Simulation of Spatially Correlated Large-Scale Parameters and Obtaining Model Parameters from Measurements

Size: px
Start display at page:

Download "Simulation of Spatially Correlated Large-Scale Parameters and Obtaining Model Parameters from Measurements"

Transcription

1 Simulation of Spatially Coelated Lage-Scale Paamete and Obtaining Model Paamete fom PER ZETTERBERG Stockholm Septembe 8 TRITA EE 8:49

2 Simulation of Spatially Coelated Lage-Scale Paamete and Obtaining Model Paamete fom Pe Zettebeg Electical Engineeing Royal Intitute of Technology Intoduction In the WINNER deliveable D54 we intoduced the concept of lage cale vaiable [] Thee ae vaiable which decibe aveage popetie of the channel in local aea uch angle-pead, hadow-fading and delay-pead They ae alway metic of the entie channel and neve pe-clute model A local aea i an aea of -3wavelength whee the lage cale paamete can be aumed contant The eaon fo calling them lage-cale paamete i that they change at appoimately the ame ate a the hadow-fading which i ometime called lage-cale fading in contat to mall-cale fading The mall-cale fading (often called fat-fading, Dopple fading o Rayleigh fading i vaying on a ub-wavelength cale Figue illutate how a mobile tavel on a tajectoy and whee the tajectoy i divided into local aea The lage-cale ae almot contant within one local-aea and change between local aea The coelation between the lage cale paamete between two poition (,y and (,y hould be a deceaing function of the Euclidian ditance between the two point Thi i a fom of patial coelation ince (,y and (,y ae epaated in pace Howeve, we note that the tem i uually ued fo mall-cale coelation between the fading of two (o moe antenna on a node (bae-tation/elay/mobile-tation,y,y 3,y3 4,y4 Figue : Illutation of a tajectoy with local aea A the tem indicate, lage-cale paamete i a vecto of andom vaiable Thee vaiable may (in the geneal cae have diffeent ditibution and be coelated (ie the coelation mati at zeo lag i not a diagonal To achieve thee objective the vecto of lage-cale (, paamete i modeled a (, = g, (* ( (,

3 [ T (, = R, y + ( μ ζ whee (, (, K m (, i a vecto of poibly patially coelated N(, independent Gauian pocee in two dimenion, R i a coelation mati, μ i vecto = ] of mean and g [ g (,K, g ( ] = ( m m Q geneal g ( i given by g ( = ( f ( whee f ( of (, y and the Q function i given by Q i a vecto of tanfomation function In t π ( = ep dt i the ditibution function It i common to model the patial coelation of the log-nomal (hadow fading by an eponential function of the Euclidean ditance Baed on thi obevation, we intoduce eponential autocoelation in the element of ie ( + ( y y { ( ( } ( E = =, y, y, y y ep λ The autocoelation of an individual lage-cale paamete (, will then no longe be eponentially (in geneal ditibuted fo two eaon Fit the miing mati R make the autocoelation of each element of the tanfomed vecto of lage cale paamete (, to become a um of eponential, and finally the tanfomation alo change the coelation Howeve, in pactice the eulting autocoelation ae geneally quite cloe to a ingle eponential In Section 5, below we how a method of how to obtain the paamete fom meauement data The meauement ae fom uban maco-cellula meauement [] Geneation of (, uing filteing Below we decibe how to geneate (, uing a filteing appoach Since the element of (, ae independent it uffice to decibe how to geneate one element of (, ay eg element ie (, Thi andom vaiable i Gauian, ha mean zeo and an autocoelation function given by ( + ( y y { ( ( } ( E = =, y, y, y y ep λ The deivation below ae baed on the theoy in [] fo two-dimenional image pocee

4 3 Baic appoach We notice that if we tat with a Gauian andom vaiable η (, which i patially white ie { (, y η( y } = δ ( δ ( y y E η,, and then pa it though a two-dimenional filte h (,, the output of that filte υ (, i given by υ (, = h(, (, y y d d η y and it autocoelation by { υ (, y (, y } (, y y h(, h(, y y y d d υ = ν = + + y E Thu by appopiately chooing h (, we can obtain (, by filteing the white map η (, In ode to elect h (, we note that the powe pectal denity of ν ie R ν ( f, f y i elated to the Fouie tanfom of h (, though Thu by etting R ( f f R ( f, f the Fouie tanfom of tanfom it ie ( f f H ( f, f R = ν, y y ν, y = y we can numeically obtain ( (, h, by fit calculating, and then taking the quae oot of the eult and invee h { } ( I R ( f, f, y = The following matlab-code obtain the filte h (, (called hy in the code in a gid of 3636 point paced λ apat whee λ i mete lambda= %% De-coelation ditance of i ampling_inteval=*lambda %% R: Two-dimenion auto-coelation function %% ize(r = (Nauto,Nauto Nauto=; %% Mut be even =(:Nauto; =(-mean(*ampling_inteval; y=(:nauto'; y=(y-mean(*ampling_inteval; % i ize (Nauto,Nauto % (i,j i the ditance fom, in a gid of point =ab(epmat(,nauto, +j*epmat(y,,nauto; R=ep(-/lambda; F=fft(R; F=(ab(F^*ep(j*angle(F; %% F i baically eal-valued But ince R(, i not oigo it will have a phae coeponding to the offet of oigo to R(, Thi i an offet we want to keep in F theefoe we copy the phaed of F h=eal(ifft(f; N=36;

