BFF1303: ELECTRICAL / ELECTRONICS ENGINEERING. Direct Current Circuits : Methods of Analysis

Size: px
Start display at page:

Download "BFF1303: ELECTRICAL / ELECTRONICS ENGINEERING. Direct Current Circuits : Methods of Analysis"

Transcription

1 BFF1303: ELECTRICAL / ELECTRONICS ENGINEERING Drect Current Crcuts : Methods of Analyss Ismal Mohd Kharuddn, Zulkfl Md Yusof Faculty of Manufacturng Engneerng Unerst Malaysa Pahang

2 Drect Current Crcut (DC)- Methods of Analyss BFF1303 ELECTRICAL/ELECTRONICS ENGINEERING Contents: Outcomes Nodal Analyss Mesh Analyss Faculty of Manufacturng Unerst Malaysa Pahang Kampus Pekan, Pahang Darul Makmur Tel: Fax: BFF1303 Electrcal/Electronc Engneerng

3 Compute the soluton of crcuts contanng lnear resstors and ndependent and dependent sources by usng node analyss Compute the soluton of crcuts contanng lnear resstors and ndependent and dependent sources by usng mesh analyss BFF1303 Electrcal/Electronc Engneerng 3 3

4 There s another method to sole for currents and oltages. Easer More methodcal Stll based on Ohm s Law, KVL and KCL The methods are the nodal and mesh analyss. Nodal analyss s based on the KCL. Mesh analyss s based on the KVL. BFF1303 Electrcal/Electronc Engneerng 4 4

5 WITHOUT VOLTAGE SOURCE Analyze the crcut usng node oltages as the crcut arables. The node oltages s chosen nstead of the elements oltages. To smplfy matters, t s frst assumed that the crcuts do not contan oltage sources. BFF1303 BFF1303 Electrcal/Electronc Engneerng Engneerng

6 Steps to determne node oltages:. Select a node as a reference node Ths reference node also called the ground, hae zero potental. BFF1303 Electrcal/Electronc Engneerng 6 6

7 . The other node (nonreference nodes) wll be assgned as 1,, BFF1303 Electrcal/Electronc Engneerng 7 7

8 . Apply KCL to each of the nonreference node. At node 1 : I1 I 1 At node : I 3 BFF1303 Electrcal/Electronc Engneerng 8 8

9 . Apply the Ohm s law to express the unknown current 1, and 3 n terms of node oltages. hgher R lower Note: Current flows from a hgher potental (poste termnal) to a lower potental (negate termnal) n resstor. BFF1303 Electrcal/Electronc Engneerng 9 9

10 R1 R 3 R 3 0 I 0 0 I I R1 R R3 R BFF1303 Electrcal/Electronc Engneerng 10 10

11 Obtan the node oltages for the followng crcut BFF1303 Electrcal/Electronc Engneerng 11 11

12 Soluton. Select a node as a reference node. The other node (nonreference nodes) wll be assgned as 1,. Apply KCL to each of the nonreference node. At node 1 : At node : BFF1303 Electrcal/Electronc Engneerng 1 1

13 . Express the currents n term of node oltages Rearrange the equaton BFF1303 Electrcal/Electronc Engneerng 13 13

14 Then n matrx form By usng Cramer s Rule V V 1 BFF1303 Electrcal/Electronc Engneerng 14 14

15 In the gen crcut, obtan the node oltages Answer 6V 1 4V BFF1303 Electrcal/Electronc Engneerng 15 15

16 For the gen crcut, determne the oltages at the nodes Answer 4.8V.4V.4V 1 3 BFF1303 Electrcal/Electronc Engneerng 16 16

17 . Select a node as a reference node Ths reference node also called the ground, hae zero potental.. Reew of steps for nodal analyss wthout oltage sources: The other node (nonreference nodes) wll be assgned as 1,,. Apply KCL to each of the nonreference node.. Apply the Ohm s law to express the unknown current 1, and 3 n terms of node oltages. hgher R lower BFF1303 Electrcal/Electronc Engneerng 17 17

18 WITH VOLTAGE SOURCE Case 1 If a oltage source s connected between the reference node and a nonreference node. The oltage at the nonreference node equal to the oltage source. 1 10V BFF1303 Electrcal/Electronc Engneerng 18 18

19 Case If the oltage source (dependent or ndependent) s connected between two nonreference nodes, the two nonreference nodes form a generalzed node or supernode. BFF1303 Electrcal/Electronc Engneerng 19 19

20 A supernode s formed by enclosng a (dependent or ndependent) oltage source connected between two nonreference nodes and any elements connected n parallel wth t. supernode BFF1303 Electrcal/Electronc Engneerng 0 0

21 A supernode requres the applcatons of both KCL and KVL. A supernode has no oltage of ts own. A supernode can be assumed as one bg node. BFF1303 Electrcal/Electronc Engneerng 1 1

22 . Select a node as a reference node Ths reference node also called the ground, hae zero potental.. Steps for nodal analyss wth oltage source: Assgn the other nodes (nonreference nodes) as 1,, and dentfy the supernode.. Apply KCL to each of the nonreference node and the supernode. Note: For supernode, apply the KCL around the supernode. Assume the supernode as one bg node BFF1303 Electrcal/Electronc Engneerng

23 . Express the currents n term of node oltages. hgher R lower. Apply KVL around the supernode. BFF1303 Electrcal/Electronc Engneerng 3 3

24 Obtan the node oltages for the followng crcut BFF1303 Electrcal/Electronc Engneerng 4 4

25 Soluton. Select a node as a reference node. Assgn the other node (nonreference nodes) as 1, and dentfy the supernode. Apply KCL to each of the nonreference node and the supernode. At node A At 70 7A At supernode BFF1303 Electrcal/Electronc Engneerng 5 5

26 . Express the currents n term of node oltages Rearrange the equaton Apply KVL around the supernode BFF1303 Electrcal/Electronc Engneerng 6 6

27 Then n matrx form By usng Cramer s Rule V V 3 1 BFF1303 Electrcal/Electronc Engneerng 7 7

28 Fnd and for the gen crcut Answer 400mV.8A BFF1303 Electrcal/Electronc Engneerng 8 8

29 Obtan the node oltages for the followng crcut BFF1303 Electrcal/Electronc Engneerng 9 9

30 Soluton. Select a node as a reference node.. Assgn the other node (nonreference nodes) as 1, and dentfy the supernode Apply KCL to each of the nonreference node and the supernode. At supernode 1-: At supernode 3-4: BFF1303 Electrcal/Electronc Engneerng

31 . Express the currents n term of node oltages BFF1303 Electrcal/Electronc Engneerng 31 31

