eak ugget the following une-&-each ethod. Pai u the n given oint in an abitay way, and find the edian loe of the n/2 line defined by thoe ai. Now coute the uoting line of, eectively, and of loe and aue thee line, eectively, ae tangent to and at oint and. Ithould be obviou why the edian i a good choice: ince half the ai have loe le than,and half have loe geate than. Theefoe, half the ai will atify the citeion, no atte whethe the loe of i geate o le than. So, in eithe cae we eliinate one oint fo half the ai, fo a total of at leat n/4 oint. Of coue if ha loe then we ae done. It i oible to find the edian loe in tie linea in n uing the ae edian finding algoith entioned in the eviou ection. The othe oeation clealy take O(n) tie. Theefoe, in linea tie we eithe to, o eliinate at leat n/4 of the oiginal oint. If we eeatedly aly thi eliination (o uning) oce on the eaining oint, we ae guaanteed to find the coon tangent, at a total cot of O(n + (3/4)n + (3/4) 2 n +...)=O(n) tie. Note that we ay eliinate a diffeent nube of oint fo and fo, but thi doe not affect the analyi. Now wecan tate the following eult. Theoe: The ue bidge of two vetically eaated oint et can be couted in linea tie.
5 -5- Coollay: Kikatick-Seidel convex hull algoith take O(n lgh) tie. Kikatick-Seidel alo howed that in te of the two aaete n and h, Ω(n lg h) i a wot-cae lowe bound to coute the convex hull (uing a geneal coutational odel known a the algebaic deciion tee odel). Theefoe, thei algoith i wotcae otial. 3D Convex Hull The convex hull of n oint in 3 can alo be couted in O(n lgn)tie by a divide-&-conue algoith. ecently, Edelbunne and Shi [EdS91] have hown that 3D convex hull can be couted in O(n lg 2 h)tie, whee h i the nube of hull vetice (extee oint). Futheoe, Kenneth Clakon and Pete Sho [ClS89] give a andoized 3D convex hull algoith with O(n lgh) exected tie. Chazelle and Matouek [ChM93] have eoted that deandoizing an algoith of [ClS89] give an O(n lgh)tie deteinitic algoith. See alo [CSY95]. efeence [BFP73] Blu, M., W. Floyd, V. Patt,. ivet,.e. Tajan, Tie bound fo election, J.ofCoute and Syte Science, vol. 7, , [CSY95] Chan, T.M.Y., J. Snoyink, C.K. Ya, Outut-enitive contuction of olytoe in fou dienion and clied Voonoi diaga in thee Poc. SODA 95, , [ChM93] Chazelle, B., and J. Matouek, Deandoizing an outut-enitive convex hull algoith in thee dienion, Manucit, [ClS89] [Dye84] [EdS91] [KiS86] Clakon, K., and P.W. Sho, Alication of ando aling in coutational geoety, II, Dicete & Coutational Geoety, vol. 4, no. 5, , Dye, M.E., inea tie algoith fo two- and thee-vaiable linea oga, SIAM J. Couting, vol. 13, , Edelbunne, H., and W. Shi, An O(n log 2 h) tie algoith fo the theedienional convex hull oble, SIAM J. Couting, vol. 20, no. 2, , Kikatick, D.G., and. Seidel, The ultiate lana convex hull algoith?, SIAM J. Couting, vol. 15, no. 1, , [Meg83] Megiddo, N., inea-tie algoith fo linea ogaing in 3 and elated oble, SIAM J. Co. 12, , [Meg84] [Meg89] Megiddo, N., inea ogaing in linea tie when the dienion i fixed, J. Aociation fo Couting Machiney (JACM) 31, , Megiddo, N., On the ball anned by ball, Dicete & Coutational Geoety, vol. 4, no. 6, , 1989.
A Class of Delay Integral Inequalities on Time Scales
Intenational Confeence on Iage, Viion and Couting (ICIVC ) IPCSIT vol 5 () () IACSIT Pe, Singaoe DOI: 7763/IPCSITV543 A Cla of Dela Integal Ineualitie on Tie Scale Qinghua Feng + School of Science, Shandong
More informationBasic propositional and. The fundamentals of deduction
Baic ooitional and edicate logic The fundamental of deduction 1 Logic and it alication Logic i the tudy of the atten of deduction Logic lay two main ole in comutation: Modeling : logical entence ae the
More informationLECTURE 14. m 1 m 2 b) Based on the second law of Newton Figure 1 similarly F21 m2 c) Based on the third law of Newton F 12
CTU 4 ] NWTON W O GVITY -The gavity law i foulated fo two point paticle with ae and at a ditance between the. Hee ae the fou tep that bing to univeal law of gavitation dicoveed by NWTON. a Baed on expeiental
More informationTest 2 phy a) How is the velocity of a particle defined? b) What is an inertial reference frame? c) Describe friction.
