Parallel Concatenated Convolutional Codes (PCCC) or Turbo Codes

Size: px
Start display at page:

Download "Parallel Concatenated Convolutional Codes (PCCC) or Turbo Codes"

Transcription

1 Conatnatd Coding Paralll Conatnatd Convoltional Cod PCCC or Trbo Cod Firt Papr: NEAR SHANNON LIMIT ERROR-CORRECTING CODING AND DECODING: TURBO CODES1 by Clad Brro, Alain Glavix and Pnya Thitimajhima Eol National Sprir d Tlommniation ENST d Brtagn, Fran Intrnational Commniation Confrn ICC, Gnva, Switzrland May 1993, pp ytmati od nonytmati on hav qivalnt form ytmati od with fd forward nodr prod l powrfl od. Convoltional od in thir ytmati fdba form ar qivalnt to th nonytmati form in ditan and nart nighbor path proprti. Howvr at low ignal to noi ratio SNR, th bit rror rat BER i lightly bttr. Figr of FB-CC and FF-CC for R=1/2 v=2. x,1 x,2 x,1 = x,2-9 -

2 X d C 1 2, 1, 2 rriv ytmati onvoltional od dlay lin L 1 Y 1 Intrlavi ng Y 2 Y C 2 2, 1, 2 rriv ytmati onvoltional od W an now dod th information qn or mov to th ond dodr whih will dod for th am information qn bt in th intrlavd form. Now w ll ma of th L i gnratd by th firt nodr. Thi an b givn a a priori L i a L I2 i -aftr intrlaving information to th ond dodr. So fftivly w an intrlav L y i and L i and fd it to th ond dodr. p ap i t =-1 and p ap i t =1 an b d aoiatd with γ, in th allation of α,β for th ond dodr. Th th otpt of th ond dodr will b of th form L app i = L y2 i L I2 i L 2 i

3 Thi finih th firt or initial fll doding tp- tp 0. L 2 i rflt th xtrini information gnratd by th ond dodr. Now in a imilar mannr a arlir w an giv - fdba th firt dodr with L 2 i γto allat α,β aftr dintrlaving a nw a priori L I1 i information to th firt dodr. Doding tp 1 Firt Dodr L app i = L y i L I1 i L 1 i Sond Dodr aftr intrlaving L 1 i L app i = L y i L I2 i L 2 i Thn from dodr two fdba L 2 i a bfor to th firt dodr aftr dintrlaving and th pro rpat. Thi i nown a itrativ doding or trbo doding. Rmmbr it i alway th xtrini information that w pa to th nxt dodr a nw a priori. W don t fdba a priori or intrini informationwhy? that wa alrady gnratd by th arlir dodr o no point in fding ba th am information

4 LEAVING x 16-STATE DECODER DEC 1 INTER- LEAVING 16-STATE DECODER DEC 2 y DEINTER- DEINTER- LEAVING DEMUX/ INSERTIO dodd otpt dˆ Th p I i t =±1 ndd to allat γan alo b obtaind from L I i whih will in trn b obtaind from L i of th arlir doding tag. Rfrn: Itrativ Doding of Binary Blo and Convoltional Cod by Joahim Hagnar, El Offr, and Ltz Pap, IEEE Tan. Info. Thory, Vol. 42, No.2, Marh 1996, pp Txt Boo Chaptr: Bort : Chaptr 8 on Convoltional Cod and Appndix A on SCC, PCC Fndamntal of Convoltional Coding: Chaptr 7- Itrativ Doding

5 PCCC Rfrn: A oft-inpt Soft-Otpt maximm A Potriori MAP Modl to Dod Paralll and Srial Conatnatd Cod S. Bndtto, D. Divalar, G. Montori, and F. Pollara TDA Progr Rport , Novmbr 1996 from JPL wb it Blo diagram: Enodr ENCODER 1 RATE=1/2 TO CHANNEL ENCODER 2 RATE=1/2 NOT TRANSMITTED TO CHANNEL Dodr. rprnt log probabiliti or woring in th log domain. From Dmod From Dmod ;I ;O Not d ;I ;ONot d SISO SISO 1 2 ;I ;O :I ;O 1 Diion SISO oft-inpt, oft-otpt Modl: implmnt MAP algorithm 13

6 Th gnral Trlli Enodr: INPUT TRELLIS OUTPUT ENCODER SCCC Srial Conatnatd Convoltional Cod Enodr: OUTER ENCODER RATE=1/2 p TO CHANNEL INNER ENCODER RATE=2/3 Dodr: From Dmod ;I SISO ;O Not d ;I INNER ;O :I 1 SISO ;O OUTER ;I ;O DECISION

7 Diffrn btwn PCCC and SCCC: PCCC: Updatd probabiliti xtrini of od ymbol ar nvr d by th doding algorithm SCCC: Both, pdatd probabiliti xtrini of th inpt and od ymbol ar d in th doding algorithm Doding algorithm i Additiv SISO algorithm A-SISO woring in th log domain ;I ;I SISO ;O ;O E S, An Edg of th Trlli Stion Th following fntion ar aoiatd with ah dg Th tarting tat S Th nding tat E Th inpt ymbol Th otpt ymbol 15

8 16 Th rlationhip btwn th fntion dpnd on th partilar nodr. A an xampl, in th a of ytmati nodr, E, alo idntifi th dg in i niqly dtrmind by. Hr it i only amd that th pair S, niqly idntifi th nding tat E thi amption i alway vrifid, a it i qivalnt to ay that givn th initial trlli tat, thr i a on-to-on orrpondn btwn inpt qn and tat qn. Th Additiv SISO Algorithm A-SISO n I I S E 1,2,..., ]} ; ] ; ] xp{ log : 1 = = = α α 1,..,0, ]} ; ] ; ] xp{ log : = = = n I I S E β β Th ar forward and baward rrion. At tim, th otpt xtrini probability ditribtion ar omptd a approximatly = = E S I O : 1 ]} ] ; ] xp{ log ; β α = = E S I O : 1 ]} ] ; ] xp{ log ; β α with initial val α 0 = 0 for =S 0 othrwi α 0 = -