32 . Apply KVL around the supernode. At loop At loop 3 0 and 3 x 4 x x At loop 3 x and x BFF1303 Electrcal/Electronc Engneerng 3 3

33 From loop 1 10 and subs ths Eq. nto and Then n matrx form BFF1303 Electrcal/Electronc Engneerng 33 33

34 By usng Cramer s Rule V BFF1303 Electrcal/Electronc Engneerng 34 34

35 V V V BFF1303 Electrcal/Electronc Engneerng 35 35

36 By usng nodal analyss obtan the node oltages for the followng crcut Answer V V V 1 3 BFF1303 Electrcal/Electronc Engneerng 36 36

37 WITHOUT CURRENT SOURCE Mesh analyss use the mesh currents as the crcut arables. Recall: nodal analyss use the node oltages as the crcut arables. Recall: a loop s a closed path wth no node passed more than once. A mesh s a loop that does not contan any other loop wthn t. BFF1303 Electrcal/Electronc Engneerng 37 37

38 Recall: nodal analyss apples KCL to fnd unknown oltages. Mesh analyss apples KVL to fnd unknown currents. abefa & bcdeb are meshes. abcdefa s not a mesh. BFF1303 Electrcal/Electronc Engneerng 38 38

39 The current through a mesh s known as mesh current. Frst, the analyss wll concentrate on crcut wth no current source. Steps to determne mesh currents:. Assgn mesh currents 1,,, n to the n meshes. The flow of the mesh. currents s conentonally assume n clockwse drecton. Determne the polarty & the drecton of current flow through each element.. Apply KCL for each node n term of mesh current.. Apply KVL to each of the n meshes. Use Ohm s law to express the oltages n terms of the mesh currents. BFF1303 Electrcal/Electronc Engneerng 39 39

40 . Assgn the mesh currents: 1 and. Determne the polarty & the drecton of current. Note: let the drecton of current at the outsde branch = drecton of the mesh current BFF1303 Electrcal/Electronc Engneerng 40 40

41 . Apply KCL. I I I 3 1 snce I I 1 1 I 3 1 Note: I for branch current, for mesh current. Apply KVL to each mesh Mesh BFF1303 Electrcal/Electronc Engneerng 41 41

42 Mesh Then n matrx form By usng Cramer s Rule A A 3 BFF1303 Electrcal/Electronc Engneerng 4 4

43 Calculate the mesh current 1 and for the followng crcut Answer.5A 0A 1 BFF1303 Electrcal/Electronc Engneerng 43 43

44 Use mesh analyss to fnd I o for the followng crcut BFF1303 Electrcal/Electronc Engneerng 44 44

45 . Assgn the mesh currents: 1 and.. Determne the polarty & the drecton of current.. Apply KCL. I o 1. Apply KVL to each mesh. Mesh BFF1303 Electrcal/Electronc Engneerng 45 45

46 Mesh Mesh Then n matrx form BFF1303 Electrcal/Electronc Engneerng 46 46

47 By usng Cramer s Rule A A Thus, I A o A 19 3 BFF1303 Electrcal/Electronc Engneerng 47 47

48 By usng mesh analyss fnd I o n the followng crcut Answer I 4A o BFF1303 Electrcal/Electronc Engneerng 48 48

49 WITH CURRENT SOURCE Case 1 When the current source exst only n one mesh Set the alue of = 5 A and wrte a mesh equaton for the other mesh n the usual way A BFF1303 Electrcal/Electronc Engneerng 49 49

50 Case When the current source exst between two meshes. need to create a supermesh by excludng the current source and any elements connected n seres wth t. BFF1303 Electrcal/Electronc Engneerng 50 50

51 NOTE: A supermesh results when two meshes hae a (dependent or ndependent) current source n common. Applyng KVL to the supermesh BFF1303 Electrcal/Electronc Engneerng 51 51

52 Applyng KCL to the crcut 1 6 Then sole the Eq. (1) and () 1 3.A.8A BFF1303 Electrcal/Electronc Engneerng 5 5

53 The current source n the supermesh prodes the constrant equaton necessary to sole for the mesh currents. A supermesh has no current of ts own. A supermesh requres the applcaton of both KVL and KCL. BFF1303 Electrcal/Electronc Engneerng 53 53

54 By usng mesh analyss fnd 1, and 3 n the followng crcut BFF1303 Electrcal/Electronc Engneerng 54 54

55 . Assgn the mesh currents: 1, and 3... Determne the polarty & the drecton of current. Applyng KCL to supermesh Notce that meshes (1) and () form a supermesh snce they hae ndependent current source n common BFF1303 Electrcal/Electronc Engneerng 55 55

56 . Apply KVL to supermesh Applyng KVL n Mesh Then n matrx form BFF1303 Electrcal/Electronc Engneerng 56 56

57 By usng Cramer s Rule A A A 76 BFF1303 Electrcal/Electronc Engneerng 57 57

58 By usng mesh analyss fnd 1, to 4 n the followng crcut 7.5 A.5 A 3.93A.143A Answer 1 3 BFF1303 Electrcal/Electronc Engneerng 58 58

Circuit Analysis I (ENGR 2405) Chapter 3 Method of Analysis Nodal(KCL) and Mesh(KVL)

Circuit Analysis I (ENGR 2405) Chapter 3 Method of Analysis Nodal(KCL) and Mesh(KVL) Crcut Analyss I (ENG 405) Chapter Method of Analyss Nodal(KCL) and Mesh(KVL) Nodal Analyss If nstead of focusng on the oltages of the crcut elements, one looks at the oltages at the nodes of the crcut,

More information

RESISTIVE CIRCUITS MULTI NODE/LOOP CIRCUIT ANALYSIS

RESISTIVE CIRCUITS MULTI NODE/LOOP CIRCUIT ANALYSIS RESSTE CRCUTS MULT NODE/LOOP CRCUT ANALYSS DEFNNG THE REFERENCE NODE S TAL 4 THESTATEMENT 4 S MEANNGLES UNTL THE REFERENCE PONT S DEFNED BY CONENTON THE GROUND SYMBOL SPECFES THE REFERENCE PONT. ALL NODE

More information

LOOP ANALYSIS. determine all currents and Voltages in IT IS DUAL TO NODE ANALYSIS - IT FIRST DETERMINES ALL CURRENTS IN A CIRCUIT

LOOP ANALYSIS. determine all currents and Voltages in IT IS DUAL TO NODE ANALYSIS - IT FIRST DETERMINES ALL CURRENTS IN A CIRCUIT LOOP ANALYSS The second systematic technique to determine all currents and oltages in a circuit T S DUAL TO NODE ANALYSS - T FRST DETERMNES ALL CURRENTS N A CRCUT AND THEN T USES OHM S LAW TO COMPUTE NECESSARY