Tet phy 40 1. a) How i the velocity of a paticle defined? b) What i an inetial efeence fae? c) Decibe fiction. phyic dealt otly with falling bodie. d) Copae the acceleation of a paticle in efeence fae
More informationImage Enhancement: Histogram-based methods
Image Enhancement: Hitogam-baed method The hitogam of a digital image with gayvalue, i the dicete function,, L n n # ixel with value Total # ixel image The function eeent the faction of the total numbe
More informationConjunctive Normal Form & Horn Clauses
Conjunctive Noal Fo & Hon Claue ok Univeity CSE 3401 Vida Movahedi ok Univeity- CSE 3401- V Movahedi 02-CNF & Hon 1 Oveview Definition of liteal claue and CNF Conveion to CNF- Pooitional logic Reeentation
More informationψ - exponential type orbitals, Frictional
ew develoment in theoy of Laguee olynomial I. I. Gueinov Deatment of Phyic, Faculty of At and Science, Onekiz Mat Univeity, Çanakkale, Tukey Abtact The new comlete othonomal et of L -Laguee tye olynomial
More informationInference for A One Way Factorial Experiment. By Ed Stanek and Elaine Puleo
Infeence fo A One Way Factoial Expeiment By Ed Stanek and Elaine Puleo. Intoduction We develop etimating equation fo Facto Level mean in a completely andomized one way factoial expeiment. Thi development
More information( ) Physics 1401 Homework Solutions - Walker, Chapter 9
Phyic 40 Conceptual Quetion CQ No Fo exaple, ey likely thee will be oe peanent deoation o the ca In thi cae, oe o the kinetic enegy that the two ca had beoe the colliion goe into wok that each ca doe on
More informationChapter 19 Webassign Help Problems
Chapte 9 Webaign Help Poblem 4 5 6 7 8 9 0 Poblem 4: The pictue fo thi poblem i a bit mileading. They eally jut give you the pictue fo Pat b. So let fix that. Hee i the pictue fo Pat (a): Pat (a) imply
More informationSolutions Practice Test PHYS 211 Exam 2
Solution Pactice Tet PHYS 11 Exam 1A We can plit thi poblem up into two pat, each one dealing with a epaate axi. Fo both the x- and y- axe, we have two foce (one given, one unknown) and we get the following
More information30 The Electric Field Due to a Continuous Distribution of Charge on a Line
hapte 0 The Electic Field Due to a ontinuous Distibution of hage on a Line 0 The Electic Field Due to a ontinuous Distibution of hage on a Line Evey integal ust include a diffeential (such as d, dt, dq,
More informationLecture 21. The Lovasz splitting-off lemma Topics in Combinatorial Optimization April 29th, 2004
18.997 Topic in Combinatorial Optimization April 29th, 2004 Lecture 21 Lecturer: Michel X. Goeman Scribe: Mohammad Mahdian 1 The Lovaz plitting-off lemma Lovaz plitting-off lemma tate the following. Theorem
More informationThen the number of elements of S of weight n is exactly the number of compositions of n into k parts.
Geneating Function In a geneal combinatoial poblem, we have a univee S of object, and we want to count the numbe of object with a cetain popety. Fo example, if S i the et of all gaph, we might want to
More informationrad rev 60sec p sec 2 rad min 2 2
NAME: EE 459/559, Exa 1, Fall 2016, D. McCalley, 75 inute allowed (unle othewie diected) Cloed Book, Cloed Note, Calculato Peitted, No Counication Device. The following infoation ay o ay not be ueful fo
More informationPerhaps the greatest success of his theory of gravity was to successfully explain the motion of the heavens planets, moons, &tc.
AP Phyic Gavity Si Iaac Newton i cedited with the dicovey of gavity. Now, of coue we know that he didn t eally dicove the thing let face it, people knew about gavity fo a long a thee have been people.
More informationContent 5.1 Angular displacement and angular velocity 5.2 Centripetal acceleration 5.3 Centripetal force. 5. Circular motion.
