Measurement Indices of Positional Uncertainty for Plane Line Segments Based on the ε
|
|
- Bridget Summers
- 5 years ago
- Views:
Transcription
1 Proceedngs of the 8th Internatonal Smposum on Spatal ccurac ssessment n Natural Resources and Envronmental Scences Shangha, P R Chna, June 5-7, 008, pp 9-5 Measurement Indces of Postonal Uncertant for Plane Lne Segments Based on the ε Model Guoqn Zhang and Changqng Zhu Informaton Engneerng Unverst, Zhengzhou 45005, Chna Mnstr of Educaton Ke Laborator of VGE, Nanjng 0046, Chna bstract Frstl, eght cases of the random lne segments e dscussed Secondl, to the eght estng cases of lne segment, the analtc epressons of the error band for the ε uncertant model of lne segment e deduced, the pameter equatons of the error band bound e gotten, and t s proved that the bound of the error band s contnuous Thrdl, the average error band wdth and the algebrac epressons of the uncertant regon ea bounded b error band e calculated Fnall, the vsual graphcs of the error band e drawn wth analtc epresson of the error band b eamples Thus, three ndees e gven to measure the precson of the lne uncertant: the average error band wdth, the uncertant regon ea and the vsual graphcs Kewords: plane lne, uncertant, ε model, error band Introducton Spatal data s one of the fundamental pts of GIS The qualt of spatal data drectl determnes the ftnessfor-use of GIS and affects the results of GIS applcatons Therefore, accurac analss of spatal data s [,] regded as one of the fundamental theoretcal resech b ssues nternatonall Pont, lne segment and plane segment e the fundamental elements of vector spatal data So, resech on uncertant of pont, lne segment and plane segment s the man resech n the uncertant of spatal data Especall the resech on lne segment s mportant n GIS, because lne segment s not onl the bass of the uncertant resech on plane segments but also the basc element n overla analss and buffer analss There e man studes for the error band model of lne segment Perkal buld ε band model that s the strp band based on the buffer of lne segment wth constant ε Usng the ε band model, Blakemore descrbed the spatal uncertant of lne segment Sh et al developed a method to buld a generalzed error model(g-band) that descrbes the postonal uncertant of lne segment G-band s composed of the envelop comng from a group of error ellpses and the pt error ellpses of the etreme ponts The analtc epresson of G-band s comple Based on above models, Lu et al descrbed a general ε model for the postonal uncertant of lne segments Zhu et al proved the geometrcal chacter of the error band of the ε model based on algebrac method For theε model, the wdth of error band s represented b the root mean sque error n normal drecton of the lne, and the error band s composed of half of the error crcle at the etreme pont In ths paper, the ε model s studed further Frstl, eght cases of the random lne segment estng e dscussed Secondl, the analtc epresson of error band bound lne for the uncertant ε model of lne segment for ts eght cases s deduced Thrdl, the average error band wdth and the algebrac epressons of the uncertant regon ea bounded b error band e calculated wth the analtc epresson Fnall, the vsual graphcs of the error band e drawn wth analtc epresson of the error band b eamples Thus, three ndees e gven to measure the precson of the lne uncertant: the average error band wdth, the uncertant regon ea and the vsual graphcs The uncertant metrcs ndees can make sure the relablt of the spatal analss and the applcaton n GIS So, the users can know the sze the ISBN: , ISBN3:
2 dstrbuton and the spatal structure of the lne segment postonal uncertant drectl, and can understand and use the GIS product better The Error Band naltc Epresson of The ε Model for Lne Segment Uncertant The error band of theε model for lne segment Suppose Z Z be a lne segment and the coordnates of the endponts e Z (, ) and Z (, ) respectvel (as Fgure shows) The vance and co-vance matr of the lne segment e represented as the followng respectvel [] : D =, D =, D = Suppose θ s the angle between the lne Z Z and -as It s known easl that θ = ctan( ( ) ( )) and θ Suppose Z (, ) be an pont at the lne segment Z Z Then there e the followng relatons among the coordnates of Z, Z and Z [] : = ( r) r () = ( r) r where r = s s, s s the dstance of Z to the end pont Z, and s s the length of the lne segment Z Z It s obvous that 0 r Known from reference [], for theε model, the wdth of error band s represented b the mean sque error at the pont Z n normal drecton of the lne, and the error band s composed of pt error crcles at the etreme ponts (as Fgure shows) In order to get the mean sque error n normal drecton of the lne, the orgnal coordnate sstem O s rotated θ antclockwse about the coordnate orgn pont O Then the new coordnate sstem O s obtaned, and n the new coordnate sstem, O as s n a accordance wth lne segment Z Z B the co-vance propagaton rule, the vance and co-vance matr of the pont Z n the new coordnate sstem O can be obtaned 0 Fg : Error band of a lne segment From reference [], t s known that the error band wdth epresson of s as the followng: where a = s the functon of the pameter r, and the = br c (), b = ( ), c = Z θ B Known from epresson [], when the error of the end ponts s determned, for theε model, the wdth of error band at an pont Z on the lne s related to the pameter r onl Therefore, the error band can be epressed n the functon about the pameter r ( 0 r ) The error band analtc epresson of the ε model for lne segment uncertant Defnton : When one s walkng from the frst etreme pont to the after etreme pont along the lne segment, the error band bound lne located at the left s named Left Bound Lne, the error band C Z D