More information

ELECTRICAL CIRCUIT AND MACHINE ENT 249/3. Methods of Analysis

ELECTRICAL CIRCUIT AND MACHINE ENT 249/3. Methods of Analysis ELECTRICAL CIRCUIT AND MACHINE ENT 49/ Methods of Analysis Introduction Nodal Analysis KCL & Ohm s Law Nodal Analysis with Voltage Sources (Supernode) KCL, Ohm s & KVL Law Mesh Analysis - KVL & Ohm s Law

More information

LOOP ANALYSIS. The second systematic technique to determine all currents and voltages in a circuit

LOOP ANALYSIS. The second systematic technique to determine all currents and voltages in a circuit LOOP ANALYSS The second systematic technique to determine all currents and voltages in a circuit T S DUAL TO NODE ANALYSS - T FRST DETERMNES ALL CURRENTS N A CRCUT AND THEN T USES OHM S LAW TO COMPUTE

More information

Chapter 3 Methods of Analysis: 2) Mesh Analysis

Chapter 3 Methods of Analysis: 2) Mesh Analysis Chapter 3 Methods of Analysis: 2) Mesh Analysis Dr. Waleed Al-Hanafy waleed alhanafy@yahoo.com Faculty of Electronic Engineering, Menoufia Univ., Egypt MSA Summer Course: Electric Circuit Analysis I (ESE

More information

i v v 6 i 2 i 3 v + (1) (2) (3) (4) (5) Substituting (4) and (5) into (3) (6) = 2 (7) (5) and (6) (8) (4) and (6) ˆ

i v v 6 i 2 i 3 v + (1) (2) (3) (4) (5) Substituting (4) and (5) into (3) (6) = 2 (7) (5) and (6) (8) (4) and (6) ˆ 5V 6 v 6 î v v Ω î Ω v v 8Ω V î v 5 6Ω 5 Mesh : 6ˆ ˆ = Mesh : ˆ 8ˆ = Mesh : ˆ ˆ ˆ 8 0 = 5 Solvng ˆ ˆ ˆ from () = Solvng ˆ ˆ ˆ from () = 7 7 Substtutng () and (5) nto () (5) and (6) 9 ˆ = A 8 ˆ = A 0 ()

More information

Method of analysis. Bởi: Sy Hien Dinh

Method of analysis. Bởi: Sy Hien Dinh Method of analysis Bởi: Sy Hien Dinh INTRODUCTION Having understood the fundamental laws of circuit theory (Ohm s law and Kirchhhoff s laws), we are now prepared to apply to develop two powerful techniques

More information

Mesh and Node Equations: Circuits Containing Dependent Sources

Mesh and Node Equations: Circuits Containing Dependent Sources Mesh nd Node Equtons: Crcuts Contnng Dependent Sources Introducton The crcuts n ths set of problems re smll crcuts tht contn sngle dependent source. These crcuts cn be nlyzed usng mesh equton or usng node

More information

Reading. 14. Subdivision curves. Recommended:

Reading. 14. Subdivision curves. Recommended: eadng ecommended: Stollntz, Deose, and Salesn. Wavelets for Computer Graphcs: heory and Applcatons, 996, secton 6.-6., A.5. 4. Subdvson curves Note: there s an error n Stollntz, et al., secton A.5. Equaton

More information

Parallelism for Nested Loops with Non-uniform and Flow Dependences

Parallelism for Nested Loops with Non-uniform and Flow Dependences Parallelsm for Nested Loops wth Non-unform and Flow Dependences Sam-Jn Jeong Dept. of Informaton & Communcaton Engneerng, Cheonan Unversty, 5, Anseo-dong, Cheonan, Chungnam, 330-80, Korea. seong@cheonan.ac.kr

More information

Solitary and Traveling Wave Solutions to a Model. of Long Range Diffusion Involving Flux with. Stability Analysis

Solitary and Traveling Wave Solutions to a Model. of Long Range Diffusion Involving Flux with. Stability Analysis Internatonal Mathematcal Forum, Vol. 6,, no. 7, 8 Soltary and Travelng Wave Solutons to a Model of Long Range ffuson Involvng Flux wth Stablty Analyss Manar A. Al-Qudah Math epartment, Rabgh Faculty of

More information

2x x l. Module 3: Element Properties Lecture 4: Lagrange and Serendipity Elements

2x x l. Module 3: Element Properties Lecture 4: Lagrange and Serendipity Elements Module 3: Element Propertes Lecture : Lagrange and Serendpty Elements 5 In last lecture note, the nterpolaton functons are derved on the bass of assumed polynomal from Pascal s trangle for the fled varable.

More information

Loop Transformations, Dependences, and Parallelization

Loop Transformations, Dependences, and Parallelization Loop Transformatons, Dependences, and Parallelzaton Announcements Mdterm s Frday from 3-4:15 n ths room Today Semester long project Data dependence recap Parallelsm and storage tradeoff Scalar expanson

More information

TN348: Openlab Module - Colocalization

TN348: Openlab Module - Colocalization TN348: Openlab Module - Colocalzaton Topc The Colocalzaton module provdes the faclty to vsualze and quantfy colocalzaton between pars of mages. The Colocalzaton wndow contans a prevew of the two mages

More information

S1 Note. Basis functions.

S1 Note. Basis functions. S1 Note. Bass functons. Contents Types of bass functons...1 The Fourer bass...2 B-splne bass...3 Power and type I error rates wth dfferent numbers of bass functons...4 Table S1. Smulaton results of type

More information

Chapter 6 Programmng the fnte element method Inow turn to the man subject of ths book: The mplementaton of the fnte element algorthm n computer programs. In order to make my dscusson as straghtforward

More information

Proper Choice of Data Used for the Estimation of Datum Transformation Parameters

Proper Choice of Data Used for the Estimation of Datum Transformation Parameters Proper Choce of Data Used for the Estmaton of Datum Transformaton Parameters Hakan S. KUTOGLU, Turkey Key words: Coordnate systems; transformaton; estmaton, relablty. SUMMARY Advances n technologes and

More information

Programming in Fortran 90 : 2017/2018

Programming in Fortran 90 : 2017/2018 Programmng n Fortran 90 : 2017/2018 Programmng n Fortran 90 : 2017/2018 Exercse 1 : Evaluaton of functon dependng on nput Wrte a program who evaluate the functon f (x,y) for any two user specfed values

More information

y and the total sum of

y and the total sum of Lnear regresson Testng for non-lnearty In analytcal chemstry, lnear regresson s commonly used n the constructon of calbraton functons requred for analytcal technques such as gas chromatography, atomc absorpton