5 i=((nauto/-(n/+:((nauto/+(n/; %% Select the tap with ma powe P=um(um(ab( h(i,i^; %% Powe of the elected tap Ptot=um(um(ab( h^; %% Powe of all tap (-P/Ptot i a meaue of the tuncation eo hy=h(i,i*inv(qt(p; %% Save eult in hy, compenate fo lo of powe Figue 3: Code fo geneation of the impule epone ( h, Aume now that we want to imulate an aea of ize 3λ 3λ fo a ingle ite We may then ue the impule epone h (, a decibed in the code of below, to obtain (, in a gid of point with paced λ To obtain (, at poition between the gid point, intepolation can be ued Npoint_out=3; Npoint_in=Npoint_out+*ize(hy,; i_gid=conv(hy,andn(npoint_in,npoint_in; %% Two-dimenional convolution %% Cop to emove tanient i_gid=i_gid(ize(hy,+(:npoint_out,ize(hy,+(:npoint_out; Figue 3: Code fo geneating (, in a gid of point fo a ingle ite 4 Tiling The appoach above ha the diadvantage of equiing lage memoy pace fo toing the map (ie the gid of ealization of (, To wok aound thi poblem we utilize cyclic convolution when geneating the gid, ay with length N ie we geneate (, in the point = Δ c, yk = Δ k, whee c, k {, K, N }, and Δ i the gid-pacing uing the cyclic convolution between h(, and a N by N ized mati of independent Gauian andom vaiable η, y The cyclic convolution i defined a ( c k N N h η c, k = c, k = k = ( (, c, k {, N } cc mod N, k k mod N We poition the impule epone in h c, k o that h c, k i non-zeo only fo c, k < N h uch a wa done in the code of Figue 3 fo N h = 36 (ie we have alo tuncated the impule epone Fo the inne point of the mati c, k, ie c, k { N h, K, N N h } (whee N h i the length of the impule epone it i clea that c,k i identical to a nomal linea (ie non-cyclic convolution between h and η Fo non inne point, the cicula convolution i identical to a linea convolution between and η, whee η i a cyclically epeated veion of η Fom thi it follow that a cyclic epetition of t c, k will have the ame autocoelation popetie a the c, k fo offet c c < N N h, < N N h Baed on thi we may epeat o tile t c, k to obtain a gid coveing any ize of an aea With pope pogamming we till only need to toe only one N by N ized mati The only diadvantage with the popoed appoach i that the ame patten will be epeated, albeit typically at ditance fa away The cyclic convolution can advantageouly be implemented with a two-dimenional dicete Fouie tanfom a illutated by the code in Figue 4 Ndft=^8; i_tilde_gid=ifft(fft(hy,ndft,ndft*fft(andn(ndft,ndft;

6 Figue 4: Illutation of computation of one tile to be epeated ove a modeled evice aea 5 Multiple Site When we have multiple bae-tation ite we in pinciple need multiple ealization of (, which again tat to tain ou memoy eouce To e-olve thi poblem we may define a ite-pecific tile fo each ite a n c, k = ( ccn mod N,( k kn mod N, c, k whee c n, k n ae ite pecific offet If the n n of diffeent bae-tation ae paced ufficiently fa apat, the pocedue will enue that the ealization of diffeent baetation in a given point will be independent a deied Again we note that by pope pogamming we till only have to toe one by N ized mati A common appoach when imulating cellula ytem i to tat with a finite evice aea a illutated in Figue 5 and the fold the edge of the imulation aea to obtain an edgele evice aea The eaon fo thi i that mobile and bae-tation nea the edge will othewie eceive le intefeence than thoe in the cente In Figue 5 we would fold bode A againt bode B and bode C againt bode D o a to ceate a Donut haped planet With thi pocedue, the uppe-left bae-tation in Figue 5 would become a neighbo bae-tation to the uppe-ight bae-tation of the ame plot The cicula convolution and tiling concept fit thi model pefect a the ealization on the edge D will be coelated with thoe on the edge C N Figue 5: Illutation of tiling and infinite imulation aea The mak the poition of the bae-tation and the quae mak the tile

7 6 Obtaining Model Paamete fom Meauement Data Below we decibe the tep of obtaining the equied model paamete fom meauement data The data wa collected fom an uban maco-cell at GHz [] The data only allow u to etimate AoD angle-pead, AoA angle-pead, and hadowfading Thu ou ( i in thi cae eponential 6 Chaacteize the ditibution of the individual element of ( In Figue 6 the ditibution of the tee component of ( 3 Ditibution of lage-cale vecto:aod pead Ditibution of lage-cale vecto:aoa pead 45 Ditibution of lage-cale vecto:shadow lo Fequency of occuance 5 Fequency of occuance Fequency of occuance Degee Degee Figue 6: Ditibution of the lage-cale paamete 5 5 Lo facto 6 Find a tanfomation g ( uch that the tanfomed lage cale vecto ( = g( ( i a vecto of Gauian andom vaiable Alo find the invee of ( g The following tanfomation have been identified ( ( (ep( if ep( ( = ep( = =, g log = g < 3 ( ( = =, 3 g 3 3 log 3 othewie Nomal pobability plot of the obtained etimate ae hown in Figue 6 Nomal pobability plot tanfomed lage-cale vecto:aod pead Nomal pobability plot tanfomed lage-cale vecto:aoa pead Nomal pobability plot tanfomed lage-cale vecto:shadow lo Pobability Pobability Pobability Data Data Data Figue 6: Nomal pobability plot of the tanfomed lage-cale paamete The invee of the tanfom ae given by ( = =, g

