The Idea. Leader Election. Outline. Why Rings? Network. We study leader election in rings. Specification of Leader Election YAIR. Historical reasons

Size: px
Start display at page:

Download "The Idea. Leader Election. Outline. Why Rings? Network. We study leader election in rings. Specification of Leader Election YAIR. Historical reasons"

Transcription

1 The Idea Leader Elecio Nework We sudy leader elecio i rigs Why Rigs? Oulie Specificaio of Leader Elecio Hisorical reasos origial moivaio: regeerae los oke i oke rig eworks Illusraes echiques ad priciples Good for lower bouds ad impossibiliy resuls YAIR Leader Elecio i Asychroous Rigs A O( 2 ) algorihm A O( log()) algorihm The Revege of he Lower Boud Leader elecio is sychroous rigs Breakig he Ω( log()) barrier

2 The Problem Los of variaios... Processes ca be i oe of wo fial saes eleced o-eleced I every execuio, exacly oe process (he leader) is eleced All oher processes are o-eleced Rig ca be uidirecioal or bidirecioal Processes ca be ideical or ca somehow be disiguishable from each oher The umber of processes may or may o be kow if o, uiform algorihms Commuicaios may be sychroous or asychroous Aoymous Neworks Call me Ishmael Processes have o uique IDs (ideical auomaa)...bu ca disiguish bewee lef ad righ Processes have uique IDs from some large oally ordered se (e.g. ) N + Operaios used o maipulae IDs ca be uresriced or limied (e.g. oly comparisos)

3 Commuicaio: Sychroous/Asychroous A Impossibiliy Resul I rouds Sychroous I each roud, a process delivers all pedig messages akes a execuio sep (possibly sedig oe or more messages)! Asychroous No upper boud o message delivery ime No ceralized clock No boud o relaive sped of processes Theorem There is o ouiform aoymous algorihm for leader elecio i sychroous rigs A Impossibiliy Resul A O( 2 ) Algorihm Le La ( 77), Chag & Robers ( 79) Theorem There is o ouiform aoymous algorihm for leader elecio i sychroous rigs Proof Suppose here exiss a aoymous ouiform algorihm A for R s.. R > 1 Lemma For every roud k of A i R, he saes of all he processes a he ed of roud k are he same Proof By iducio o k If some process eers he leader sae, hey all do upo receivig o message! sed uid i o lef (clockwise) upo receivig m from righ case! m.uid > uid i :!! sed m o lef! m.uid < uid i :!! discard m! m.uid = uid i :!! leader := i!! sed <ermiae, i > o lef!! ermiae edcase upo receivig <ermiae, i> from righ! leader := i! sed <ermiae, i> o lef! ermiae Asychroous ad Uiform Process wih highes uid is eleced leader - all oher uids are swallowed Time complexiy: O() Message complexiy: O( 2 ) Boud is igh:!!

4 A O( log ) Algorihm Hirscheberg & Siclair (1980) Bidirecioal rig I each phase k, p i : seds uid i oke lef ad righ oke ieded o ravel disace! 2 k ad ur back coiues ouboud oly if greaer ha okes o pah processes always forward iboud oke p i leader if i receives ow oke while goig ouboud A O( log ) Algorihm Hirscheberg & Siclair (1980) Bidirecioal rig I each phase k, proocol elecs oe wier (process wih highes uid) for each! k-eighborhood a k-eighborhood icludes! 2k+1! processes Afer O(log ) phases, here is oly oe wier! A O( log ) Algorihm Hirscheberg & Siclair (1980) Bidirecioal rig A O( log ) Algorihm Hirscheberg & Siclair (1980) Bidirecioal rig I each phase k, proocol elecs oe wier (process wih highes uid) for each! k-eighborhood a k-eighborhood icludes! 2k+1! processes Phase 0 I each phase k, proocol elecs oe wier (process wih highes uid) for each! k-eighborhood a k-eighborhood icludes! 2k+1! processes Phase 1 Afer O(log ) phases, here is oly oe wier! Afer O(log ) phases, here is oly oe wier!

5 A O( log ) Algorihm Hirscheberg & Siclair (1980) Bidirecioal rig A O( log ) Algorihm Hirscheberg & Siclair (1980) Bidirecioal rig I each phase k, proocol elecs oe wier (process wih highes uid) for each! k-eighborhood a k-eighborhood icludes! 2k+1! processes Phase 2 I each phase k, proocol elecs oe wier (process wih highes uid) for each! k-eighborhood a k-eighborhood icludes! 2k+1! processes Phase 3 Afer O(log ) phases, here is oly oe wier! Afer O(log ) phases, here is oly oe wier! Boudig message complexiy Lemma For every k 1 he umber of processes ha are phase k wiers are a mos Proof Two wiers cao have fewer ha processes bewee hem Message complexiy: 4 Phase 0 2 k +1 2 k Boudig message complexiy Lemma For every k 1 he umber of processes ha are phase k wiers are a mos Proof Two wiers cao have fewer ha processes bewee hem Message complexiy: log( 1) Phase 0 k=1 2 k +1 2 k # of phases before 1 wier

6 Boudig message complexiy Lemma For every k 1 he umber of processes ha are phase k wiers are a mos Proof Two wiers cao have fewer ha processes bewee hem Message complexiy: Phase 0 log( 1) {4 k k=1 # of phases before 1 wier # of messages per wier 2 k +1 2 k Boudig message complexiy Lemma For every k 1 he umber of processes ha are phase k wiers are a mos Proof Two wiers cao have fewer ha processes bewee hem Message complexiy: log( 1) Phase 0 k=1 # of phases before 1 wier 4 2 k { # of messages per wier 2 k 1 +1 # of wiers per phase 2 k +1 2 k Boudig message complexiy Lemma For every k 1 he umber of processes ha are phase k wiers are a mos Proof Two wiers cao have fewer ha processes bewee hem Message complexiy: log( 1) ermiaio Phase 0 k=1 # of phases before 1 wier 4 2 k { # of messages per wier 2 k 1 +1 # of wiers per phase 2 k +1 2 k Message complexiy Lemma For every k 1 he umber of processes ha are phase k wiers are a mos Proof Two wiers cao have fewer ha processes bewee hem Message complexiy: log( 1) ermiaio Phase 0 k=1 # of phases before 1 wier 4 2 k { # of messages per wier 2 k 2 k 1 < 8(log + 2) # of wiers per phase 2 k 1 +1

7 The Revege of he Lower Boud We have see: Facs a simple O( 2 ) algorihm a more clever O( log ) algorihm Ω( log ) lower boud i asychroous eworks Ω( log ) lower bouds i sychroous eworks whe usig oly comparisos Breakig hrough Ω( log ) Sychroous rigs UID are posiive iegers, maipulaed usig arbirary operaios No Uiform is kow o all!uidirecioal! commuicaio! O( ) messages! Uiform! is o kow!uidirecioal! commuicaio!o( ) messages! Wha abou ime complexiy? Ad ow, for somehig compleely differe RANDOMIZATION Wha is i good for? I geeral does o affec impossibiliy resuls leader elecio i aoymous eworks wors case bouds cosesus i fewer ha f +1 rouds Bu i makes a differece whe combied wih weakeig he problem saeme

8 Radomized leader elecio Trasiio fucio akes as ipu a radom umber from a bouded rage uder some fixed disribuio Theorem A secod look a aoymous rigs There is a radomized algorihm ha, wih probabiliy c>1/e elecs a leader i a sychroous rig sedig O( 2 ) messages Weaker problem defiiio for LE: Safey: I every global sae of every execuio, a mos oe process is i he eleced sae Liveess: A leas oe process is eleced wih some o-zero probabiliy The oe-sho algorihm The ieraed algorihm Iiially {!!! 1 wih probabiliy 1 1/ id i :=!!! 2 wih probabiliy 1/! sed id i o lef upo receivig S from righ! if S = he!! if id i is uique maximum of S he!!! eleced := rue!! else!!! eleced := false! else!! sed S id i o lef Oe execuio for each eleme of R = {1, 2} Algorihm ermiaes whe exacly oe process has id =2 Probabiliy of ermiaio c : ( ) ( ( = 1 1 ) 1 ( c> 1 1 ) 1 e Message complexiy: O( 2 ) ) 1 If oe execuio does o ermiae wih a leader, ry agai! How may imes? I he wors case, ifiiely may! Bu i he expeced case?