More information

LU Decomposition Method Jamie Trahan, Autar Kaw, Kevin Martin University of South Florida United States of America

LU Decomposition Method Jamie Trahan, Autar Kaw, Kevin Martin University of South Florida United States of America nbm_sle_sm_ludecomp.nb 1 LU Decomposton Method Jame Trahan, Autar Kaw, Kevn Martn Unverst of South Florda Unted States of Amerca aw@eng.usf.edu nbm_sle_sm_ludecomp.nb 2 Introducton When solvng multple

More information

The Greedy Method. Outline and Reading. Change Money Problem. Greedy Algorithms. Applications of the Greedy Strategy. The Greedy Method Technique

The Greedy Method. Outline and Reading. Change Money Problem. Greedy Algorithms. Applications of the Greedy Strategy. The Greedy Method Technique //00 :0 AM Outlne and Readng The Greedy Method The Greedy Method Technque (secton.) Fractonal Knapsack Problem (secton..) Task Schedulng (secton..) Mnmum Spannng Trees (secton.) Change Money Problem Greedy

More information

SLAM Summer School 2006 Practical 2: SLAM using Monocular Vision

SLAM Summer School 2006 Practical 2: SLAM using Monocular Vision SLAM Summer School 2006 Practcal 2: SLAM usng Monocular Vson Javer Cvera, Unversty of Zaragoza Andrew J. Davson, Imperal College London J.M.M Montel, Unversty of Zaragoza. josemar@unzar.es, jcvera@unzar.es,

More information

An Application of the Dulmage-Mendelsohn Decomposition to Sparse Null Space Bases of Full Row Rank Matrices

An Application of the Dulmage-Mendelsohn Decomposition to Sparse Null Space Bases of Full Row Rank Matrices Internatonal Mathematcal Forum, Vol 7, 2012, no 52, 2549-2554 An Applcaton of the Dulmage-Mendelsohn Decomposton to Sparse Null Space Bases of Full Row Rank Matrces Mostafa Khorramzadeh Department of Mathematcal

More information

6.854 Advanced Algorithms Petar Maymounkov Problem Set 11 (November 23, 2005) With: Benjamin Rossman, Oren Weimann, and Pouya Kheradpour

6.854 Advanced Algorithms Petar Maymounkov Problem Set 11 (November 23, 2005) With: Benjamin Rossman, Oren Weimann, and Pouya Kheradpour 6.854 Advanced Algorthms Petar Maymounkov Problem Set 11 (November 23, 2005) Wth: Benjamn Rossman, Oren Wemann, and Pouya Kheradpour Problem 1. We reduce vertex cover to MAX-SAT wth weghts, such that the

More information

Compiler Design. Spring Register Allocation. Sample Exercises and Solutions. Prof. Pedro C. Diniz

Compiler Design. Spring Register Allocation. Sample Exercises and Solutions. Prof. Pedro C. Diniz Compler Desgn Sprng 2014 Regster Allocaton Sample Exercses and Solutons Prof. Pedro C. Dnz USC / Informaton Scences Insttute 4676 Admralty Way, Sute 1001 Marna del Rey, Calforna 90292 pedro@s.edu Regster

More information

NODAL AND LOOP ANALYSIS TECHNIQUES. Develop systematic techniques to determine all the voltages and currents in a circuit NODE ANALYSIS

NODAL AND LOOP ANALYSIS TECHNIQUES. Develop systematic techniques to determine all the voltages and currents in a circuit NODE ANALYSIS NODAL AND LOOP ANALYSS TECHNQUES LEANNG GOALS NODAL ANALYSS LOOP ANALYSS Develop systematic techniques to determine all the voltages and currents in a circuit NODE ANALYSS One of the systematic ways to

More information

An Optimal Algorithm for Prufer Codes *

An Optimal Algorithm for Prufer Codes * J. Software Engneerng & Applcatons, 2009, 2: 111-115 do:10.4236/jsea.2009.22016 Publshed Onlne July 2009 (www.scrp.org/journal/jsea) An Optmal Algorthm for Prufer Codes * Xaodong Wang 1, 2, Le Wang 3,

More information

Complex Numbers. Now we also saw that if a and b were both positive then ab = a b. For a second let s forget that restriction and do the following.

Complex Numbers. Now we also saw that if a and b were both positive then ab = a b. For a second let s forget that restriction and do the following. Complex Numbers The last topc n ths secton s not really related to most of what we ve done n ths chapter, although t s somewhat related to the radcals secton as we wll see. We also won t need the materal

More information

Module 6: FEM for Plates and Shells Lecture 6: Finite Element Analysis of Shell

Module 6: FEM for Plates and Shells Lecture 6: Finite Element Analysis of Shell Module 6: FEM for Plates and Shells Lecture 6: Fnte Element Analyss of Shell 3 6.6. Introducton A shell s a curved surface, whch by vrtue of ther shape can wthstand both membrane and bendng forces. A shell

More information

1.4 Circuit Theorems

1.4 Circuit Theorems . Crcut Theorems. v,? (C)V, 5 6 (D) V, 6 5. A smple equvlent crcut of the termnl 6 v, network shown n fg. P.. s Fg. P... (A)V, (B)V, v (C)V,5 (D)V,5 Fg. P....,? 5 V, v (A) (B) Fg. P... (A)A, 0 (B) 0 A,

More information

The Codesign Challenge

The Codesign Challenge ECE 4530 Codesgn Challenge Fall 2007 Hardware/Software Codesgn The Codesgn Challenge Objectves In the codesgn challenge, your task s to accelerate a gven software reference mplementaton as fast as possble.

More information

Radial Basis Functions

Radial Basis Functions Radal Bass Functons Mesh Reconstructon Input: pont cloud Output: water-tght manfold mesh Explct Connectvty estmaton Implct Sgned dstance functon estmaton Image from: Reconstructon and Representaton of

More information

The mesh-current method

The mesh-current method The mesh-current method Equivalent resistance Voltage / current dividers Source transformations Node voltages Mesh currents Superposition Mirror image of the node-voltage method. Define mesh currents flowing

More information

AMath 483/583 Lecture 21 May 13, Notes: Notes: Jacobi iteration. Notes: Jacobi with OpenMP coarse grain

AMath 483/583 Lecture 21 May 13, Notes: Notes: Jacobi iteration. Notes: Jacobi with OpenMP coarse grain AMath 483/583 Lecture 21 May 13, 2011 Today: OpenMP and MPI versons of Jacob teraton Gauss-Sedel and SOR teratve methods Next week: More MPI Debuggng and totalvew GPU computng Read: Class notes and references