9 imilarly βn = 0 for =S n othrwi β n = - So w rpla log and xp with maximm val. Th w hav th following t of qation. E α = max : = {α -1 S ;I] ;I]}, =1,2..,n S β = max : = {β 1 E 1 ;I] 1 ;I]}, =n-1,,0 ;O = max := {α -1 S ;I] β E ]} ;O = max := {α -1 S ;I] β E ]} Gnrally for rial onatnatd od: OUTER CODE- NON RECURSIVE or NON-Fd ba, Non ytmati INNER CODE- RECURSIVE SYSTEMATIC or Fd-ba Sytmati It i n that th prforman of SCCC i ally bttr than that of PCCC. BER SCCC PCCC Error Floor Efft in PCCC E b /N 0 17

10 Th mmation involvd in th algorithm ar allatd ing trlli dg, rathr than ing pair of tat. Thi ma th algorithm gnral and apabl of daling with paralll dg itabl for TCM. Th A-SISO algorithm at Bit Lvl Conidr a rat ½ onvoltional nodr. U inpt and C 1, and C 2, otpt bit at tim, taing val {0,1}. Thrfor on th trlli dg at tim w hav, 1,, 2,. Drop for impliity. Dfin th rliability LLR of a bit Z taing val {0,1} at tim a P Z = 1;.] λ Z;.] log = Z = 1;.] Z = 0;.] P Z = 0;.] E α = max : = {α -1 S λ ;I] 1 λ C 1 ;I] 2 λ C 2 ;I] } h α β = max : S = {β 1 E λ 1 ;I] 1 λ 1 C 1 ;I] 2 λ 1 C 2 ;I] } h β with initial val α 0 = 0 if =S 0 and α 0 = - othrwi and β n =0 if =S n and β n = - othrwi. h α and h β ar normalization ontant. For th innr dodr, whih i onntd to th AWGN hannl, w hav λ C 1 ;I]= 2A/σ 2 r 1, λ C 2 ;I]= 2A/σ 2 r 2, whr r i, = A2Z i - 1 i,, i=1,2 i th rivd ampl at th otpt of th mathd filtr, i {-1,1} and n i, i th zro man indpndnt idntially ditribtd i.i.d. Gaian noi ampl with varian σ 2. 18

11 Th xtrini bit information for U,C 1 and C 2 an b obtaind a λ U;O = max :=1 {α -1 S 1 λ C 1 ;I] 2 λ C 2 ;I] β E ]} - max :=0 {α -1 S 1 λ C 1 ;I] 2 λ C 2 ;I] β E ]} λ C 1 ;O = max :1=1 {α -1 S λ U;I] 2 λ C 2 ;I] β E ]} - max :1=0 {α -1 S λ U;I] 2 λ C 2 ;I] β E ]} λ C 2 ;O = max :2=1 {α -1 S λ U;I] 1 λ C 1 ;I] β E ]} - max :2=0 {α -1 S λ U;I] 1 λ C 1 ;I] β E ]} Paramtr for PCCC In gnral for a Convoltional od CC w min i dfind a th minimm information wight in th rror vnt of th CC. w min = 1 for non rriv od w min = 2 for rriv od. Th rror offiint in p b rror intrlaving gain for a PCCC with larg intrlaving lngth go a N 1-w min, whr N i th intrlavr lngth. 19

12 Th for rriv CC th intrlaving gain or BER rdtion go a 1/N. On th othr hand all nonrriv CC and blo od hav w min = 1, o h od ar not fl in Paralll Conatnatd Cod. Th nxt mot important ontitnt od paramtr i z min, th minimm parity-h wight in th od qn with w=2. For a larg rang of SNR, th bhavior of PCCC i dtrmind by th fftiv fr ditan d fr,ff = 2 2 z min. It i poibl to ahiv z min = n-12 v-1 2 with a rat 1/n rriv CC with mmory v. PCCC xhibit rror floor fft dfind a th hang of lop of BER rv for Trbo od at lowr BER. Initially th oding gain inra with th nmbr of itration. Howvr, aftr a nmbr of itration in AWGN th prforman improvmnt i marginal. Extnion to onidr: 1. Trbo od with mltilvl modlation 2. Trbo TCM 3. Itrativ Eqalization and Doding Trbo Eqalization. 20

Master Thesis Seminar

Master Thesis Seminar Mar Thi minar Hlinki Univriy of Thnology Dparmn of Elrial and Commniaion Enginring Commniaion laboraory Mar hi rforman Evalaion of rially Conanad pa-tim Cod by Aboda Abdlla Ali prvior: prof vn-gav Häggman

More information

Iterative Data Detection and Channel Estimation for Single-Parity Check-Product Coded MIMO Wireless Communications System

Iterative Data Detection and Channel Estimation for Single-Parity Check-Product Coded MIMO Wireless Communications System Itrativ Data Dttion and Channl Estimation for Singl-Parity Ch-Produt Codd MIMO Wirlss Communiations Systm Muladi *, N. Fisal, S. K. Yusof Dpartmnt of Tlmatis and Opti Communiations Fa. of Eltrial Eng.,

More information

SER/BER in a Fading Channel

SER/BER in a Fading Channel SER/BER in a Fading Channl Major points for a fading channl: * SNR is a R.V. or R.P. * SER(BER) dpnds on th SNR conditional SER(BER). * Two prformanc masurs: outag probability and avrag SER(BER). * Ovrall,

More information

u 3 = u 3 (x 1, x 2, x 3 )

u 3 = u 3 (x 1, x 2, x 3 ) Lctur 23: Curvilinar Coordinats (RHB 8.0 It is oftn convnint to work with variabls othr than th Cartsian coordinats x i ( = x, y, z. For xampl in Lctur 5 w mt sphrical polar and cylindrical polar coordinats.