9 The ieraed algorihm Summary If oe execuio does o ermiae wih a leader, ry agai! How may imes? I he wors case, ifiiely may! Bu i he expeced case? Expeced value of T: E[T ]= x T x Pr[T = x] Probabiliy of success i ieraio i : c (1 c) i 1 Expeced umber of ieraios: i c (1 c) i 1 d = c (1 c) i d 1 = c dc dc 1 (1 c) = 1/c < e i=0 i=0 No deermiisic soluio for aoymous rigs No soluio for uiform aoymous rigs (eve whe usig radomizaio) Proocols wih O( 2 ) ad O( log ) messages for uiform rigs Ω( log ) lower boud o message complexiy for pracical proocols O() message complexiy for uiform sychroous rigs

10 Clock sychroizaio Clock sychroizaio??? Give me all files ha have chaged sice 12:00pm There you go... Wai... wha??? 13:00 13:00 12:01 Wha is he ime? Hard ruh: clocks drif apar Clock drif Exeral vs ieral sychroizaio Boud o drif: ρ (1 ρ)( ) H() H( ) (1 + ρ)( ) H() (clock ime) (1 + ρ) Exeral Clock Sychroizaio: keeps clock wihi some maximum deviaio from a exeral ime source. Ieral Clock Sychroizaio: keeps clocks wihi some maximum deviaio from each oher. ρ is ypically small (10-6 ) ρ ρ =1+ρ 1 1+ρ =1 ρ (1 ρ) (real ime) exchage of ifo abou imig eves of differe sysems ca ake acios a real-ime deadlies ca measure duraio of disribued aciviies ha sar o oe process ad ermiae o aoher ca oally order eves ha occur i a disribued sysem

11 Probabilisic Clock Sychroizaio (Crisia) Maser-Slave archiecure Maser ca be coeced o exeral ime source Slaves read maser s clock ad! adjus heir ow How accuraely ca a slave read he maser s clock? The Idea Clock accuracy depeds o message roudrip ime if roudrip is small, maser ad slave cao have drifed by much! No upper boud o message delivery, so o ceraiy of accurae eough readig... bu very accurae readig ca be achieved by repeaed aemps Seup ad assumpios The proocol Goal: Sychroize he slave s clock wih he maser (real ime) = x (real ime) mi P () slave P () ime=? ime= T Q() T Q(x) maser Q() Assume ha miimum delay is kow Assume ha clock drifs are kow ( ρ for boh) Quesio: wha is Q(x)?

12 Ideal sceario Problem #1: message delay (real ime) P () mi mi = x Q(x) =T + mi Perfec sychroizaio! P () Q() P () mi mi + α 2d mi + β T 2d mi β =2d 2mi Q() T Q(x) =T +2d mi Q() T T + mi Assume o clock drif P () Q() 2d mi mi T Q(x) =T + mi β =0 Problem #2: slave drif Problem #3: maser drif P () mi + α 2d 2D mi + β P () mi + α 2d 2D mi + β = x Q() T Q() T 2d(1 ρ) 2D 2d(1 + ρ) Durig he maser s clock drifs Eve if you kow β, here is sill some uceraiy!

13 Crisia s algorihm Crisia s algorihm mi + α 2d mi + β = x α, β 0 Naive esimaio: Q(x) =T +(mi + β) (ake maser s drif io accou) P () 2D Q(x) [T +(mi + β)(1 ρ),t +(mi + β) (1 + ρ) ] 0 β 2d 2mi (ake delay io accou) ime=? ime= T Q(x) [T +(mi+0)(1 ρ),t +(mi+2d 2mi)(1 + ρ)] =[T +(mi)(1 ρ),t +(2d mi)(1 + ρ)] Q() T Q(x) =? 2d 2D(1 + ρ) (ake slaveʼs drif io accou) Q(x) [T +(mi)(1 ρ),t +(2D(1 + ρ) mi)(1 + ρ)] =[T +(mi)(1 ρ),t +2D(1 + 2ρ) mi(1 + ρ)] Slave s esimaio ad precisio Slave s bes guess: Maximum error: Q(x) =T + D(1 + 2ρ) mi ρ e = D(1 + 2ρ) mi You ca keep ryig, uil you achieve he required precisio H() (clock ime) Adjusig he clock Afer sychroizig: If slave simply ses creae ime discoiuiies. P (x) =Q(x) H() (clock ime), i could (real ime) (real ime)

14 Adjusig he clock Adjusig he clock Logical clock C() =H()+A() C(x) =L : eed o adjus so ha C(x + α) =M + α Hardware clock Adjusme fucio Use liear adjusme fucio A() =mh()+n m = M L,N = L (1 + m)h α H() (clock ime) H() (clock ime) C() (logical ime) M α C() (logical ime) α L L M (real ime) (real ime) x (real ime) x (real ime) Nework Time Proocol Hierarchical srucure Each level is called a sraum The oldes disribued proocol sill ruig o he Iere Hierarchical archiecure Laecy-olera, jier-olera, faulolera.. very olera! Sraum 0: aomic clocks Sraum 1: ime servers wih direc coecios o sraum 0 Sraum 2: Use sraum 1 as ime sources ad work as server o sraum 3 ec... Accuracy is loosely coupled wih sraum level 3 2 1

15 Very olera. How? Marzullo s algorihm Tolerace o jier, laecy, fauls: redudacy Each machie seds NTP requess o may oher servers o he same or he previous sraum The sychroizaio proocol bewee wo machies is similar o Crisia s algorihm For each respose, we geerae a uple <T,δ> which defies a ierval [T-δ,T+δ] How o combie hose iervals? [8,12] [11,13] [10,12] [11,12] Give M source iervals, fid he larges ierval ha is coaied i he larges umber of source iervals 10±2 11±1 12±1 11.5± Marzullo s algorihm Give M source iervals, fid he larges ierval ha is coaied i he larges umber of source iervals The iuiio Visi he edpois lef-o-righ Cou how may source iervals are acive a each ime [8,12] [11,13] [14,15] 10±2 12±1 14.5±0.5 Icrease cou a sarig pois, decrease a edig pois 10±2 12±1 14.5± ± ±