More information

USING GRAPHING SKILLS

USING GRAPHING SKILLS Name: BOLOGY: Date: _ Class: USNG GRAPHNG SKLLS NTRODUCTON: Recorded data can be plotted on a graph. A graph s a pctoral representaton of nformaton recorded n a data table. t s used to show a relatonshp

More information

Solving two-person zero-sum game by Matlab

Solving two-person zero-sum game by Matlab Appled Mechancs and Materals Onlne: 2011-02-02 ISSN: 1662-7482, Vols. 50-51, pp 262-265 do:10.4028/www.scentfc.net/amm.50-51.262 2011 Trans Tech Publcatons, Swtzerland Solvng two-person zero-sum game by

More information

APPLICATION OF MULTIVARIATE LOSS FUNCTION FOR ASSESSMENT OF THE QUALITY OF TECHNOLOGICAL PROCESS MANAGEMENT

APPLICATION OF MULTIVARIATE LOSS FUNCTION FOR ASSESSMENT OF THE QUALITY OF TECHNOLOGICAL PROCESS MANAGEMENT 3. - 5. 5., Brno, Czech Republc, EU APPLICATION OF MULTIVARIATE LOSS FUNCTION FOR ASSESSMENT OF THE QUALITY OF TECHNOLOGICAL PROCESS MANAGEMENT Abstract Josef TOŠENOVSKÝ ) Lenka MONSPORTOVÁ ) Flp TOŠENOVSKÝ

More information

Loop Transformations for Parallelism & Locality. Review. Scalar Expansion. Scalar Expansion: Motivation

Loop Transformations for Parallelism & Locality. Review. Scalar Expansion. Scalar Expansion: Motivation Loop Transformatons for Parallelsm & Localty Last week Data dependences and loops Loop transformatons Parallelzaton Loop nterchange Today Scalar expanson for removng false dependences Loop nterchange Loop

More information

NUMERICAL SOLVING OPTIMAL CONTROL PROBLEMS BY THE METHOD OF VARIATIONS

NUMERICAL SOLVING OPTIMAL CONTROL PROBLEMS BY THE METHOD OF VARIATIONS ARPN Journal of Engneerng and Appled Scences 006-017 Asan Research Publshng Network (ARPN). All rghts reserved. NUMERICAL SOLVING OPTIMAL CONTROL PROBLEMS BY THE METHOD OF VARIATIONS Igor Grgoryev, Svetlana

More information

CS 534: Computer Vision Model Fitting

CS 534: Computer Vision Model Fitting CS 534: Computer Vson Model Fttng Sprng 004 Ahmed Elgammal Dept of Computer Scence CS 534 Model Fttng - 1 Outlnes Model fttng s mportant Least-squares fttng Maxmum lkelhood estmaton MAP estmaton Robust

More information

Loop Permutation. Loop Transformations for Parallelism & Locality. Legality of Loop Interchange. Loop Interchange (cont)

Loop Permutation. Loop Transformations for Parallelism & Locality. Legality of Loop Interchange. Loop Interchange (cont) Loop Transformatons for Parallelsm & Localty Prevously Data dependences and loops Loop transformatons Parallelzaton Loop nterchange Today Loop nterchange Loop transformatons and transformaton frameworks

More information

Analysis of Continuous Beams in General

Analysis of Continuous Beams in General Analyss of Contnuous Beams n General Contnuous beams consdered here are prsmatc, rgdly connected to each beam segment and supported at varous ponts along the beam. onts are selected at ponts of support,

More information

Face Recognition University at Buffalo CSE666 Lecture Slides Resources:

Face Recognition University at Buffalo CSE666 Lecture Slides Resources: Face Recognton Unversty at Buffalo CSE666 Lecture Sldes Resources: http://www.face-rec.org/algorthms/ Overvew of face recognton algorthms Correlaton - Pxel based correspondence between two face mages Structural

More information

CHARUTAR VIDYA MANDAL S SEMCOM Vallabh Vidyanagar

CHARUTAR VIDYA MANDAL S SEMCOM Vallabh Vidyanagar CHARUTAR VIDYA MANDAL S SEMCOM Vallabh Vdyanagar Faculty Name: Am D. Trved Class: SYBCA Subject: US03CBCA03 (Advanced Data & Fle Structure) *UNIT 1 (ARRAYS AND TREES) **INTRODUCTION TO ARRAYS If we want

More information

ROBOT KINEMATICS. ME Robotics ME Robotics

ROBOT KINEMATICS. ME Robotics ME Robotics ROBOT KINEMATICS Purpose: The purpose of ths chapter s to ntroduce you to robot knematcs, and the concepts related to both open and closed knematcs chans. Forward knematcs s dstngushed from nverse knematcs.

More information

Sum of Linear and Fractional Multiobjective Programming Problem under Fuzzy Rules Constraints

Sum of Linear and Fractional Multiobjective Programming Problem under Fuzzy Rules Constraints Australan Journal of Basc and Appled Scences, 2(4): 1204-1208, 2008 ISSN 1991-8178 Sum of Lnear and Fractonal Multobjectve Programmng Problem under Fuzzy Rules Constrants 1 2 Sanjay Jan and Kalash Lachhwan

More information

Preconditioning Parallel Sparse Iterative Solvers for Circuit Simulation

Preconditioning Parallel Sparse Iterative Solvers for Circuit Simulation Precondtonng Parallel Sparse Iteratve Solvers for Crcut Smulaton A. Basermann, U. Jaekel, and K. Hachya 1 Introducton One mportant mathematcal problem n smulaton of large electrcal crcuts s the soluton

More information

Course Introduction. Algorithm 8/31/2017. COSC 320 Advanced Data Structures and Algorithms. COSC 320 Advanced Data Structures and Algorithms

Course Introduction. Algorithm 8/31/2017. COSC 320 Advanced Data Structures and Algorithms. COSC 320 Advanced Data Structures and Algorithms Course Introducton Course Topcs Exams, abs, Proects A quc loo at a few algorthms 1 Advanced Data Structures and Algorthms Descrpton: We are gong to dscuss algorthm complexty analyss, algorthm desgn technques

More information

Problem Set 3 Solutions

Problem Set 3 Solutions Introducton to Algorthms October 4, 2002 Massachusetts Insttute of Technology 6046J/18410J Professors Erk Demane and Shaf Goldwasser Handout 14 Problem Set 3 Solutons (Exercses were not to be turned n,

More information

Introduction to Geometrical Optics - a 2D ray tracing Excel model for spherical mirrors - Part 2

Introduction to Geometrical Optics - a 2D ray tracing Excel model for spherical mirrors - Part 2 Introducton to Geometrcal Optcs - a D ra tracng Ecel model for sphercal mrrors - Part b George ungu - Ths s a tutoral eplanng the creaton of an eact D ra tracng model for both sphercal concave and sphercal

More information

MIXED INTEGER-DISCRETE-CONTINUOUS OPTIMIZATION BY DIFFERENTIAL EVOLUTION Part 1: the optimization method

MIXED INTEGER-DISCRETE-CONTINUOUS OPTIMIZATION BY DIFFERENTIAL EVOLUTION Part 1: the optimization method MIED INTEGER-DISCRETE-CONTINUOUS OPTIMIZATION BY DIFFERENTIAL EVOLUTION Part : the optmzaton method Joun Lampnen Unversty of Vaasa Department of Informaton Technology and Producton Economcs P. O. Box 700

More information

Support Vector Machines

Support Vector Machines /9/207 MIST.6060 Busness Intellgence and Data Mnng What are Support Vector Machnes? Support Vector Machnes Support Vector Machnes (SVMs) are supervsed learnng technques that analyze data and recognze patterns.