5. Cicula otion By Liew Sau oh Content 5.1 Angula diplaceent and angula elocity 5. Centipetal acceleation 5.3 Centipetal foce Objectie a) expe angula diplaceent in adian b) define angula elocity and peiod
More informationCMSC 425: Lecture 5 More on Geometry and Geometric Programming
CMSC 425: Lectue 5 Moe on Geomety and Geometic Pogamming Moe Geometic Pogamming: In this lectue we continue the discussion of basic geometic ogamming fom the eious lectue. We will discuss coodinate systems
More informationChapter 8 Sampling. Contents. Dr. Norrarat Wattanamongkhol. Lecturer. Department of Electrical Engineering, Engineering Faculty, sampling
Content Chate 8 Samling Lectue D Noaat Wattanamongkhol Samling Theoem Samling of Continuou-Time Signal 3 Poceing Continuou-Time Signal 4 Samling of Dicete-Time Signal 5 Multi-ate Samling Deatment of Electical
More informationFall 2004/05 Solutions to Assignment 5: The Stationary Phase Method Provided by Mustafa Sabri Kilic. I(x) = e ixt e it5 /5 dt (1) Z J(λ) =
8.35 Fall 24/5 Solution to Aignment 5: The Stationay Phae Method Povided by Mutafa Sabi Kilic. Find the leading tem fo each of the integal below fo λ >>. (a) R eiλt3 dt (b) R e iλt2 dt (c) R eiλ co t dt
More informationSecond Order Fuzzy S-Hausdorff Spaces
Inten J Fuzzy Mathematical Achive Vol 1, 013, 41-48 ISSN: 30-34 (P), 30-350 (online) Publihed on 9 Febuay 013 wwweeachmathciog Intenational Jounal o Second Ode Fuzzy S-Haudo Space AKalaichelvi Depatment
More informationTHE BICYCLE RACE ALBERT SCHUELLER
THE BICYCLE RACE ALBERT SCHUELLER. INTRODUCTION We will conider the ituation of a cyclit paing a refrehent tation in a bicycle race and the relative poition of the cyclit and her chaing upport car. The
More informationLecture 23: Central Force Motion
Lectue 3: Cental Foce Motion Many of the foces we encounte in natue act between two paticles along the line connecting the Gavity, electicity, and the stong nuclea foce ae exaples These types of foces
More informationHomework Set 4 Physics 319 Classical Mechanics. m m k. x, x, x, x T U x x x x l 2. x x x x. x x x x
Poble 78 a) The agangian i Hoewok Set 4 Phyic 319 Claical Mechanic k b) In te of the cente of a cooinate an x x1 x x1 x xc x x x x x1 xc x xc x x x x x1 xc x xc x, x, x, x T U x x x x l 1 1 1 1 1 1 1 1
More informationGravity. David Barwacz 7778 Thornapple Bayou SE, Grand Rapids, MI David Barwacz 12/03/2003
avity David Bawacz 7778 Thonapple Bayou, and Rapid, MI 495 David Bawacz /3/3 http://membe.titon.net/daveb Uing the concept dicued in the peceding pape ( http://membe.titon.net/daveb ), I will now deive
More informationSection 25 Describing Rotational Motion
Section 25 Decibing Rotational Motion What do object do and wh do the do it? We have a ve thoough eplanation in tem of kinematic, foce, eneg and momentum. Thi include Newton thee law of motion and two
More informationDetermining the Best Linear Unbiased Predictor of PSU Means with the Data. included with the Random Variables. Ed Stanek
Detemining te Bet Linea Unbiaed Pedicto of PSU ean wit te Data included wit te andom Vaiable Ed Stanek Intoduction We develop te equation fo te bet linea unbiaed pedicto of PSU mean in a two tage andom
More informationMon , (.12) Rotational + Translational RE 11.b Tues.
Mon..-.3, (.) Rotational + Tanlational RE.b Tue. EP0 Mon..4-.6, (.3) Angula Momentum & Toque RE.c Tue. Wed..7 -.9, (.) Toque EP RE.d ab Fi. Rotation Coue Eval.0 Quantization, Quiz RE.e Mon. Review fo Final
More informationASTR 3740 Relativity & Cosmology Spring Answers to Problem Set 4.