3 bound lne located at the rght s named Rght Bound Lne, half of the error crcle at the frst etreme pont s named Left Error Semcrcle, and half of the error crcle at the after etreme pont s named Rght Error Semcrcle From the defnton of the ε model of lne segment uncertant and defnton, t s known easl that the error band bound lne s composed of 4 pts: left bound lne = f ( ), rght bound lne = f ( ), left error semcrcle = f 3 ( ) and rght error semcrcle = f 4 ( ) Resech shows that there e 8 cases of the random lne segment: () <, < ;() >, < ;(3) <, > ;(4) >, > ;(5) =, < ; (6) =, > ;(7) <, = ;(8) >, = The analtc epresson of the error band bound lne wll be dscussed n the followng sectons to the 8 cases of the random lne segment for the ε model The analtc epresson of the error band bound lne when Frstl, the analtc epresson of the error band bound lne for the ε model of lne segment s dscussed when < and <, shown as Fgure () f P Z Q Z f () O θ Z Fg : The bound lne of the error band when < and < ( ⅰ) The analtc epresson of the left bound lne = f ( ) Suppose P(, ) s an pont at the left bound lne = f ( ) Draw a lne through the pont P perpendcul to the lne segment Z Z, and the perpendcul foot s Z (, ) Suppose Z PQ = θ It s known from the defnton of the error band that PZ = So we have PQ = = cos θ, QZ = = snθ From formula (), (), and the formula mentoned above, the coordnate epresson of an pont P (, ) at the left bound lne s obtaned: = cosθ = ( r) r f( ) = snθ = ( r) r br c cosθ br c snθ (0 r ) θ and a, b, c e related to the coordnates and the vance-covance of the etreme ponts, that s, the e constant So the coordnate of an pont P (, ) at the left bound lne s the functon about the pameter r Therefore, the pameter equaton of the left bound lne about r can be get, where the range of r s ( 0,) (ⅱ) The analtc epresson of the rght bound lne = f ( ) Smll, the analtc epresson of the rght bound lne = f ( ) can be obtaned: = cosθ = ( r) r f( ) = snθ = ( r) r br c cosθ br c snθ (ⅲ) The analtc epresson of the left error semcrcle = f ( ) 3 (0 r ) (3) (4)
4 It s known that the center of the error crcle at the frst etreme pont Z s Z and the radus s The left error semcrcle can be got b cuttng the error crcle through the lne D whch perpendcul to the lne segment Z Z So, the pameter equaton of the left error semcrcle s : = sn t 3 f3( ) ( θ t θ ) (5) = cost (ⅳ) The analtc epresson of the rght error semcrcle = f ( ) Smll, the pameter equaton of the rght semerror crcle s: = sn t f4( ) = cost 4 ( θ t θ In the same wa, we have the analtc epresson of the error band bound lne when >, <, =, <, <, = or >, =, and the analtc epresson of the error band bound lne s the same as the analtc epresson when <, < To conclude, the analtc epresson of the error band bound lne when s formula (3)-(6) The analtc epresson of the error band bound lne when > Same as the dervaton process n the secton, we can get the analtc epresson of the error band bound lne when <, >, >, > or =, > (That s > ) The analtc epresson of the left bound lne = f ( ) : = cosθ = ( r) r f( ) = snθ = ( r) r The analtc epresson of the rght bound lne = f ( ) : = cosθ = ( r) r f( ) = snθ = ( r) r The analtc epresson of the left error semcrcle = f 3 ( ) : = sn t f3( ) = cost ) br c cosθ br c snθ br c cosθ br c snθ ( θ t θ The analtc epresson of the rght error semcrcle = f 4 ( ) : = sn t f4( t) = cost ) 3 ( θ t θ ) (0 r ) (0 r ) Known from the analtc epresson of the error band bound lne (3)-(0), the equaton that an pont at the error band bound lne satsfes s determned b the coordnaton and ts vance-covance of the lne segment, s endponts Z, ) and Z, ), that s, the error band s determned b the relevant ( ( nformaton of the lne segment, s endponts Vsualzaton model can be drawn easl wth the analtc epresson of the error band bound lne 3 The contnut of the error band bound lne for the ε model of lne segment Known from secton and the defnton of theε model, the functon of the error band bound lne s composed of 4 pecewse functons: the left bound lne = f ( ), the rght bound lne = f ( ), the left error semcrcle = f 3 ( ) and the rght error semcrcle = f 4 ( ) From formula (3)-(0), the 4 pecewse functons s contnuous n the pecewse nterval, so, to resech on the contnut of the error band (6) (7) (8) (9) (0)
5 bound lne, the stud on the contnut at the pecewse ponts s enough That s, the contnut at the pecewse ponts B C D s need to studed (known from fgure ) When, calculated from formula (5), the pameter t = θ at the pont n the left error semcrcle and the coordnaton of the pont s: sn( ) = θ = cosθ () = cos( θ ) = snθ Known from the contnut of the crcle equaton, the functon of the error band bound lne s leftcontnuous at the pont Now we stud the rght-contnuous at the pont From formula (3), judgng the rght contnut of functon s to calculatng lmt : lm = lm[( r) = = = r br c cosθ ] c cosθ cosθ r 0 r 0 () lm = lm[( r) r br c snθ ] = c snθ = snθ = r 0 r 0 So, the functon s rght-contnuous at the pont Therefore, the functon s contnuous at the pont when It s the same when > Provng b the same method, the functon s contnuous at the ponts B C D Therefore, the error band bound lne for the ε model of lne segment s a contnuous closed curve 3 Measurement ndees of postonal uncertant for lne segment based on ε model Now the analtc epresson of the error band bound lne for the ε uncertant model of lne segment for ts eght cases have been deduced Wth the analtc epresson of the error band bound lne, we can draw the vsual graph and calculate the average error band wdth and eas of the error band Thus, three ndees e gven to measure the precson of the lne uncertant: the vsual graph, the average error band wdth and the uncertant regon ea The uncertant metrcs ndees can make sure the relablt of the spatal analss and the applcaton n GIS So, the users can know the sze the dstrbuton and the spatal structure of the lne segment postonal uncertant drectl, and can understand and use the GIS product better 3 The vsual graphcs of the error band