Basic definitions and relations

Size: px
Start display at page:

Download "Basic definitions and relations"

Transcription

1 Basic definiions and relaions Lecurer: Dmiri A. Molchanov hp://

2 Kendall s noaion for queuing sysems: Arrival processes; Service ime disribuions; Examples. Lile s resul: Basic resul; Proof; Example. Lecure: Basic definiions and relaions 2

3 1. Kendall s noaion for queuing sysems exponenial arrivals exponenial service Erlang arrivals hyperexponenial service infinie # of waiing posiions limied # of waiing posiions exponenial service general arrivals general service general arrivals K servers infinie # of waiing posiions infinie # of waiing posiions Figure 1: Differen ypes of queuing sysems. Quesion: how o represen i in a compac form? Lecure: Basic definiions and relaions 3

4 Which elemens we have o describe: arrival process; service ime disribuion; how many servers does he sysem have; are here waiing posiions in he sysem; if yes, how many waiing posiion does he sysem have; wha is he service discipline; are here special rules applicable o sysem: are here vacaions of he server; do he arrivals occur in baches or no; are here prioriies in service for cerain cusomers. Noe: we should say a leas he class of arrivals, deparures, # of servers... Lecure: Basic definiions and relaions 4

5 A simple noaion of queuing sysem: Kendall in 60 h ; proposed o use a leers o describe characerisics of queuing sysem; leers are separaed by slashes (5 posiions): / / / / (1) The firs posiion is for he arrival process: M: exponenial (M here sands for Markovian arrivals); E k : Erlang of order k; H k : hyperexponenial of order k; D: consan; PH: phase ype; GI: general uncorrelaed; G: general correlaed. Lecure: Basic definiions and relaions 5

6 Some non-renewal well-known coninuous-ime processes: IPP: inerruped Poisson process; SPP: swiched Poison process; MMPP: Markov modulaed Poisson process; MAP: Markovian arrival process; BMAP: Bach Markovian arrival process; Some non-renewal well-known discree-ime processes: IBP: inerruped Bernoulli Process; SBP: swiched Bernoulli process; MMBP: Markov modulaed Bernoulli process; D-MAP: discree-ime Markovian arrival process; D-BMAP: discree-ime Bach Markovian arrival process; Lecure: Basic definiions and relaions 6

7 Second posiion: service process: M: exponenial; E k : Erlang of order k; H k : hyperexponenial of order k; D: consan; PH: phase ype; G: general. Noe he following: service imes are usually assumed o be uncorrelaed (here G implies uncorrelaed); someimes his may no be rue. Third place: number of servers; here mus be a leas one; can be. Lecure: Basic definiions and relaions 7

8 Some examples of queuing sysems in Kendall s noaion are as follows: M/M/1 M/PH/10 MAP/PH/1. (2) oher places (4h and 5h) are assumed o be infinie. Fourh place: capaciy of he sysem: should be a leas 1; capaciy of no he number of waiing posiions; capaciy = # of waiing posiions # of servers. M/PH/10/N, M/M/1/K. (3) if his place may be omied; MAP/PH/1. (4) Lecure: Basic definiions and relaions 8

9 Fifh place: arrival populaion: can be finie: arrival process of broken machines o repairmen queue (number of machines may be finie). can be infinie: call arrival process o a elephone exchange. is omied when infinie! The following is imporan: fifh posiion someimes incorrecly used o denoe he service discipline; service discipline should be given separaely (no place in Kendall noaion)! The following service disciplines are he mos common: firs come, firs served (FCFS), i.e. in order of arrivals; random order (RANDOM); las come, firs served (LCFS); processor sharing (PS). Lecure: Basic definiions and relaions 9

10 M/M/1 exponenial arrivals exponenial service Erlang arrivals E k /H k /1/K hyperexponenial service infinie # of waiing posiions limied # of waiing posiions general arrivals GI/G/1 general service general arrivals GI/M/K exponenial service K servers infinie # of waiing posiions infinie # of waiing posiions Figure 2: Differen ypes of queuing sysems and heir Kendall s noaion. Lecure: Basic definiions and relaions 10