8 ( ( ln( < = g ( ln 3 = othewie ( 3 = = 3 g Etimate the paamete λ, K,λm Plot the etimated theoetical auto-coelation coefficient function obtained fom the model (* in the plot of analyi item pat 3 The paamete ae tuned by hand The fitted lope ae given by 7m, m and 7m, epectively The fitted cuve ae plotted in Figue 63 Coelation function of tanfomed SL paamete: numbe and numbe Coelation function of tanfomed SL paamete: numbe and numbe Coelation function of tanfomed SL paamete: numbe and numbe Coelation function of tanfomed SL paamete: numbe and numbe Coelation function of tanfomed SL paamete: numbe and numbe Coelation function of tanfomed SL paamete: numbe 3 and numbe Figue 63: Meaued auto-coelation function (geen and fitted eponential cuve (blue 64 Analyi item pat 5: Geneate data and check ome ditibution and co-coelation The following figue how a compaion of the actually meaued and the imulated angle-pead The imulated angle-pead can become negative Thi can be olved with a imple thehold function Ditibution of lage-cale vecto:aoa pead Simulated DoA angle-pead Fequency of occuance Fequency of occuance Degee Angle-pead Figue 64: Meaued and imulated angle-pead in left and ight ubfigue epectively The mati off meaued coelation coefficient fo the untanfomed data i given by

9 c= c= c=3 = = 38 4 = The mati of imulated coelation coefficient of the tanfomed data i given by c= c= c=3 = 4 48 = 4 36 = Refeence [] William K Patt, Digital Image Poceing, John Wiley and Son, ISBN

Histogram Processing

Histogram 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 information

Inference for A One Way Factorial Experiment. By Ed Stanek and Elaine Puleo

Inference 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

Chapter 19 Webassign Help Problems

Chapter 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 information

TRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the

TRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the Chapte 15 RAVELING WAVES 15.1 Simple Wave Motion Wave in which the ditubance i pependicula to the diection of popagation ae called the tanvee wave. Wave in which the ditubance i paallel to the diection

More information

Gravity. David Barwacz 7778 Thornapple Bayou SE, Grand Rapids, MI David Barwacz 12/03/2003

Gravity. 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 information

Solutions Practice Test PHYS 211 Exam 2

Solutions 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 information

Theory. Single Soil Layer. ProShake User s Manual

Theory. Single Soil Layer. ProShake User s Manual PoShake Ue Manual Theoy PoShake ue a fequency domain appoach to olve the gound epone poblem. In imple tem, the input motion i epeented a the um of a eie of ine wave of diffeent amplitude, fequencie, and

More information

ASTR 3740 Relativity & Cosmology Spring Answers to Problem Set 4.

ASTR 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 information

Precision Spectrophotometry

Precision 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 information

A Neural Network for the Travelling Salesman Problem with a Well Behaved Energy Function

A Neural Network for the Travelling Salesman Problem with a Well Behaved Energy Function A Neual Netwok fo the Tavelling Saleman Poblem with a Well Behaved Enegy Function Maco Budinich and Babaa Roaio Dipatimento di Fiica & INFN, Via Valeio, 347 Tiete, Italy E-mail: mbh@tiete.infn.it (Contibuted

More information

THROUGHPUT OF LARGE WIRELESS NETWORKS ON SQUARE, HEXAGONAL AND TRIANGULAR GRIDS. Kezhu Hong, Yingbo Hua

THROUGHPUT OF LARGE WIRELESS NETWORKS ON SQUARE, HEXAGONAL AND TRIANGULAR GRIDS. Kezhu Hong, Yingbo Hua THROUGHPUT OF LARGE WIRELESS NETWORKS ON SQUARE, HEAGONAL AND TRIANGULAR GRIDS Kezhu Hong, Yingbo Hua Dept. of Electical Engineeing Univeity of Califonia Riveide, CA 9252 {khong,yhua}@ee.uc.edu ABSTRACT

More information

Fall 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) =

Fall 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 information

QUADRATIC DEPENDENCE MEASURE FOR NONLINEAR BLIND SOURCES SEPARATION

QUADRATIC DEPENDENCE MEASURE FOR NONLINEAR BLIND SOURCES SEPARATION QUADRATI DPNDN MASUR FR NNLINAR BLIND SURS SPARATIN Sophie Achad Dinh Tuan Pham Univ. of Genoble Laboatoy of Modeling and omputation IMAG.N.R.S. B.P. 5X 84 Genoble edex Fance Sophie.Achad@imag.f Dinh-Tuan.Pham@imag.f

More information

Chapter 8 Sampling. Contents. Dr. Norrarat Wattanamongkhol. Lecturer. Department of Electrical Engineering, Engineering Faculty, sampling

Chapter 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 information

Considerations Regarding the Flux Estimation in Induction Generator with Application at the Control of Unconventional Energetic Conversion Systems

Considerations 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 information

Determining the Best Linear Unbiased Predictor of PSU Means with the Data. included with the Random Variables. Ed Stanek

Determining 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 information

How can you find the dimensions of a square or a circle when you are given its area? When you multiply a number by itself, you square the number.

How can you find the dimensions of a square or a circle when you are given its area? When you multiply a number by itself, you square the number. 7. Finding Squae Root How can you find the dimenion of a quae o a cicle when you ae given it aea? When you multiply a numbe by itelf, you quae the numbe. Symbol fo quaing i the exponent. = = 6 quaed i

More information

γ from B D(Kπ)K and B D(KX)K, X=3π or ππ 0

γ from B D(Kπ)K and B D(KX)K, X=3π or ππ 0 fom and X, X= o 0 Jim Libby, Andew Powell and Guy Wilkinon Univeity of Oxfod 8th Januay 007 Gamma meeting 1 Outline The AS technique to meaue Uing o 0 : intoducing the coheence facto Meauing the coheence

More information

Theorem 2: Proof: Note 1: Proof: Note 2:

Theorem 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 information

Then the number of elements of S of weight n is exactly the number of compositions of n into k parts.