More information

[ ] 1+ lim G( s) 1+ s + s G s s G s Kacc SYSTEM PERFORMANCE. Since. Lecture 10: Steady-state Errors. Steady-state Errors. Then

[ ] 1+ lim G( s) 1+ s + s G s s G s Kacc SYSTEM PERFORMANCE. Since. Lecture 10: Steady-state Errors. Steady-state Errors. Then SYSTEM PERFORMANCE Lctur 0: Stady-tat Error Stady-tat Error Lctur 0: Stady-tat Error Dr.alyana Vluvolu Stady-tat rror can b found by applying th final valu thorm and i givn by lim ( t) lim E ( ) t 0 providd

More information

A Study on Simulating Convolutional Codes and Turbo Codes

A Study on Simulating Convolutional Codes and Turbo Codes A Study on Simulating Convolutional Code and Turbo Code Final Report By Daniel Chang July 27, 2001 Advior: Dr. P. Kinman Executive Summary Thi project include the deign of imulation of everal convolutional

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by D. Klain Vrsion 207.0.05 Corrctions and commnts ar wlcom. Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix A A k I + A + k!

More information

(1) Then we could wave our hands over this and it would become:

(1) Then we could wave our hands over this and it would become: MAT* K285 Spring 28 Anthony Bnoit 4/17/28 Wk 12: Laplac Tranform Rading: Kohlr & Johnon, Chaptr 5 to p. 35 HW: 5.1: 3, 7, 1*, 19 5.2: 1, 5*, 13*, 19, 45* 5.3: 1, 11*, 19 * Pla writ-up th problm natly and

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 Corrctions and commnts ar wlcom Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix () A A k I + A + k!

More information

Chapter 6 Folding. Folding

Chapter 6 Folding. Folding Chaptr 6 Folding Wintr 1 Mokhtar Abolaz Folding Th folding transformation is usd to systmatically dtrmin th control circuits in DSP architctur whr multipl algorithm oprations ar tim-multiplxd to a singl

More information

Search sequence databases 3 10/25/2016

Search sequence databases 3 10/25/2016 Sarch squnc databass 3 10/25/2016 Etrm valu distribution Ø Suppos X is a random variabl with probability dnsity function p(, w sampl a larg numbr S of indpndnt valus of X from this distribution for an

More information

Junction Tree Algorithm 1. David Barber

Junction Tree Algorithm 1. David Barber Juntion Tr Algorithm 1 David Barbr Univrsity Collg London 1 Ths slids aompany th book Baysian Rasoning and Mahin Larning. Th book and dmos an b downloadd from www.s.ul.a.uk/staff/d.barbr/brml. Fdbak and

More information

Chapter 10 Time-Domain Analysis and Design of Control Systems

Chapter 10 Time-Domain Analysis and Design of Control Systems ME 43 Sytm Dynamic & Control Sction 0-5: Stady Stat Error and Sytm Typ Chaptr 0 Tim-Domain Analyi and Dign of Control Sytm 0.5 STEADY STATE ERRORS AND SYSTEM TYPES A. Bazoun Stady-tat rror contitut an

More information

1 Minimum Cut Problem

1 Minimum Cut Problem CS 6 Lctur 6 Min Cut and argr s Algorithm Scribs: Png Hui How (05), Virginia Dat: May 4, 06 Minimum Cut Problm Today, w introduc th minimum cut problm. This problm has many motivations, on of which coms

More information

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes Procdings of th 9th WSEAS Intrnational Confrnc on APPLICATIONS of COMPUTER ENGINEERING A Sub-Optimal Log-Domain Dcoding Algorithm for Non-Binary LDPC Cods CHIRAG DADLANI and RANJAN BOSE Dpartmnt of Elctrical

More information

EECE 301 Signals & Systems Prof. Mark Fowler

EECE 301 Signals & Systems Prof. Mark Fowler EECE 301 Signals & Systms Prof. Mark Fowlr ot St #21 D-T Signals: Rlation btwn DFT, DTFT, & CTFT 1/16 W can us th DFT to implmnt numrical FT procssing This nabls us to numrically analyz a signal to find

More information

Utilizing exact and Monte Carlo methods to investigate properties of the Blume Capel Model applied to a nine site lattice.

Utilizing exact and Monte Carlo methods to investigate properties of the Blume Capel Model applied to a nine site lattice. Utilizing xat and Mont Carlo mthods to invstigat proprtis of th Blum Capl Modl applid to a nin sit latti Nik Franios Writing various xat and Mont Carlo omputr algorithms in C languag, I usd th Blum Capl

More information

Computing and Communications -- Network Coding

Computing and Communications -- Network Coding 89 90 98 00 Computing and Communications -- Ntwork Coding Dr. Zhiyong Chn Institut of Wirlss Communications Tchnology Shanghai Jiao Tong Univrsity China Lctur 5- Nov. 05 0 Classical Information Thory Sourc

More information

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields Lctur 37 (Schrödingr Equation) Physics 6-01 Spring 018 Douglas Filds Rducd Mass OK, so th Bohr modl of th atom givs nrgy lvls: E n 1 k m n 4 But, this has on problm it was dvlopd assuming th acclration

More information

3 Finite Element Parametric Geometry

3 Finite Element Parametric Geometry 3 Finit Elmnt Paramtric Gomtry 3. Introduction Th intgral of a matrix is th matrix containing th intgral of ach and vry on of its original componnts. Practical finit lmnt analysis rquirs intgrating matrics,

More information

Higher order derivatives

Higher order derivatives Robrto s Nots on Diffrntial Calculus Chaptr 4: Basic diffrntiation ruls Sction 7 Highr ordr drivativs What you nd to know alrady: Basic diffrntiation ruls. What you can larn hr: How to rpat th procss of

