Fall ACS Meeting November 4-6, 1997

Size: px
Start display at page:

Download "Fall ACS Meeting November 4-6, 1997"

Transcription

1 Optiml Configution of Combined GPP/DSP/FPGA Systems fo Miniml SWAP by John K. Antonio Deptment of Compute Science College of Engineeing Texs Tech Univesity Fll ACS Meeting Novembe

2 Outline Pogm Objectives nd Schedule of Milestones Repesenttive Exmples of Cuent Wo Competing STAP Weight Solves Powe Pediction Model fo FPGAs Optiml Configution fo SAR Pocessing Questions/Answes 2

3 Pogm Objectives Demonstte dvntges of combined use of GPP DSP nd FPGA technologies fo SAR nd STAP pplictions Demonstte dvntges/disdvntges of diffeent FPGA designs nd implementtions in tems of powe consumption nd el-estte equiements Develop nd evlute powe pediction models fo GPP/DSP/FPGA pototype system Development of foml optimiztions fo configuing GPP/DSP/FPGA systems 3

4 Pogm Objectives Incopotion of dt chcteistics nd equiements in optimizing system configution dynmic nge numeicl ccucy Incopotion of multiple GPP/DSP lgoithms FPGA designs nd implementtions nd dt epesenttions in optimizing system configution Time-domin vs. fequency-domin convolutions QR vs. conjugte gdient STAP weight solve Fixed-point vs. bloc floting point vs. floting point 4

5 Schedule of Milestones June 1997 Dec June 1998 Dec June 1999 Dec Optiml GPP/DSP Config. fo SAR Implement SAR on GPP/DSP Optiml GPP/DSP/FPGA Config. fo SAR Optiml GPP/DSP/FPGA Config. fo SAR/STAP Inte-GPP/DSP Comm. Simulto fo STAP Implement STAP on GPP/DSP Design SAR Line Filteing fo FPGA Design STAP Itetive Weight Solve fo FPGA Develop FPGA Powe Consumption Simulto Optiml GPP/DSP Config. fo STAP Implement SAR Line Filteing on FPGA Implement STAP Itetive Weight Solve on FPGA Optiml GPP/DSP/FPGA Config. fo STAP Implement SAR on GPP/DSP/FPGA Pltfom Implement STAP on GPP/DSP/FPGA Pltfom GPP/DSP/FPGA Pltfom Constuction nd Independent Testing of GPP/DSP nd FPGA Subsystems GPP/DSP nd FPGA Subsystem Integtion nd Testing Demonstte Combined SAR/STAP on GPP/DSP/FPGA Pltfom Key GPP/DSP Sub-System Resech/Design Implement/Test FPGA Sub-System Resech/Design Implement/Test GPP/DSP/FPGA System Resech/Design 5 Implement/Test

6 Outline Pogm Objectives nd Schedule of Milestones Repesenttive Exmples of Cuent Wo Competing STAP Weight Solves Powe Pediction Model fo FPGAs Optiml Configution fo SAR Pocessing Questions/Answes 6

7 Refeences fo STAP J. Wd Spce-Time Adptive Pocessing fo Aibone Rd Technicl Repot 1015 MIT Lincoln Lbotoy Lexington MA K. C. Cin J. A. Toes nd R. T. Willims R. A. Gmes Poject Lede RT_STAP: Rel-Time Spce-Time Adptive Pocessing Benchm MITRE Technicl Repot MTR 96B Feb MCARM Dt Files Rome Lbotoy D. G. Luenbege Line nd Nonline Pogmming Addison- Wesley Reding MA

8 Fomultion of STAP Weight Eqution Dt Mtix Needed fo Clculting Weights fo th Dopple Bin nd m th Rnge Segment Using 3 d x : Ode ^ Dopple-Fctoed STAP L 1 3L L Chnnels Dopple m th Rnge Segment with N R cells ψ m 1 N R H x x N R 1 8

9 9 R N R L N L m 3 : ^ STAP Weight Clcultion Using QR Decomposition m m N x x m H R H R N N R ψ s m w m γ ψ The Weight Eqution: s N m w R R s m w R R N w Q R Q R N R T T R T T R γ γ 1 1 * 1 1 * * * QR m T QR-Decomposition :

10 10 Using Conjugte Gdient Appoch to Solve the Weight Eqution CG fo Solving : ψw s Initiliztion T T T T d d d d g g d s w g d d d d g w w Ψ Ψ + Ψ Ψ set Choose d g w s d w Ψ Itetion

11 Peliminy Numeicl Studies Reltive Eo nd FLOP count Vs. Tolence fo N 125 Dt File: e pulses 28 Weight Vectos Computed QR CG Reltive Eo FLOP Count Tolence Tolence 11

12 Peliminy Numeicl Studies Reltive Eo nd FLOP count Vs. Tolence fo N 250 Dt File: e pulses 28 Weight Vectos Computed QR CG Reltive Eo FLOP Count Tolence Tolence 12

13 Implementtion of Conjugte Gdient on FPGAs Esie nd Moe Efficient to Implement on FPGA Hdwe thn QR Decomposition Appoch: Stte Mchine Design ψ Numeicl Opetions Floting point Bloc floting point Fixed point w j w j + 1 No. of vibles No. of bits/vible Dynmic Rnge Accucy Registes 13

14 QR Decomposition: QR Decomposition vesus Conjugte Gdient Suitble fo GPP/DSP implementtion Good pefomnce fo smll vlues of N R Conjugte Gdient: Suitble fo eithe GPP/DSP o FPGA implementtions Good pefomnce fo lge vlues of N R Povides wy to blnce desied pecision nd computtionl effot FPGA implementtions offe mny design pmetes e.g. dt epesenttion no. bits vible etc. 14

15 Conceptul Illusttion of Tde-Offs gphs shown e hypotheticl CG on GPP/DSP QR on GPP/DSP CG on FPGA - Floting Point CG on FPGA - Bloc Floting Point CG on FPGA - Fixed Point Computtionl Complexity Powe Requiements {Pecision Accucy Dyn. Rnge L N } Multidimensionl Pmete Spce {Pecision Accucy Dyn. Rnge L N } Multidimensionl Pmete Spce 15

16 Outline Pogm Objectives nd Schedule of Milestones Repesenttive Exmples of Cuent Wo Competing STAP Weight Solves Powe Pediction Model fo FPGAs Optiml Configution fo SAR Pocessing Questions/Answes 16

17 Refeences fo FPGA Powe Pediction K. P. Pe nd E. J. McClusey Pobbilistic Tetment of Genel Combintoil Netwos IEEE Tns. Computes Vol. C-24 June 1975 pp Kushi Roy nd Sht Psd Cicuit Activity Bsed Logic Synthesis fo Low Powe Relible Opetions IEEE Tns. VLSI Systems Vol. 1 No. 4 Dec.1993 pp. Kushi Roy Powe Dissiption Diven FPGA Plce nd Route unde Timing Constints School of Electicl nd Compute Engineeing Pudue Univesity. C4000 Seies Field Pogmmble Gte Ays ilinx Inc. Septembe