More information

Sequential search. Building Java Programs Chapter 13. Sequential search. Sequential search

Sequential search. Building Java Programs Chapter 13. Sequential search. Sequential search Sequental search Buldng Java Programs Chapter 13 Searchng and Sortng sequental search: Locates a target value n an array/lst by examnng each element from start to fnsh. How many elements wll t need to

More information

UNIT 2 : INEQUALITIES AND CONVEX SETS

UNIT 2 : INEQUALITIES AND CONVEX SETS UNT 2 : NEQUALTES AND CONVEX SETS ' Structure 2. ntroducton Objectves, nequaltes and ther Graphs Convex Sets and ther Geometry Noton of Convex Sets Extreme Ponts of Convex Set Hyper Planes and Half Spaces

More information

Problem Definitions and Evaluation Criteria for Computational Expensive Optimization

Problem Definitions and Evaluation Criteria for Computational Expensive Optimization Problem efntons and Evaluaton Crtera for Computatonal Expensve Optmzaton B. Lu 1, Q. Chen and Q. Zhang 3, J. J. Lang 4, P. N. Suganthan, B. Y. Qu 6 1 epartment of Computng, Glyndwr Unversty, UK Faclty

More information

5 The Primal-Dual Method

5 The Primal-Dual Method 5 The Prmal-Dual Method Orgnally desgned as a method for solvng lnear programs, where t reduces weghted optmzaton problems to smpler combnatoral ones, the prmal-dual method (PDM) has receved much attenton

More information

Priority queues and heaps Professors Clark F. Olson and Carol Zander

Priority queues and heaps Professors Clark F. Olson and Carol Zander Prorty queues and eaps Professors Clark F. Olson and Carol Zander Prorty queues A common abstract data type (ADT) n computer scence s te prorty queue. As you mgt expect from te name, eac tem n te prorty

More information

SENSITIVITY ANALYSIS IN LINEAR PROGRAMMING USING A CALCULATOR

SENSITIVITY ANALYSIS IN LINEAR PROGRAMMING USING A CALCULATOR SENSITIVITY ANALYSIS IN LINEAR PROGRAMMING USING A CALCULATOR Judth Aronow Rchard Jarvnen Independent Consultant Dept of Math/Stat 559 Frost Wnona State Unversty Beaumont, TX 7776 Wnona, MN 55987 aronowju@hal.lamar.edu

More information

Routability Driven Modification Method of Monotonic Via Assignment for 2-layer Ball Grid Array Packages

Routability Driven Modification Method of Monotonic Via Assignment for 2-layer Ball Grid Array Packages Routablty Drven Modfcaton Method of Monotonc Va Assgnment for 2-layer Ball Grd Array Pacages Yoch Tomoa Atsush Taahash Department of Communcatons and Integrated Systems, Toyo Insttute of Technology 2 12

More information

A fault tree analysis strategy using binary decision diagrams

A fault tree analysis strategy using binary decision diagrams Loughborough Unversty Insttutonal Repostory A fault tree analyss strategy usng bnary decson dagrams Ths tem was submtted to Loughborough Unversty's Insttutonal Repostory by the/an author. Addtonal Informaton:

More information

Positive Semi-definite Programming Localization in Wireless Sensor Networks

Positive Semi-definite Programming Localization in Wireless Sensor Networks Postve Sem-defnte Programmng Localzaton n Wreless Sensor etworks Shengdong Xe 1,, Jn Wang, Aqun Hu 1, Yunl Gu, Jang Xu, 1 School of Informaton Scence and Engneerng, Southeast Unversty, 10096, anjng Computer

More information

Lecture 13: High-dimensional Images

Lecture 13: High-dimensional Images Lec : Hgh-dmensonal Images Grayscale Images Lecture : Hgh-dmensonal Images Math 90 Prof. Todd Wttman The Ctadel A grayscale mage s an nteger-valued D matrx. An 8-bt mage takes on values between 0 and 55.

More information

the nber of vertces n the graph. spannng tree T beng part of a par of maxmally dstant trees s called extremal. Extremal trees are useful n the mxed an

the nber of vertces n the graph. spannng tree T beng part of a par of maxmally dstant trees s called extremal. Extremal trees are useful n the mxed an On Central Spannng Trees of a Graph S. Bezrukov Unverstat-GH Paderborn FB Mathematk/Informatk Furstenallee 11 D{33102 Paderborn F. Kaderal, W. Poguntke FernUnverstat Hagen LG Kommunkatonssysteme Bergscher

More information

Routing on Switch Matrix Multi-FPGA Systems

Routing on Switch Matrix Multi-FPGA Systems Routng on Swtch Matrx Mult-FPGA Systems Abdel Enou and N. Ranganathan Center for Mcroelectroncs Research Department of Computer Scence and Engneerng Unversty of South Florda Tampa, FL 33620 Abstract In

More information

Categories and Subject Descriptors B.7.2 [Integrated Circuits]: Design Aids Verification. General Terms Algorithms

Categories and Subject Descriptors B.7.2 [Integrated Circuits]: Design Aids Verification. General Terms Algorithms 3. Fndng Determnstc Soluton from Underdetermned Equaton: Large-Scale Performance Modelng by Least Angle Regresson Xn L ECE Department, Carnege Mellon Unversty Forbs Avenue, Pttsburgh, PA 3 xnl@ece.cmu.edu

More information

AP PHYSICS B 2008 SCORING GUIDELINES

AP PHYSICS B 2008 SCORING GUIDELINES AP PHYSICS B 2008 SCORING GUIDELINES General Notes About 2008 AP Physcs Scorng Gudelnes 1. The solutons contan the most common method of solvng the free-response questons and the allocaton of ponts for