for the ε model of lne segment Vsualzaton s a knd of technolog wa, through whch some data can be converted nto graphcs and new knowledge can be gotten Wth the analtc epresson of the error band bound lne defned n secton b formula (5)-(), we can draw the vsual graphcs of the uncertant for lne segment through programmng The vsual graph can epress the error band well 3 The algebrac epresson of average error band wdth s The average error band wdth ε s calculated b the followng formula: ε s = dr = 0 0 s a b br cdr = 4a a b c b 4a ε 4ac b c 3 8 a a b a( a b c) ln b ac (3) 33 The algebrac epresson of the ea of the uncertant regon bounded b error band Obvousl, when the endponts nformaton of lne segment s certant, the uncertant regon bounded b error band s bgger and the uncertant of the lne segment s more So t s sgnfcant to calculate the ea of the uncertant regon bounded b error band and make t a matr to measure the postonal uncertant of lne segment Known from the defnton of the ε model, t s composed of 3 pts: two error semcrcles at the endponts and the mddle regon between the left bound lne and the rght bound lne, so the ea of the error band s the ea sum of, 3 and and 3 denote the ea of the left error semcrcle and the rght error semcrcle respectvel, and denote the ea of the mddle regon between the left bound lne and the rght bound lne We have the followng formulas: 3
6 = l ε s a b = l a =, 3 =, (4) b a b c a where l s the length of the lne segment 4ac b c 3 4 a a b a( a b c) ln b ac, (5) From formulas (4) and (5), the algebrac epresson of the ea of the uncertant regon bounded b error band s obtaned as followng: = (6) The uncertant regon ea of lne segment s related to the etreme pont coordnates and ther vance-covance onl 4 Eamples and analss Now lne segments s dscussed as eamples, and ther coordnates e Z (500,00), Z (550,30) ; Z (50,80), Z (30,30) Ther vance-covance e gven n tab Lne segment Tab Orgnal data of the vance and co-vance of the lne segments Wth the analtc epresson (3)-(0), we can draw the vsual graph of lne segment and b programmng Graph 3-3 show results Fg 3: The error band when < and < Fg 3: The error band when < and > The ea of error band for lne segment and s : and It s shown n the vsual graph that the error band bound lne s a contnuous and closed curve From the vsual graph, the average error band wdth and the ea of error band, t s shown that the uncertant regon ea of lne segment s bgger when the error s bgger, the uncertant regon ea of lne segment s smaller when the error s smaller, and error band wth the shape lger at etreme ponts and smaller at mddle The result has been proofed n reference [4] 5 Concluson Error band uncertant ε model for lne segment can represent the error of lne segment Measurement ndees of postonal uncertant for lne segment based on ε model e studed n ths paper Eght cases of the random lne segment estng e dscussed frstl, then the analtc epresson of the error band bound lne for the uncertant ε model of lne segments for ts eght cases s deduced The functon of the error band bound lne s composed of 4 pecewse functons 4
7 It s proofed that the error band bound lne for the uncertant ε model of lne segments s a contnuous and closed curve 3 Wth the analtc epresson of the error band bound lne, the vsual graph of uncertant for lne segment can be drawn and the average error band wdth and the algebrac epressons of the uncertant regon ea bounded b error band can be calculated Thus, three ndees e gven to measure the precson of the lne uncertant: the vsual graph, the average error band wdth and the uncertant regon ea The uncertant metrcs ndees can make sure the relablt of the spatal analss and the applcaton n GIS So, the users can know the sze the dstrbuton and the spatal structure of the lne segment postonal uncertant drectl, and can understand and use the GIS product better 6 cknowledgement The work s supported b the fund from NSFC (Project No: ) 7 References [] Lu DJ, Sh WZ, Tong XH, Sun HC, ccurac nalss and Qualt Control of Spatal Data n GIS Shangha: Shangha Press of Scence and Technolog, 999 [] Sh WZ, Prncple of Modelng Uncertantes n Spatal Data and nalss Bejng: Press of Scence, 005 [3] Lu DJ, Hua H, More Dscusson to Modelng Uncertant n Lne Prmtves n GIS cta Geodatca et Ctographca Snca, 998, 7: [4] Zhu CQ, Zhang GQ, Sh WZ lgebrac Resech on Geometrcal Chacterstcof error Band for D Lne Segment Uncertant ε Model cta Geodatca et Ctographca Snca, 007, 36: [5] Zhang GQ, Zhu CQ, Zhou B, etc Uncertant ε Model of Spatal Crcul Curve eeatures n GIS cta Geodatca et Ctographca Snca, 005, 34: [6] LIU WB, DI HL, The naltc epresson of geometrc fgure on plan lnes error band cta Geodatca et Ctographca Snca, 998, 7: 3~37 [7] Lu C, Zhan Y, Probablt nalss of error Band of Plane Lne Segments n GIS Journal of Tongj Unverst, 007, 35: [8] Sh WZ, Lu WB, Stochastc Process-Based Model for Postonal error of Lne Segments n GIS Internatonal Journal of Geographcal Informaton Scence, 000, 4(000),
The Quadratic Trigonometric Bézier Curve with Single Shape Parameter
J. Basc. Appl. Sc. Res., (3541-546, 01 01, TextRoad Publcaton ISSN 090-4304 Journal of Basc and Appled Scentfc Research www.textroad.com The Quadratc Trgonometrc Bézer Curve wth Sngle Shape Parameter Uzma
More informationPART 8. Partial Differential Equations PDEs
he Islamc Unverst of Gaza Facult of Engneerng Cvl Engneerng Department Numercal Analss ECIV 3306 PAR 8 Partal Dfferental Equatons PDEs Chapter 9; Fnte Dfference: Ellptc Equatons Assocate Prof. Mazen Abualtaef
More informationCHAPTER-5 INFORMATION MEASURE OF FUZZY MATRIX AND FUZZY BINARY RELATION
CAPTER- INFORMATION MEASURE OF FUZZY MATRI AN FUZZY BINARY RELATION Introducton The basc concept of the fuzz matr theor s ver smple and can be appled to socal and natural stuatons A branch of fuzz matr
More informationGrid Generation around a Cylinder by Complex Potential Functions