16 Preprocessig For each source ierval [T 1,T 2], creae 2 uples of he form <ime, ype>: <T 1,-1> (sar of ierval) <T 2,+1> (ed of ierval) Sor all uples accordig o ime Example: Source iervals: [8,12], [11,13], [14,15] Tuples: <8,-1> <12,+1> <11,-1> <13,+1> <14, -1> <15, +1> Sored: <8,-1> <11,-1> <12,+1> <13,+1> <14, -1> <15, +1> 10±2 11.5±0.5 12±1 14.5± The algorihm bes=0, cou=0 for all uples<ime[i],ype[i]> { cou = cou - ype[i] if(cou>bes) { bes=cou bessar=ime[i] besed=ime[i+1] } } reur [bessar, besed] Noes: cou: umbers of acive iervals bes: bes umbers of acive iervals we have see cou=cou-ype[i] : if i s a sarpoi (ype=-1), icrease cou, else decrease i if(cou>bes) : if his is he highes umber of acive iervals we have see, le he bes ierval be [ ime[i], ime[i+1] ] If he ex poi is a sarpoi, i will replace his bes ierval If he ex poi is a edpoi, i will ed his bes ierval The algorihm a work Sored: <8,-1> <11,-1> <12,+1> <13,+1> <14, -1> <15, +1> Ii: bes=0, cou=0 <8,-1> : cou = cou - (-1) = 1 Is cou>bes? Yes bes=1, bessar=8, besed=11 <11,-1> : cou = cou - (-1) = 2 Is cou>bes? Yes bes=2, bessar=11, besed=12 <12,+1> : cou = cou - (+1) = 1 Is cou>bes? No <13,+1> : cou = cou - (+1) = 0 Is cou>bes? No <14, -1> : cou = cou - (-1) = 1 Is cou>bes? No <15, +1 : cou = cou - (+1) = 0 Is cou>bes? No 10±2 12± reur [11,12] 14.5±0.5 NTP imesamps How o represe ime? Tuesday April 19h 2011, 17:55:00? CDT? NTP: 64-bi UTC imesamp 32 bis 32 bis offse i secods sub-secod precisio offse = #secods sice Jauary 1, 1900 Wraps aroud every 2 32 secods = 136 years Firs wrap-aroud: 2036 Soluio: 128-bi imesamp. Eough o provide uambiguous ime represeaio uil he uiverse goes dim

Extremal graph theory II: K t and K t,t

Extremal graph theory II: K t and K t,t Exremal graph heory II: K ad K, Lecure Graph Theory 06 EPFL Frak de Zeeuw I his lecure, we geeralize he wo mai heorems from he las lecure, from riagles K 3 o complee graphs K, ad from squares K, o complee

More information

COS 522: Complexity Theory : Boaz Barak Handout 10: Parallel Repetition Lemma

COS 522: Complexity Theory : Boaz Barak Handout 10: Parallel Repetition Lemma COS 522: Complexiy Theory : Boaz Barak Hadou 0: Parallel Repeiio Lemma Readig: () A Parallel Repeiio Theorem / Ra Raz (available o his websie) (2) Parallel Repeiio: Simplificaios ad he No-Sigallig Case

More information

1 Notes on Little s Law (l = λw)

1 Notes on Little s Law (l = λw) Copyrigh c 26 by Karl Sigma Noes o Lile s Law (l λw) We cosider here a famous ad very useful law i queueig heory called Lile s Law, also kow as l λw, which assers ha he ime average umber of cusomers i

More information

Big O Notation for Time Complexity of Algorithms

Big O Notation for Time Complexity of Algorithms BRONX COMMUNITY COLLEGE of he Ciy Uiversiy of New York DEPARTMENT OF MATHEMATICS AND COMPUTER SCIENCE CSI 33 Secio E01 Hadou 1 Fall 2014 Sepember 3, 2014 Big O Noaio for Time Complexiy of Algorihms Time

More information

Clock Skew and Signal Representation

Clock Skew and Signal Representation Clock Skew ad Sigal Represeaio Ch. 7 IBM Power 4 Chip 0/7/004 08 frequecy domai Program Iroducio ad moivaio Sequeial circuis, clock imig, Basic ools for frequecy domai aalysis Fourier series sigal represeaio

More information

CSE 241 Algorithms and Data Structures 10/14/2015. Skip Lists

CSE 241 Algorithms and Data Structures 10/14/2015. Skip Lists CSE 41 Algorihms ad Daa Srucures 10/14/015 Skip Liss This hadou gives he skip lis mehods ha we discussed i class. A skip lis is a ordered, doublyliked lis wih some exra poiers ha allow us o jump over muliple

More information

Notes 03 largely plagiarized by %khc

Notes 03 largely plagiarized by %khc 1 1 Discree-Time Covoluio Noes 03 largely plagiarized by %khc Le s begi our discussio of covoluio i discree-ime, sice life is somewha easier i ha domai. We sar wih a sigal x[] ha will be he ipu io our

More information

EGR 544 Communication Theory

EGR 544 Communication Theory EGR 544 Commuicaio heory 7. Represeaio of Digially Modulaed Sigals II Z. Aliyazicioglu Elecrical ad Compuer Egieerig Deparme Cal Poly Pomoa Represeaio of Digial Modulaio wih Memory Liear Digial Modulaio

More information

The Eigen Function of Linear Systems

The Eigen Function of Linear Systems 1/25/211 The Eige Fucio of Liear Sysems.doc 1/7 The Eige Fucio of Liear Sysems Recall ha ha we ca express (expad) a ime-limied sigal wih a weighed summaio of basis fucios: v ( ) a ψ ( ) = where v ( ) =

More information

Math 6710, Fall 2016 Final Exam Solutions

Math 6710, Fall 2016 Final Exam Solutions Mah 67, Fall 6 Fial Exam Soluios. Firs, a sude poied ou a suble hig: if P (X i p >, he X + + X (X + + X / ( evaluaes o / wih probabiliy p >. This is roublesome because a radom variable is supposed o be

More information

BEST LINEAR FORECASTS VS. BEST POSSIBLE FORECASTS

BEST LINEAR FORECASTS VS. BEST POSSIBLE FORECASTS BEST LINEAR FORECASTS VS. BEST POSSIBLE FORECASTS Opimal ear Forecasig Alhough we have o meioed hem explicily so far i he course, here are geeral saisical priciples for derivig he bes liear forecas, ad

More information

Section 8 Convolution and Deconvolution

Section 8 Convolution and Deconvolution APPLICATIONS IN SIGNAL PROCESSING Secio 8 Covoluio ad Decovoluio This docume illusraes several echiques for carryig ou covoluio ad decovoluio i Mahcad. There are several operaors available for hese fucios:

More information

K3 p K2 p Kp 0 p 2 p 3 p

K3 p K2 p Kp 0 p 2 p 3 p Mah 80-00 Mo Ar 0 Chaer 9 Fourier Series ad alicaios o differeial equaios (ad arial differeial equaios) 9.-9. Fourier series defiiio ad covergece. The idea of Fourier series is relaed o he liear algebra

More information

Lecture 9: Polynomial Approximations

Lecture 9: Polynomial Approximations CS 70: Complexiy Theory /6/009 Lecure 9: Polyomial Approximaios Isrucor: Dieer va Melkebeek Scribe: Phil Rydzewski & Piramaayagam Arumuga Naiar Las ime, we proved ha o cosa deph circui ca evaluae he pariy

More information

Lecture 15 First Properties of the Brownian Motion

Lecture 15 First Properties of the Brownian Motion Lecure 15: Firs Properies 1 of 8 Course: Theory of Probabiliy II Term: Sprig 2015 Isrucor: Gorda Zikovic Lecure 15 Firs Properies of he Browia Moio This lecure deals wih some of he more immediae properies