11 2. Lile s resul Lile s resul: mos general and mos powerful resul; holds for a wide variey of queuing sysem; relaes he following: mean number of cusomers in he sysem (mean queue lengh); mean sojourn ime of cusomer in he sysem; mean number of cusomers enering he sysem per ime uni. Le us define: L: mean queue lengh; W : mean waiing ime of cusomers in he sysem (sojourn ime); λ: mean number of cusomers enering he sysem per ime uni. Lecure: Basic definiions and relaions 11

12 Lile s law: L = λw. (5) his resuls was firsly published by Lile in Noes on Lile s resul: in order o hold queue mus be sable (service rae > arrival rae); he only resul ha holds for almos all queuing sysems; λ is he acual arrival rae! rejecion due o queue is full p (1 p) Figure 3: Acual arrival rae when number of waiing posiions is limied. Lecure: Basic definiions and relaions 12

13 2.1. Inuiive explanaion of he Lile s resul Consider a queuing sysem: i does no maer wha is he arrival process; i does no maer wha is he service process; for simpliciy we assume infinie number of waiing posiions. Operaion sraegy is as follows: cusomers ener he sysem a a random ime; wai o ge service in he buffer; afer service hey leave he sysem. We consider: arrival process as cumulaive number of arrivals in [0, ); deparure process as cumulaive number of deparures in [0, ). Lecure: Basic definiions and relaions 13

14 Cumulaive number of arrivals/deparures arrival process waiing ime in he sysem if FCFS deparure process number of cusomers in he sysem Time Figure 4: Illusraion of differen quaniies associaed wih a queue. Lecure: Basic definiions and relaions 14

15 Consider a ime period T and inroduce he following noaions: N(T ): number of arrivals in he period T ; A(T ): he oal service imes of all cusomers in he period T : he area beween curves; physical meaning: he carried raffic volume. λ(t ) = N(T )/T : he average arrival rae in he period T ; W (T ) = A(T )/N(T ): mean holding ime in sysem per cusomer in period T ; L(T ) = A(T )/T : he mean number of cusomers in he sysem in he period T. Then, he following relaion beween hese variables holds: L(T ) = A(T ) T = W (T )N(T ) T = λ(t )W (T ). (6) Lecure: Basic definiions and relaions 15

16 Assume he following limiing values exis: lim λ(t ) = λ, lim T W (T ) = W. (7) T Then, he following limi also exiss: Finally, we have Lile s formula: L: mean number of cusomers; λ: rae a which cusomers ener he queue; W : mean waiing ime. The following is imporan: Lile s resul binds inpu parameer λ: we usually know; oupu parameers L and W : we do no know. lim L(T ) = L, (8) T L = λw. (9) Lecure: Basic definiions and relaions 16

17 2.2. Example: how we usually use Lile s resul Consider a simple queuing sysem, M/M/1 queuing sysem. Such queuing sysem is characerized by: renewal arrival process wih exponenially disribued inerarrival imes; exponenially disribued service imes; single server; infinie number of waiing posiions. Le us define hew following: λ: he mean arrival rae of cusomers o he sysem; µ mean service rae of he server; E[W ] mean waiing ime, E[T ] mean sojourn ime. Lecure: Basic definiions and relaions 17

18 For sabiliy we assume ρ = λ/µ < 1: in his case number of cusomers does no grow o infiniy. I can be shown ha: E[N] = we will derive his resuls laer in he following lecure. ρ (1 ρ). (10) We can ge boh mean sojourn ime and mean waiing ime: E[T ] = E[N] λ E[W ] = E[N] λ = 1 µ(1 ρ), 1 µ = ρ µ(1 ρ). (11) Noe: E[N] and E[W ] when ρ and Lile s law does no applicable! Lecure: Basic definiions and relaions 18