18 FPGA Powe Consumption Inteconnection fbic Logic bloc Most of the logic/e in the FPGA is used to oute signls. As signls tvese this netwo of tnsistos thee cn be significnt powe consumption. 18

19 Powe Dissiption in CMOS Lege Cuent Dynmic Cpcitnce Chging Cuent Most impotnt fo CMOS Dependnt on cloc fequency Dependnt on signl ctivity Tnsient Cuent 19

20 Time-Domin Modeling Vey pecise esults Computtionlly expensive x 1 x 2 x 3 y x 1 t: x 2 t: x 3 t : xx : 1 2 t xx 1 2x3 t: x 1 x 2 y Clcultion of instntneous powe: pt x 3 20

21 Pobbilistic Modeling ps: the pobbility tht signl s ttins logicl vlue of tue t ny given cloc cycle. As: the pobbility tht signl s tnsitions t ny given cloc cycle. p cloc p x p x A cloc 1. 0 A x A x p x A x

22 Pobbilistic Modeling x 1 x 2 x 3 Acceptble esults Computtionlly inexpensive y x 1 t: x 2 t: x 3 t : xx : 1 2 t xx 1 2x3 t: p0.88 A0.10 p0.29 A0.17 p0.69 A0.27 p0.83 A0.17 p0.10 A0.13 x 1 x 2 x 3 y P Clcultion of vege powe: 1 CV vg 2 2 A g g ll gtes 22

23 Pobbilistic Model Implementtion ps 1 As 1 ps 2 As 2 Step 1: Pobbilistic infomtion is distilled fom the input dt nd pesented to the model. Step 2: Pobbilistic dt popgtes thoughout the model depositing ctivity infomtion s it does so. Step 3: Powe is estimted using ctivity mesues nd nown CMOS gte cpcitnces. ps 3 As 3 23

24 Outline Pogm Objectives nd Schedule of Milestones Repesenttive Exmples of Cuent Wo Competing STAP Weight Solves Powe Pediction Model fo FPGAs Optiml Configution fo SAR Pocessing Questions/Answes 24

25 Refeences fo Optiml Configution fo SAR Pocessing J. T. Muehing nd J. K. Antonio Optiml Configution of n Embedded Pllel System fo Synthetic Apetue Rd Pocessing Poc. Int l Conf. on Signl Pocessing Applictions & Technology Boston MA Oct pp T. Einstein Reltime Synthetic Apetue Rd Pocessing on the RACE Multicompute Appliction Note Mecuy Computing Systems Inc. Chelmsfod MA J. C. Culnde nd R. N. McDonough Synthetic Apetue Rd: Systems nd Signl Pocessing John Wiley & Sons New Yo NY SHARC DSP Compute Nodes 3.3-Volt Mecuy Computing Systems Inc. Chelmsfod MA

26 GPP/DSP Appoch fo SAR Pocessing Rnge Pocessing shown coss 3 nge pocessos Azimuth Pocessing shown coss 4 zimuth pocessos K S Pulse No. 1 Distibuted Cone-Tun Rnge Smples 1 K 1 Rnge Smples 1 S Pulse No. whee S is the zimuth section length nd K is the nge efeence enel size 26

27 The Sectioned Convolution fo the Azimuth Pocessing FFT size Kenel Ovelp Discd Section Lge Ovelp/Section tio Smll zimuth memoy lge numbe zimuth pocessos Smll Ovelp/Section tio Lge zimuth memoy smll numbe zimuth pocessos 27

28 Deivtions fo Memoy nd Pocessos fo GPP/DSP Systems P v 6δF + α γr + 10δF lg F s 2 γδ P vr s α + F 6+ 10lg F γs 2 δ M 16Rv 6δF + α γr + 10δF lg F s s 3 γδ M 2 R λr+ 2δ S s 3 δ whee P nd P e the numbe of equied pocessos nd M nd M e the memoy equiements in Mbytes fo nge nd zimuth pocessing espectively 28

29 Detemining Optiml Configutions fo GPP/DSP Systems Detemine configutions fo the CNs numbe of CNs of ech configution nd section size to stisfy pocesso nd memoy equiements nd minimize powe consumption Nottion nd Definitions: CN Configution: Specifies the dughtecd type nd numbe of nge nd zimuth pocessos pe configued CN Y: The two possible CN configutions T Y T : Dughtecd type fo ech CN configution 29

30 Detemining Optiml Configutions fo GPP/DSP Systems Nottion nd Definitions continued: Y : Numbe of nge pocessos pe CN fo ech configution Y : Numbe of zimuth pocessos pe CN fo ech configution N N Y : Numbe of CNs of configutions nd Y Π CN : Powe pe CN s function of dughtecd type M CN : Memoy pe CN s function of dughtecd type P CN : Pocessos pe CN s function of dughtecd type 30

31 Y T CN T CN T CN T CN Y Y T CN Y T CN S Y Y N N K S F Y P Y Y P S P S M Y P M Y Y M S P S M P M M Y N N S P Y N N P Y Π N Π N Z Minimize: Subject to: Optimiztion Fomultion fo GPP/DSP Systems

32 Powe Consumption in Optiml Configution 32

33 % Powe Incese of Nominl Ove Optiml Configution 33

34 Optiml CN Configutions 400 v T Y Y Y T δ 34

35 Detemining Optiml Configutions fo GPP/DSP/FPGA Systems Assume FPGAs e used fo nge pocessing Additionl Nottion nd Definitions: D : Dynmic nge equied fo nge pocessing A : Accucy equied fo nge pocessing I : Incoming dt te depends on δ v R R s T u : Dt type used floting bloc o fixed B u : Numbe of bits used fo dt epesenttion depends on D A T u Cl u : Cloc te used depends on I T u B u 35

36 Detemining Optiml Configutions fo GPP/DSP/FPGA Systems Additionl Nottion nd Definitions continued: G u : Numbe of FPGA chips used fo nge pocessing depends on I T u B u Π G : Powe consumption of FPGAs depends on Cl u T u B u G u Ongoing Wo Deiving pecise eltionships mong bove tems Extending cuent GPP/DSP optimiztion fomultion to include FPGA utiliztion 36

37 Outline Pogm Objectives nd Schedule of Milestones Repesenttive Exmples of Cuent Wo Competing STAP Weight Solves Powe Pediction Model fo FPGAs Optiml Configution fo SAR Pocessing Questions/Answes 37

Discrete Model Parametrization

Discrete Model Parametrization Poceedings of Intentionl cientific Confeence of FME ession 4: Automtion Contol nd Applied Infomtics Ppe 9 Discete Model Pmetition NOKIEVIČ, Pet Doc,Ing,Cc Deptment of Contol ystems nd Instumenttion, Fculty