More information

Ideal Amplifier/Attenuator. Memoryless. where k is some real constant. Integrator. System with memory

Ideal Amplifier/Attenuator. Memoryless. where k is some real constant. Integrator. System with memory Liear Time-Ivaria Sysems (LTI Sysems) Oulie Basic Sysem Properies Memoryless ad sysems wih memory (saic or dyamic) Causal ad o-causal sysems (Causaliy) Liear ad o-liear sysems (Lieariy) Sable ad o-sable

More information

Exercise 3 Stochastic Models of Manufacturing Systems 4T400, 6 May

Exercise 3 Stochastic Models of Manufacturing Systems 4T400, 6 May Exercise 3 Sochasic Models of Maufacurig Sysems 4T4, 6 May. Each week a very popular loery i Adorra pris 4 ickes. Each ickes has wo 4-digi umbers o i, oe visible ad he oher covered. The umbers are radomly

More information

Online Supplement to Reactive Tabu Search in a Team-Learning Problem

Online Supplement to Reactive Tabu Search in a Team-Learning Problem Olie Suppleme o Reacive abu Search i a eam-learig Problem Yueli She School of Ieraioal Busiess Admiisraio, Shaghai Uiversiy of Fiace ad Ecoomics, Shaghai 00433, People s Republic of Chia, she.yueli@mail.shufe.edu.c

More information

Using Linnik's Identity to Approximate the Prime Counting Function with the Logarithmic Integral

Using Linnik's Identity to Approximate the Prime Counting Function with the Logarithmic Integral Usig Lii's Ideiy o Approimae he Prime Couig Fucio wih he Logarihmic Iegral Naha McKezie /26/2 aha@icecreambreafas.com Summary:This paper will show ha summig Lii's ideiy from 2 o ad arragig erms i a cerai

More information

C(p, ) 13 N. Nuclear reactions generate energy create new isotopes and elements. Notation for stellar rates: p 12

C(p, ) 13 N. Nuclear reactions generate energy create new isotopes and elements. Notation for stellar rates: p 12 Iroducio o sellar reacio raes Nuclear reacios geerae eergy creae ew isoopes ad elemes Noaio for sellar raes: p C 3 N C(p,) 3 N The heavier arge ucleus (Lab: arge) he ligher icomig projecile (Lab: beam)

More information

Calculus Limits. Limit of a function.. 1. One-Sided Limits...1. Infinite limits 2. Vertical Asymptotes...3. Calculating Limits Using the Limit Laws.

Calculus Limits. Limit of a function.. 1. One-Sided Limits...1. Infinite limits 2. Vertical Asymptotes...3. Calculating Limits Using the Limit Laws. Limi of a fucio.. Oe-Sided..... Ifiie limis Verical Asympoes... Calculaig Usig he Limi Laws.5 The Squeeze Theorem.6 The Precise Defiiio of a Limi......7 Coiuiy.8 Iermediae Value Theorem..9 Refereces..

More information

Clock Skew and Signal Representation. Program. Timing Engineering

Clock Skew and Signal Representation. Program. Timing Engineering lock Skew ad Sigal epreseaio h. 7 IBM Power 4 hip Iroducio ad moivaio Sequeial circuis, clock imig, Basic ools for frequecy domai aalysis Fourier series sigal represeaio Periodic sigals ca be represeed

More information

Fresnel Dragging Explained

Fresnel Dragging Explained Fresel Draggig Explaied 07/05/008 Decla Traill Decla@espace.e.au The Fresel Draggig Coefficie required o explai he resul of he Fizeau experime ca be easily explaied by usig he priciples of Eergy Field

More information

2 f(x) dx = 1, 0. 2f(x 1) dx d) 1 4t t6 t. t 2 dt i)

2 f(x) dx = 1, 0. 2f(x 1) dx d) 1 4t t6 t. t 2 dt i) Mah PracTes Be sure o review Lab (ad all labs) There are los of good quesios o i a) Sae he Mea Value Theorem ad draw a graph ha illusraes b) Name a impora heorem where he Mea Value Theorem was used i he

More information

Review Answers for E&CE 700T02

Review Answers for E&CE 700T02 Review Aswers for E&CE 700T0 . Deermie he curre soluio, all possible direcios, ad sepsizes wheher improvig or o for he simple able below: 4 b ma c 0 0 0-4 6 0 - B N B N ^0 0 0 curre sol =, = Ch for - -

More information

Time Dependent Queuing

Time Dependent Queuing Time Depede Queuig Mark S. Daski Deparme of IE/MS, Norhweser Uiversiy Evaso, IL 628 Sprig, 26 Oulie Will look a M/M/s sysem Numerically iegraio of Chapma- Kolmogorov equaios Iroducio o Time Depede Queue

More information

λiv Av = 0 or ( λi Av ) = 0. In order for a vector v to be an eigenvector, it must be in the kernel of λi

λiv Av = 0 or ( λi Av ) = 0. In order for a vector v to be an eigenvector, it must be in the kernel of λi Liear lgebra Lecure #9 Noes This week s lecure focuses o wha migh be called he srucural aalysis of liear rasformaios Wha are he irisic properies of a liear rasformaio? re here ay fixed direcios? The discussio

More information

Solutions to selected problems from the midterm exam Math 222 Winter 2015

Solutions to selected problems from the midterm exam Math 222 Winter 2015 Soluios o seleced problems from he miderm eam Mah Wier 5. Derive he Maclauri series for he followig fucios. (cf. Pracice Problem 4 log( + (a L( d. Soluio: We have he Maclauri series log( + + 3 3 4 4 +...,

More information

12 Getting Started With Fourier Analysis

12 Getting Started With Fourier Analysis Commuicaios Egieerig MSc - Prelimiary Readig Geig Sared Wih Fourier Aalysis Fourier aalysis is cocered wih he represeaio of sigals i erms of he sums of sie, cosie or complex oscillaio waveforms. We ll

More information

B. Maddah INDE 504 Simulation 09/02/17

B. Maddah INDE 504 Simulation 09/02/17 B. Maddah INDE 54 Simulaio 9/2/7 Queueig Primer Wha is a queueig sysem? A queueig sysem cosiss of servers (resources) ha provide service o cusomers (eiies). A Cusomer requesig service will sar service

More information

ECE-314 Fall 2012 Review Questions

ECE-314 Fall 2012 Review Questions ECE-34 Fall 0 Review Quesios. A liear ime-ivaria sysem has he ipu-oupu characerisics show i he firs row of he diagram below. Deermie he oupu for he ipu show o he secod row of he diagram. Jusify your aswer.