More information

NAG Fortran Library Chapter Introduction. G10 Smoothing in Statistics

NAG Fortran Library Chapter Introduction. G10 Smoothing in Statistics Introducton G10 NAG Fortran Lbrary Chapter Introducton G10 Smoothng n Statstcs Contents 1 Scope of the Chapter... 2 2 Background to the Problems... 2 2.1 Smoothng Methods... 2 2.2 Smoothng Splnes and Regresson

More information

Analysis of 3D Cracks in an Arbitrary Geometry with Weld Residual Stress

Analysis of 3D Cracks in an Arbitrary Geometry with Weld Residual Stress Analyss of 3D Cracks n an Arbtrary Geometry wth Weld Resdual Stress Greg Thorwald, Ph.D. Ted L. Anderson, Ph.D. Structural Relablty Technology, Boulder, CO Abstract Materals contanng flaws lke nclusons

More information

Solutions to Programming Assignment Five Interpolation and Numerical Differentiation

Solutions to Programming Assignment Five Interpolation and Numerical Differentiation College of Engneerng and Coputer Scence Mechancal Engneerng Departent Mechancal Engneerng 309 Nuercal Analyss of Engneerng Systes Sprng 04 Nuber: 537 Instructor: Larry Caretto Solutons to Prograng Assgnent

More information

Classification / Regression Support Vector Machines

Classification / Regression Support Vector Machines Classfcaton / Regresson Support Vector Machnes Jeff Howbert Introducton to Machne Learnng Wnter 04 Topcs SVM classfers for lnearly separable classes SVM classfers for non-lnearly separable classes SVM

More information

Machine Learning. Support Vector Machines. (contains material adapted from talks by Constantin F. Aliferis & Ioannis Tsamardinos, and Martin Law)

Machine Learning. Support Vector Machines. (contains material adapted from talks by Constantin F. Aliferis & Ioannis Tsamardinos, and Martin Law) Machne Learnng Support Vector Machnes (contans materal adapted from talks by Constantn F. Alfers & Ioanns Tsamardnos, and Martn Law) Bryan Pardo, Machne Learnng: EECS 349 Fall 2014 Support Vector Machnes

More information

Module Management Tool in Software Development Organizations

Module Management Tool in Software Development Organizations Journal of Computer Scence (5): 8-, 7 ISSN 59-66 7 Scence Publcatons Management Tool n Software Development Organzatons Ahmad A. Al-Rababah and Mohammad A. Al-Rababah Faculty of IT, Al-Ahlyyah Amman Unversty,

More information

Intra-Parametric Analysis of a Fuzzy MOLP

Intra-Parametric Analysis of a Fuzzy MOLP Intra-Parametrc Analyss of a Fuzzy MOLP a MIAO-LING WANG a Department of Industral Engneerng and Management a Mnghsn Insttute of Technology and Hsnchu Tawan, ROC b HSIAO-FAN WANG b Insttute of Industral

More information

NETWORKS of dynamical systems appear in a variety of

NETWORKS of dynamical systems appear in a variety of Necessary and Suffcent Topologcal Condtons for Identfablty of Dynamcal Networks Henk J. van Waarde, Petro Tes, and M. Kanat Camlbel arxv:807.09v [math.oc] 2 Jul 208 Abstract Ths paper deals wth dynamcal

More information

A Topology-aware Random Walk

A Topology-aware Random Walk A Topology-aware Random Walk Inkwan Yu, Rchard Newman Dept. of CISE, Unversty of Florda, Ganesvlle, Florda, USA Abstract When a graph can be decomposed nto clusters of well connected subgraphs, t s possble

More information

Structure from Motion

Structure from Motion Structure from Moton Structure from Moton For now, statc scene and movng camera Equvalentl, rgdl movng scene and statc camera Lmtng case of stereo wth man cameras Lmtng case of multvew camera calbraton

More information

A SYSTOLIC APPROACH TO LOOP PARTITIONING AND MAPPING INTO FIXED SIZE DISTRIBUTED MEMORY ARCHITECTURES

A SYSTOLIC APPROACH TO LOOP PARTITIONING AND MAPPING INTO FIXED SIZE DISTRIBUTED MEMORY ARCHITECTURES A SYSOLIC APPROACH O LOOP PARIIONING AND MAPPING INO FIXED SIZE DISRIBUED MEMORY ARCHIECURES Ioanns Drosts, Nektaros Kozrs, George Papakonstantnou and Panayots sanakas Natonal echncal Unversty of Athens

More information

Angle-Independent 3D Reconstruction. Ji Zhang Mireille Boutin Daniel Aliaga

Angle-Independent 3D Reconstruction. Ji Zhang Mireille Boutin Daniel Aliaga Angle-Independent 3D Reconstructon J Zhang Mrelle Boutn Danel Alaga Goal: Structure from Moton To reconstruct the 3D geometry of a scene from a set of pctures (e.g. a move of the scene pont reconstructon

More information

LLVM passes and Intro to Loop Transformation Frameworks

LLVM passes and Intro to Loop Transformation Frameworks LLVM passes and Intro to Loop Transformaton Frameworks Announcements Ths class s recorded and wll be n D2L panapto. No quz Monday after sprng break. Wll be dong md-semester class feedback. Today LLVM passes

More information

CE 221 Data Structures and Algorithms

CE 221 Data Structures and Algorithms CE 1 ata Structures and Algorthms Chapter 4: Trees BST Text: Read Wess, 4.3 Izmr Unversty of Economcs 1 The Search Tree AT Bnary Search Trees An mportant applcaton of bnary trees s n searchng. Let us assume

More information

Quality Improvement Algorithm for Tetrahedral Mesh Based on Optimal Delaunay Triangulation

Quality Improvement Algorithm for Tetrahedral Mesh Based on Optimal Delaunay Triangulation Intellgent Informaton Management, 013, 5, 191-195 Publshed Onlne November 013 (http://www.scrp.org/journal/m) http://dx.do.org/10.36/m.013.5601 Qualty Improvement Algorthm for Tetrahedral Mesh Based on

More information

On the diameter of random planar graphs

On the diameter of random planar graphs On the dameter of random planar graphs Gullaume Chapuy, CNRS & LIAFA, Pars jont work wth Érc Fusy, Pars, Omer Gménez, ex-barcelona, Marc Noy, Barcelona. Probablty and Graphs, Eurandom, Endhoven, 04. Planar

More information

A New Approach For the Ranking of Fuzzy Sets With Different Heights

A New Approach For the Ranking of Fuzzy Sets With Different Heights New pproach For the ankng of Fuzzy Sets Wth Dfferent Heghts Pushpnder Sngh School of Mathematcs Computer pplcatons Thapar Unversty, Patala-7 00 Inda pushpndersnl@gmalcom STCT ankng of fuzzy sets plays

More information

GSLM Operations Research II Fall 13/14

GSLM Operations Research II Fall 13/14 GSLM 58 Operatons Research II Fall /4 6. Separable Programmng Consder a general NLP mn f(x) s.t. g j (x) b j j =. m. Defnton 6.. The NLP s a separable program f ts objectve functon and all constrants are

More information

Accessibility Analysis for the Automatic Contact and Non-contact Inspection on Coordinate Measuring Machines

Accessibility Analysis for the Automatic Contact and Non-contact Inspection on Coordinate Measuring Machines Proceedngs of the World Congress on Engneerng 008 Vol I Accessblty Analyss for the Automatc Contact and Non-contact Inspecton on Coordnate Measurng Machnes B. J. Álvarez, P. Fernández, J. C. Rco and G.