More information

Important design issues and engineering applications of SDOF system Frequency response Functions

Important design issues and engineering applications of SDOF system Frequency response Functions Impotnt design issues nd engineeing pplictions of SDOF system Fequency esponse Functions The following desciptions show typicl questions elted to the design nd dynmic pefomnce of second-ode mechnicl system

More information

Multiple-input multiple-output (MIMO) communication systems. Advanced Modulation and Coding : MIMO Communication Systems 1

Multiple-input multiple-output (MIMO) communication systems. Advanced Modulation and Coding : MIMO Communication Systems 1 Multiple-input multiple-output (MIMO) communiction systems Advnced Modultion nd Coding : MIMO Communiction Systems System model # # #n #m eceive tnsmitte infobits infobits #N #N N tnsmit ntenns N (k) M

More information

Data Structures. Element Uniqueness Problem. Hash Tables. Example. Hash Tables. Dana Shapira. 19 x 1. ) h(x 4. ) h(x 2. ) h(x 3. h(x 1. x 4. x 2.

Data Structures. Element Uniqueness Problem. Hash Tables. Example. Hash Tables. Dana Shapira. 19 x 1. ) h(x 4. ) h(x 2. ) h(x 3. h(x 1. x 4. x 2. Element Uniqueness Poblem Dt Stuctues Let x,..., xn < m Detemine whethe thee exist i j such tht x i =x j Sot Algoithm Bucket Sot Dn Shpi Hsh Tbles fo (i=;i

More information

Chapter 6 Frequency Response & System Concepts

Chapter 6 Frequency Response & System Concepts hpte 6 Fequency esponse & ystem oncepts Jesung Jng stedy stte (fequency) esponse Phso nottion Filte v v Foced esponse by inusoidl Excittion ( t) dv v v dv v cos t dt dt ince the focing fuction is sinusoid,

More information

Previously. Extensions to backstepping controller designs. Tracking using backstepping Suppose we consider the general system

Previously. Extensions to backstepping controller designs. Tracking using backstepping Suppose we consider the general system 436-459 Advnced contol nd utomtion Extensions to bckstepping contolle designs Tcking Obseves (nonline dmping) Peviously Lst lectue we looked t designing nonline contolles using the bckstepping technique

More information

General Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface

General Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface Genel Physics II Chpte 3: Guss w We now wnt to quickly discuss one of the moe useful tools fo clculting the electic field, nmely Guss lw. In ode to undestnd Guss s lw, it seems we need to know the concept

More information

Lecture 10. Solution of Nonlinear Equations - II

Lecture 10. Solution of Nonlinear Equations - II Fied point Poblems Lectue Solution o Nonline Equtions - II Given unction g : R R, vlue such tht gis clled ied point o the unction g, since is unchnged when g is pplied to it. Whees with nonline eqution

More information

Quality control. Final exam: 2012/1/12 (Thur), 9:00-12:00 Q1 Q2 Q3 Q4 Q5 YOUR NAME

Quality control. Final exam: 2012/1/12 (Thur), 9:00-12:00 Q1 Q2 Q3 Q4 Q5 YOUR NAME Qulity contol Finl exm: // (Thu), 9:-: Q Q Q3 Q4 Q5 YOUR NAME NOTE: Plese wite down the deivtion of you nswe vey clely fo ll questions. The scoe will be educed when you only wite nswe. Also, the scoe will

More information

FI 2201 Electromagnetism

FI 2201 Electromagnetism FI 1 Electomgnetism Alexnde A. Isknd, Ph.D. Physics of Mgnetism nd Photonics Resech Goup Electosttics ELECTRIC PTENTIALS 1 Recll tht we e inteested to clculte the electic field of some chge distiution.

More information

This immediately suggests an inverse-square law for a "piece" of current along the line.

This immediately suggests an inverse-square law for a piece of current along the line. Electomgnetic Theoy (EMT) Pof Rui, UNC Asheville, doctophys on YouTube Chpte T Notes The iot-svt Lw T nvese-sque Lw fo Mgnetism Compe the mgnitude of the electic field t distnce wy fom n infinite line

More information

RELATIVE KINEMATICS. q 2 R 12. u 1 O 2 S 2 S 1. r 1 O 1. Figure 1

RELATIVE KINEMATICS. q 2 R 12. u 1 O 2 S 2 S 1. r 1 O 1. Figure 1 RELAIVE KINEMAICS he equtions of motion fo point P will be nlyzed in two diffeent efeence systems. One efeence system is inetil, fixed to the gound, the second system is moving in the physicl spce nd the

More information

Chapter 7. Kleene s Theorem. 7.1 Kleene s Theorem. The following theorem is the most important and fundamental result in the theory of FA s:

Chapter 7. Kleene s Theorem. 7.1 Kleene s Theorem. The following theorem is the most important and fundamental result in the theory of FA s: Chpte 7 Kleene s Theoem 7.1 Kleene s Theoem The following theoem is the most impotnt nd fundmentl esult in the theoy of FA s: Theoem 6 Any lnguge tht cn e defined y eithe egul expession, o finite utomt,

More information

SAR FOCUSING: SCALED INVERSE FOURIER TRANSFORMATION

SAR FOCUSING: SCALED INVERSE FOURIER TRANSFORMATION Univesität Siegen Poject Secto - Optiml Signl Pocessing - Senso Dt Fusion, Remote Sensing - SAR ZESS SAR FOCUSING: SCALED INVERSE FOURIER TRANSFORMATION AND CHIRP SCALING O. Loeld, A. Hein Univesity o

More information

Ch 26 - Capacitance! What s Next! Review! Lab this week!

Ch 26 - Capacitance! What s Next! Review! Lab this week! Ch 26 - Cpcitnce! Wht s Next! Cpcitnce" One week unit tht hs oth theoeticl n pcticl pplictions! Cuent & Resistnce" Moving chges, finlly!! Diect Cuent Cicuits! Pcticl pplictions of ll the stuff tht we ve

More information

Addressing the envelope

Addressing the envelope Addessing the envelope by P. Hnd* nd D. Wisemn J o u n l Synopsis Most col plnts must un unde conditions of vying feed conditions o e sked to poduce qulities diffeent fom tht used in the design. This cn

More information

Fourier-Bessel Expansions with Arbitrary Radial Boundaries

Fourier-Bessel Expansions with Arbitrary Radial Boundaries Applied Mthemtics,,, - doi:./m.. Pulished Online My (http://www.scirp.og/jounl/m) Astct Fouie-Bessel Expnsions with Aity Rdil Boundies Muhmmd A. Mushef P. O. Box, Jeddh, Sudi Ai E-mil: mmushef@yhoo.co.uk

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 Electicl nd Compute Engineeing, Conell Univesity ECE 303: Electomgnetic Fields nd Wves Fll 007 Homewok 3 Due on Sep. 14, 007 by 5:00 PM Reding Assignments: i) Review the lectue notes. ii) Relevnt