ASTR 3740 Relativity & Comology Sping 019. Anwe to Poblem Set 4. 1. Tajectoie of paticle in the Schwazchild geomety The equation of motion fo a maive paticle feely falling in the Schwazchild geomety ae
More informationFigure 1 Siemens PSSE Web Site
Stability Analyi of Dynamic Sytem. In the lat few lecture we have een how mall ignal Lalace domain model may be contructed of the dynamic erformance of ower ytem. The tability of uch ytem i a matter of
More informationALOIS PANHOLZER AND HELMUT PRODINGER
ASYMPTOTIC RESULTS FOR THE NUMBER OF PATHS IN A GRID ALOIS PANHOLZER AND HELMUT PRODINGER Abstact. In two ecent papes, Albecht and White, and Hischhon, espectively, consideed the poble of counting the
More informationFI 2201 Electromagnetism
FI Electomagnetim Aleande A. Ikanda, Ph.D. Phyic of Magnetim and Photonic Reeach Goup ecto Analyi CURILINEAR COORDINAES, DIRAC DELA FUNCION AND HEORY OF ECOR FIELDS Cuvilinea Coodinate Sytem Cateian coodinate:
More informationProblem Set 8 Solutions
Deign and Analyi of Algorithm April 29, 2015 Maachuett Intitute of Technology 6.046J/18.410J Prof. Erik Demaine, Srini Devada, and Nancy Lynch Problem Set 8 Solution Problem Set 8 Solution Thi problem
More informationSeveral new identities involving Euler and Bernoulli polynomials
Bull. Math. Soc. Sci. Math. Roumanie Tome 9107 No. 1, 016, 101 108 Seveal new identitie involving Eule and Benoulli polynomial by Wang Xiaoying and Zhang Wenpeng Abtact The main pupoe of thi pape i uing
More informationCan a watch-sized electromagnet deflect a bullet? (from James Bond movie)
Can a peon be blown away by a bullet? et' ay a bullet of a 0.06 k i ovin at a velocity of 300 /. And let' alo ay that it ebed itelf inide a peon. Could thi peon be thut back at hih peed (i.e. blown away)?
More informationOn the Efficiency of Markets with Two-sided Proportional Allocation Mechanisms
On the Efficiency of Maket with Two-ided Pootional Allocation Mechanim Volodymy Kulehov and Adian Vetta Deatment of Mathematic and Statitic, and School of Comute Science, McGill Univeity volodymy.kulehov@mail.mcgill.ca,
More informationPricing and Service Decisions of Supply Chain in an Uncertain Environment
Engineeing Lette, 4:4, EL_4_4_9 Picing and Sevice Deciion of Supply Chain in an Uncetain Envionent Shengju Sang F FAbtact In a to-echelon upply chain yte ith one anufactue and one etaile, the picing and
More informationChapter 4. The Laplace Transform Method
Chapter 4. The Laplace Tranform Method The Laplace Tranform i a tranformation, meaning that it change a function into a new function. Actually, it i a linear tranformation, becaue it convert a linear combination
More informationEstimation and Prediction from Inverse Rayleigh. Distribution Based on Lower Record Values
Applied Matheatical Science, Vol. 4,, no. 6, 357-366 Etiation and Pediction fo Invee Rayleigh Ditibution Baed on Lowe Recod Value A. Solian, Ea A. Ain,a and Alaa A. Abd-El Aziz a e-ail: e_ain@yahoo.co
More informationPolar Coordinates. a) (2; 30 ) b) (5; 120 ) c) (6; 270 ) d) (9; 330 ) e) (4; 45 )
Pola Coodinates We now intoduce anothe method of labelling oints in a lane. We stat by xing a oint in the lane. It is called the ole. A standad choice fo the ole is the oigin (0; 0) fo the Catezian coodinate
More information11.5 MAP Estimator MAP avoids this Computational Problem!