More information

PHA 5127 Answers Homework 2 Fall 2001

PHA 5127 Answers Homework 2 Fall 2001 PH 5127 nswrs Homwork 2 Fall 2001 OK, bfor you rad th answrs, many of you spnt a lot of tim on this homwork. Plas, nxt tim if you hav qustions plas com talk/ask us. Thr is no nd to suffr (wll a littl suffring

More information

EEO 401 Digital Signal Processing Prof. Mark Fowler

EEO 401 Digital Signal Processing Prof. Mark Fowler EEO 401 Digital Signal Procssing Prof. Mark Fowlr ot St #18 Introduction to DFT (via th DTFT) Rading Assignmnt: Sct. 7.1 of Proakis & Manolakis 1/24 Discrt Fourir Transform (DFT) W v sn that th DTFT is

More information

4.2 Design of Sections for Flexure

4.2 Design of Sections for Flexure 4. Dsign of Sctions for Flxur This sction covrs th following topics Prliminary Dsign Final Dsign for Typ 1 Mmbrs Spcial Cas Calculation of Momnt Dmand For simply supportd prstrssd bams, th maximum momnt

More information

The pn junction: 2 Current vs Voltage (IV) characteristics

The pn junction: 2 Current vs Voltage (IV) characteristics Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n

More information

A Propagating Wave Packet Group Velocity Dispersion

A Propagating Wave Packet Group Velocity Dispersion Lctur 8 Phys 375 A Propagating Wav Packt Group Vlocity Disprsion Ovrviw and Motivation: In th last lctur w lookd at a localizd solution t) to th 1D fr-particl Schrödingr quation (SE) that corrsponds to

More information

Text: WMM, Chapter 5. Sections , ,

Text: WMM, Chapter 5. Sections , , Lcturs 6 - Continuous Probabilit Distributions Tt: WMM, Chaptr 5. Sctions 6.-6.4, 6.6-6.8, 7.-7. In th prvious sction, w introduc som of th common probabilit distribution functions (PDFs) for discrt sampl

More information

1 Isoparametric Concept

1 Isoparametric Concept UNIVERSITY OF CALIFORNIA BERKELEY Dpartmnt of Civil Enginring Spring 06 Structural Enginring, Mchanics and Matrials Profssor: S. Govindj Nots on D isoparamtric lmnts Isoparamtric Concpt Th isoparamtric

More information

with Dirichlet boundary conditions on the rectangle Ω = [0, 1] [0, 2]. Here,

with Dirichlet boundary conditions on the rectangle Ω = [0, 1] [0, 2]. Here, Numrical Eampl In thi final chaptr, w tart b illutrating om known rult in th thor and thn procd to giv a fw novl ampl. All ampl conidr th quation F(u) = u f(u) = g, (-) with Dirichlt boundar condition

More information

Chapter 10. The singular integral Introducing S(n) and J(n)

Chapter 10. The singular integral Introducing S(n) and J(n) Chaptr Th singular intgral Our aim in this chaptr is to rplac th functions S (n) and J (n) by mor convnint xprssions; ths will b calld th singular sris S(n) and th singular intgral J(n). This will b don

More information

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the Copyright itutcom 005 Fr download & print from wwwitutcom Do not rproduc by othr mans Functions and graphs Powr functions Th graph of n y, for n Q (st of rational numbrs) y is a straight lin through th

More information

Basic Polyhedral theory

Basic Polyhedral theory Basic Polyhdral thory Th st P = { A b} is calld a polyhdron. Lmma 1. Eithr th systm A = b, b 0, 0 has a solution or thr is a vctorπ such that π A 0, πb < 0 Thr cass, if solution in top row dos not ist

More information

Outline. Why speech processing? Speech signal processing. Advanced Multimedia Signal Processing #5:Speech Signal Processing 2 -Processing-

Outline. Why speech processing? Speech signal processing. Advanced Multimedia Signal Processing #5:Speech Signal Processing 2 -Processing- Outlin Advancd Multimdia Signal Procssing #5:Spch Signal Procssing -Procssing- Intllignt Elctronic Systms Group Dpt. of Elctronic Enginring, UEC Basis of Spch Procssing Nois Rmoval Spctral Subtraction

More information

perm4 A cnt 0 for for if A i 1 A i cnt cnt 1 cnt i j. j k. k l. i k. j l. i l

perm4 A cnt 0 for for if A i 1 A i cnt cnt 1 cnt i j. j k. k l. i k. j l. i l h 4D, 4th Rank, Antisytric nsor and th 4D Equivalnt to th Cross Product or Mor Fun with nsors!!! Richard R Shiffan Digital Graphics Assoc 8 Dunkirk Av LA, Ca 95 rrs@isidu his docunt dscribs th four dinsional

More information

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches. Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M

More information

Where k is either given or determined from the data and c is an arbitrary constant.

Where k is either given or determined from the data and c is an arbitrary constant. Exponntial growth and dcay applications W wish to solv an quation that has a drivativ. dy ky k > dx This quation says that th rat of chang of th function is proportional to th function. Th solution is

More information

MATHEMATICS PAPER IB COORDINATE GEOMETRY(2D &3D) AND CALCULUS. Note: This question paper consists of three sections A,B and C.