More information

Solution of fuzzy multi-objective nonlinear programming problem using interval arithmetic based alpha-cut

Solution of fuzzy multi-objective nonlinear programming problem using interval arithmetic based alpha-cut Intentionl Jounl of Sttistics nd Applied Mthemtics 016; 1(3): 1-5 ISSN: 456-145 Mths 016; 1(3): 1-5 016 Stts & Mths www.mthsounl.com Received: 05-07-016 Accepted: 06-08-016 C Lognthn Dept of Mthemtics

More information

Chapter Direct Method of Interpolation More Examples Mechanical Engineering

Chapter Direct Method of Interpolation More Examples Mechanical Engineering Chpte 5 iect Method o Intepoltion Moe Exmples Mechnicl Engineeing Exmple Fo the pupose o shinking tunnion into hub, the eduction o dimete o tunnion sht by cooling it though tempetue chnge o is given by

More information

ITI Introduction to Computing II

ITI Introduction to Computing II ITI 1121. Intoduction to Computing II Mcel Tucotte School of Electicl Engineeing nd Compute Science Abstct dt type: Stck Stck-bsed lgoithms Vesion of Febuy 2, 2013 Abstct These lectue notes e ment to be

More information

( ) D x ( s) if r s (3) ( ) (6) ( r) = d dr D x

( ) D x ( s) if r s (3) ( ) (6) ( r) = d dr D x SIO 22B, Rudnick dpted fom Dvis III. Single vile sttistics The next few lectues e intended s eview of fundmentl sttistics. The gol is to hve us ll speking the sme lnguge s we move to moe dvnced topics.

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 Electicl nd Compute Engineeing, Conell Univesity ECE 303: Electomgnetic Fields nd Wves Fll 007 Homewok 4 Due on Sep. 1, 007 by 5:00 PM Reding Assignments: i) Review the lectue notes. ii) Relevnt

More information

EECE 260 Electrical Circuits Prof. Mark Fowler

EECE 260 Electrical Circuits Prof. Mark Fowler EECE 60 Electicl Cicuits Pof. Mk Fowle Complex Numbe Review /6 Complex Numbes Complex numbes ise s oots of polynomils. Definition of imginy # nd some esulting popeties: ( ( )( ) )( ) Recll tht the solution

More information

SMOOTH GRAPH SIGNAL RECOVERY VIA EFFICIENT LAPLACIAN SOLVERS

SMOOTH GRAPH SIGNAL RECOVERY VIA EFFICIENT LAPLACIAN SOLVERS SMOOTH GRAPH SIGNAL RECOVERY VIA EFFICIENT LAPLACIAN SOLVERS Git Bbzdeh Eslmlou, Alexnde Jung 2, Nobet Goetz Institute of Telecommunictions, TU Wien, Austi; {gitbbzdeh, nobetgoetz}@nttuwienct 2 Dept of

More information

Review of Mathematical Concepts

Review of Mathematical Concepts ENEE 322: Signls nd Systems view of Mthemticl Concepts This hndout contins ief eview of mthemticl concepts which e vitlly impotnt to ENEE 322: Signls nd Systems. Since this mteil is coveed in vious couses

More information

7.5-Determinants in Two Variables

7.5-Determinants in Two Variables 7.-eteminnts in Two Vibles efinition of eteminnt The deteminnt of sque mti is el numbe ssocited with the mti. Eve sque mti hs deteminnt. The deteminnt of mti is the single ent of the mti. The deteminnt

More information

Electronic Supplementary Material

Electronic Supplementary Material Electonic Supplementy Mteil On the coevolution of socil esponsiveness nd behvioul consistency Mx Wolf, G Snde vn Doon & Fnz J Weissing Poc R Soc B 78, 440-448; 0 Bsic set-up of the model Conside the model

More information

9.4 The response of equilibrium to temperature (continued)

9.4 The response of equilibrium to temperature (continued) 9.4 The esponse of equilibium to tempetue (continued) In the lst lectue, we studied how the chemicl equilibium esponds to the vition of pessue nd tempetue. At the end, we deived the vn t off eqution: d

More information

Plane Wave Expansion Method (PWEM)

Plane Wave Expansion Method (PWEM) /15/18 Instucto D. Rymond Rumpf (915) 747 6958 cumpf@utep.edu EE 5337 Computtionl Electomgnetics Lectue #19 Plne Wve Expnsion Method (PWEM) Lectue 19 These notes my contin copyighted mteil obtined unde

More information

Friedmannien equations

Friedmannien equations ..6 Fiedmnnien equtions FLRW metic is : ds c The metic intevl is: dt ( t) d ( ) hee f ( ) is function which detemines globl geometic l popety of D spce. f d sin d One cn put it in the Einstein equtions

More information

Multi-agent Framework for Fault Detection & Diagnosis in Transient Operations

Multi-agent Framework for Fault Detection & Diagnosis in Transient Operations 7 th Euopen Symposium on Compute Aided Pocess Engineesing ESCAPE7 V. Plesu nd P.S. Agchi (Editos) 2007 Elsevie B.V. All ights eseved. Multi-gent Fmewok fo Fult Detection & Dignosis in Tnsient Opetions

More information

Lecture 4. Beyond the Hückel π-electron theory. Charge density is an important parameter that is used widely to explain properties of molecules.

Lecture 4. Beyond the Hückel π-electron theory. Charge density is an important parameter that is used widely to explain properties of molecules. Lectue 4. Beyond the Hückel π-electon theoy 4. Chge densities nd bond odes Chge density is n impotnt pmete tht is used widely to explin popeties of molecules. An electon in n obitl ψ = c φ hs density distibution

More information

CHAPTER 18: ELECTRIC CHARGE AND ELECTRIC FIELD

CHAPTER 18: ELECTRIC CHARGE AND ELECTRIC FIELD ollege Physics Student s Mnul hpte 8 HAPTR 8: LTRI HARG AD LTRI ILD 8. STATI LTRIITY AD HARG: OSRVATIO O HARG. ommon sttic electicity involves chges nging fom nnocoulombs to micocoulombs. () How mny electons

More information

SPA7010U/SPA7010P: THE GALAXY. Solutions for Coursework 1. Questions distributed on: 25 January 2018.