.5 MAP timator ecall that the hit-or-mi cot function gave the MAP etimator it maimize the a oteriori PDF Q: Given that the MMS etimator i the mot natural one why would we conider the MAP etimator? A: If
More informationGraphs of Sine and Cosine Functions
Gaphs of Sine and Cosine Functions In pevious sections, we defined the tigonometic o cicula functions in tems of the movement of a point aound the cicumfeence of a unit cicle, o the angle fomed by the
More informationJORDAN CANONICAL FORM AND ITS APPLICATIONS
JORDAN CANONICAL FORM AND ITS APPLICATIONS Shivani Gupta 1, Kaajot Kau 2 1,2 Matheatics Depatent, Khalsa College Fo Woen, Ludhiana (India) ABSTRACT This pape gives a basic notion to the Jodan canonical
More informationAvailable online through ISSN
Intenational eseach Jounal of Pue Algeba -() 01 98-0 Available online though wwwjpainfo ISSN 8 907 SOE ESULTS ON THE GOUP INVESE OF BLOCK ATIX OVE IGHT OE DOAINS Hanyu Zhang* Goup of athematical Jidong
More informationGeometry Contest 2013
eomety ontet 013 1. One pizza ha a diamete twice the diamete of a malle pizza. What i the atio of the aea of the lage pizza to the aea of the malle pizza? ) to 1 ) to 1 ) to 1 ) 1 to ) to 1. In ectangle
More information7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281
72 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 28 and i 2 Show how Euler formula (page 33) can then be ued to deduce the reult a ( a) 2 b 2 {e at co bt} {e at in bt} b ( a) 2 b 2 5 Under what condition
More informationHistogram Processing
Hitogam Poceing Lectue 4 (Chapte 3) Hitogam Poceing The hitogam of a digital image with gay level fom to L- i a dicete function h( )=n, whee: i the th gay level n i the numbe of pixel in the image with
More informationUniversal Gravitation
Add Ipotant Univeal Gavitation Pae: 7 Note/Cue Hee Unit: Dynaic (oce & Gavitation Univeal Gavitation Unit: Dynaic (oce & Gavitation NGSS Standad: HS-PS-4 MA Cuiculu aewok (00:.7 AP Phyic Leanin Objective:.B..,.B..,
More informationA Crash Course in (2 2) Matrices
A Cash Couse in ( ) Matices Seveal weeks woth of matix algeba in an hou (Relax, we will only stuy the simplest case, that of matices) Review topics: What is a matix (pl matices)? A matix is a ectangula
More informationOnline-routing on the butterfly network: probabilistic analysis
Online-outing on the buttefly netwok: obabilistic analysis Andey Gubichev 19.09.008 Contents 1 Intoduction: definitions 1 Aveage case behavio of the geedy algoithm 3.1 Bounds on congestion................................
More informationA note on rescalings of the skew-normal distribution
Poyeccione Jounal of Mathematic Vol. 31, N o 3, pp. 197-07, Septembe 01. Univeidad Católica del Note Antofagata - Chile A note on ecaling of the kew-nomal ditibution OSVALDO VENEGAS Univeidad Católica
More informationIntroduction to Laplace Transform Techniques in Circuit Analysis
Unit 6 Introduction to Laplace Tranform Technique in Circuit Analyi In thi unit we conider the application of Laplace Tranform to circuit analyi. A relevant dicuion of the one-ided Laplace tranform i found
More informationThe Archimedean Circles of Schoch and Woo
Foum Geometicoum Volume 4 (2004) 27 34. FRUM GEM ISSN 1534-1178 The Achimedean Cicles of Schoch and Woo Hioshi kumua and Masayuki Watanabe Abstact. We genealize the Achimedean cicles in an abelos (shoemake
More informationJoint Estimation of Clock Skew and Offset in Pairwise Broadcast Synchronization Mechanism
1 Joint tiation of Clock Skew and Offet in Paiwie Boadcat Synchonization Mechani Xuanyu Cao 1,, Feng Yang 1, Xiaoying Gan 1, Jing Liu 1, Liang Qian 1, Xiaohua Tian 1 and Xinbing Wang 1,3 1 Deatent of lectonic
More informationData Structures and Algorithm Analysis (CSC317) Randomized algorithms (part 2)
Data Stuctues and Algoithm Analysis (CSC317) Randomized algoithms (at 2) Hiing oblem - eview c Cost to inteview (low i ) Cost to fie/hie (exensive ) n Total numbe candidates m Total numbe hied c h O(c
More informationA Bijective Approach to the Permutational Power of a Priority Queue
A Bijective Appoach to the Pemutational Powe of a Pioity Queue Ia M. Gessel Kuang-Yeh Wang Depatment of Mathematics Bandeis Univesity Waltham, MA 02254-9110 Abstact A pioity queue tansfoms an input pemutation
More informationPhysics 2A Chapter 10 - Moment of Inertia Fall 2018
Physics Chapte 0 - oment of netia Fall 08 The moment of inetia of a otating object is a measue of its otational inetia in the same way that the mass of an object is a measue of its inetia fo linea motion.