MATHEMATICS PAPER IB COORDINATE GEOMETRY(2D &3D) AND CALCULUS. Note: This question paper consists of three sections A,B and C. MATHEMATICS PAPER IB COORDINATE GEOMETRY(D &D) AND CALCULUS. TIME : hrs Ma. Marks.75 Not: This qustion papr consists of thr sctions A,B and C. SECTION A VERY SHORT ANSWER TYPE QUESTIONS. 0X =0.If th portion

More information

Problem Set 6 Solutions

Problem Set 6 Solutions 6.04/18.06J Mathmatics for Computr Scinc March 15, 005 Srini Dvadas and Eric Lhman Problm St 6 Solutions Du: Monday, March 8 at 9 PM in Room 3-044 Problm 1. Sammy th Shark is a financial srvic providr

More information

Pipe flow friction, small vs. big pipes

Pipe flow friction, small vs. big pipes Friction actor (t/0 t o pip) Friction small vs larg pips J. Chaurtt May 016 It is an intrsting act that riction is highr in small pips than largr pips or th sam vlocity o low and th sam lngth. Friction

More information

15. Stress-Strain behavior of soils

15. Stress-Strain behavior of soils 15. Strss-Strain bhavior of soils Sand bhavior Usually shard undr draind conditions (rlativly high prmability mans xcss por prssurs ar not gnratd). Paramtrs govrning sand bhaviour is: Rlativ dnsity Effctiv

More information

L 1 = L G 1 F-matrix: too many F ij s even at quadratic-only level

L 1 = L G 1 F-matrix: too many F ij s even at quadratic-only level 5.76 Lctur #6 //94 Pag of 8 pag Lctur #6: Polyatomic Vibration III: -Vctor and H O Lat tim: I got tuck on L G L mut b L L L G F-matrix: too many F ij vn at quadratic-only lvl It obviou! Intrnal coordinat:

More information

DIFFERENTIAL EQUATION

DIFFERENTIAL EQUATION MD DIFFERENTIAL EQUATION Sllabus : Ordinar diffrntial quations, thir ordr and dgr. Formation of diffrntial quations. Solution of diffrntial quations b th mthod of sparation of variabls, solution of homognous

More information

Sundials and Linear Algebra

Sundials and Linear Algebra Sundials and Linar Algbra M. Scot Swan July 2, 25 Most txts on crating sundials ar dirctd towards thos who ar solly intrstd in making and using sundials and usually assums minimal mathmatical background.

More information

ENGR 7181 LECTURE NOTES WEEK 5 Dr. Amir G. Aghdam Concordia University

ENGR 7181 LECTURE NOTES WEEK 5 Dr. Amir G. Aghdam Concordia University ENGR 78 LETURE NOTES WEEK 5 r. mir G. dam onordia Univrity ilinar Tranformation - W will now introdu anotr mtod of tranformation from -plan to t - plan and vi vra. - Ti tranformation i bad on t trapoidal

More information

2008 AP Calculus BC Multiple Choice Exam

2008 AP Calculus BC Multiple Choice Exam 008 AP Multipl Choic Eam Nam 008 AP Calculus BC Multipl Choic Eam Sction No Calculator Activ AP Calculus 008 BC Multipl Choic. At tim t 0, a particl moving in th -plan is th acclration vctor of th particl

More information

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013 18.782 Introduction to Arithmtic Gomtry Fall 2013 Lctur #20 11/14/2013 20.1 Dgr thorm for morphisms of curvs Lt us rstat th thorm givn at th nd of th last lctur, which w will now prov. Thorm 20.1. Lt φ:

More information

MATH 1080 Test 2-SOLUTIONS Spring

MATH 1080 Test 2-SOLUTIONS Spring MATH Tst -SOLUTIONS Spring 5. Considr th curv dfind by x = ln( 3y + 7) on th intrval y. a. (5 points) St up but do not simplify or valuat an intgral rprsnting th lngth of th curv on th givn intrval. =

More information

EXST Regression Techniques Page 1

EXST Regression Techniques Page 1 EXST704 - Rgrssion Tchniqus Pag 1 Masurmnt rrors in X W hav assumd that all variation is in Y. Masurmnt rror in this variabl will not ffct th rsults, as long as thy ar uncorrlatd and unbiasd, sinc thy

More information

Probability and Stochastic Processes: A Friendly Introduction for Electrical and Computer Engineers Roy D. Yates and David J.

Probability and Stochastic Processes: A Friendly Introduction for Electrical and Computer Engineers Roy D. Yates and David J. Probability and Stochastic Procsss: A Frindly Introduction for Elctrical and Computr Enginrs Roy D. Yats and David J. Goodman Problm Solutions : Yats and Goodman,4.3. 4.3.4 4.3. 4.4. 4.4.4 4.4.6 4.. 4..7

More information

Chapter 13 GMM for Linear Factor Models in Discount Factor form. GMM on the pricing errors gives a crosssectional

Chapter 13 GMM for Linear Factor Models in Discount Factor form. GMM on the pricing errors gives a crosssectional Chaptr 13 GMM for Linar Factor Modls in Discount Factor form GMM on th pricing rrors givs a crosssctional rgrssion h cas of xcss rturns Hors rac sting for charactristic sting for pricd factors: lambdas

More information

Integral Calculus What is integral calculus?

Integral Calculus What is integral calculus? Intgral Calulus What is intgral alulus? In diffrntial alulus w diffrntiat a funtion to obtain anothr funtion alld drivativ. Intgral alulus is onrnd with th opposit pross. Rvrsing th pross of diffrntiation

More information

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark Answr omwork 5 PA527 Fall 999 Jff Stark A patint is bing tratd with Drug X in a clinical stting. Upon admiion, an IV bolus dos of 000mg was givn which yildd an initial concntration of 5.56 µg/ml. A fw

More information

Engineering Differential Equations Practice Final Exam Solutions Fall 2011

Engineering Differential Equations Practice Final Exam Solutions Fall 2011 9.6 Enginring Diffrntial Equation Practic Final Exam Solution Fall 0 Problm. (0 pt.) Solv th following initial valu problm: x y = xy, y() = 4. Thi i a linar d.. bcau y and y appar only to th firt powr.