SPA7010U/SPA7010P: THE GALAXY. Solutions for Coursework 1. Questions distributed on: 25 January 2018. SPA7U/SPA7P: THE GALAXY Solutions fo Cousewok Questions distibuted on: 25 Jnuy 28. Solution. Assessed question] We e told tht this is fint glxy, so essentilly we hve to ty to clssify it bsed on its spectl

More information

10 Statistical Distributions Solutions

10 Statistical Distributions Solutions Communictions Engineeing MSc - Peliminy Reding 1 Sttisticl Distiutions Solutions 1) Pove tht the vince of unifom distiution with minimum vlue nd mximum vlue ( is ) 1. The vince is the men of the sques

More information

Optimization. x = 22 corresponds to local maximum by second derivative test

Optimization. x = 22 corresponds to local maximum by second derivative test Optimiztion Lectue 17 discussed the exteme vlues of functions. This lectue will pply the lesson fom Lectue 17 to wod poblems. In this section, it is impotnt to emembe we e in Clculus I nd e deling one-vible

More information

Michael Rotkowitz 1,2

Michael Rotkowitz 1,2 Novembe 23, 2006 edited Line Contolles e Unifomly Optiml fo the Witsenhusen Counteexmple Michel Rotkowitz 1,2 IEEE Confeence on Decision nd Contol, 2006 Abstct In 1968, Witsenhusen intoduced his celebted

More information

Probabilistic Retrieval

Probabilistic Retrieval CS 630 Lectue 4: 02/07/2006 Lectue: Lillin Lee Scibes: Pete Bbinski, Dvid Lin Pobbilistic Retievl I. Nïve Beginnings. Motivtions b. Flse Stt : A Pobbilistic Model without Vition? II. Fomultion. Tems nd

More information

Two dimensional polar coordinate system in airy stress functions

Two dimensional polar coordinate system in airy stress functions I J C T A, 9(9), 6, pp. 433-44 Intentionl Science Pess Two dimensionl pol coodinte system in iy stess functions S. Senthil nd P. Sek ABSTRACT Stisfy the given equtions, boundy conditions nd bihmonic eqution.in

More information

Homework 3 MAE 118C Problems 2, 5, 7, 10, 14, 15, 18, 23, 30, 31 from Chapter 5, Lamarsh & Baratta. The flux for a point source is:

Homework 3 MAE 118C Problems 2, 5, 7, 10, 14, 15, 18, 23, 30, 31 from Chapter 5, Lamarsh & Baratta. The flux for a point source is: . Homewok 3 MAE 8C Poblems, 5, 7, 0, 4, 5, 8, 3, 30, 3 fom Chpte 5, msh & Btt Point souces emit nuetons/sec t points,,, n 3 fin the flux cuent hlf wy between one sie of the tingle (blck ot). The flux fo

More information

Electric Potential. and Equipotentials

Electric Potential. and Equipotentials Electic Potentil nd Euipotentils U Electicl Potentil Review: W wok done y foce in going fom to long pth. l d E dl F W dl F θ Δ l d E W U U U Δ Δ l d E W U U U U potentil enegy electic potentil Potentil

More information

Tests for Correlation on Bivariate Non-Normal Data

Tests for Correlation on Bivariate Non-Normal Data Jounl of Moden Applied Sttisticl Methods Volume 0 Issue Aticle 9 --0 Tests fo Coeltion on Bivite Non-Noml Dt L. Bevesdof Noth Colin Stte Univesity, lounneb@gmil.com Ping S Univesity of Noth Floid, ps@unf.edu

More information

D-STABLE ROBUST RELIABLE CONTROL FOR UNCERTAIN DELTA OPERATOR SYSTEMS

D-STABLE ROBUST RELIABLE CONTROL FOR UNCERTAIN DELTA OPERATOR SYSTEMS Jounl of Theoeticl nd Applied nfomtion Technology 8 th Febuy 3. Vol. 48 No.3 5-3 JATT & LLS. All ights eseved. SSN: 99-8645 www.jtit.og E-SSN: 87-395 D-STABLE ROBUST RELABLE CONTROL FOR UNCERTAN DELTA

More information

Qualitative Analysis for Solutions of a Class of. Nonlinear Ordinary Differential Equations

Qualitative Analysis for Solutions of a Class of. Nonlinear Ordinary Differential Equations Adv. Theo. Appl. Mech., Vol. 7, 2014, no. 1, 1-7 HIKARI Ltd, www.m-hiki.com http://dx.doi.og/10.12988/tm.2014.458 Qulittive Anlysis fo Solutions of Clss of Nonline Odiny Diffeentil Equtions Juxin Li *,

More information

The Formulas of Vector Calculus John Cullinan

The Formulas of Vector Calculus John Cullinan The Fomuls of Vecto lculus John ullinn Anlytic Geomety A vecto v is n n-tuple of el numbes: v = (v 1,..., v n ). Given two vectos v, w n, ddition nd multipliction with scl t e defined by Hee is bief list

More information

Physics 604 Problem Set 1 Due Sept 16, 2010

Physics 604 Problem Set 1 Due Sept 16, 2010 Physics 64 Polem et 1 Due ept 16 1 1) ) Inside good conducto the electic field is eo (electons in the conducto ecuse they e fee to move move in wy to cncel ny electic field impessed on the conducto inside

More information

Radial geodesics in Schwarzschild spacetime

Radial geodesics in Schwarzschild spacetime Rdil geodesics in Schwzschild spcetime Spheiclly symmetic solutions to the Einstein eqution tke the fom ds dt d dθ sin θdϕ whee is constnt. We lso hve the connection components, which now tke the fom using

More information

Chapter 25: Current, Resistance and Electromotive Force. Charge carrier motion in a conductor in two parts

Chapter 25: Current, Resistance and Electromotive Force. Charge carrier motion in a conductor in two parts Chpte 5: Cuent, esistnce nd Electomotive Foce Chge cie motion in conducto in two pts Constnt Acceletion F m qe ndomizing Collisions (momentum, enegy) =>esulting Motion Avege motion = Dift elocity = v d

More information

STUDY OF THE UNIFORM MAGNETIC FIELD DOMAINS (3D) IN THE CASE OF THE HELMHOLTZ COILS

STUDY OF THE UNIFORM MAGNETIC FIELD DOMAINS (3D) IN THE CASE OF THE HELMHOLTZ COILS STUDY OF THE UNIFORM MAGNETIC FIED DOMAINS (3D) IN THE CASE OF THE HEMHOTZ COIS FORIN ENACHE, GHEORGHE GAVRIĂ, EMI CAZACU, Key wods: Unifom mgnetic field, Helmholt coils. Helmholt coils e used to estblish

More information

Week 10: DTMC Applications Ranking Web Pages & Slotted ALOHA. Network Performance 10-1

Week 10: DTMC Applications Ranking Web Pages & Slotted ALOHA. Network Performance 10-1 Week : DTMC Alictions Rnking Web ges & Slotted ALOHA etwok efonce - Outline Aly the theoy of discete tie Mkov chins: Google s nking of web-ges Wht ge is the use ost likely seching fo? Foulte web-gh s Mkov

More information

Deterministic simulation of a NFA with k symbol lookahead

Deterministic simulation of a NFA with k symbol lookahead Deteministic simultion of NFA with k symbol lookhed SOFSEM 7 Bl Rvikum, Clifoni Stte Univesity (joint wok with Nic Snten, Univesity of Wteloo) Oveview Definitions: DFA, NFA nd lookhed DFA Motivtion: utomted