More information

Recognizing Faces. Outline

Recognizing Faces. Outline Recognzng Faces Drk Colbry Outlne Introducton and Motvaton Defnng a feature vector Prncpal Component Analyss Lnear Dscrmnate Analyss !"" #$""% http://www.nfotech.oulu.f/annual/2004 + &'()*) '+)* 2 ! &

More information

Concurrent Apriori Data Mining Algorithms

Concurrent Apriori Data Mining Algorithms Concurrent Apror Data Mnng Algorthms Vassl Halatchev Department of Electrcal Engneerng and Computer Scence York Unversty, Toronto October 8, 2015 Outlne Why t s mportant Introducton to Assocaton Rule Mnng

More information

Assignment # 2. Farrukh Jabeen Algorithms 510 Assignment #2 Due Date: June 15, 2009.

Assignment # 2. Farrukh Jabeen Algorithms 510 Assignment #2 Due Date: June 15, 2009. Farrukh Jabeen Algorthms 51 Assgnment #2 Due Date: June 15, 29. Assgnment # 2 Chapter 3 Dscrete Fourer Transforms Implement the FFT for the DFT. Descrbed n sectons 3.1 and 3.2. Delverables: 1. Concse descrpton

More information

Optimization of Local Routing for Connected Nodes with Single Output Ports - Part I: Theory

Optimization of Local Routing for Connected Nodes with Single Output Ports - Part I: Theory U J.T. (: 33- (pr. 0 Optmzaton of Local Routng for Connected odes wth Sngle Output Ports - Part I: Theory Dobr tanassov Batovsk Faculty of Scence and Technology ssumpton Unversty Bangkok Thaland E-mal:

More information

Exercises (Part 4) Introduction to R UCLA/CCPR. John Fox, February 2005

Exercises (Part 4) Introduction to R UCLA/CCPR. John Fox, February 2005 Exercses (Part 4) Introducton to R UCLA/CCPR John Fox, February 2005 1. A challengng problem: Iterated weghted least squares (IWLS) s a standard method of fttng generalzed lnear models to data. As descrbed

More information

Face Recognition Based on SVM and 2DPCA

Face Recognition Based on SVM and 2DPCA Vol. 4, o. 3, September, 2011 Face Recognton Based on SVM and 2DPCA Tha Hoang Le, Len Bu Faculty of Informaton Technology, HCMC Unversty of Scence Faculty of Informaton Scences and Engneerng, Unversty

More information

What are the camera parameters? Where are the light sources? What is the mapping from radiance to pixel color? Want to solve for 3D geometry

What are the camera parameters? Where are the light sources? What is the mapping from radiance to pixel color? Want to solve for 3D geometry Today: Calbraton What are the camera parameters? Where are the lght sources? What s the mappng from radance to pel color? Why Calbrate? Want to solve for D geometry Alternatve approach Solve for D shape

More information

Routing in Degree-constrained FSO Mesh Networks

Routing in Degree-constrained FSO Mesh Networks Internatonal Journal of Hybrd Informaton Technology Vol., No., Aprl, 009 Routng n Degree-constraned FSO Mesh Networks Zpng Hu, Pramode Verma, and James Sluss Jr. School of Electrcal & Computer Engneerng

More information

Transaction-Consistent Global Checkpoints in a Distributed Database System

Transaction-Consistent Global Checkpoints in a Distributed Database System Proceedngs of the World Congress on Engneerng 2008 Vol I Transacton-Consstent Global Checkponts n a Dstrbuted Database System Jang Wu, D. Manvannan and Bhavan Thurasngham Abstract Checkpontng and rollback

More information

GLOBAL REGISTRATION OF NON STATIC 3D LIDAR POINT CLOUDS: SVD FACTORISATION AND ROBUST GPA METHODS

GLOBAL REGISTRATION OF NON STATIC 3D LIDAR POINT CLOUDS: SVD FACTORISATION AND ROBUST GPA METHODS GLOBAL REGISRAION OF NON SAIC 3D LIDAR POIN CLOUDS: SVD FACORISAION AND ROBUS GPA EHODS Fabo Croslla*, Alberto Benat Unversty of Udne, Dp d Georsorse e errtoro, Va Cotonfco 4, I-33 UDINE (Italy) fabo.croslla@unud.t,

More information

A Network Bandwidth Computation Technique for IP Storage with QoS Guarantees

A Network Bandwidth Computation Technique for IP Storage with QoS Guarantees A Network Bandwdth Computaton Technque for IP Storage wth QoS Guarantees Young Jn Nam 1, Junkl Ryu 1, Chank Park 1, and Jong Suk Ahn 2 1 Department of Computer Scence and Engneerng Pohang Unversty of Scence

More information

Chapter 4. Non-Uniform Offsetting and Hollowing by Using Biarcs Fitting for Rapid Prototyping Processes

Chapter 4. Non-Uniform Offsetting and Hollowing by Using Biarcs Fitting for Rapid Prototyping Processes Chapter 4 Non-Unform Offsettng and Hollowng by Usng Barcs Fttng for Rapd Prototypng Processes Ths chapter presents a new method of Non-Unform offsettng and usng barc fttngs to hollow out sold objects or

More information

Harmonic Coordinates for Character Articulation PIXAR

Harmonic Coordinates for Character Articulation PIXAR Harmonc Coordnates for Character Artculaton PIXAR Pushkar Josh Mark Meyer Tony DeRose Bran Green Tom Sanock We have a complex source mesh nsde of a smpler cage mesh We want vertex deformatons appled to

More information

Wavefront Reconstructor

Wavefront Reconstructor A Dstrbuted Smplex B-Splne Based Wavefront Reconstructor Coen de Vsser and Mchel Verhaegen 14-12-201212 2012 Delft Unversty of Technology Contents Introducton Wavefront reconstructon usng Smplex B-Splnes

More information