More information

1997 AP Calculus AB: Section I, Part A

1997 AP Calculus AB: Section I, Part A 997 AP Calculus AB: Sction I, Part A 50 Minuts No Calculator Not: Unlss othrwis spcifid, th domain of a function f is assumd to b th st of all ral numbrs for which f () is a ral numbr.. (4 6 ) d= 4 6 6

More information

That is, we start with a general matrix: And end with a simpler matrix:

That is, we start with a general matrix: And end with a simpler matrix: DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss

More information

MA1506 Tutorial 2 Solutions. Question 1. (1a) 1 ) y x. e x. 1 exp (in general, Integrating factor is. ye dx. So ) (1b) e e. e c.

MA1506 Tutorial 2 Solutions. Question 1. (1a) 1 ) y x. e x. 1 exp (in general, Integrating factor is. ye dx. So ) (1b) e e. e c. MA56 utorial Solutions Qustion a Intgrating fator is ln p p in gnral, multipl b p So b ln p p sin his kin is all a Brnoulli quation -- st Sin w fin Y, Y Y, Y Y p Qustion Dfin v / hn our quation is v μ

More information

4037 ADDITIONAL MATHEMATICS

4037 ADDITIONAL MATHEMATICS CAMBRIDGE INTERNATIONAL EXAMINATIONS GCE Ordinary Lvl MARK SCHEME for th Octobr/Novmbr 0 sris 40 ADDITIONAL MATHEMATICS 40/ Papr, maimum raw mark 80 This mark schm is publishd as an aid to tachrs and candidats,

More information

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim.

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim. MTH rviw part b Lucian Mitroiu Th LOG and EXP functions Th ponntial function p : R, dfind as Proprtis: lim > lim p Eponntial function Y 8 6 - -8-6 - - X Th natural logarithm function ln in US- log: function

More information

surface of a dielectric-metal interface. It is commonly used today for discovering the ways in

surface of a dielectric-metal interface. It is commonly used today for discovering the ways in Surfac plasmon rsonanc is snsitiv mchanism for obsrving slight changs nar th surfac of a dilctric-mtal intrfac. It is commonl usd toda for discovring th was in which protins intract with thir nvironmnt,

More information

Brief Introduction to Statistical Mechanics

Brief Introduction to Statistical Mechanics Brif Introduction to Statistical Mchanics. Purpos: Ths nots ar intndd to provid a vry quick introduction to Statistical Mchanics. Th fild is of cours far mor vast than could b containd in ths fw pags.

More information

Forces. Quantum ElectroDynamics. α = = We have now:

Forces. Quantum ElectroDynamics. α = = We have now: W hav now: Forcs Considrd th gnral proprtis of forcs mdiatd by xchang (Yukawa potntial); Examind consrvation laws which ar obyd by (som) forcs. W will nxt look at thr forcs in mor dtail: Elctromagntic

More information

Solution of Assignment #2

Solution of Assignment #2 olution of Assignmnt #2 Instructor: Alirza imchi Qustion #: For simplicity, assum that th distribution function of T is continuous. Th distribution function of R is: F R ( r = P( R r = P( log ( T r = P(log

More information

Propositional Logic. Combinatorial Problem Solving (CPS) Albert Oliveras Enric Rodríguez-Carbonell. May 17, 2018

Propositional Logic. Combinatorial Problem Solving (CPS) Albert Oliveras Enric Rodríguez-Carbonell. May 17, 2018 Propositional Logic Combinatorial Problm Solving (CPS) Albrt Olivras Enric Rodríguz-Carbonll May 17, 2018 Ovrviw of th sssion Dfinition of Propositional Logic Gnral Concpts in Logic Rduction to SAT CNFs

More information

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 0 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat th

More information

DISCRETE TIME FOURIER TRANSFORM (DTFT)

DISCRETE TIME FOURIER TRANSFORM (DTFT) DISCRETE TIME FOURIER TRANSFORM (DTFT) Th dicrt-tim Fourir Tranform x x n xn n n Th Invr dicrt-tim Fourir Tranform (IDTFT) x n Not: ( ) i a complx valud continuou function = π f [rad/c] f i th digital

More information

Lecture 19: Free Energies in Modern Computational Statistical Thermodynamics: WHAM and Related Methods

Lecture 19: Free Energies in Modern Computational Statistical Thermodynamics: WHAM and Related Methods Statistical Thrmodynamics Lctur 19: Fr Enrgis in Modrn Computational Statistical Thrmodynamics: WHAM and Rlatd Mthods Dr. Ronald M. Lvy ronlvy@tmpl.du Dfinitions Canonical nsmbl: A N, V,T = k B T ln Q

More information

Volterra Kernel Estimation for Nonlinear Communication Channels Using Deterministic Sequences

Volterra Kernel Estimation for Nonlinear Communication Channels Using Deterministic Sequences 1 Voltrra Krnl Estimation for Nonlinar Communication Channls Using Dtrministic Squncs Endr M. Ekşioğlu and Ahmt H. Kayran Dpartmnt of Elctrical and Elctronics Enginring, Istanbul Tchnical Univrsity, Istanbul,

More information

Lie Groups HW7. Wang Shuai. November 2015

Lie Groups HW7. Wang Shuai. November 2015 Li roups HW7 Wang Shuai Novmbr 015 1 Lt (π, V b a complx rprsntation of a compact group, show that V has an invariant non-dgnratd Hrmitian form. For any givn Hrmitian form on V, (for xampl (u, v = i u

More information

Image Filtering: Noise Removal, Sharpening, Deblurring. Yao Wang Polytechnic University, Brooklyn, NY11201

Image Filtering: Noise Removal, Sharpening, Deblurring. Yao Wang Polytechnic University, Brooklyn, NY11201 Imag Filtring: Nois Rmoval, Sharpning, Dblurring Yao Wang Polytchnic Univrsity, Brooklyn, NY http://wb.poly.du/~yao Outlin Nois rmoval by avraging iltr Nois rmoval by mdian iltr Sharpning Edg nhancmnt

More information

Encoder. Encoder 2. ,...,u N-1. 0,v (0) ,u 1. ] v (0) =[v (0) 0,v (1) v (1) =[v (1) 0,v (2) v (2) =[v (2) (a) u v (0) v (1) v (2) (b) N-1] 1,...