Research Journal of Appled Scences, Engneerng and Technolog 4(): 53-535, 0 ISSN: 040-7467 Mawell Scentfc Organzaton, 0 Submtted: December 0, 0 Accepted: Januar, 0 Publshed: June 0, 0 Grd Generaton around
More informationAvailable online Journal of Chemical and Pharmaceutical Research, 2014, 6(5): Research Article
Avalable onlne www.ocpr.com Journal of Chemcal and Pharmaceutcal Research 4 6(5):7-76 Research Artcle ISSN : 975-7384 CODEN(USA) : JCPRC5 Stud on relatonshp between nvestment n scence and technolog and
More informationApplication to Plane (rigid) frame structure
Advanced Computatonal echancs 18 Chapter 4 Applcaton to Plane rgd frame structure 1. Dscusson on degrees of freedom In case of truss structures, t was enough that the element force equaton provdes onl
More informationCHAPTER 4. Vector Spaces
man 2007/2/16 page 234 CHAPTER 4 Vector Spaces To crtcze mathematcs for ts abstracton s to mss the pont entrel. Abstracton s what makes mathematcs work. Ian Stewart The man am of ths tet s to stud lnear
More informationSection 8.3 Polar Form of Complex Numbers
80 Chapter 8 Secton 8 Polar Form of Complex Numbers From prevous classes, you may have encountered magnary numbers the square roots of negatve numbers and, more generally, complex numbers whch are the
More informationCHAPTER 4 MAX-MIN AVERAGE COMPOSITION METHOD FOR DECISION MAKING USING INTUITIONISTIC FUZZY SETS
56 CHAPER 4 MAX-MIN AVERAGE COMPOSIION MEHOD FOR DECISION MAKING USING INUIIONISIC FUZZY SES 4.1 INRODUCION Intutonstc fuzz max-mn average composton method s proposed to construct the decson makng for
More informationMore metrics on cartesian products
More metrcs on cartesan products If (X, d ) are metrc spaces for 1 n, then n Secton II4 of the lecture notes we defned three metrcs on X whose underlyng topologes are the product topology The purpose of
More informationThe Order Relation and Trace Inequalities for. Hermitian Operators
Internatonal Mathematcal Forum, Vol 3, 08, no, 507-57 HIKARI Ltd, wwwm-hkarcom https://doorg/0988/mf088055 The Order Relaton and Trace Inequaltes for Hermtan Operators Y Huang School of Informaton Scence
More informationError Analysis of Sensor Geometric Factor for the Multi-node Cooperative Localization Accuracy
INERNAIONAL JOURNAL OF CIRCUIS, SYSEMS AND SIGNAL PROCESSING Volume, 7 Error Analss of Sensor Geometrc Factor for the Mult-node Cooperatve Localzaton Accurac Yao Fan Abstract he localzaton accurac s ver
More informationA REVIEW OF ERROR ANALYSIS
A REVIEW OF ERROR AALYI EEP Laborator EVE-4860 / MAE-4370 Updated 006 Error Analss In the laborator we measure phscal uanttes. All measurements are subject to some uncertantes. Error analss s the stud
More informationMTH 263 Practice Test #1 Spring 1999
Pat Ross MTH 6 Practce Test # Sprng 999 Name. Fnd the area of the regon bounded by the graph r =acos (θ). Observe: Ths s a crcle of radus a, for r =acos (θ) r =a ³ x r r =ax x + y =ax x ax + y =0 x ax
More informationχ x B E (c) Figure 2.1.1: (a) a material particle in a body, (b) a place in space, (c) a configuration of the body
Secton.. Moton.. The Materal Body and Moton hyscal materals n the real world are modeled usng an abstract mathematcal entty called a body. Ths body conssts of an nfnte number of materal partcles. Shown
More informationInternational Journal of Mathematical Archive-3(3), 2012, Page: Available online through ISSN
Internatonal Journal of Mathematcal Archve-3(3), 2012, Page: 1136-1140 Avalable onlne through www.ma.nfo ISSN 2229 5046 ARITHMETIC OPERATIONS OF FOCAL ELEMENTS AND THEIR CORRESPONDING BASIC PROBABILITY
More informationUnit 5: Quadratic Equations & Functions
Date Perod Unt 5: Quadratc Equatons & Functons DAY TOPIC 1 Modelng Data wth Quadratc Functons Factorng Quadratc Epressons 3 Solvng Quadratc Equatons 4 Comple Numbers Smplfcaton, Addton/Subtracton & Multplcaton
More informationAn Application of Fuzzy Hypotheses Testing in Radar Detection
Proceedngs of the th WSES Internatonal Conference on FUZZY SYSEMS n pplcaton of Fuy Hypotheses estng n Radar Detecton.K.ELSHERIF, F.M.BBDY, G.M.BDELHMID Department of Mathematcs Mltary echncal Collage
More informationCubic Trigonometric Rational Wat Bezier Curves
Cubc Trgonometrc Ratonal Wat Bezer Curves Urvash Mshra Department of Mathematcs Mata Gujr Mahla Mahavdyalaya Jabalpur Madhya Pradesh Inda Abstract- A new knd of Ratonal cubc Bézer bass functon by the blendng
More informationThe Algorithm of Simplex Integration in Three-Dimension and
The Algorthm of Smple Integraton n Three-Dmenson and Its Characterstc Analss WU Yan-qang CHEN Guang-q JIANG Za-sen ZHANG Long LIU Xao-a ZHAO Jng The Algorthm of Smple Integraton n Three-Dmenson and Its
More informationChapter 8. Potential Energy and Conservation of Energy
Chapter 8 Potental Energy and Conservaton of Energy In ths chapter we wll ntroduce the followng concepts: Potental Energy Conservatve and non-conservatve forces Mechancal Energy Conservaton of Mechancal
More informationModule 14: THE INTEGRAL Exploring Calculus
Module 14: THE INTEGRAL Explorng Calculus Part I Approxmatons and the Defnte Integral It was known n the 1600s before the calculus was developed that the area of an rregularly shaped regon could be approxmated
More informationResearch Article Shape Preserving Interpolation using Rational Cubic Spline
Research Journal of Appled Scences, Engneerng and Technolog 8(2): 67-78, 4 DOI:.9026/rjaset.8.96 ISSN: 40-749; e-issn: 40-7467 4 Mawell Scentfc Publcaton Corp. Submtted: Januar, 4 Accepted: Februar, 4
More informationSCALARS AND VECTORS All physical quantities in engineering mechanics are measured using either scalars or vectors.
SCALARS AND ECTORS All phscal uanttes n engneerng mechancs are measured usng ether scalars or vectors. Scalar. A scalar s an postve or negatve phscal uantt that can be completel specfed b ts magntude.