19 2.3. Prove of he Lile s law Noe he following: here are a number of proves for Lile s law; for specific queuing sysems hey sill appear! We give he proof for he case: ρ = λ/µ << 1; noe: we explicily imply ha sysem empies infiniely ofen. We assume he following: we sar wih empy sysem; consider ime inerval [0, ); is he ime when he sysem is also empy; A() number of arrivals in [0, ); C() number of service compleions in [0, ). Lecure: Basic definiions and relaions 19

20 Cumulaive numbers 5 4 T T 3 T T 2 T 1 a 1 a 2 a 3 a 4 a 5 d 1 d 2 d 3 d 4 d 5 Figure 5: Illusraion of imes spen in he sysem T i, i = 1, 2,.... Lecure: Basic definiions and relaions 20

21 For any ime : jobs compleed by T i 0 N(s)d(s) jobs arrived by T i. (12) Dividing by we ge: jobs compleed by T i 0 N(s)d(s) jobs arrived by T i. (13) Muliplying and dividing by C() and A(): jobs compleed by T i C() N(s)d(s) 0 C() jobs arrived by T i A() A(). (14) Taking limis as : jobs compleed by T i C() lim lim C() lim 0 N(s)d(s) lim jobs arrived by T i A() lim A(). (15) Lecure: Basic definiions and relaions 21

22 Consider: lim jobs compleed by T i C() lim C() lim 0 N(s)d(s) lim jobs arrived by T i A() lim A(). (16) We ge: E[T ]ν E[N] λe[t ], (17) ν is he mean deparure rae; λ is he mean arrival rae; E[T ] is he mean sojourn ime; E[N] is he mean number of cusomers. For sable sysems (µ > λ) we have ν = λ leading o: E[N] = λe[t ]. (18) Lecure: Basic definiions and relaions 22

23 2.4. Example Simple example: a bank visied by 24 cusomers per hour on average; cusomers form a queue when all ellers are busy; he mean queue lengh is observed o be 2.4 cusomers; he mean service ime is 5 minues; wha are he mean arrival rae, waiing ime, sojourn ime, offered raffic load? Soluion: he mean arrival rae o he sysem is: λ = he mean waiing ime of cusomers: = 0.4, cusomers per minue. (19) E[W ] = E[N] λ = = 6, minues. (20) Lecure: Basic definiions and relaions 23

24 he mean sojourn ime (ime spen by cusomer in he bank) is: E[T ] = E[W ] + 1 µ = = 11, minues. (21) he mean number of cusomers in he bank is: he offered raffic load is: E[N] = λe[t ] = = 4.4, cusomers. (22) ρ = λ 1 µ = = 2, (23) he mean number of cusomers being served a any ime is 2. Noe he following: one eller can carry load ρ < 1; if here are less han 2 ellers, queue will be unsable: number of waiing cusomers will grow o infiniy; queue is sable if ρ > λn/µ, where n is he number of ellers. Lecure: Basic definiions and relaions 24

5. Stochastic processes (1)

5. Stochastic processes (1) Lec05.pp S-38.45 - Inroducion o Teleraffic Theory Spring 2005 Conens Basic conceps Poisson process 2 Sochasic processes () Consider some quaniy in a eleraffic (or any) sysem I ypically evolves in ime randomly

More information

Lecture 4 Notes (Little s Theorem)

Lecture 4 Notes (Little s Theorem) Lecure 4 Noes (Lile s Theorem) This lecure concerns one of he mos imporan (and simples) heorems in Queuing Theory, Lile s Theorem. More informaion can be found in he course book, Bersekas & Gallagher,

More information

IS 709/809: Computational Methods in IS Research. Queueing Theory Introduction

IS 709/809: Computational Methods in IS Research. Queueing Theory Introduction IS 709/809: Compuaional Mehods in IS Research Queueing Theory Inroducion Nirmalya Roy Deparmen of Informaion Sysems Universiy of Maryland Balimore Couny www.umbc.edu Inroducion: Saisics of hings Waiing