Encoder. Encoder 2. ,...,u N-1. 0,v (0) ,u 1. ] v (0) =[v (0) 0,v (1) v (1) =[v (1) 0,v (2) v (2) =[v (2) (a) u v (0) v (1) v (2) (b) N-1] 1,... Chapter 16 Turbo Coding As noted in Chapter 1, Shannon's noisy channel coding theorem implies that arbitrarily low decoding error probabilities can be achieved at any transmission rate R less than the

More information

Efficient Computation of EXIT Functions for Non-Binary Iterative Decoding

Efficient Computation of EXIT Functions for Non-Binary Iterative Decoding TO BE PUBLISHED IN IEEE TRANSACTIONS ON COMMUNCATIONS, DECEMBER 2006 Efficient Computation of EXIT Functions for Non-Binary Iterative Decoding Jörg Kliewer, Senior Member, IEEE, Soon Xin Ng, Member, IEEE,

More information

Engineering 323 Beautiful HW #13 Page 1 of 6 Brown Problem 5-12

Engineering 323 Beautiful HW #13 Page 1 of 6 Brown Problem 5-12 Enginring Bautiful HW #1 Pag 1 of 6 5.1 Two componnts of a minicomputr hav th following joint pdf for thir usful liftims X and Y: = x(1+ x and y othrwis a. What is th probability that th liftim X of th

More information

THE IMPACT OF A PRIORI INFORMATION ON THE MAP EQUALIZER PERFORMANCE WITH M-PSK MODULATION

THE IMPACT OF A PRIORI INFORMATION ON THE MAP EQUALIZER PERFORMANCE WITH M-PSK MODULATION 5th Europan Signal Procssing Confrnc (EUSIPCO 007), Poznan, Poland, Sptmbr 3-7, 007, copyright by EURASIP THE IMPACT OF A PRIORI INFORMATION ON THE MAP EQUALIZER PERFORMANCE WITH M-PSK MODULATION Chaabouni

More information

Problem Set #2 Due: Friday April 20, 2018 at 5 PM.

Problem Set #2 Due: Friday April 20, 2018 at 5 PM. 1 EE102B Spring 2018 Signal Procssing and Linar Systms II Goldsmith Problm St #2 Du: Friday April 20, 2018 at 5 PM. 1. Non-idal sampling and rcovry of idal sampls by discrt-tim filtring 30 pts) Considr

More information

Jul 4, 2005 turbo_code_primer Revision 0.0. Turbo Code Primer

Jul 4, 2005 turbo_code_primer Revision 0.0. Turbo Code Primer Jul 4, 5 turbo_code_primer Reviion. Turbo Code Primer. Introduction Thi document give a quick tutorial on MAP baed turbo coder. Section develop the background theory. Section work through a imple numerical

More information

Numbering Systems Basic Building Blocks Scaling and Round-off Noise. Number Representation. Floating vs. Fixed point. DSP Design.

Numbering Systems Basic Building Blocks Scaling and Round-off Noise. Number Representation. Floating vs. Fixed point. DSP Design. Numbring Systms Basic Building Blocks Scaling and Round-off Nois Numbr Rprsntation Viktor Öwall viktor.owall@it.lth.s Floating vs. Fixd point In floating point a valu is rprsntd by mantissa dtrmining th

More information

Assignment 4 Biophys 4322/5322

Assignment 4 Biophys 4322/5322 Assignmnt 4 Biophys 4322/5322 Tylr Shndruk Fbruary 28, 202 Problm Phillips 7.3. Part a R-onsidr dimoglobin utilizing th anonial nsmbl maning rdriv Eq. 3 from Phillips Chaptr 7. For a anonial nsmbl p E

More information

a 1and x is any real number.

a 1and x is any real number. Calcls Nots Eponnts an Logarithms Eponntial Fnction: Has th form y a, whr a 0, a an is any ral nmbr. Graph y, Graph y ln y y Th Natral Bas (Elr s nmbr): An irrational nmbr, symboliz by th lttr, appars

More information

2.3 Matrix Formulation

2.3 Matrix Formulation 23 Matrix Formulation 43 A mor complicatd xampl ariss for a nonlinar systm of diffrntial quations Considr th following xampl Exampl 23 x y + x( x 2 y 2 y x + y( x 2 y 2 (233 Transforming to polar coordinats,

More information

Homotopy perturbation technique

Homotopy perturbation technique Comput. Mthods Appl. Mch. Engrg. 178 (1999) 257±262 www.lsvir.com/locat/cma Homotopy prturbation tchniqu Ji-Huan H 1 Shanghai Univrsity, Shanghai Institut of Applid Mathmatics and Mchanics, Shanghai 272,

More information

1. (25pts) Answer the following questions. Justify your answers. (Use the space provided below and the next page)

1. (25pts) Answer the following questions. Justify your answers. (Use the space provided below and the next page) Phyi 6 xam#3 1. (pt) Anwr th foowing qution. Jutify your anwr. (U th pa providd bow and th nxt pag) a). Two inrtia obrvr ar in rativ motion. Whih of th foowing quantiti wi thy agr or diagr on? i) thir

More information

Title: Vibrational structure of electronic transition

Title: Vibrational structure of electronic transition Titl: Vibrational structur of lctronic transition Pag- Th band spctrum sn in th Ultra-Violt (UV) and visibl (VIS) rgions of th lctromagntic spctrum can not intrprtd as vibrational and rotational spctrum

More information

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012 Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor

More information

Differential Equations

Differential Equations UNIT I Diffrntial Equations.0 INTRODUCTION W li in a world of intrrlatd changing ntitis. Th locit of a falling bod changs with distanc, th position of th arth changs with tim, th ara of a circl changs

More information

Uncertainty in non-linear long-term behavior and buckling of. shallow concrete-filled steel tubular arches