Then 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 information

Eddy Currents in Permanent Magnets of a Multi-pole Direct Drive Motor

Eddy Currents in Permanent Magnets of a Multi-pole Direct Drive Motor Acta Technica Jauineni Vol. 6. No. 1. 2013 Eddy Cuent in Pemanent Magnet of a Multi-pole Diect Dive Moto G. Gotovac 1, G. Lampic 1, D. Miljavec 2 Elaphe Ltd. 1, Univeity of Ljubljana, Faculty of Electical

More information

Why Reduce Dimensionality? Feature Selection vs Extraction. Subset Selection

Why Reduce Dimensionality? Feature Selection vs Extraction. Subset Selection Dimenionality Reduction Why Reduce Dimenionality? Olive lide: Alpaydin Numbeed blue lide: Haykin, Neual Netwok: A Compehenive Foundation, Second edition, Pentice-Hall, Uppe Saddle Rive:NJ,. Black lide:

More information

Above Flux Estimation Issues in Induction Generators with Application at Energy Conversion Systems

Above Flux Estimation Issues in Induction Generators with Application at Energy Conversion Systems Acta Polytechnica Hungaica Vol. 3, No. 3, 2006 Above Flux Etimation Iue in Induction Geneato with Application at Enegy Conveion Sytem Ioif Szeidet, Octavian Potean, Ioan Filip, Vaa Citian Depatment of

More information

Estimation and Confidence Intervals: Additional Topics

Estimation and Confidence Intervals: Additional Topics Chapte 8 Etimation and Confidence Inteval: Additional Topic Thi chapte imply follow the method in Chapte 7 fo foming confidence inteval The text i a bit dioganized hee o hopefully we can implify Etimation:

More information

Honors Classical Physics I

Honors Classical Physics I Hono Claical Phyic I PHY141 Lectue 9 Newton Law of Gavity Pleae et you Clicke Channel to 1 9/15/014 Lectue 9 1 Newton Law of Gavity Gavitational attaction i the foce that act between object that have a

More information

Detailed solution of IES 2014 (ECE) Conventional Paper II. solve I 0 and use same formula again. Saturation region

Detailed solution of IES 2014 (ECE) Conventional Paper II. solve I 0 and use same formula again. Saturation region etailed olution of IS 4 (C) Conventional Pape II qv qv Sol. (a) IC I e Ie K K 4 I =.7 Fo I C = m olve I and ue ame fomula again K IC V ln 5ln 4 q I.7 =.8576 Volt Sol. (b) VGS VS Vupply 5V N MOS channel,

More information

one primary direction in which heat transfers (generally the smallest dimension) simple model good representation for solving engineering problems

one 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 information

Rotational Kinetic Energy

Rotational 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 information

Lesson 5. Chapter 7. Wiener Filters. Bengt Mandersson. r x k We assume uncorrelated noise v(n). LTH. September 2010

Lesson 5. Chapter 7. Wiener Filters. Bengt Mandersson. r x k We assume uncorrelated noise v(n). LTH. September 2010 Optimal Sigal Poceig Leo 5 Chapte 7 Wiee Filte I thi chapte we will ue the model how below. The igal ito the eceive i ( ( iga. Nomally, thi igal i ditubed by additive white oie v(. The ifomatio i i (.

More information

Section 25 Describing Rotational Motion

Section 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 information

Simulink Model of Direct Torque Control of Induction Machine

Simulink Model of Direct Torque Control of Induction Machine Ameican Jounal of Applied Science 5 (8): 1083-1090, 2008 ISSN 1546-9239 2008 Science Publication Simulink Model of Diect Toque Contol of Induction Machine H.F. Abdul Wahab and H. Sanui Faculty of Engineeing,

More information

MATERIAL SPREADING AND COMPACTION IN POWDER-BASED SOLID FREEFORM FABRICATION METHODS: MATHEMATICAL MODELING

MATERIAL SPREADING AND COMPACTION IN POWDER-BASED SOLID FREEFORM FABRICATION METHODS: MATHEMATICAL MODELING MATERIAL SPREADING AND COMPACTION IN POWDER-BASED SOLID FREEFORM FABRICATION METHODS: MATHEMATICAL MODELING Yae Shanjani and Ehan Toyekani Depatment of Mechanical and Mechatonic Engineeing, Univeity of

More information

Revision of Lecture Eight

Revision of Lecture Eight Revision of Lectue Eight Baseband equivalent system and equiements of optimal tansmit and eceive filteing: (1) achieve zeo ISI, and () maximise the eceive SNR Thee detection schemes: Theshold detection

More information

Image Enhancement: Histogram-based methods

Image 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 information

Suppose the medium is not homogeneous (gravity waves impinging on a beach,

Suppose the medium is not homogeneous (gravity waves impinging on a beach, Slowly vaying media: Ray theoy Suppose the medium is not homogeneous (gavity waves impinging on a beach, i.e. a vaying depth). Then a pue plane wave whose popeties ae constant in space and time is not

More information

V V The circumflex (^) tells us this is a unit vector

V 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 information

ME 3600 Control Systems Frequency Domain Analysis

ME 3600 Control Systems Frequency Domain Analysis ME 3600 Contol Systems Fequency Domain Analysis The fequency esponse of a system is defined as the steady-state esponse of the system to a sinusoidal (hamonic) input. Fo linea systems, the esulting steady-state

More information

New On-Line Algorithms for the Page Replication Problem. Susanne Albers y Hisashi Koga z. Abstract

New On-Line Algorithms for the Page Replication Problem. Susanne Albers y Hisashi Koga z. Abstract New On-Line Algoithm fo the Page Replication Poblem Suanne Albe y Hiahi Koga z Abtact We peent impoved competitive on-line algoithm fo the page eplication poblem and concentate on impotant netwok topologie

More information

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007 School of Electical and Compute Engineeing, Conell Univesity ECE 303: Electomagnetic Fields and Waves Fall 007 Homewok 8 Due on Oct. 19, 007 by 5:00 PM Reading Assignments: i) Review the lectue notes.