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

T L. t=1. Proof of Lemma 1. Using the marginal cost accounting in Equation(4) and standard arguments. t )+Π RB. t )+K 1(Q RB

T L. t=1. Proof of Lemma 1. Using the marginal cost accounting in Equation(4) and standard arguments. t )+Π RB. t )+K 1(Q RB Elecronic Companion EC.1. Proofs of Technical Lemmas and Theorems LEMMA 1. Le C(RB) be he oal cos incurred by he RB policy. Then we have, T L E[C(RB)] 3 E[Z RB ]. (EC.1) Proof of Lemma 1. Using he marginal

More information

Homework 4 (Stats 620, Winter 2017) Due Tuesday Feb 14, in class Questions are derived from problems in Stochastic Processes by S. Ross.

Homework 4 (Stats 620, Winter 2017) Due Tuesday Feb 14, in class Questions are derived from problems in Stochastic Processes by S. Ross. Homework 4 (Sas 62, Winer 217) Due Tuesday Feb 14, in class Quesions are derived from problems in Sochasic Processes by S. Ross. 1. Le A() and Y () denoe respecively he age and excess a. Find: (a) P{Y

More information

Chapter 3 Common Families of Distributions

Chapter 3 Common Families of Distributions Chaer 3 Common Families of Disribuions Secion 31 - Inroducion Purose of his Chaer: Caalog many of common saisical disribuions (families of disribuions ha are indeed by one or more arameers) Wha we should

More information

EE 315 Notes. Gürdal Arslan CLASS 1. (Sections ) What is a signal?

EE 315 Notes. Gürdal Arslan CLASS 1. (Sections ) What is a signal? EE 35 Noes Gürdal Arslan CLASS (Secions.-.2) Wha is a signal? In his class, a signal is some funcion of ime and i represens how some physical quaniy changes over some window of ime. Examples: velociy of

More information

Introduction to Probability and Statistics Slides 4 Chapter 4

Introduction to Probability and Statistics Slides 4 Chapter 4 Inroducion o Probabiliy and Saisics Slides 4 Chaper 4 Ammar M. Sarhan, asarhan@mahsa.dal.ca Deparmen of Mahemaics and Saisics, Dalhousie Universiy Fall Semeser 8 Dr. Ammar Sarhan Chaper 4 Coninuous Random

More information

Continuous Time Linear Time Invariant (LTI) Systems. Dr. Ali Hussein Muqaibel. Introduction

Continuous Time Linear Time Invariant (LTI) Systems. Dr. Ali Hussein Muqaibel. Introduction /9/ Coninuous Time Linear Time Invarian (LTI) Sysems Why LTI? Inroducion Many physical sysems. Easy o solve mahemaically Available informaion abou analysis and design. We can apply superposiion LTI Sysem

More information

Vehicle Arrival Models : Headway

Vehicle Arrival Models : Headway Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where

More information

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Simulaion-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Week Descripion Reading Maerial 2 Compuer Simulaion of Dynamic Models Finie Difference, coninuous saes, discree ime Simple Mehods Euler Trapezoid

More information

in Engineering Prof. Dr. Michael Havbro Faber ETH Zurich, Switzerland Swiss Federal Institute of Technology

in Engineering Prof. Dr. Michael Havbro Faber ETH Zurich, Switzerland Swiss Federal Institute of Technology Risk and Saey in Engineering Pro. Dr. Michael Havbro Faber ETH Zurich, Swizerland Conens o Today's Lecure Inroducion o ime varian reliabiliy analysis The Poisson process The ormal process Assessmen o he

More information

Diebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles

Diebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles Diebold, Chaper 7 Francis X. Diebold, Elemens of Forecasing, 4h Ediion (Mason, Ohio: Cengage Learning, 006). Chaper 7. Characerizing Cycles Afer compleing his reading you should be able o: Define covariance

More information

Continuous Time Markov Chain (Markov Process)