More informationTHE SMOOTH INDENTATION OF A CYLINDRICAL INDENTOR AND ANGLE-PLY LAMINATES
THE SMOOTH INDENTATION OF A CYLINDRICAL INDENTOR AND ANGLE-PLY LAMINATES W. C. Lao Department of Cvl Engneerng, Feng Cha Unverst 00 Wen Hwa Rd, Tachung, Tawan SUMMARY: The ndentaton etween clndrcal ndentor
More informationDefinition. Measures of Dispersion. Measures of Dispersion. Definition. The Range. Measures of Dispersion 3/24/2014
Measures of Dsperson Defenton Range Interquartle Range Varance and Standard Devaton Defnton Measures of dsperson are descrptve statstcs that descrbe how smlar a set of scores are to each other The more
More informationThe Fundamental Theorem of Algebra. Objective To use the Fundamental Theorem of Algebra to solve polynomial equations with complex solutions
5-6 The Fundamental Theorem of Algebra Content Standards N.CN.7 Solve quadratc equatons wth real coeffcents that have comple solutons. N.CN.8 Etend polnomal denttes to the comple numbers. Also N.CN.9,
More informationModule 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur
Module 3 LOSSY IMAGE COMPRESSION SYSTEMS Verson ECE IIT, Kharagpur Lesson 6 Theory of Quantzaton Verson ECE IIT, Kharagpur Instructonal Objectves At the end of ths lesson, the students should be able to:
More informationKinematics in 2-Dimensions. Projectile Motion
Knematcs n -Dmensons Projectle Moton A medeval trebuchet b Kolderer, c1507 http://members.net.net.au/~rmne/ht/ht0.html#5 Readng Assgnment: Chapter 4, Sectons -6 Introducton: In medeval das, people had
More informationStatistical Inference. 2.3 Summary Statistics Measures of Center and Spread. parameters ( population characteristics )
Ismor Fscher, 8//008 Stat 54 / -8.3 Summary Statstcs Measures of Center and Spread Dstrbuton of dscrete contnuous POPULATION Random Varable, numercal True center =??? True spread =???? parameters ( populaton
More informationA New Scrambling Evaluation Scheme based on Spatial Distribution Entropy and Centroid Difference of Bit-plane
A New Scramblng Evaluaton Scheme based on Spatal Dstrbuton Entropy and Centrod Dfference of Bt-plane Lang Zhao *, Avshek Adhkar Kouch Sakura * * Graduate School of Informaton Scence and Electrcal Engneerng,
More informationWeek3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity
Week3, Chapter 4 Moton n Two Dmensons Lecture Quz A partcle confned to moton along the x axs moves wth constant acceleraton from x =.0 m to x = 8.0 m durng a 1-s tme nterval. The velocty of the partcle
More informationModule 2. Random Processes. Version 2 ECE IIT, Kharagpur
Module Random Processes Lesson 6 Functons of Random Varables After readng ths lesson, ou wll learn about cdf of functon of a random varable. Formula for determnng the pdf of a random varable. Let, X be
More informationSociété de Calcul Mathématique SA
Socété de Calcul Mathématque SA Outls d'ade à la décson Tools for decson help Probablstc Studes: Normalzng the Hstograms Bernard Beauzamy December, 202 I. General constructon of the hstogram Any probablstc
More information9. Complex Numbers. 1. Numbers revisited. 2. Imaginary number i: General form of complex numbers. 3. Manipulation of complex numbers
9. Comple Numbers. Numbers revsted. Imagnar number : General form of comple numbers 3. Manpulaton of comple numbers 4. The Argand dagram 5. The polar form for comple numbers 9.. Numbers revsted We saw
More informationExponential Type Product Estimator for Finite Population Mean with Information on Auxiliary Attribute
Avalable at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 193-9466 Vol. 10, Issue 1 (June 015), pp. 106-113 Applcatons and Appled Mathematcs: An Internatonal Journal (AAM) Exponental Tpe Product Estmator
More informationPhysics 5153 Classical Mechanics. Principle of Virtual Work-1
P. Guterrez 1 Introducton Physcs 5153 Classcal Mechancs Prncple of Vrtual Work The frst varatonal prncple we encounter n mechancs s the prncple of vrtual work. It establshes the equlbrum condton of a mechancal
More informationBinding energy of a Cooper pairs with non-zero center of mass momentum in d-wave superconductors
Bndng energ of a Cooper pars wth non-zero center of mass momentum n d-wave superconductors M.V. remn and I.. Lubn Kazan State Unverst Kremlevsaa 8 Kazan 420008 Russan Federaton -mal: gor606@rambler.ru
More informationAn Improved multiple fractal algorithm
Advanced Scence and Technology Letters Vol.31 (MulGraB 213), pp.184-188 http://dx.do.org/1.1427/astl.213.31.41 An Improved multple fractal algorthm Yun Ln, Xaochu Xu, Jnfeng Pang College of Informaton
More informationNumerical Methods. ME Mechanical Lab I. Mechanical Engineering ME Lab I
5 9 Mechancal Engneerng -.30 ME Lab I ME.30 Mechancal Lab I Numercal Methods Volt Sne Seres.5 0.5 SIN(X) 0 3 7 5 9 33 37 4 45 49 53 57 6 65 69 73 77 8 85 89 93 97 0-0.5 Normalzed Squared Functon - 0.07
More informationOrientation Model of Elite Education and Mass Education
Proceedngs of the 8th Internatonal Conference on Innovaton & Management 723 Orentaton Model of Elte Educaton and Mass Educaton Ye Peng Huanggang Normal Unversty, Huanggang, P.R.Chna, 438 (E-mal: yepeng@hgnc.edu.cn)
More informationCENTROID (AĞIRLIK MERKEZİ )
CENTOD (ĞLK MEKEZİ ) centrod s a geometrcal concept arsng from parallel forces. Tus, onl parallel forces possess a centrod. Centrod s tougt of as te pont were te wole wegt of a pscal od or sstem of partcles
More informationModeling curves. Graphs: y = ax+b, y = sin(x) Implicit ax + by + c = 0, x 2 +y 2 =r 2 Parametric:
Modelng curves Types of Curves Graphs: y = ax+b, y = sn(x) Implct ax + by + c = 0, x 2 +y 2 =r 2 Parametrc: x = ax + bxt x = cos t y = ay + byt y = snt Parametrc are the most common mplct are also used,
More informationVisualization of Data Subject to Positive Constraints
ISSN 746-7659 England UK Journal of Informaton and Computng Scence Vol. No. 6 pp. 49-6 Vsualzaton of Data Subect to Postve Constrants Malk Zawwar Hussan and Mara Hussan Department of Mathematcs Unverst
More informationOPTIMISATION. Introduction Single Variable Unconstrained Optimisation Multivariable Unconstrained Optimisation Linear Programming
OPTIMIATION Introducton ngle Varable Unconstraned Optmsaton Multvarable Unconstraned Optmsaton Lnear Programmng Chapter Optmsaton /. Introducton In an engneerng analss, sometmes etremtes, ether mnmum or