More information

Problem 1. Part b. Part a. Wayne Witzke ProblemSet #1 PHY 361. Calculate x, the expected value of x, defined by

Problem 1. Part b. Part a. Wayne Witzke ProblemSet #1 PHY 361. Calculate x, the expected value of x, defined by Poblem Pat a The nomal distibution Gaussian distibution o bell cuve has the fom f Ce µ Calculate the nomalization facto C by equiing the distibution to be nomalized f Substituting in f, defined above,

More information

CHAPTER 3 CLASSICAL CONTROL TECHNIQUES FOR AC DRIVES

CHAPTER 3 CLASSICAL CONTROL TECHNIQUES FOR AC DRIVES 44 CHAPTER 3 CLASSICAL CONTROL TECHNIQUES FOR AC DRIVES 3.1 INTRODUCTION The contolle equied fo AC dive can be divided into two majo type: cala contol and vecto contol (Boe 1976). In cala contol, which

More information

Supplemental Materials. Advanced Thermoelectrics Governed by Single Parabolic Band Model:

Supplemental Materials. Advanced Thermoelectrics Governed by Single Parabolic Band Model: Electonic Supplementay Mateial (ESI) fo Phyical Chemity Chemical Phyic. Thi jounal i The Royal Society of Chemity 04 Supplemental Mateial Advanced Themoelectic Govened by Single Paabolic and Model: Mg

More information

Static Electric Fields. Coulomb s Law Ε = 4πε. Gauss s Law. Electric Potential. Electrical Properties of Materials. Dielectrics. Capacitance E.

Static Electric Fields. Coulomb s Law Ε = 4πε. Gauss s Law. Electric Potential. Electrical Properties of Materials. Dielectrics. Capacitance E. Coulomb Law Ε Gau Law Electic Potential E Electical Popetie of Mateial Conducto J σe ielectic Capacitance Rˆ V q 4πε R ρ v 2 Static Electic Field εe E.1 Intoduction Example: Electic field due to a chage

More information

Development of Model Reduction using Stability Equation and Cauer Continued Fraction Method

Development of Model Reduction using Stability Equation and Cauer Continued Fraction Method Intenational Jounal of Electical and Compute Engineeing. ISSN 0974-90 Volume 5, Numbe (03), pp. -7 Intenational Reeach Publication Houe http://www.iphoue.com Development of Model Reduction uing Stability

More information

On a proper definition of spin current

On a proper definition of spin current On a pope definition of pin cuent Qian Niu Univeity of Texa at Autin P. Zhang, Shi, Xiao, and Niu (cond-mat 0503505) P. Zhang and Niu (cond-mat/0406436) Culce, Sinova, Sintyn, Jungwith, MacDonald, and

More information

Derivations in Classical Electrodynamics

Derivations in Classical Electrodynamics Deivation in Claical Electodynamic Andew Foete Januay 8, 009 Content Explanation Idea 3 Integation 3. A Special Integation by Pat.................................. 3 3. Anothe Special Integation by Pat...............................

More information

Shrinkage Estimation of Reliability Function for Some Lifetime Distributions

Shrinkage Estimation of Reliability Function for Some Lifetime Distributions Ameican Jounal of Computational and Applied Mathematic 4, 4(3): 9-96 DOI:.593/j.ajcam.443.4 Shinkage Etimation of eliability Function fo Some Lifetime Ditibution anjita Pandey Depatment of Statitic, niveity

More information

Perhaps the greatest success of his theory of gravity was to successfully explain the motion of the heavens planets, moons, &tc.

Perhaps 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 information

The Analysis of the Influence of the Independent Suspension on the Comfort for a Mine Truck

The Analysis of the Influence of the Independent Suspension on the Comfort for a Mine Truck 16 3 d Intenational Confeence on Vehicle, Mechanical and Electical Engineeing (ICVMEE 16 ISBN: 978-1-6595-37- The Analyi of the Influence of the Independent Supenion on the Comfot fo a Mine Tuck JINGMING

More information

Fast DCT-based image convolution algorithms and application to image resampling and hologram reconstruction

Fast DCT-based image convolution algorithms and application to image resampling and hologram reconstruction Fast DCT-based image convolution algoithms and application to image esampling and hologam econstuction Leonid Bilevich* a and Leonid Yaoslavsy** a a Depatment of Physical Electonics, Faculty of Engineeing,

More information

3.1 Random variables

3.1 Random variables 3 Chapte III Random Vaiables 3 Random vaiables A sample space S may be difficult to descibe if the elements of S ae not numbes discuss how we can use a ule by which an element s of S may be associated

More information

CSCE 478/878 Lecture 4: Experimental Design and Analysis. Stephen Scott. 3 Building a tree on the training set Introduction. Outline.