More informationPhysics 110. Exam #1. September 30, 2016
Phyic 110 Exa #1 Septebe 30, 016 Nae Pleae ead and follow thee intuction caefully: Read all poble caefully befoe attepting to olve the. You wok ut be legible, and the oganization clea. You ut how all wok,
More informationOn the quadratic support of strongly convex functions
Int. J. Nonlinea Anal. Appl. 7 2016 No. 1, 15-20 ISSN: 2008-6822 electonic http://dx.doi.og/10.22075/ijnaa.2015.273 On the quadatic uppot of tongly convex function S. Abbazadeh a,b,, M. Ehaghi Godji a
More informationCOLLAPSING WALLS THEOREM
COLLAPSING WALLS THEOREM IGOR PAK AND ROM PINCHASI Abstact. Let P R 3 be a pyamid with the base a convex polygon Q. We show that when othe faces ae collapsed (otated aound the edges onto the plane spanned
More information66 Lecture 3 Random Search Tree i unique. Lemma 3. Let X and Y be totally ordered et, and let be a function aigning a ditinct riority in Y to each ele
Lecture 3 Random Search Tree In thi lecture we will decribe a very imle robabilitic data tructure that allow inert, delete, and memberhi tet (among other oeration) in exected logarithmic time. Thee reult
More informationarxiv: v1 [cs.lo] 11 Aug 2017
STAR HEIGHT VIA GAMES MIKO LAJ BOJAŃCZYK axiv:1708.03603v1 [c.lo] 11 Aug 2017 Abtact. Thi ae ooe a new algoithm deciding the ta height oblem. A hown by Kiten, the ta height oblem educe to a oblem concening
More informationAnalysis of Arithmetic. Analysis of Arithmetic. Analysis of Arithmetic Round-Off Errors. Analysis of Arithmetic. Analysis of Arithmetic
In the fixed-oint imlementation of a digital filte only the esult of the multilication oeation is quantied The eesentation of a actical multilie with the quantie at its outut is shown below u v Q ^v The
More informationRotational Kinetic Energy
Add Impotant Rotational Kinetic Enegy Page: 353 NGSS Standad: N/A Rotational Kinetic Enegy MA Cuiculum Famewok (006):.1,.,.3 AP Phyic 1 Leaning Objective: N/A, but olling poblem have appeaed on peviou
More informationOn Locally Convex Topological Vector Space Valued Null Function Space c 0 (S,T, Φ, ξ, u) Defined by Semi Norm and Orlicz Function
Jounal of Intitute of Science and Technology, 204, 9(): 62-68, Intitute of Science and Technology, T.U. On Locally Convex Topological Vecto Space Valued Null Function Space c 0 (S,T, Φ, ξ, u) Defined by
More informationVector d is a linear vector function of vector d when the following relationships hold:
Appendix 4 Dyadic Analysis DEFINITION ecto d is a linea vecto function of vecto d when the following elationships hold: d x = a xxd x + a xy d y + a xz d z d y = a yxd x + a yy d y + a yz d z d z = a zxd
More informationTwo figures are similar fi gures when they have the same shape but not necessarily the same size.