More informationOne Dimensional Axial Deformations
One Dmensonal al Deformatons In ths secton, a specfc smple geometr s consdered, that of a long and thn straght component loaded n such a wa that t deforms n the aal drecton onl. The -as s taken as the
More informationMathematical Preparations
1 Introducton Mathematcal Preparatons The theory of relatvty was developed to explan experments whch studed the propagaton of electromagnetc radaton n movng coordnate systems. Wthn expermental error the
More informationA new Approach for Solving Linear Ordinary Differential Equations
, ISSN 974-57X (Onlne), ISSN 974-5718 (Prnt), Vol. ; Issue No. 1; Year 14, Copyrght 13-14 by CESER PUBLICATIONS A new Approach for Solvng Lnear Ordnary Dfferental Equatons Fawz Abdelwahd Department of
More informationNon-linear Canonical Correlation Analysis Using a RBF Network
ESANN' proceedngs - European Smposum on Artfcal Neural Networks Bruges (Belgum), 4-6 Aprl, d-sde publ., ISBN -97--, pp. 57-5 Non-lnear Canoncal Correlaton Analss Usng a RBF Network Sukhbnder Kumar, Elane
More informationRigid body simulation
Rgd bod smulaton Rgd bod smulaton Once we consder an object wth spacal etent, partcle sstem smulaton s no longer suffcent Problems Problems Unconstraned sstem rotatonal moton torques and angular momentum
More informationAP Physics 1 & 2 Summer Assignment
AP Physcs 1 & 2 Summer Assgnment AP Physcs 1 requres an exceptonal profcency n algebra, trgonometry, and geometry. It was desgned by a select group of college professors and hgh school scence teachers
More informationSolutions to Homework 7, Mathematics 1. 1 x. (arccos x) (arccos x) 1
Solutons to Homework 7, Mathematcs 1 Problem 1: a Prove that arccos 1 1 for 1, 1. b* Startng from the defnton of the dervatve, prove that arccos + 1, arccos 1. Hnt: For arccos arccos π + 1, the defnton
More informationOn Tiling for Some Types of Manifolds. and their Folding
Appled Mathematcal Scences, Vol. 3, 009, no. 6, 75-84 On Tlng for Some Types of Manfolds and ther Foldng H. Rafat Mathematcs Department, Faculty of Scence Tanta Unversty, Tanta Egypt hshamrafat005@yahoo.com
More informationA new method of boundary treatment in Heat conduction problems with finite element method
Avalale onlne at www.scencedrect.com Proceda Engneerng 6 (11) 675 68 Frst Internatonal Smposum on Mne Safet Scence and Engneerng A new method of oundar treatment n Heat conducton prolems wth fnte element
More informationFuzzy Boundaries of Sample Selection Model
Proceedngs of the 9th WSES Internatonal Conference on ppled Mathematcs, Istanbul, Turkey, May 7-9, 006 (pp309-34) Fuzzy Boundares of Sample Selecton Model L. MUHMD SFIIH, NTON BDULBSH KMIL, M. T. BU OSMN
More informationCENTROID (AĞIRLIK MERKEZİ )
CENTOD (ĞLK MEKEZİ ) centrod s a geometrcal concept arsng from parallel forces. Tus, onl parallel forces possess a centrod. Centrod s tougt of as te pont were te wole wegt of a pscal od or sstem of partcles
More informationInvestigation of the Relationship between Diesel Fuel Properties and Emissions from Engines with Fuzzy Linear Regression
www.esc.org Internatonal Journal of Energ Scence (IJES) Volume 3 Issue 2, Aprl 2013 Investgaton of the Relatonshp between Desel Fuel Propertes and Emssons from Engnes wth Fuzz Lnear Regresson Yuanwang
More informationPHY224H1F/324H1S Notes on Error Analysis
PHY4HF/34HS otes on Error nalss Reerences: J.R. Talor: n Introducton to Error nalss: The Stud o Uncertantes n Phscs Measurements, nd ed., Unverst Scence ooks, 997 P.R. evngton, D.H. Robnson: Data Reducton
More informationPower law and dimension of the maximum value for belief distribution with the max Deng entropy
Power law and dmenson of the maxmum value for belef dstrbuton wth the max Deng entropy Bngy Kang a, a College of Informaton Engneerng, Northwest A&F Unversty, Yanglng, Shaanx, 712100, Chna. Abstract Deng
More informationInductance Calculation for Conductors of Arbitrary Shape
CRYO/02/028 Aprl 5, 2002 Inductance Calculaton for Conductors of Arbtrary Shape L. Bottura Dstrbuton: Internal Summary In ths note we descrbe a method for the numercal calculaton of nductances among conductors
More informationNumerical Solutions of a Generalized Nth Order Boundary Value Problems Using Power Series Approximation Method
Appled Mathematcs, 6, 7, 5-4 Publshed Onlne Jul 6 n ScRes. http://www.scrp.org/journal/am http://.do.org/.436/am.6.77 umercal Solutons of a Generalzed th Order Boundar Value Problems Usng Power Seres Approxmaton
More informationDEGREE REDUCTION OF BÉZIER CURVES USING CONSTRAINED CHEBYSHEV POLYNOMIALS OF THE SECOND KIND
ANZIAM J. 45(003), 195 05 DEGREE REDUCTION OF BÉZIER CURVES USING CONSTRAINED CHEBYSHEV POLYNOMIALS OF THE SECOND KIND YOUNG JOON AHN 1 (Receved 3 August, 001; revsed 7 June, 00) Abstract In ths paper
More informationNew Method for Solving Poisson Equation. on Irregular Domains
Appled Mathematcal Scences Vol. 6 01 no. 8 369 380 New Method for Solvng Posson Equaton on Irregular Domans J. Izadan and N. Karamooz Department of Mathematcs Facult of Scences Mashhad BranchIslamc Azad
More informationOperating conditions of a mine fan under conditions of variable resistance
Paper No. 11 ISMS 216 Operatng condtons of a mne fan under condtons of varable resstance Zhang Ynghua a, Chen L a, b, Huang Zhan a, *, Gao Yukun a a State Key Laboratory of Hgh-Effcent Mnng and Safety
More informationChapter 3 Differentiation and Integration
MEE07 Computer Modelng Technques n Engneerng Chapter Derentaton and Integraton Reerence: An Introducton to Numercal Computatons, nd edton, S. yakowtz and F. zdarovsky, Mawell/Macmllan, 990. Derentaton
More informationModule 3: Element Properties Lecture 1: Natural Coordinates
Module 3: Element Propertes Lecture : Natural Coordnates Natural coordnate system s bascally a local coordnate system whch allows the specfcaton of a pont wthn the element by a set of dmensonless numbers
More informationMath1110 (Spring 2009) Prelim 3 - Solutions
Math 1110 (Sprng 2009) Solutons to Prelm 3 (04/21/2009) 1 Queston 1. (16 ponts) Short answer. Math1110 (Sprng 2009) Prelm 3 - Solutons x a 1 (a) (4 ponts) Please evaluate lm, where a and b are postve numbers.