CSCE 478/878 Lecture 4: Experimental Design and Analysis. Stephen Scott. 3 Building a tree on the training set Introduction. Outline. In Homewok, you ae (supposedly) Choosing a data set 2 Extacting a test set of size > 3 3 Building a tee on the taining set 4 Testing on the test set 5 Repoting the accuacy (Adapted fom Ethem Alpaydin and

More information

AERODYNAMIC DESIGN METHOD FOR SUPERSONIC SLENDER BODY USING AN INVERSE PROBLEM

AERODYNAMIC DESIGN METHOD FOR SUPERSONIC SLENDER BODY USING AN INVERSE PROBLEM AERODYNAMIC DESIGN METHOD FOR SUPERSONIC SLENDER BODY Kia Matuhima*, Ikki Yamamichi**, Naoko Tokugawa*** * Dept. Engineeing, Univeity of Toyama, Gofuku 3190, Toyama 930-8555, JAPAN. Phone: +81-76-445-6796,

More information

SIMPLE LOW-ORDER AND INTEGRAL-ACTION CONTROLLER SYNTHESIS FOR MIMO SYSTEMS WITH TIME DELAYS

SIMPLE LOW-ORDER AND INTEGRAL-ACTION CONTROLLER SYNTHESIS FOR MIMO SYSTEMS WITH TIME DELAYS Appl. Comput. Math., V.10, N.2, 2011, pp.242-249 SIMPLE LOW-ORDER AND INTEGRAL-ACTION CONTROLLER SYNTHESIS FOR MIMO SYSTEMS WITH TIME DELAYS A.N. GÜNDEŞ1, A.N. METE 2 Abtact. A imple finite-dimenional

More information

DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS

DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS DOING PHYIC WITH MTLB COMPUTTIONL OPTIC FOUNDTION OF CLR DIFFRCTION THEORY Ian Coope chool of Physics, Univesity of ydney ian.coope@sydney.edu.au DOWNLOD DIRECTORY FOR MTLB CRIPT View document: Numeical

More information

Pearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms

Pearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms Peason s Chi-Squae Test Modifications fo Compaison of Unweighted and Weighted Histogams and Two Weighted Histogams Univesity of Akueyi, Bogi, v/noduslód, IS-6 Akueyi, Iceland E-mail: nikolai@unak.is Two

More information

arxiv: v1 [math.cv] 7 Nov 2018

arxiv: 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 information

3. Perturbation of Kerr BH

3. Perturbation of Kerr BH 3. Petubation of Ke BH hoizon at Δ = 0 ( = ± ) Unfotunately, it i technically fomidable to deal with the metic petubation of Ke BH becaue of coupling between and θ Nevethele, thee exit a fomalim (Newman-Penoe

More information

Contact impedance of grounded and capacitive electrodes

Contact impedance of grounded and capacitive electrodes Abstact Contact impedance of gounded and capacitive electodes Andeas Hödt Institut fü Geophysik und extateestische Physik, TU Baunschweig The contact impedance of electodes detemines how much cuent can

More information

Chapter 3 Optical Systems with Annular Pupils

Chapter 3 Optical Systems with Annular Pupils Chapte 3 Optical Systems with Annula Pupils 3 INTRODUCTION In this chapte, we discuss the imaging popeties of a system with an annula pupil in a manne simila to those fo a system with a cicula pupil The

More information

Homework Set 3 Physics 319 Classical Mechanics

Homework Set 3 Physics 319 Classical Mechanics Homewok Set 3 Phsics 319 lassical Mechanics Poblem 5.13 a) To fin the equilibium position (whee thee is no foce) set the eivative of the potential to zeo U 1 R U0 R U 0 at R R b) If R is much smalle than

More information

Equations of 2-body motion

Equations of 2-body motion Equation of -body motion The fundamental eqn. of claical atodynamic i Newton Law of Univeal Gavitation: F g = Gm i i i ˆ i (1) We ae inteeted in atellite in obit about ingle planet, o (1) educe to the

More information

Laser Doppler Velocimetry (LDV)

Laser Doppler Velocimetry (LDV) AeE 545 cla note #1 Lae Dopple elocimety (LD) Pat - 01 Hui Hu Depatment o Aeopace Engineeing, Iowa State Univeity Ame, Iowa 50011, U.S.A Technique o Flow elocity Meauement Intuive technique Pitot-tatic

More information

Introduction to Arrays

Introduction to Arrays Intoduction to Aays Page 1 Intoduction to Aays The antennas we have studied so fa have vey low diectivity / gain. While this is good fo boadcast applications (whee we want unifom coveage), thee ae cases

More information

Mathematical Modeling of Metabolic Processes in a Living Organism in Relation to Nutrition

Mathematical Modeling of Metabolic Processes in a Living Organism in Relation to Nutrition Mathematical Modeling of Metabolic Pocee in a Living Oganim in Relation to Nutition Dimitova N., Makov S. Depatment Biomathematic Intitute of Mathematic and Infomatic Bulgaian Academy of Science 8 Acad.

More information

Lecture No. 6 (Waves) The Doppler Effect

Lecture No. 6 (Waves) The Doppler Effect Lectue No. 6 (Wave) The Dopple Eect 1) A ound ouce i moving at 80 m/ towad a tationay litene that i tanding in till ai. (a) Find the wavelength o the ound in the egion between the ouce and the litene.

More information

10/04/18. P [P(x)] 1 negl(n).

10/04/18. P [P(x)] 1 negl(n). Mastemath, Sping 208 Into to Lattice lgs & Cypto Lectue 0 0/04/8 Lectues: D. Dadush, L. Ducas Scibe: K. de Boe Intoduction In this lectue, we will teat two main pats. Duing the fist pat we continue the

More information

Let {X n, n 1} be a sequence of independent and identically distributed random variables with a common cdf F (x) and pdf f(x).