NDIN O PIION. o be poficient in math, ou need to ue clea definition in dicuion with othe and in ou own eaoning. imilait and anfomation ential uetion When a figue i tanlated, eflected, otated, o dilated
More informationBogoliubov Transformation in Classical Mechanics
Bogoliubov Tranformation in Claical Mechanic Canonical Tranformation Suppoe we have a et of complex canonical variable, {a j }, and would like to conider another et of variable, {b }, b b ({a j }). How
More informationone primary direction in which heat transfers (generally the smallest dimension) simple model good representation for solving engineering problems
CHAPTER 3: One-Dimenional Steady-State Conduction one pimay diection in which heat tanfe (geneally the mallet dimenion) imple model good epeentation fo olving engineeing poblem 3. Plane Wall 3.. hot fluid
More information556: MATHEMATICAL STATISTICS I
556: MATHEMATICAL STATISTICS I CHAPTER 5: STOCHASTIC CONVERGENCE The following efinitions ae state in tems of scala anom vaiables, but exten natually to vecto anom vaiables efine on the same obability
More informationScale Efficiency in DEA and DEA-R with Weight Restrictions
Available online at http://ijdea.rbiau.ac.ir Int. J. Data Envelopent Analyi (ISSN 2345-458X) Vol.2, No.2, Year 2014 Article ID IJDEA-00226, 5 page Reearch Article International Journal of Data Envelopent
More informationarxiv: v1 [math.nt] 12 May 2017
SEQUENCES OF CONSECUTIVE HAPPY NUMBERS IN NEGATIVE BASES HELEN G. GRUNDMAN AND PAMELA E. HARRIS axiv:1705.04648v1 [math.nt] 12 May 2017 ABSTRACT. Fo b 2 and e 2, let S e,b : Z Z 0 be the function taking
More information1 Random Variable. Why Random Variable? Discrete Random Variable. Discrete Random Variable. Discrete Distributions - 1 DD1-1
Rando Vaiable Pobability Distibutions and Pobability Densities Definition: If S is a saple space with a pobability easue and is a eal-valued function defined ove the eleents of S, then is called a ando
More informationConvex Hulls of Curves Sam Burton
Convex Hull of Curve Sam Burton 1 Introduction Thi paper will primarily be concerned with determining the face of convex hull of curve of the form C = {(t, t a, t b ) t [ 1, 1]}, a < b N in R 3. We hall
More informationOrbital Angular Momentum Eigenfunctions
Obital Angula Moentu Eigenfunctions Michael Fowle 1/11/08 Intoduction In the last lectue we established that the opeatos J Jz have a coon set of eigenkets j J j = j( j+ 1 ) j Jz j = j whee j ae integes
More informationLecture 8: Period Finding: Simon s Problem over Z N
Quantum Computation (CMU 8-859BB, Fall 205) Lecture 8: Period Finding: Simon Problem over Z October 5, 205 Lecturer: John Wright Scribe: icola Rech Problem A mentioned previouly, period finding i a rephraing
More informationBoise State University Department of Electrical and Computer Engineering ECE470 Electric Machines
Boie State Univeity Depatment of Electical and Compute Engineeing ECE470 Electic Machine Deivation of the Pe-Phae Steady-State Equivalent Cicuit of a hee-phae Induction Machine Nomenclatue θ: oto haft
More informationV V The circumflex (^) tells us this is a unit vector
Vecto Vecto have Diection and Magnitude Mike ailey mjb@c.oegontate.edu Magnitude: V V V V x y z vecto.pptx Vecto Can lo e Defined a the oitional Diffeence etween Two oint 3 Unit Vecto have a Magnitude
More informationAddition of Angular Momentum
Addition of Angula Moentu We ve leaned tat angula oentu i ipotant in quantu ecanic Obital angula oentu L Spin angula oentu S Fo ultielecton ato, we need to lean to add angula oentu Multiple electon, eac
More informationDesign By Emulation (Indirect Method)
Deign By Emulation (Indirect Method he baic trategy here i, that Given a continuou tranfer function, it i required to find the bet dicrete equivalent uch that the ignal produced by paing an input ignal
More informationCentral limit theorem for functions of weakly dependent variables
Int. Statistical Inst.: Poc. 58th Wold Statistical Congess, 2011, Dublin (Session CPS058 p.5362 Cental liit theoe fo functions of weakly dependent vaiables Jensen, Jens Ledet Aahus Univesity, Depatent
More informationKepler s problem gravitational attraction
Kele s oblem gavitational attaction Summay of fomulas deived fo two-body motion Let the two masses be m and m. The total mass is M = m + m, the educed mass is µ = m m /(m + m ). The gavitational otential
More informationPrecision Spectrophotometry
Peciion Spectophotomety Pupoe The pinciple of peciion pectophotomety ae illutated in thi expeiment by the detemination of chomium (III). ppaatu Spectophotomete (B&L Spec 20 D) Cuvette (minimum 2) Pipet:
More informationOn the ratio of maximum and minimum degree in maximal intersecting families