More informationColor Rendering Uncertainty
Australan Journal of Basc and Appled Scences 4(10): 4601-4608 010 ISSN 1991-8178 Color Renderng Uncertanty 1 A.el Bally M.M. El-Ganany 3 A. Al-amel 1 Physcs Department Photometry department- NIS Abstract:
More informationThe Jacobsthal and Jacobsthal-Lucas Numbers via Square Roots of Matrices
Internatonal Mathematcal Forum, Vol 11, 2016, no 11, 513-520 HIKARI Ltd, wwwm-hkarcom http://dxdoorg/1012988/mf20166442 The Jacobsthal and Jacobsthal-Lucas Numbers va Square Roots of Matrces Saadet Arslan
More informationFor all questions, answer choice E) NOTA" means none of the above answers is correct.
0 MA Natonal Conventon For all questons, answer choce " means none of the above answers s correct.. In calculus, one learns of functon representatons that are nfnte seres called power 3 4 5 seres. For
More informationkq r 2 2kQ 2kQ (A) (B) (C) (D)
PHYS 1202W MULTIPL CHOIC QUSTIONS QUIZ #1 Answer the followng multple choce questons on the bubble sheet. Choose the best answer, 5 pts each. MC1 An uncharged metal sphere wll (A) be repelled by a charged
More informationANALYSIS OF ELECTROMAGNETIC FIELD USING THE CONSTRAINED INTERPOLATION PROFILE METHOD PHÂN TÍCH TRƯỜNG ĐIỆN TỪ SỬ DỤNG PHƯƠNG PHÁP CIP
ANALYSIS OF ELECTROMAGNETIC FIELD USING THE CONSTRAINED INTERPOLATION PROFILE METHOD PHÂN TÍCH TRƯỜNG ĐIỆN TỪ SỬ DỤNG PHƯƠNG PHÁP CIP LÊ VŨ HƯNG Cao đẳng kỹ thuật quốc ga Kushro, Nhật Bản Kushro Natonal
More informationCHAPTER 10 ROTATIONAL MOTION
CHAPTER 0 ROTATONAL MOTON 0. ANGULAR VELOCTY Consder argd body rotates about a fxed axs through pont O n x-y plane as shown. Any partcle at pont P n ths rgd body rotates n a crcle of radus r about O. The
More informationAffine transformations and convexity
Affne transformatons and convexty The purpose of ths document s to prove some basc propertes of affne transformatons nvolvng convex sets. Here are a few onlne references for background nformaton: http://math.ucr.edu/
More informationComparative Studies of Law of Conservation of Energy. and Law Clusters of Conservation of Generalized Energy
Comparatve Studes of Law of Conservaton of Energy and Law Clusters of Conservaton of Generalzed Energy No.3 of Comparatve Physcs Seres Papers Fu Yuhua (CNOOC Research Insttute, E-mal:fuyh1945@sna.com)
More informationAPPENDIX 2 FITTING A STRAIGHT LINE TO OBSERVATIONS
Unversty of Oulu Student Laboratory n Physcs Laboratory Exercses n Physcs 1 1 APPEDIX FITTIG A STRAIGHT LIE TO OBSERVATIOS In the physcal measurements we often make a seres of measurements of the dependent
More informationResource Allocation and Decision Analysis (ECON 8010) Spring 2014 Foundations of Regression Analysis
Resource Allocaton and Decson Analss (ECON 800) Sprng 04 Foundatons of Regresson Analss Readng: Regresson Analss (ECON 800 Coursepak, Page 3) Defntons and Concepts: Regresson Analss statstcal technques
More informationACTM State Calculus Competition Saturday April 30, 2011
ACTM State Calculus Competton Saturday Aprl 30, 2011 ACTM State Calculus Competton Sprng 2011 Page 1 Instructons: For questons 1 through 25, mark the best answer choce on the answer sheet provde Afterward
More informationUncertainty as the Overlap of Alternate Conditional Distributions
Uncertanty as the Overlap of Alternate Condtonal Dstrbutons Olena Babak and Clayton V. Deutsch Centre for Computatonal Geostatstcs Department of Cvl & Envronmental Engneerng Unversty of Alberta An mportant
More informationElshaboury SM et al.; Sch. J. Phys. Math. Stat., 2015; Vol-2; Issue-2B (Mar-May); pp
Elshabour SM et al.; Sch. J. Phs. Math. Stat. 5; Vol-; Issue-B (Mar-Ma); pp-69-75 Scholars Journal of Phscs Mathematcs Statstcs Sch. J. Phs. Math. Stat. 5; (B):69-75 Scholars Academc Scentfc Publshers
More informationCOMPLEX NUMBERS AND QUADRATIC EQUATIONS
COMPLEX NUMBERS AND QUADRATIC EQUATIONS INTRODUCTION We know that x 0 for all x R e the square of a real number (whether postve, negatve or ero) s non-negatve Hence the equatons x, x, x + 7 0 etc are not
More informationStudy on Non-Linear Dynamic Characteristic of Vehicle. Suspension Rubber Component
Study on Non-Lnear Dynamc Characterstc of Vehcle Suspenson Rubber Component Zhan Wenzhang Ln Y Sh GuobaoJln Unversty of TechnologyChangchun, Chna Wang Lgong (MDI, Chna [Abstract] The dynamc characterstc
More informationˆ (0.10 m) E ( N m /C ) 36 ˆj ( j C m)
7.. = = 3 = 4 = 5. The electrc feld s constant everywhere between the plates. Ths s ndcated by the electrc feld vectors, whch are all the same length and n the same drecton. 7.5. Model: The dstances to
More informationNumerical Solution of Ordinary Differential Equations
Numercal Methods (CENG 00) CHAPTER-VI Numercal Soluton of Ordnar Dfferental Equatons 6 Introducton Dfferental equatons are equatons composed of an unknown functon and ts dervatves The followng are examples
More informationSpatial Statistics and Analysis Methods (for GEOG 104 class).