More information

Moment Generating Function

Moment Generating Function 1 Mome Geeraig Fucio m h mome m m m E[ ] x f ( x) dx m h ceral mome m m m E[( ) ] ( ) ( x ) f ( x) dx Mome Geeraig Fucio For a real, M () E[ e ] e k x k e p ( x ) discree x k e f ( x) dx coiuous Example

More information

6/10/2014. Definition. Time series Data. Time series Graph. Components of time series. Time series Seasonal. Time series Trend

6/10/2014. Definition. Time series Data. Time series Graph. Components of time series. Time series Seasonal. Time series Trend 6//4 Defiiio Time series Daa A ime series Measures he same pheomeo a equal iervals of ime Time series Graph Compoes of ime series 5 5 5-5 7 Q 7 Q 7 Q 3 7 Q 4 8 Q 8 Q 8 Q 3 8 Q 4 9 Q 9 Q 9 Q 3 9 Q 4 Q Q

More information

Review Exercises for Chapter 9

Review Exercises for Chapter 9 0_090R.qd //0 : PM Page 88 88 CHAPTER 9 Ifiie Series I Eercises ad, wrie a epressio for he h erm of he sequece..,., 5, 0,,,, 0,... 7,... I Eercises, mach he sequece wih is graph. [The graphs are labeled

More information

MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.265/15.070J Fall 2013 Lecture 4 9/16/2013. Applications of the large deviation technique

MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.265/15.070J Fall 2013 Lecture 4 9/16/2013. Applications of the large deviation technique MASSACHUSETTS ISTITUTE OF TECHOLOGY 6.265/5.070J Fall 203 Lecure 4 9/6/203 Applicaios of he large deviaio echique Coe.. Isurace problem 2. Queueig problem 3. Buffer overflow probabiliy Safey capial for

More information

th m m m m central moment : E[( X X) ] ( X X) ( x X) f ( x)

th m m m m central moment : E[( X X) ] ( X X) ( x X) f ( x) 1 Trasform Techiques h m m m m mome : E[ ] x f ( x) dx h m m m m ceral mome : E[( ) ] ( ) ( x) f ( x) dx A coveie wa of fidig he momes of a radom variable is he mome geeraig fucio (MGF). Oher rasform echiques

More information

Supplement for SADAGRAD: Strongly Adaptive Stochastic Gradient Methods"

Supplement for SADAGRAD: Strongly Adaptive Stochastic Gradient Methods Suppleme for SADAGRAD: Srogly Adapive Sochasic Gradie Mehods" Zaiyi Che * 1 Yi Xu * Ehog Che 1 iabao Yag 1. Proof of Proposiio 1 Proposiio 1. Le ɛ > 0 be fixed, H 0 γi, γ g, EF (w 1 ) F (w ) ɛ 0 ad ieraio

More information

14.02 Principles of Macroeconomics Fall 2005

14.02 Principles of Macroeconomics Fall 2005 14.02 Priciples of Macroecoomics Fall 2005 Quiz 2 Tuesday, November 8, 2005 7:30 PM 9 PM Please, aswer he followig quesios. Wrie your aswers direcly o he quiz. You ca achieve a oal of 100 pois. There are

More information

ODEs II, Supplement to Lectures 6 & 7: The Jordan Normal Form: Solving Autonomous, Homogeneous Linear Systems. April 2, 2003

ODEs II, Supplement to Lectures 6 & 7: The Jordan Normal Form: Solving Autonomous, Homogeneous Linear Systems. April 2, 2003 ODEs II, Suppleme o Lecures 6 & 7: The Jorda Normal Form: Solvig Auoomous, Homogeeous Liear Sysems April 2, 23 I his oe, we describe he Jorda ormal form of a marix ad use i o solve a geeral homogeeous

More information

OLS bias for econometric models with errors-in-variables. The Lucas-critique Supplementary note to Lecture 17

OLS bias for econometric models with errors-in-variables. The Lucas-critique Supplementary note to Lecture 17 OLS bias for ecoomeric models wih errors-i-variables. The Lucas-criique Supplemeary oe o Lecure 7 RNy May 6, 03 Properies of OLS i RE models I Lecure 7 we discussed he followig example of a raioal expecaios

More information

1. Solve by the method of undetermined coefficients and by the method of variation of parameters. (4)

1. Solve by the method of undetermined coefficients and by the method of variation of parameters. (4) 7 Differeial equaios Review Solve by he mehod of udeermied coefficies ad by he mehod of variaio of parameers (4) y y = si Soluio; we firs solve he homogeeous equaio (4) y y = 4 The correspodig characerisic

More information

Comparison between Fourier and Corrected Fourier Series Methods

Comparison between Fourier and Corrected Fourier Series Methods Malaysia Joural of Mahemaical Scieces 7(): 73-8 (13) MALAYSIAN JOURNAL OF MATHEMATICAL SCIENCES Joural homepage: hp://eispem.upm.edu.my/oural Compariso bewee Fourier ad Correced Fourier Series Mehods 1

More information

STK4080/9080 Survival and event history analysis

STK4080/9080 Survival and event history analysis STK48/98 Survival ad eve hisory aalysis Marigales i discree ime Cosider a sochasic process The process M is a marigale if Lecure 3: Marigales ad oher sochasic processes i discree ime (recap) where (formally

More information

Statistical Estimation

Statistical Estimation Learig Objecives Cofidece Levels, Iervals ad T-es Kow he differece bewee poi ad ierval esimaio. Esimae a populaio mea from a sample mea f large sample sizes. Esimae a populaio mea from a sample mea f small

More information

The analysis of the method on the one variable function s limit Ke Wu

The analysis of the method on the one variable function s limit Ke Wu Ieraioal Coferece o Advaces i Mechaical Egieerig ad Idusrial Iformaics (AMEII 5) The aalysis of he mehod o he oe variable fucio s i Ke Wu Deparme of Mahemaics ad Saisics Zaozhuag Uiversiy Zaozhuag 776

More information

Comparisons Between RV, ARV and WRV

Comparisons Between RV, ARV and WRV Comparisos Bewee RV, ARV ad WRV Cao Gag,Guo Migyua School of Maageme ad Ecoomics, Tiaji Uiversiy, Tiaji,30007 Absrac: Realized Volailiy (RV) have bee widely used sice i was pu forward by Aderso ad Bollerslev

More information

Mathematical Statistics. 1 Introduction to the materials to be covered in this course

Mathematical Statistics. 1 Introduction to the materials to be covered in this course Mahemaical Saisics Iroducio o he maerials o be covered i his course. Uivariae & Mulivariae r.v s 2. Borl-Caelli Lemma Large Deviaios. e.g. X,, X are iid r.v s, P ( X + + X where I(A) is a umber depedig

More information

Union-Find Partition Structures Goodrich, Tamassia Union-Find 1

Union-Find Partition Structures Goodrich, Tamassia Union-Find 1 Uio-Fid Pariio Srucures 004 Goodrich, Tamassia Uio-Fid Pariios wih Uio-Fid Operaios makesex: Creae a sileo se coaii he eleme x ad reur he posiio sori x i his se uioa,b : Reur he se A U B, desroyi he old

More information

Electrical Engineering Department Network Lab.