More information

Integrals and Polygamma Representations for Binomial Sums

Integrals and Polygamma Representations for Binomial Sums 3 47 6 3 Jounl of Intege Sequences, Vol. 3 (, Aticle..8 Integls nd Polygmm Repesenttions fo Binomil Sums Anthony Sofo School of Engineeing nd Science Victoi Univesity PO Box 448 Melboune City, VIC 8 Austli

More information

Chapter 25: Current, Resistance and Electromotive Force. ~10-4 m/s Typical speeds ~ 10 6 m/s

Chapter 25: Current, Resistance and Electromotive Force. ~10-4 m/s Typical speeds ~ 10 6 m/s Chpte 5: Cuent, esistnce nd lectomotive Foce Chge cie motion in conducto in two pts Constnt Acceletion F m q ndomizing Collisions (momentum, enegy) >esulting Motion http://phys3p.sl.psu.edu/phys_nim/m/ndom_wlk.vi

More information

(a) Counter-Clockwise (b) Clockwise ()N (c) No rotation (d) Not enough information

(a) Counter-Clockwise (b) Clockwise ()N (c) No rotation (d) Not enough information m m m00 kg dult, m0 kg bby. he seesw stts fom est. Which diection will it ottes? ( Counte-Clockwise (b Clockwise ( (c o ottion ti (d ot enough infomtion Effect of Constnt et oque.3 A constnt non-zeo toque

More information

U>, and is negative. Electric Potential Energy

U>, and is negative. Electric Potential Energy Electic Potentil Enegy Think of gvittionl potentil enegy. When the lock is moved veticlly up ginst gvity, the gvittionl foce does negtive wok (you do positive wok), nd the potentil enegy (U) inceses. When

More information

Algebra Based Physics. Gravitational Force. PSI Honors universal gravitation presentation Update Fall 2016.notebookNovember 10, 2016

Algebra Based Physics. Gravitational Force. PSI Honors universal gravitation presentation Update Fall 2016.notebookNovember 10, 2016 Newton's Lw of Univesl Gvittion Gvittionl Foce lick on the topic to go to tht section Gvittionl Field lgeb sed Physics Newton's Lw of Univesl Gvittion Sufce Gvity Gvittionl Field in Spce Keple's Thid Lw

More information

Reference-Dependent Stochastic User Equilibrium with Endogenous Reference Points

Reference-Dependent Stochastic User Equilibrium with Endogenous Reference Points EJTIR Issue 3(2), 203 pp. 47-68 ISSN: 567-74 www.eti.tbm.tudelft.nl Refeence-Dependent Stochstic Use Equilibium with Endogenous Refeence Points Polo Delle Site, Fncesco Filippi nd Cludi Cstldi Deptment

More information

A Deep Convolutional Neural Network Based on Nested Residue Number System

A Deep Convolutional Neural Network Based on Nested Residue Number System A Deep Convolutional Neual Netwok Based on Nested Residue Numbe System Hioki Nakahaa Ehime Univesity, Japan Tsutomu Sasao Meiji Univesity, Japan Abstact A pe-tained deep convolutional neual netwok (DCNN)

More information

Mark Scheme (Results) January 2008

Mark Scheme (Results) January 2008 Mk Scheme (Results) Jnuy 00 GCE GCE Mthemtics (6679/0) Edecel Limited. Registeed in Englnd nd Wles No. 4496750 Registeed Office: One90 High Holbon, London WCV 7BH Jnuy 00 6679 Mechnics M Mk Scheme Question

More information

Mathematical formulation of the F 0 motor model

Mathematical formulation of the F 0 motor model negy Tnsduction in TP Synthse: Supplement Mthemticl fomultion of the F 0 moto model. Mkov chin model fo the evolution of the oto stte The fou possible potontion sttes of the two oto sp61 sites t the otostto

More information

Class Summary. be functions and f( D) , we define the composition of f with g, denoted g f by

Class Summary. be functions and f( D) , we define the composition of f with g, denoted g f by Clss Summy.5 Eponentil Functions.6 Invese Functions nd Logithms A function f is ule tht ssigns to ech element D ectly one element, clled f( ), in. Fo emple : function not function Given functions f, g:

More information

Effective Performance Improvement of Hawt Blades using Optimization Technique Process

Effective Performance Improvement of Hawt Blades using Optimization Technique Process Intentionl Jounl of Engineeing nd Mngement Resech, Vol.-, Issue-1, Febuy 01 ISSN No.: 50-0758 Pges: -9 www.ijem.net Effective Pefomnce Impovement of Hwt Bldes using Optimiztion Technique Pocess R. SenthilKum

More information

ASTR415: Problem Set #6

ASTR415: Problem Set #6 ASTR45: Poblem Set #6 Cuan D. Muhlbege Univesity of Mayland (Dated: May 7, 27) Using existing implementations of the leapfog and Runge-Kutta methods fo solving coupled odinay diffeential equations, seveal

More information

10 m, so the distance from the Sun to the Moon during a solar eclipse is. The mass of the Sun, Earth, and Moon are = =

10 m, so the distance from the Sun to the Moon during a solar eclipse is. The mass of the Sun, Earth, and Moon are = = Chpte 1 nivesl Gvittion 11 *P1. () The un-th distnce is 1.4 nd the th-moon 8 distnce is.84, so the distnce fom the un to the Moon duing sol eclipse is 11 8 11 1.4.84 = 1.4 The mss of the un, th, nd Moon

More information

NS-IBTS indices calculation procedure

NS-IBTS indices calculation procedure ICES Dt Cente DATRAS 1.1 NS-IBTS indices 2013 DATRAS Pocedue Document NS-IBTS indices clcultion pocedue Contents Genel... 2 I Rw ge dt CA -> Age-length key by RFA fo defined ge nge ALK... 4 II Rw length

More information

Measurements of Particle Size Distribution Based on Mie Scattering Theory and Markov Chain Inversion Algorithm

Measurements of Particle Size Distribution Based on Mie Scattering Theory and Markov Chain Inversion Algorithm JOURNA OF SOFTWARE, VO. 7, NO., OCTOBER 39 Mesuements of Pticle Size Distibution Bsed on Mie Sctteing Theoy nd Mkov Chin Invesion Algoithm Zi Ye Deptment of Infomtion nd Electonic Engineeing, Chin Univesity

More information

Numerical Investigation of Flow in a New DC Pump MHD

Numerical Investigation of Flow in a New DC Pump MHD Jounl of pplied Fluid Mechnics, Vol., No., pp. 3-8, 9. vilble online t www.jfmonline.net, ISSN 735-3645. Numeicl Investigtion of Flow in New DC Pump MHD N. Bennecib, S. Did nd R. bdessemed 3 Univesity