Continuous Time Markov Chain (Markov Process) Coninuous Time Markov Chain (Markov Process) The sae sace is a se of all non-negaive inegers The sysem can change is sae a any ime ( ) denoes he sae of he sysem a ime The random rocess ( ) forms a coninuous-ime

More information

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan Ground Rules PC11 Fundamenals of Physics I Lecures 3 and 4 Moion in One Dimension A/Prof Tay Seng Chuan 1 Swich off your handphone and pager Swich off your lapop compuer and keep i No alking while lecure

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

on the interval (x + 1) 0! x < ", where x represents feet from the first fence post. How many square feet of fence had to be painted?

on the interval (x + 1) 0! x < , where x represents feet from the first fence post. How many square feet of fence had to be painted? Calculus II MAT 46 Improper Inegrals A mahemaician asked a fence painer o complee he unique ask of paining one side of a fence whose face could be described by he funcion y f (x on he inerval (x + x

More information

Transform Techniques. Moment Generating Function

Transform Techniques. Moment Generating Function Transform Techniques A convenien way of finding he momens of a random variable is he momen generaing funcion (MGF). Oher ransform echniques are characerisic funcion, z-ransform, and Laplace ransform. Momen

More information

Solutions to Assignment 1

Solutions to Assignment 1 MA 2326 Differenial Equaions Insrucor: Peronela Radu Friday, February 8, 203 Soluions o Assignmen. Find he general soluions of he following ODEs: (a) 2 x = an x Soluion: I is a separable equaion as we

More information

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is UNIT IMPULSE RESPONSE, UNIT STEP RESPONSE, STABILITY. Uni impulse funcion (Dirac dela funcion, dela funcion) rigorously defined is no sricly a funcion, bu disribuion (or measure), precise reamen requires

More information

Inventory Control of Perishable Items in a Two-Echelon Supply Chain

Inventory Control of Perishable Items in a Two-Echelon Supply Chain Journal of Indusrial Engineering, Universiy of ehran, Special Issue,, PP. 69-77 69 Invenory Conrol of Perishable Iems in a wo-echelon Supply Chain Fariborz Jolai *, Elmira Gheisariha and Farnaz Nojavan

More information

Sterilization D Values

Sterilization D Values Seriliaion D Values Seriliaion by seam consis of he simple observaion ha baceria die over ime during exposure o hea. They do no all live for a finie period of hea exposure and hen suddenly die a once,

More information

Matlab and Python programming: how to get started

Matlab and Python programming: how to get started Malab and Pyhon programming: how o ge sared Equipping readers he skills o wrie programs o explore complex sysems and discover ineresing paerns from big daa is one of he main goals of his book. In his chaper,

More information

Lecture 4 Kinetics of a particle Part 3: Impulse and Momentum

Lecture 4 Kinetics of a particle Part 3: Impulse and Momentum MEE Engineering Mechanics II Lecure 4 Lecure 4 Kineics of a paricle Par 3: Impulse and Momenum Linear impulse and momenum Saring from he equaion of moion for a paricle of mass m which is subjeced o an

More information

Linear Response Theory: The connection between QFT and experiments

Linear Response Theory: The connection between QFT and experiments Phys540.nb 39 3 Linear Response Theory: The connecion beween QFT and experimens 3.1. Basic conceps and ideas Q: How do we measure he conduciviy of a meal? A: we firs inroduce a weak elecric field E, and

More information

18 Biological models with discrete time

18 Biological models with discrete time 8 Biological models wih discree ime The mos imporan applicaions, however, may be pedagogical. The elegan body of mahemaical heory peraining o linear sysems (Fourier analysis, orhogonal funcions, and so

More information

EE 435. Lecture 31. Absolute and Relative Accuracy DAC Design. The String DAC

EE 435. Lecture 31. Absolute and Relative Accuracy DAC Design. The String DAC EE 435 Lecure 3 Absolue and Relaive Accuracy DAC Design The Sring DAC . Review from las lecure. DFT Simulaion from Malab Quanizaion Noise DACs and ADCs generally quanize boh ampliude and ime If convering