Electrical Engineering Department Network Lab. Par:- Elecrical Egieerig Deparme Nework Lab. Deermiaio of differe parameers of -por eworks ad verificaio of heir ierrelaio ships. Objecive: - To deermie Y, ad ABD parameers of sigle ad cascaded wo Por

More information

N! AND THE GAMMA FUNCTION

N! AND THE GAMMA FUNCTION N! AND THE GAMMA FUNCTION Cosider he produc of he firs posiive iegers- 3 4 5 6 (-) =! Oe calls his produc he facorial ad has ha produc of he firs five iegers equals 5!=0. Direcly relaed o he discree! fucio

More information

An interesting result about subset sums. Nitu Kitchloo. Lior Pachter. November 27, Abstract

An interesting result about subset sums. Nitu Kitchloo. Lior Pachter. November 27, Abstract A ieresig resul abou subse sums Niu Kichloo Lior Pacher November 27, 1993 Absrac We cosider he problem of deermiig he umber of subses B f1; 2; : : :; g such ha P b2b b k mod, where k is a residue class

More information

ECE 340 Lecture 15 and 16: Diffusion of Carriers Class Outline:

ECE 340 Lecture 15 and 16: Diffusion of Carriers Class Outline: ECE 340 Lecure 5 ad 6: iffusio of Carriers Class Oulie: iffusio rocesses iffusio ad rif of Carriers Thigs you should kow whe you leave Key Quesios Why do carriers diffuse? Wha haes whe we add a elecric

More information

Four equations describe the dynamic solution to RBC model. Consumption-leisure efficiency condition. Consumption-investment efficiency condition

Four equations describe the dynamic solution to RBC model. Consumption-leisure efficiency condition. Consumption-investment efficiency condition LINEARIZING AND APPROXIMATING THE RBC MODEL SEPTEMBER 7, 200 For f( x, y, z ), mulivariable Taylor liear expasio aroud ( x, yz, ) f ( x, y, z) f( x, y, z) + f ( x, y, z)( x x) + f ( x, y, z)( y y) + f

More information

A Two-Level Quantum Analysis of ERP Data for Mock-Interrogation Trials. Michael Schillaci Jennifer Vendemia Robert Buzan Eric Green

A Two-Level Quantum Analysis of ERP Data for Mock-Interrogation Trials. Michael Schillaci Jennifer Vendemia Robert Buzan Eric Green A Two-Level Quaum Aalysis of ERP Daa for Mock-Ierrogaio Trials Michael Schillaci Jeifer Vedemia Rober Buza Eric Gree Oulie Experimeal Paradigm 4 Low Workload; Sigle Sessio; 39 8 High Workload; Muliple

More information

SUMMATION OF INFINITE SERIES REVISITED

SUMMATION OF INFINITE SERIES REVISITED SUMMATION OF INFINITE SERIES REVISITED I several aricles over he las decade o his web page we have show how o sum cerai iiie series icludig he geomeric series. We wa here o eed his discussio o he geeral

More information

Class 36. Thin-film interference. Thin Film Interference. Thin Film Interference. Thin-film interference

Class 36. Thin-film interference. Thin Film Interference. Thin Film Interference. Thin-film interference Thi Film Ierferece Thi- ierferece Ierferece ewee ligh waves is he reaso ha hi s, such as soap ules, show colorful paers. Phoo credi: Mila Zikova, via Wikipedia Thi- ierferece This is kow as hi- ierferece

More information

Union-Find Partition Structures

Union-Find Partition Structures Uio-Fid //4 : Preseaio for use wih he exbook Daa Srucures ad Alorihms i Java, h ediio, by M. T. Goodrich, R. Tamassia, ad M. H. Goldwasser, Wiley, 04 Uio-Fid Pariio Srucures 04 Goodrich, Tamassia, Goldwasser

More information

Lecture 8 April 18, 2018

Lecture 8 April 18, 2018 Sas 300C: Theory of Saisics Sprig 2018 Lecure 8 April 18, 2018 Prof Emmauel Cades Scribe: Emmauel Cades Oulie Ageda: Muliple Tesig Problems 1 Empirical Process Viewpoi of BHq 2 Empirical Process Viewpoi

More information

NEWTON METHOD FOR DETERMINING THE OPTIMAL REPLENISHMENT POLICY FOR EPQ MODEL WITH PRESENT VALUE

NEWTON METHOD FOR DETERMINING THE OPTIMAL REPLENISHMENT POLICY FOR EPQ MODEL WITH PRESENT VALUE Yugoslav Joural of Operaios Research 8 (2008, Number, 53-6 DOI: 02298/YUJOR080053W NEWTON METHOD FOR DETERMINING THE OPTIMAL REPLENISHMENT POLICY FOR EPQ MODEL WITH PRESENT VALUE Jeff Kuo-Jug WU, Hsui-Li

More information

Conditional Probability and Conditional Expectation

Conditional Probability and Conditional Expectation Hadou #8 for B902308 prig 2002 lecure dae: 3/06/2002 Codiioal Probabiliy ad Codiioal Epecaio uppose X ad Y are wo radom variables The codiioal probabiliy of Y y give X is } { }, { } { X P X y Y P X y Y

More information

CSE 202: Design and Analysis of Algorithms Lecture 16

CSE 202: Design and Analysis of Algorithms Lecture 16 CSE 202: Desig ad Aalysis of Algorihms Lecure 16 Isrucor: Kamalia Chaudhuri Iequaliy 1: Marov s Iequaliy Pr(X=x) Pr(X >= a) 0 x a If X is a radom variable which aes o-egaive values, ad a > 0, he Pr[X a]

More information

Outline. simplest HMM (1) simple HMMs? simplest HMM (2) Parameter estimation for discrete hidden Markov models

Outline. simplest HMM (1) simple HMMs? simplest HMM (2) Parameter estimation for discrete hidden Markov models Oulie Parameer esimaio for discree idde Markov models Juko Murakami () ad Tomas Taylor (2). Vicoria Uiversiy of Welligo 2. Arizoa Sae Uiversiy Descripio of simple idde Markov models Maximum likeliood esimae

More information

Discrete-Time Signals and Systems. Introduction to Digital Signal Processing. Independent Variable. What is a Signal? What is a System?

Discrete-Time Signals and Systems. Introduction to Digital Signal Processing. Independent Variable. What is a Signal? What is a System? Discree-Time Sigals ad Sysems Iroducio o Digial Sigal Processig Professor Deepa Kudur Uiversiy of Toroo Referece: Secios. -.4 of Joh G. Proakis ad Dimiris G. Maolakis, Digial Sigal Processig: Priciples,

More information

Pure Math 30: Explained!

Pure Math 30: Explained! ure Mah : Explaied! www.puremah.com 6 Logarihms Lesso ar Basic Expoeial Applicaios Expoeial Growh & Decay: Siuaios followig his ype of chage ca be modeled usig he formula: (b) A = Fuure Amou A o = iial

More information

LIMITS OF FUNCTIONS (I)

LIMITS OF FUNCTIONS (I) LIMITS OF FUNCTIO (I ELEMENTARY FUNCTIO: (Elemeary fucios are NOT piecewise fucios Cosa Fucios: f(x k, where k R Polyomials: f(x a + a x + a x + a x + + a x, where a, a,..., a R Raioal Fucios: f(x P (x,

More information

t = s D Overview of Tests Two-Sample t-test: Independent Samples Independent Samples t-test Difference between Means in a Two-sample Experiment

t = s D Overview of Tests Two-Sample t-test: Independent Samples Independent Samples t-test Difference between Means in a Two-sample Experiment Overview of Te Two-Sample -Te: Idepede Sample Chaper 4 z-te Oe Sample -Te Relaed Sample -Te Idepede Sample -Te Compare oe ample o a populaio Compare wo ample Differece bewee Mea i a Two-ample Experime

More information

Energy Density / Energy Flux / Total Energy in 1D. Key Mathematics: density, flux, and the continuity equation.