More information

Elastic scattering of 4 He atoms at the surface of liquid helium

Elastic scattering of 4 He atoms at the surface of liquid helium Indin Jounl of Pue & Applied Physics Vol. 48, Octobe, pp. 743-748 Elstic sctteing of 4 He toms t the sufce of liquid helium P K Toongey, K M Khnn, Y K Ayodo, W T Skw, F G Knyeki, R T Eki, R N Kimengichi

More information

Radiowave Propagation Modelling using the Uniform Theory of Diffraction

Radiowave Propagation Modelling using the Uniform Theory of Diffraction Deptment of lecticl nd lectonic ngineeing Pt IV Poject Repot Ye 2003 inl Repot Rdiowve Popgtion Modelling using the Unifom Theoy of Diffction chool of ngineeing The Univesity of Aucklnd Cho-Wei Chng 2365708

More information

Language Processors F29LP2, Lecture 5

Language Processors F29LP2, Lecture 5 Lnguge Pocessos F29LP2, Lectue 5 Jmie Gy Feuy 2, 2014 1 / 1 Nondeteministic Finite Automt (NFA) NFA genelise deteministic finite utomt (DFA). They llow sevel (0, 1, o moe thn 1) outgoing tnsitions with

More information

Physics 1502: Lecture 2 Today s Agenda

Physics 1502: Lecture 2 Today s Agenda 1 Lectue 1 Phsics 1502: Lectue 2 Tod s Agend Announcements: Lectues posted on: www.phs.uconn.edu/~cote/ HW ssignments, solutions etc. Homewok #1: On Mstephsics this Fid Homewoks posted on Msteingphsics

More information

Production Mechanism of Quark Gluon Plasma in Heavy Ion Collision. Ambar Jain And V.Ravishankar

Production Mechanism of Quark Gluon Plasma in Heavy Ion Collision. Ambar Jain And V.Ravishankar Poduction Mechnism of Quk Gluon Plsm in Hevy Ion Collision Amb Jin And V.Rvishnk Pimy im of theoeticlly studying URHIC is to undestnd Poduction of quks nd gluons tht fom the bulk of the plsm ( ) t 0 Thei

More information

Scientific Computing & Modelling NV, Vrije Universiteit, Theoretical Chemistry, De Boelelaan 1083, 1081 HV Amsterdam, The Netherlands c

Scientific Computing & Modelling NV, Vrije Universiteit, Theoretical Chemistry, De Boelelaan 1083, 1081 HV Amsterdam, The Netherlands c Electonic Supplementy Mteil (ESI) fo Physicl Chemisty Chemicl Physics. This jounl is The Royl Society of Chemisty 2014 Suppoting Infomtion fo: Pedicting phosphoescent lifetimes nd zeo-field splitting of

More information

Prof. Dr. Yong-Su Na (32-206, Tel )

Prof. Dr. Yong-Su Na (32-206, Tel ) Fusion Recto Technology I (459.76, 3 Cedits) Pof. D. Yong-Su N (3-6, Tel. 88-74) Contents Week 1. Mgnetic Confinement Week -3. Fusion Recto Enegetics Week 4. sic Tokmk Plsm Pmetes Week 5. Plsm Heting nd

More information

Illustrating the space-time coordinates of the events associated with the apparent and the actual position of a light source

Illustrating the space-time coordinates of the events associated with the apparent and the actual position of a light source Illustting the spe-time oointes of the events ssoite with the ppent n the tul position of light soue Benh Rothenstein ), Stefn Popesu ) n Geoge J. Spi 3) ) Politehni Univesity of Timiso, Physis Deptment,

More information

dx was area under f ( x ) if ( ) 0

dx was area under f ( x ) if ( ) 0 13. Line Integls Line integls e simil to single integl, f ( x) dx ws e unde f ( x ) if ( ) 0 Insted of integting ove n intevl [, ] (, ) f xy ds f x., we integte ove cuve, (in the xy-plne). **Figue - get

More information

3.1 Magnetic Fields. Oersted and Ampere

3.1 Magnetic Fields. Oersted and Ampere 3.1 Mgnetic Fields Oested nd Ampee The definition of mgnetic induction, B Fields of smll loop (dipole) Mgnetic fields in mtte: ) feomgnetism ) mgnetiztion, (M ) c) mgnetic susceptiility, m d) mgnetic field,

More information

AXIAL GAP ELECTROSTATIC WOBBLE MICROMOTOR

AXIAL GAP ELECTROSTATIC WOBBLE MICROMOTOR XIL GP ELETOSTTI WOLE MIOMOTO nc TOMESU Soin NTONIU F.M.G. TOMESU Electicl Engineeing Dept. POLITEHNI Univesity uchest ãzvn MOEI ING OMNI uchest The toque vesus ngle mechnicl chcteistic of n xil gp electosttic

More information

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3 DEPATMENT OF CIVIL AND ENVIONMENTAL ENGINEEING FLID MECHANICS III Solutions to Poblem Sheet 3 1. An tmospheic vote is moelle s combintion of viscous coe otting s soli boy with ngul velocity Ω n n iottionl

More information

THEORY OF EQUATIONS OBJECTIVE PROBLEMS. If the eqution x 6x 0 0 ) - ) 4) -. If the sum of two oots of the eqution k is -48 ) 6 ) 48 4) 4. If the poduct of two oots of 4 ) -4 ) 4) - 4. If one oot of is

More information

Comparative Studies of Law of Gravity and General Relativity. No.1 of Comparative Physics Series Papers

Comparative Studies of Law of Gravity and General Relativity. No.1 of Comparative Physics Series Papers Comptive Studies of Lw of Gvity nd Genel Reltivity No. of Comptive hysics Seies pes Fu Yuhu (CNOOC Resech Institute, E-mil:fuyh945@sin.com) Abstct: As No. of comptive physics seies ppes, this ppe discusses

More information

RELATIONSHIP BETWEEN DESIGN RESPONSE SPECTRA FOR RARE AND FREQUENT EARTHQUAKE LEVELS

RELATIONSHIP BETWEEN DESIGN RESPONSE SPECTRA FOR RARE AND FREQUENT EARTHQUAKE LEVELS th Wold Confeence on Ethquke Engineeing ncouve, B.C., Cnd ugust -6, 00 Ppe No. 9 ELIONHIP BEWEEN EIGN EPONE PEC O E N EQUEN EHQUKE LEEL Yingmin LI Cheng HI Ming LI Ling HN UMMY It is known tht uilding

More information

Focal plane invariant algorithm for digital reconstruction of holograms recorded in the near diffraction zone

Focal plane invariant algorithm for digital reconstruction of holograms recorded in the near diffraction zone Focl plne invint lgoithm fo digitl econstuction of hologms ecoded in the ne diffction zone L. Yoslvs,. Ben-Dvid, Dept. of Intedisciplin Studies, Fcult of Engineeing, Tel Aviv Univesit, 69978 Tel Aviv,