Spatal Statstcs and Analyss Methods (for GEOG 104 class). Provded by Dr. An L, San Dego State Unversty. 1 Ponts Types of spatal data Pont pattern analyss (PPA; such as nearest neghbor dstance, quadrat
More informationGaussian Mixture Models
Lab Gaussan Mxture Models Lab Objectve: Understand the formulaton of Gaussan Mxture Models (GMMs) and how to estmate GMM parameters. You ve already seen GMMs as the observaton dstrbuton n certan contnuous
More informationLecture 12: Discrete Laplacian
Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly
More informationError Bars in both X and Y
Error Bars n both X and Y Wrong ways to ft a lne : 1. y(x) a x +b (σ x 0). x(y) c y + d (σ y 0) 3. splt dfference between 1 and. Example: Prmordal He abundance: Extrapolate ft lne to [ O / H ] 0. [ He
More informationResearch Article Convexity-preserving using Rational Cubic Spline Interpolation
Research Journal of Appled Scences Engneerng and Technolog (3): 31-3 1 DOI:.19/rjaset..97 ISSN: -79; e-issn: -77 1 Mawell Scentfc Publcaton Corp. Submtted: October 13 Accepted: December 13 Publshed: Jul
More informationGravitational Acceleration: A case of constant acceleration (approx. 2 hr.) (6/7/11)
Gravtatonal Acceleraton: A case of constant acceleraton (approx. hr.) (6/7/11) Introducton The gravtatonal force s one of the fundamental forces of nature. Under the nfluence of ths force all objects havng
More informationChapter 3. r r. Position, Velocity, and Acceleration Revisited
Chapter 3 Poston, Velocty, and Acceleraton Revsted The poston vector of a partcle s a vector drawn from the orgn to the locaton of the partcle. In two dmensons: r = x ˆ+ yj ˆ (1) The dsplacement vector
More informationWeek 9 Chapter 10 Section 1-5
Week 9 Chapter 10 Secton 1-5 Rotaton Rgd Object A rgd object s one that s nondeformable The relatve locatons of all partcles makng up the object reman constant All real objects are deformable to some extent,
More informationMathematics Intersection of Lines
a place of mnd F A C U L T Y O F E D U C A T I O N Department of Currculum and Pedagog Mathematcs Intersecton of Lnes Scence and Mathematcs Educaton Research Group Supported b UBC Teachng and Learnng Enhancement
More informationProjective change between two Special (α, β)- Finsler Metrics
Internatonal Journal of Trend n Research and Development, Volume 2(6), ISSN 2394-9333 www.jtrd.com Projectve change between two Specal (, β)- Fnsler Metrcs Gayathr.K 1 and Narasmhamurthy.S.K 2 1 Assstant
More informationEcon107 Applied Econometrics Topic 3: Classical Model (Studenmund, Chapter 4)
I. Classcal Assumptons Econ7 Appled Econometrcs Topc 3: Classcal Model (Studenmund, Chapter 4) We have defned OLS and studed some algebrac propertes of OLS. In ths topc we wll study statstcal propertes
More informationOn the relationships among queue lengths at arrival, departure, and random epochs in the discrete-time queue with D-BMAP arrivals
On the relatonshps among queue lengths at arrval departure and random epochs n the dscrete-tme queue wth D-BMAP arrvals Nam K. Km Seo H. Chang Kung C. Chae * Department of Industral Engneerng Korea Advanced
More informationArmy Ants Tunneling for Classical Simulations
Electronc Supplementary Materal (ESI) for Chemcal Scence. Ths journal s The Royal Socety of Chemstry 2014 electronc supplementary nformaton (ESI) for Chemcal Scence Army Ants Tunnelng for Classcal Smulatons
More informationSpectral Graph Theory and its Applications September 16, Lecture 5
Spectral Graph Theory and ts Applcatons September 16, 2004 Lecturer: Danel A. Spelman Lecture 5 5.1 Introducton In ths lecture, we wll prove the followng theorem: Theorem 5.1.1. Let G be a planar graph
More informationOn the Multicriteria Integer Network Flow Problem
BULGARIAN ACADEMY OF SCIENCES CYBERNETICS AND INFORMATION TECHNOLOGIES Volume 5, No 2 Sofa 2005 On the Multcrtera Integer Network Flow Problem Vassl Vasslev, Marana Nkolova, Maryana Vassleva Insttute of
More informationMeasurement and Uncertainties
Phs L-L Introducton Measurement and Uncertantes An measurement s uncertan to some degree. No measurng nstrument s calbrated to nfnte precson, nor are an two measurements ever performed under eactl the
More information