Energy Density / Energy Flux / Total Energy in 1D. Key Mathematics: density, flux, and the continuity equation. ecure Phys 375 Eergy Desiy / Eergy Flu / oal Eergy i D Overview ad Moivaio: Fro your sudy of waves i iroducory physics you should be aware ha waves ca raspor eergy fro oe place o aoher cosider he geeraio

More information

In this section we will study periodic signals in terms of their frequency f t is said to be periodic if (4.1)

In this section we will study periodic signals in terms of their frequency f t is said to be periodic if (4.1) Fourier Series Iroducio I his secio we will sudy periodic sigals i ers o heir requecy is said o be periodic i coe Reid ha a sigal ( ) ( ) ( ) () or every, where is a uber Fro his deiiio i ollows ha ( )

More information

Chapter 2: Time-Domain Representations of Linear Time-Invariant Systems. Chih-Wei Liu

Chapter 2: Time-Domain Representations of Linear Time-Invariant Systems. Chih-Wei Liu Caper : Time-Domai Represeaios of Liear Time-Ivaria Sysems Ci-Wei Liu Oulie Iroucio Te Covoluio Sum Covoluio Sum Evaluaio Proceure Te Covoluio Iegral Covoluio Iegral Evaluaio Proceure Iercoecios of LTI

More information

Calculus BC 2015 Scoring Guidelines

Calculus BC 2015 Scoring Guidelines AP Calculus BC 5 Scorig Guidelies 5 The College Board. College Board, Advaced Placeme Program, AP, AP Ceral, ad he acor logo are regisered rademarks of he College Board. AP Ceral is he official olie home

More information

6.003: Signals and Systems

6.003: Signals and Systems 6.003: Sigals ad Sysems Lecure 8 March 2, 2010 6.003: Sigals ad Sysems Mid-erm Examiaio #1 Tomorrow, Wedesday, March 3, 7:30-9:30pm. No reciaios omorrow. Coverage: Represeaios of CT ad DT Sysems Lecures

More information

Economics 8723 Macroeconomic Theory Problem Set 2 Professor Sanjay Chugh Spring 2017

Economics 8723 Macroeconomic Theory Problem Set 2 Professor Sanjay Chugh Spring 2017 Deparme of Ecoomics The Ohio Sae Uiversiy Ecoomics 8723 Macroecoomic Theory Problem Se 2 Professor Sajay Chugh Sprig 207 Labor Icome Taxes, Nash-Bargaied Wages, ad Proporioally-Bargaied Wages. I a ecoomy

More information

CS623: Introduction to Computing with Neural Nets (lecture-10) Pushpak Bhattacharyya Computer Science and Engineering Department IIT Bombay

CS623: Introduction to Computing with Neural Nets (lecture-10) Pushpak Bhattacharyya Computer Science and Engineering Department IIT Bombay CS6: Iroducio o Compuig ih Neural Nes lecure- Pushpak Bhaacharyya Compuer Sciece ad Egieerig Deparme IIT Bombay Tilig Algorihm repea A kid of divide ad coquer sraegy Give he classes i he daa, ru he percepro

More information

6.003 Homework #5 Solutions

6.003 Homework #5 Solutions 6. Homework #5 Soluios Problems. DT covoluio Le y represe he DT sigal ha resuls whe f is covolved wih g, i.e., y[] = (f g)[] which is someimes wrie as y[] = f[] g[]. Deermie closed-form expressios for

More information

BAYESIAN ESTIMATION METHOD FOR PARAMETER OF EPIDEMIC SIR REED-FROST MODEL. Puji Kurniawan M

BAYESIAN ESTIMATION METHOD FOR PARAMETER OF EPIDEMIC SIR REED-FROST MODEL. Puji Kurniawan M BAYESAN ESTMATON METHOD FOR PARAMETER OF EPDEMC SR REED-FROST MODEL Puji Kuriawa M447 ABSTRACT. fecious diseases is a impora healh problem i he mos of couries, belogig o doesia. Some of ifecious diseases

More information

INVESTMENT PROJECT EFFICIENCY EVALUATION

INVESTMENT PROJECT EFFICIENCY EVALUATION 368 Miljeko Crjac Domiika Crjac INVESTMENT PROJECT EFFICIENCY EVALUATION Miljeko Crjac Professor Faculy of Ecoomics Drsc Domiika Crjac Faculy of Elecrical Egieerig Osijek Summary Fiacial efficiecy of ivesme

More information

LINEAR APPROXIMATION OF THE BASELINE RBC MODEL JANUARY 29, 2013

LINEAR APPROXIMATION OF THE BASELINE RBC MODEL JANUARY 29, 2013 LINEAR APPROXIMATION OF THE BASELINE RBC MODEL JANUARY 29, 203 Iroducio LINEARIZATION OF THE RBC MODEL For f( x, y, z ) = 0, mulivariable Taylor liear expasio aroud f( x, y, z) f( x, y, z) + f ( x, y,

More information

King Fahd University of Petroleum & Minerals Computer Engineering g Dept

King Fahd University of Petroleum & Minerals Computer Engineering g Dept Kig Fahd Uiversiy of Peroleum & Mierals Compuer Egieerig g Dep COE 4 Daa ad Compuer Commuicaios erm Dr. shraf S. Hasa Mahmoud Rm -4 Ex. 74 Email: ashraf@kfupm.edu.sa 9/8/ Dr. shraf S. Hasa Mahmoud Lecure

More information

Department of Mathematical and Statistical Sciences University of Alberta

Department of Mathematical and Statistical Sciences University of Alberta MATH 4 (R) Wier 008 Iermediae Calculus I Soluios o Problem Se # Due: Friday Jauary 8, 008 Deparme of Mahemaical ad Saisical Scieces Uiversiy of Albera Quesio. [Sec.., #] Fid a formula for he geeral erm

More information

Actuarial Society of India

Actuarial Society of India Acuarial Sociey of Idia EXAMINAIONS Jue 5 C4 (3) Models oal Marks - 5 Idicaive Soluio Q. (i) a) Le U deoe he process described by 3 ad V deoe he process described by 4. he 5 e 5 PU [ ] PV [ ] ( e ).538!

More information

FIXED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE

FIXED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE Mohia & Samaa, Vol. 1, No. II, December, 016, pp 34-49. ORIGINAL RESEARCH ARTICLE OPEN ACCESS FIED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE 1 Mohia S. *, Samaa T. K. 1 Deparme of Mahemaics, Sudhir Memorial

More information

A TAUBERIAN THEOREM FOR THE WEIGHTED MEAN METHOD OF SUMMABILITY

A TAUBERIAN THEOREM FOR THE WEIGHTED MEAN METHOD OF SUMMABILITY U.P.B. Sci. Bull., Series A, Vol. 78, Iss. 2, 206 ISSN 223-7027 A TAUBERIAN THEOREM FOR THE WEIGHTED MEAN METHOD OF SUMMABILITY İbrahim Çaak I his paper we obai a Tauberia codiio i erms of he weighed classical

More information

6.01: Introduction to EECS I Lecture 3 February 15, 2011

6.01: Introduction to EECS I Lecture 3 February 15, 2011 6.01: Iroducio o EECS I Lecure 3 February 15, 2011 6.01: Iroducio o EECS I Sigals ad Sysems Module 1 Summary: Sofware Egieerig Focused o absracio ad modulariy i sofware egieerig. Topics: procedures, daa

More information

F.Y. Diploma : Sem. II [AE/CH/FG/ME/PT/PG] Applied Mathematics

F.Y. Diploma : Sem. II [AE/CH/FG/ME/PT/PG] Applied Mathematics F.Y. Diploma : Sem. II [AE/CH/FG/ME/PT/PG] Applied Mahemaics Prelim Quesio Paper Soluio Q. Aemp ay FIVE of he followig : [0] Q.(a) Defie Eve ad odd fucios. [] As.: A fucio f() is said o be eve fucio if