Let {X n, n 1} be a sequence of independent and identically distributed random variables with a common cdf F (x) and pdf f(x). Kangweon-Kyungki Math Jou 2 24, No, pp 5 22 RCURRNC RLATION FOR QUOTINTS OF TH POWR DISTRIBUTION BY RCORD VALUS Min-Young Lee and Se-Kyung Chang Abtact In thi pape we etablih ome ecuence elation atified

More information

Sensorless Control of Induction Motor Drives

Sensorless Control of Induction Motor Drives Poceeding of the IEEE, Vol. 9, No. 8, Aug., pp. 359-394 Senole Contol of Induction Moto Dive Joachim Holtz, Fellow, IEEE Electical Machine and Dive Goup, Univeity of Wuppetal 497 Wuppetal Gemany Abtact

More information

Pulse Neutron Neutron (PNN) tool logging for porosity Some theoretical aspects

Pulse Neutron Neutron (PNN) tool logging for porosity Some theoretical aspects Pulse Neuton Neuton (PNN) tool logging fo poosity Some theoetical aspects Intoduction Pehaps the most citicism of Pulse Neuton Neuon (PNN) logging methods has been chage that PNN is to sensitive to the

More information

Announcements. Description Linear Angular position x θ displacement x θ rate of change of position v x ω x = = θ average rate of change of position

Announcements. Description Linear Angular position x θ displacement x θ rate of change of position v x ω x = = θ average rate of change of position Announcement In the lectue link Look o tet 1 beakdown liting the topic o the quetion. Look o m umma o topic o the eam. We ll ue it on the eiew net Tueda. Look o a lit o baic phic act eleant o thi eam.

More information

HRW 7e Chapter 13 Page 1 of 5

HRW 7e Chapter 13 Page 1 of 5 HW 7e Chapte Pae o 5 Halliday/enick/Walke 7e Chapte Gaitation The manitude o the oce o one paticle on the othe i ien by F = Gm m /, whee m and m ae the mae, i thei epaation, and G i the unieal aitational

More information

Information Retrieval Advanced IR models. Luca Bondi

Information Retrieval Advanced IR models. Luca Bondi Advanced IR models Luca Bondi Advanced IR models 2 (LSI) Pobabilistic Latent Semantic Analysis (plsa) Vecto Space Model 3 Stating point: Vecto Space Model Documents and queies epesented as vectos in the

More information

Approximation Techniques for Spatial Data

Approximation Techniques for Spatial Data Appoximation Technique fo Spatial Data Abhinandan Da Conell Univeity ada@c.conell.edu Johanne Gehke Conell Univeity johanne@c.conell.edu Miek Riedewald Conell Univeity miek@c.conell.edu ABSTRACT Spatial

More information

FRACTIONAL ORDER SYSTEM IDENTIFICATION BASED ON GENETIC ALGORITHMS

FRACTIONAL ORDER SYSTEM IDENTIFICATION BASED ON GENETIC ALGORITHMS Jounal of Engineeing Science and Technology Vol. 8, No. 6 (2013) 713-722 School of Engineeing, Taylo niveity FRACTIONAL ORDER SSTEM IDENTIFICATION BASED ON GENETIC ALGORITHMS MAZIN Z. OTHMAN*, EMAD A.

More information

Boise State University Department of Electrical and Computer Engineering ECE470 Electric Machines

Boise 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 information

CHAPTER 2 MATHEMATICAL MODELING OF WIND ENERGY SYSTEMS

CHAPTER 2 MATHEMATICAL MODELING OF WIND ENERGY SYSTEMS 17 CHAPTER 2 MATHEMATICAL MODELING OF WIND ENERGY SYSTEMS 2.1 DESCRIPTION The development of wind enegy ytem and advance in powe electonic have enabled an efficient futue fo wind enegy. Ou imulation tudy

More information

Geometry Contest 2013

Geometry 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 information

COMPLEX MODE SUPERPOSITION METHOD CONSIDERING THE EFFECT OF MULTIPLE FOLD EIGENVALUE IN SEISMIC DESIGN

COMPLEX MODE SUPERPOSITION METHOD CONSIDERING THE EFFECT OF MULTIPLE FOLD EIGENVALUE IN SEISMIC DESIGN The 4 th Wold Confeence on Eathquae Engineeing Octobe -7, 008, Being, China COMPLEX MODE SUPERPOSITION METHOD CONSIDERING THE EFFECT OF MULTIPLE FOLD EIGENVALUE IN SEISMIC DESIGN Ruifang Yu,, Xiyuan Zhou

More information

AE 245 homework #9 solutions

AE 245 homework #9 solutions AE 245 homewok #9 olution Tim Smith 13 Apil 2000 1 Poblem1 In the Apollo miion fom the Eath to the Moon, the Satun thid tage povided the tan-luna inetion bun that tanfeed the Apollo pacecaft fom a low

More information

FI 2201 Electromagnetism

FI 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 information

A Generalized Two Axes Model of a Squirrel-Cage Induction Motor for Rotor Fault Diagnosis

A Generalized Two Axes Model of a Squirrel-Cage Induction Motor for Rotor Fault Diagnosis SEBIAN JOUNAL OF ELECTICAL ENGINEEING Vol. 5, No. 1, ay 2008, 155-170 A Genealized Two Axe odel of a Squiel-Cage Induction oto fo oto Fault Diagnoi Sami Hamdani 1, Oma Touhami 2, achid Ibtiouen 2 Abtact:

More information

Rotational Motion. Lecture 6. Chapter 4. Physics I. Course website:

Rotational Motion. Lecture 6. Chapter 4. Physics I. Course website: Lectue 6 Chapte 4 Physics I Rotational Motion Couse website: http://faculty.uml.edu/andiy_danylov/teaching/physicsi Today we ae going to discuss: Chapte 4: Unifom Cicula Motion: Section 4.4 Nonunifom Cicula

More information

PHYSICS 151 Notes for Online Lecture 2.6

PHYSICS 151 Notes for Online Lecture 2.6 PHYSICS 151 Note fo Online Lectue.6 Toque: The whole eaon that we want to woy about cente of ma i that we ae limited to lookin at point mae unle we know how to deal with otation. Let eviit the metetick.