Uncertainty in non-linear long-term behavior and buckling of. shallow concrete-filled steel tubular arches CCM14 8-3 th July, Cambridg, England Unrtainty in non-linar long-trm bhavior and bukling of shallow onrt-filld stl tubular arhs *X. Shi¹, W. Gao¹, Y.L. Pi¹ 1 Shool of Civil and Environmnt Enginring, Th

More information

11/13/17. directed graphs. CS 220: Discrete Structures and their Applications. relations and directed graphs; transitive closure zybooks

11/13/17. directed graphs. CS 220: Discrete Structures and their Applications. relations and directed graphs; transitive closure zybooks dirctd graphs CS 220: Discrt Strctrs and thir Applications rlations and dirctd graphs; transiti closr zybooks 9.3-9.6 G=(V, E) rtics dgs dgs rtics/ nods Edg (, ) gos from rtx to rtx. in-dgr of a rtx: th

More information

Unfired pressure vessels- Part 3: Design

Unfired pressure vessels- Part 3: Design Unfird prssur vssls- Part 3: Dsign Analysis prformd by: Analysis prformd by: Analysis vrsion: According to procdur: Calculation cas: Unfird prssur vssls EDMS Rfrnc: EF EN 13445-3 V1 Introduction: This

More information

EEO 401 Digital Signal Processing Prof. Mark Fowler

EEO 401 Digital Signal Processing Prof. Mark Fowler EEO 401 Digital Signal Procssing Prof. Mark Fowlr Dtails of th ot St #19 Rading Assignmnt: Sct. 7.1.2, 7.1.3, & 7.2 of Proakis & Manolakis Dfinition of th So Givn signal data points x[n] for n = 0,, -1

More information

Superposition. Thinning

Superposition. Thinning Suprposition STAT253/317 Wintr 213 Lctur 11 Yibi Huang Fbruary 1, 213 5.3 Th Poisson Procsss 5.4 Gnralizations of th Poisson Procsss Th sum of two indpndnt Poisson procsss with rspctiv rats λ 1 and λ 2,

More information

Laboratory work # 8 (14) EXPERIMENTAL ESTIMATION OF CRITICAL STRESSES IN STRINGER UNDER COMPRESSION

Laboratory work # 8 (14) EXPERIMENTAL ESTIMATION OF CRITICAL STRESSES IN STRINGER UNDER COMPRESSION Laboratory wor # 8 (14) XPRIMNTAL STIMATION OF CRITICAL STRSSS IN STRINGR UNDR COMPRSSION At action of comprssing ffort on a bar (column, rod, and stringr) two inds of loss of stability ar possibl: 1)

More information

Exchange rates in the long run (Purchasing Power Parity: PPP)

Exchange rates in the long run (Purchasing Power Parity: PPP) Exchang rats in th long run (Purchasing Powr Parity: PPP) Jan J. Michalk JJ Michalk Th law of on pric: i for a product i; P i = E N/ * P i Or quivalntly: E N/ = P i / P i Ida: Th sam product should hav

More information

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis Middl East Tchnical Univrsity Dpartmnt of Mchanical Enginring ME 43 Introduction to Finit Elmnt Analysis Chaptr 3 Computr Implmntation of D FEM Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt

More information

INTRODUCTION TO AUTOMATIC CONTROLS INDEX LAPLACE TRANSFORMS

INTRODUCTION TO AUTOMATIC CONTROLS INDEX LAPLACE TRANSFORMS adjoint...6 block diagram...4 clod loop ytm... 5, 0 E()...6 (t)...6 rror tady tat tracking...6 tracking...6...6 gloary... 0 impul function...3 input...5 invr Laplac tranform, INTRODUCTION TO AUTOMATIC

More information

Dealing with quantitative data and problem solving life is a story problem! Attacking Quantitative Problems

Dealing with quantitative data and problem solving life is a story problem! Attacking Quantitative Problems Daling with quantitati data and problm soling lif is a story problm! A larg portion of scinc inols quantitati data that has both alu and units. Units can sa your butt! Nd handl on mtric prfixs Dimnsional

More information

Chapter 7: Channel coding:convolutional codes

Chapter 7: Channel coding:convolutional codes Chapter 7: : Convolutional codes University of Limoges meghdadi@ensil.unilim.fr Reference : Digital communications by John Proakis; Wireless communication by Andreas Goldsmith Encoder representation Communication

More information

The Turbo Principle in Wireless Communications

The Turbo Principle in Wireless Communications The Turbo Principle in Wireless Communications Joachim Hagenauer Institute for Communications Engineering () Munich University of Technology (TUM) D-80290 München, Germany Nordic Radio Symposium, Oulu,

More information

Supplementary Materials

Supplementary Materials 6 Supplmntary Matrials APPENDIX A PHYSICAL INTERPRETATION OF FUEL-RATE-SPEED FUNCTION A truck running on a road with grad/slop θ positiv if moving up and ngativ if moving down facs thr rsistancs: arodynamic

More information

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula 7. Intgration by Parts Each drivativ formula givs ris to a corrsponding intgral formula, as w v sn many tims. Th drivativ product rul yilds a vry usful intgration tchniqu calld intgration by parts. Starting

More information

First order differential equation Linear equation; Method of integrating factors

First order differential equation Linear equation; Method of integrating factors First orr iffrntial quation Linar quation; Mtho of intgrating factors Exampl 1: Rwrit th lft han si as th rivativ of th prouct of y an som function by prouct rul irctly. Solving th first orr iffrntial

More information

Multiple Short Term Infusion Homework # 5 PHA 5127

Multiple Short Term Infusion Homework # 5 PHA 5127 Multipl Short rm Infusion Homwork # 5 PHA 527 A rug is aministr as a short trm infusion. h avrag pharmacokintic paramtrs for this rug ar: k 0.40 hr - V 28 L his rug follows a on-compartmnt boy mol. A 300

More information