More information

Solution. 1 Solutions of Homework 6. Sangchul Lee. April 28, Problem 1.1 [Dur10, Exercise ]

Solution. 1 Solutions of Homework 6. Sangchul Lee. April 28, Problem 1.1 [Dur10, Exercise ] Soluio Sagchul Lee April 28, 28 Soluios of Homework 6 Problem. [Dur, Exercise 2.3.2] Le A be a sequece of idepede eves wih PA < for all. Show ha P A = implies PA i.o. =. Proof. Noice ha = P A c = P A c

More information

A Note on Random k-sat for Moderately Growing k

A Note on Random k-sat for Moderately Growing k A Noe o Radom k-sat for Moderaely Growig k Ju Liu LMIB ad School of Mahemaics ad Sysems Sciece, Beihag Uiversiy, Beijig, 100191, P.R. Chia juliu@smss.buaa.edu.c Zogsheg Gao LMIB ad School of Mahemaics

More information

ANALYSIS OF THE CHAOS DYNAMICS IN (X n,x n+1) PLANE

ANALYSIS OF THE CHAOS DYNAMICS IN (X n,x n+1) PLANE ANALYSIS OF THE CHAOS DYNAMICS IN (X,X ) PLANE Soegiao Soelisioo, The Houw Liog Badug Isiue of Techolog (ITB) Idoesia soegiao@sude.fi.ib.ac.id Absrac I he las decade, sudies of chaoic ssem are more ofe

More information

Paper 3A3 The Equations of Fluid Flow and Their Numerical Solution Handout 1

Paper 3A3 The Equations of Fluid Flow and Their Numerical Solution Handout 1 Paper 3A3 The Equaios of Fluid Flow ad Their Numerical Soluio Hadou Iroducio A grea ma fluid flow problems are ow solved b use of Compuaioal Fluid Damics (CFD) packages. Oe of he major obsacles o he good

More information

Convergence theorems. Chapter Sampling

Convergence theorems. Chapter Sampling Chaper Covergece heorems We ve already discussed he difficuly i defiig he probabiliy measure i erms of a experimeal frequecy measureme. The hear of he problem lies i he defiiio of he limi, ad his was se

More information

EEC 483 Computer Organization

EEC 483 Computer Organization EEC 8 Compuer Orgaizaio Chaper. Overview of Pipeliig Chau Yu Laudry Example Laudry Example A, Bria, Cahy, Dave each have oe load of clohe o wah, dry, ad fold Waher ake 0 miue A B C D Dryer ake 0 miue Folder

More information

CLOSED FORM EVALUATION OF RESTRICTED SUMS CONTAINING SQUARES OF FIBONOMIAL COEFFICIENTS

CLOSED FORM EVALUATION OF RESTRICTED SUMS CONTAINING SQUARES OF FIBONOMIAL COEFFICIENTS PB Sci Bull, Series A, Vol 78, Iss 4, 2016 ISSN 1223-7027 CLOSED FORM EVALATION OF RESTRICTED SMS CONTAINING SQARES OF FIBONOMIAL COEFFICIENTS Emrah Kılıc 1, Helmu Prodiger 2 We give a sysemaic approach

More information

5.74 Introductory Quantum Mechanics II

5.74 Introductory Quantum Mechanics II MIT OpeCourseWare hp://ocw.mi.edu 5.74 Iroducory Quaum Mechaics II Sprig 009 For iformaio aou ciig hese maerials or our Terms of Use, visi: hp://ocw.mi.edu/erms. drei Tokmakoff, MIT Deparme of Chemisry,

More information

LINEAR APPROXIMATION OF THE BASELINE RBC MODEL SEPTEMBER 17, 2013

LINEAR APPROXIMATION OF THE BASELINE RBC MODEL SEPTEMBER 17, 2013 LINEAR APPROXIMATION OF THE BASELINE RBC MODEL SEPTEMBER 7, 203 Iroducio LINEARIZATION OF THE RBC MODEL For f( xyz,, ) = 0, mulivariable Taylor liear expasio aroud f( xyz,, ) f( xyz,, ) + f( xyz,, )( x

More information

Applying the Moment Generating Functions to the Study of Probability Distributions

Applying the Moment Generating Functions to the Study of Probability Distributions 3 Iformaica Ecoomică, r (4)/007 Applyi he Mome Geerai Fucios o he Sudy of Probabiliy Disribuios Silvia SPĂTARU Academy of Ecoomic Sudies, Buchares I his paper, we describe a ool o aid i provi heorems abou

More information

Economics 8723 Macroeconomic Theory Problem Set 3 Sketch of Solutions Professor Sanjay Chugh Spring 2017

Economics 8723 Macroeconomic Theory Problem Set 3 Sketch of Solutions Professor Sanjay Chugh Spring 2017 Deparme of Ecoomic The Ohio Sae Uiveriy Ecoomic 8723 Macroecoomic Theory Problem Se 3 Skech of Soluio Profeor Sajay Chugh Sprig 27 Taylor Saggered Nomial Price-Seig Model There are wo group of moopoliically-compeiive

More information

10.3 Autocorrelation Function of Ergodic RP 10.4 Power Spectral Density of Ergodic RP 10.5 Normal RP (Gaussian RP)

10.3 Autocorrelation Function of Ergodic RP 10.4 Power Spectral Density of Ergodic RP 10.5 Normal RP (Gaussian RP) ENGG450 Probabiliy ad Saisics for Egieers Iroducio 3 Probabiliy 4 Probabiliy disribuios 5 Probabiliy Desiies Orgaizaio ad descripio of daa 6 Samplig disribuios 7 Ifereces cocerig a mea 8 Comparig wo reames

More information

MATH 507a ASSIGNMENT 4 SOLUTIONS FALL 2018 Prof. Alexander. g (x) dx = g(b) g(0) = g(b),

MATH 507a ASSIGNMENT 4 SOLUTIONS FALL 2018 Prof. Alexander. g (x) dx = g(b) g(0) = g(b), MATH 57a ASSIGNMENT 4 SOLUTIONS FALL 28 Prof. Alexader (2.3.8)(a) Le g(x) = x/( + x) for x. The g (x) = /( + x) 2 is decreasig, so for a, b, g(a + b) g(a) = a+b a g (x) dx b so g(a + b) g(a) + g(b). Sice

More information

Instructor: Barry McQuarrie Page 1 of 5

Instructor: Barry McQuarrie Page 1 of 5 Procedure for Solving radical equaions 1. Algebraically isolae one radical by iself on one side of equal sign. 2. Raise each side of he equaion o an appropriae power o remove he radical. 3. Simplify. 4.

More information

arxiv: v3 [math.co] 25 May 2013

arxiv: v3 [math.co] 25 May 2013 Log pahs ad cycles i radom subgraphs of graphs wih large miimum degree arxiv:1207.0312v3 [mah.co] 25 May 2013 Michael Krivelevich Choogbum Lee Bey Sudaov Absrac For a give fiie graph G of miimum degree

More information

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still. Lecure - Kinemaics in One Dimension Displacemen, Velociy and Acceleraion Everyhing in he world is moving. Nohing says sill. Moion occurs a all scales of he universe, saring from he moion of elecrons in

More information