On the atio of maximum and minimum degee in maximal intesecting families Zoltán Lóánt Nagy Lale Özkahya Balázs Patkós Máté Vize Mach 6, 013 Abstact To study how balanced o unbalanced a maximal intesecting
More informationFARADAY'S LAW dt
FAADAY'S LAW 31.1 Faaday's Law of Induction In the peious chapte we leaned that electic cuent poduces agnetic field. Afte this ipotant discoey, scientists wondeed: if electic cuent poduces agnetic field,
More information7.2. Coulomb s Law. The Electric Force
Coulomb s aw Recall that chaged objects attact some objects and epel othes at a distance, without making any contact with those objects Electic foce,, o the foce acting between two chaged objects, is somewhat
More informationThe Normal Stress Dıstribution in an Infinite. Elastic Body with a Locally Curved and Hollow. Fiber under Geometrical Nonlinear Statement
Nonlinea Analyi and Diffeential quation Vol. 4 06 no. 6 95-04 HIKARI td www.m-hikai.com htt://dx.doi.og/0.988/nade.06.656 The Nomal Ste Dıtibution in an Infinite latic Body with a ocally Cuved and Hollow
More informationr cos, and y r sin with the origin of coordinate system located at
Lectue 3-3 Kinematics of Rotation Duing ou peious lectues we hae consideed diffeent examples of motion in one and seeal dimensions. But in each case the moing object was consideed as a paticle-like object,
More informationAP Physics Centripetal Acceleration
AP Phyic Centipetal Acceleation All of ou motion tudie thu fa hae dealt with taight-line tuff. We haen t dealt with thing changing diection duing thei tael. Thi type of motion i called angula motion. A
More informationarxiv: v1 [math.cv] 7 Nov 2018
INTERMEDIATE HANKEL OPERATORS ON THE FOCK SPACE OLIVIA CONSTANTIN axiv:181103137v1 [mathcv] 7 Nov 2018 Abtact We contuct a natual equence of middle Hankel opeato on the Fock pace, ie opeato which ae intemediate
More informationChapter 5 Linear Equations: Basic Theory and Practice
Chapte 5 inea Equations: Basic Theoy and actice In this chapte and the next, we ae inteested in the linea algebaic equation AX = b, (5-1) whee A is an m n matix, X is an n 1 vecto to be solved fo, and
More informationFREE Download Study Package from website: &
.. Linea Combinations: (a) (b) (c) (d) Given a finite set of vectos a b c,,,... then the vecto xa + yb + zc +... is called a linea combination of a, b, c,... fo any x, y, z... R. We have the following
More informationMath 124B February 02, 2012
Math 24B Febuay 02, 202 Vikto Gigoyan 8 Laplace s equation: popeties We have aleady encounteed Laplace s equation in the context of stationay heat conduction and wave phenomena. Recall that in two spatial
More informationConsiderations Regarding the Flux Estimation in Induction Generator with Application at the Control of Unconventional Energetic Conversion Systems
Conideation Regading the Flux Etimation in Induction Geneato with Application at the Contol of Unconventional Enegetic Conveion Sytem Ioif Szeidet, Octavian Potean, Ioan Filip, Vaa Citian Depatment of
More informationPhysics 181. Assignment 4
Physics 181 Assignment 4 Solutions 1. A sphee has within it a gavitational field given by g = g, whee g is constant and is the position vecto of the field point elative to the cente of the sphee. This
More informationTheorem 2: Proof: Note 1: Proof: Note 2:
A New 3-Dimenional Polynomial Intepolation Method: An Algoithmic Appoach Amitava Chattejee* and Rupak Bhattachayya** A new 3-dimenional intepolation method i intoduced in thi pape. Coeponding to the method
More informationImpulse and Momentum
Impule and Momentum 1. A ca poee 20,000 unit of momentum. What would be the ca' new momentum if... A. it elocity wee doubled. B. it elocity wee tipled. C. it ma wee doubled (by adding moe paenge and a
More informationLecture 2 Phys 798S Spring 2016 Steven Anlage. The heart and soul of superconductivity is the Meissner Effect. This feature uniquely distinguishes
ecture Phy 798S Spring 6 Steven Anlage The heart and oul of uperconductivity i the Meiner Effect. Thi feature uniquely ditinguihe uperconductivity fro any other tate of atter. Here we dicu oe iple phenoenological
More informationrt () is constant. We know how to find the length of the radius vector by r( t) r( t) r( t)
Cicula Motion Fom ancient times cicula tajectoies hae occupied a special place in ou model of the Uniese. Although these obits hae been eplaced by the moe geneal elliptical geomety, cicula motion is still
More informationChapter 5 Consistency, Zero Stability, and the Dahlquist Equivalence Theorem
Chapter 5 Conitency, Zero Stability, and the Dahlquit Equivalence Theorem In Chapter 2 we dicued convergence of numerical method and gave an experimental method for finding the rate of convergence (aka,
More information