More information

EXTENDING THE OLAP FRAMEWORK FOR AUTOMATED EXPLANATORY TASKS

EXTENDING THE OLAP FRAMEWORK FOR AUTOMATED EXPLANATORY TASKS EXTENDING THE OLAP FRAMEWORK FOR AUTOMATED EXPLANATORY TASKS Emiel Con 1, Hennie Dniels 1,2 1 Esmus Univesity Rottedm, ERIM Institute of Advnced Mngement Studies, PO Box 90153, 3000 DR Rottedm, The Nethelnds,

More information

Math 4318 : Real Analysis II Mid-Term Exam 1 14 February 2013

Math 4318 : Real Analysis II Mid-Term Exam 1 14 February 2013 Mth 4318 : Rel Anlysis II Mid-Tem Exm 1 14 Febuy 2013 Nme: Definitions: Tue/Flse: Poofs: 1. 2. 3. 4. 5. 6. Totl: Definitions nd Sttements of Theoems 1. (2 points) Fo function f(x) defined on (, b) nd fo

More information

Find this material useful? You can help our team to keep this site up and bring you even more content consider donating via the link on our site.

Find this material useful? You can help our team to keep this site up and bring you even more content consider donating via the link on our site. Find this mteil useful? You cn help ou tem to keep this site up nd bing you even moe content conside donting vi the link on ou site. Still hving touble undestnding the mteil? Check out ou Tutoing pge to

More information

Available online at ScienceDirect. Procedia Engineering 91 (2014 ) 32 36

Available online at   ScienceDirect. Procedia Engineering 91 (2014 ) 32 36 Aville online t wwwsciencediectcom ScienceDiect Pocedi Engineeing 91 (014 ) 3 36 XXIII R-S-P semin Theoeticl Foundtion of Civil Engineeing (3RSP) (TFoCE 014) Stess Stte of Rdil Inhomogeneous Semi Sphee

More information

π,π is the angle FROM a! TO b

π,π is the angle FROM a! TO b Mth 151: 1.2 The Dot Poduct We hve scled vectos (o, multiplied vectos y el nume clled scl) nd dded vectos (in ectngul component fom). Cn we multiply vectos togethe? The nswe is YES! In fct, thee e two

More information

Investigations of Boundary Treatments in Incompressible Smoothed Particle Hydrodynamics for Fluid-Structural Interactions

Investigations of Boundary Treatments in Incompressible Smoothed Particle Hydrodynamics for Fluid-Structural Interactions Recent Reseches in Mechnics Investigtions of Boundy Tetments in Incompessile Smoothed Pticle Hydodynmics fo Fluid-Stuctul Intections Fnfn Sun, Mingyi Tn, nd Jing T Xing Astct Two oundy tetment methods

More information

Modelling of Low Velocity Impact Damage in Laminated Composites

Modelling of Low Velocity Impact Damage in Laminated Composites Modelling of Lo Velocity Impct mge in Lminted Composites J. Lee*, C. Soutis*, P. T. Cutis nd C. Kong** *Aeospce Engineeing, The Univesity of Sheffield, Sheffield S 3J, UK efence Science nd Technology Lbotoy,

More information

Collection of Formulas

Collection of Formulas Collection of Fomuls Electomgnetic Fields EITF8 Deptment of Electicl nd Infomtion Technology Lund Univesity, Sweden August 8 / ELECTOSTATICS field point '' ' Oigin ' Souce point Coulomb s Lw The foce F

More information

igid nd non-leky two-comptment building. Yu et l [8] developed non-line govening equtions by consideing the effect of bckgound lekge. Howeve, thee e n

igid nd non-leky two-comptment building. Yu et l [8] developed non-line govening equtions by consideing the effect of bckgound lekge. Howeve, thee e n The Seventh Intentionl Colloquium on Bluff Body Aeodynmics nd Applictions (BBAA7) Shnghi, Chin; Septembe -, Coupled vibtion between wind-induced intenl pessues nd lge spn oof fo two-comptment building

More information

1 Using Integration to Find Arc Lengths and Surface Areas

1 Using Integration to Find Arc Lengths and Surface Areas Novembe 9, 8 MAT86 Week Justin Ko Using Integtion to Find Ac Lengths nd Sufce Aes. Ac Length Fomul: If f () is continuous on [, b], then the c length of the cuve = f() on the intevl [, b] is given b s

More information

CHAPTER 2 ELECTROSTATIC POTENTIAL

CHAPTER 2 ELECTROSTATIC POTENTIAL 1 CHAPTER ELECTROSTATIC POTENTIAL 1 Intoduction Imgine tht some egion of spce, such s the oom you e sitting in, is pemeted by n electic field (Pehps thee e ll sots of electiclly chged bodies outside the

More information

New Procedure for Optimal Design of Sequential Experiments in Kinetic Models

New Procedure for Optimal Design of Sequential Experiments in Kinetic Models 62 Ind. Eng. Chem. Res. 1994,33,62-68 New Pocedue fo Optiml Design of Sequentil Expeiments in Kinetic Models Vincenzo G. Dovi,' Ande P. Revebei, nd Leond0 Acevedo-Dutet ISTIC-UnivesitB di Genov, Vi Ope

More information

Chapter 21: Electric Charge and Electric Field

Chapter 21: Electric Charge and Electric Field Chpte 1: Electic Chge nd Electic Field Electic Chge Ancient Gees ~ 600 BC Sttic electicit: electic chge vi fiction (see lso fig 1.1) (Attempted) pith bll demonsttion: inds of popeties objects with sme

More information

4.2 Boussinesq s Theory. Contents

4.2 Boussinesq s Theory. Contents 00477 Pvement Stuctue 4. Stesses in Flexible vement Contents 4. Intoductions to concet of stess nd stin in continuum mechnics 4. Boussinesq s Theoy 4. Bumiste s Theoy 4.4 Thee Lye System Weekset Sung Chte

More information

Lectures # He-like systems. October 31 November 4,6

Lectures # He-like systems. October 31 November 4,6 Lectue #5-7 7 Octoe 3 oveme 4,6 Self-conitent field Htee-Foc eqution: He-lie ytem Htee-Foc eqution: cloed-hell hell ytem Chpte 3, pge 6-77, Lectue on Atomic Phyic He-lie ytem H (, h ( + h ( + h ( Z Z:

More information

Dan G. Cacuci Department of Mechanical Engineering, University of South Carolina

Dan G. Cacuci Department of Mechanical Engineering, University of South Carolina SECOND-ORDER ADJOINT SENSITIVITY ANALYSIS METHODOLOGY ( nd -ASAM) FOR LARGE-SCALE NONLINEAR SYSTEMS: II. APPLICATION TO A NONLINEAR HEAT CONDUCTION BENCHMARK Dn G. Ccuci Deptment of Mechnicl Engineeing

More information