More information

Generating a Random Collection of Discrete Joint Probability Distributions Subject to Partial Information

Generating a Random Collection of Discrete Joint Probability Distributions Subject to Partial Information Methodol Comput Appl Pobab DOI 10.1007/11009-01-99-9 Geneating a Random Collection of Dicete Joint Pobability Ditibution Subject to Patial Infomation Lui V. Montiel J. Eic Bickel Received: 4 Octobe 011

More information

Maximum Likelihood Logistic Regression With Auxiliary Information

Maximum Likelihood Logistic Regression With Auxiliary Information niveity of Wollongong Reeach Online Cente fo Statitical Suvey Methodology Woking Pape Seie Faculty of Engineeing and Infomation Science 2008 Maximum Likelihood Logitic Regeion With Auxiliay Infomation

More information

A note on rescalings of the skew-normal distribution

A 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 information

Homework # 3 Solution Key

Homework # 3 Solution Key PHYSICS 631: Geneal Relativity Homewok # 3 Solution Key 1. You e on you hono not to do this one by hand. I ealize you can use a compute o simply look it up. Please don t. In a flat space, the metic in

More information

$ i. !((( dv vol. Physics 8.02 Quiz One Equations Fall q 1 q 2 r 2 C = 2 C! V 2 = Q 2 2C F = 4!" or. r ˆ = points from source q to observer

$ i. !((( dv vol. Physics 8.02 Quiz One Equations Fall q 1 q 2 r 2 C = 2 C! V 2 = Q 2 2C F = 4! or. r ˆ = points from source q to observer Physics 8.0 Quiz One Equations Fall 006 F = 1 4" o q 1 q = q q ˆ 3 4" o = E 4" o ˆ = points fom souce q to obseve 1 dq E = # ˆ 4" 0 V "## E "d A = Q inside closed suface o d A points fom inside to V =

More information

TP A.4 Post-impact cue ball trajectory for any cut angle, speed, and spin

TP A.4 Post-impact cue ball trajectory for any cut angle, speed, and spin technical poof TP A.4 Pot-impact cue ball tajectoy fo any cut anle, peed, and pin uppotin: The Illutated Pinciple of Pool and Billiad http://billiad.colotate.edu by Daid G. Alciatoe, PhD, PE ("D. Dae")

More information

COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS

COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS Pogess In Electomagnetics Reseach, PIER 73, 93 105, 2007 COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS T.-X. Song, Y.-H. Liu, and J.-M. Xiong School of Mechanical Engineeing

More information

Lecture 04: HFK Propagation Physical Optics II (Optical Sciences 330) (Updated: Friday, April 29, 2005, 8:05 PM) W.J. Dallas

Lecture 04: HFK Propagation Physical Optics II (Optical Sciences 330) (Updated: Friday, April 29, 2005, 8:05 PM) W.J. Dallas C:\Dallas\0_Couses\0_OpSci_330\0 Lectue Notes\04 HfkPopagation.doc: Page of 9 Lectue 04: HFK Popagation Physical Optics II (Optical Sciences 330) (Updated: Fiday, Apil 9, 005, 8:05 PM) W.J. Dallas The

More information

arxiv: v2 [physics.data-an] 15 Jul 2015

arxiv: v2 [physics.data-an] 15 Jul 2015 Limitation of the Least Squae Method in the Evaluation of Dimension of Factal Bownian Motions BINGQIANG QIAO,, SIMING LIU, OUDUN ZENG, XIANG LI, and BENZONG DAI Depatment of Physics, Yunnan Univesity,

More information

VECTOR CONTROL OF INDUCTION MOTOR DRIVE BY USING THE CONSTANT SWITCHING FREQUENCY CURRENT CONTROLLER FOR REDUCED RIPPLE

VECTOR CONTROL OF INDUCTION MOTOR DRIVE BY USING THE CONSTANT SWITCHING FREQUENCY CURRENT CONTROLLER FOR REDUCED RIPPLE Acta Electotechnica et Infomatica, Vol. 3, No. 3, 203, 27 33, DOI: 0.2478/aeei-203-0036 27 VECTOR CONTROL OF INDUCTION MOTOR DRIVE BY USING THE CONSTANT SWITCHING FREQUENCY CURRENT CONTROLLER FOR REDUCED

More information

TELE4652 Mobile and Satellite Communications

TELE4652 Mobile and Satellite Communications Mobile and Satellite Communications Lectue 3 Radio Channel Modelling Channel Models If one was to walk away fom a base station, and measue the powe level eceived, a plot would like this: Channel Models

More information

Compactly Supported Radial Basis Functions

Compactly Supported Radial Basis Functions Chapte 4 Compactly Suppoted Radial Basis Functions As we saw ealie, compactly suppoted functions Φ that ae tuly stictly conditionally positive definite of ode m > do not exist The compact suppot automatically

More information

Shot-geophone migration for seismic data

Shot-geophone migration for seismic data Shot-geophone migation fo eimic data Chi Stolk Depatment of Applied Mathematic, Univeity of Twente, The Netheland ouce x Seimic data poceing eceive x h time... ubuface Contempoay pimaie only poceing: Body

More information

Basic propositional and. The fundamentals of deduction

Basic 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 information

Absolute Specifications: A typical absolute specification of a lowpass filter is shown in figure 1 where:

Absolute Specifications: A typical absolute specification of a lowpass filter is shown in figure 1 where: FIR FILTER DESIGN The design of an digital filte is caied out in thee steps: ) Specification: Befoe we can design a filte we must have some specifications. These ae detemined by the application. ) Appoximations

More information

LECTURE 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

LECTURE 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 information