More information

Appendix to Creating Work Breaks From Available Idleness

Appendix to Creating Work Breaks From Available Idleness Appendix o Creaing Work Breaks From Available Idleness Xu Sun and Ward Whi Deparmen of Indusrial Engineering and Operaions Research, Columbia Universiy, New York, NY, 127; {xs2235,ww24}@columbia.edu Sepember

More information

Performance Evaluation of Quantum Merging: Negative Queue Length

Performance Evaluation of Quantum Merging: Negative Queue Length Performance Evaluaion of Quanum Merging: Negaive Queue Lengh Hiroshi Toyoizumi oyoizumi@waseda.jp Waseda Universiy Nishi-waseda -6-, Shinjuku, Tokyo 69-8050 TEL: +8-3-30-93 FAX: +8-3-586-987 Absrac We

More information

KINEMATICS IN ONE DIMENSION

KINEMATICS IN ONE DIMENSION KINEMATICS IN ONE DIMENSION PREVIEW Kinemaics is he sudy of how hings move how far (disance and displacemen), how fas (speed and velociy), and how fas ha how fas changes (acceleraion). We say ha an objec

More information

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,

More information

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n Module Fick s laws of diffusion Fick s laws of diffusion and hin film soluion Adolf Fick (1855) proposed: d J α d d d J (mole/m s) flu (m /s) diffusion coefficien and (mole/m 3 ) concenraion of ions, aoms

More information

Stability analysis of parallel server systems under longest queue first

Stability analysis of parallel server systems under longest queue first Mah Meh Oper Res (2011) 74:257 279 DOI 10.1007/s00186-011-0362-5 ORIGINAL ARTICLE Sabiliy analysis of parallel server sysems under longes queue firs Golshid Baharian Tolga Tezcan Received: 15 November

More information

LAPLACE TRANSFORM AND TRANSFER FUNCTION

LAPLACE TRANSFORM AND TRANSFER FUNCTION CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION Professor Dae Ryook Yang Spring 2018 Dep. of Chemical and Biological Engineering 5-1 Road Map of he Lecure V Laplace Transform and Transfer funcions

More information

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes Half-Range Series 2.5 Inroducion In his Secion we address he following problem: Can we find a Fourier series expansion of a funcion defined over a finie inerval? Of course we recognise ha such a funcion

More information

6. Stochastic calculus with jump processes

6. Stochastic calculus with jump processes A) Trading sraegies (1/3) Marke wih d asses S = (S 1,, S d ) A rading sraegy can be modelled wih a vecor φ describing he quaniies invesed in each asse a each insan : φ = (φ 1,, φ d ) The value a of a porfolio

More information

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t M ah 5 2 7 Fall 2 0 0 9 L ecure 1 0 O c. 7, 2 0 0 9 Hamilon- J acobi Equaion: Explici Formulas In his lecure we ry o apply he mehod of characerisics o he Hamilon-Jacobi equaion: u + H D u, x = 0 in R n

More information

Logic in computer science

Logic in computer science Logic in compuer science Logic plays an imporan role in compuer science Logic is ofen called he calculus of compuer science Logic plays a similar role in compuer science o ha played by calculus in he physical

More information

Transient Little s Law for the First and Second Moments of G/M/1/N Queue Measures

Transient Little s Law for the First and Second Moments of G/M/1/N Queue Measures J. Service Science & Managemen,, 3, 5-59 doi:.436/ssm..3458 Published Online December (hp://www.scirp.org/ournal/ssm) Transien ile s aw for he Firs and Second Momens of G/M//N Queue Measures Avi Herbon,,

More information

Signals and Systems Linear Time-Invariant (LTI) Systems

Signals and Systems Linear Time-Invariant (LTI) Systems Signals and Sysems Linear Time-Invarian (LTI) Sysems Chang-Su Kim Discree-Time LTI Sysems Represening Signals in Terms of Impulses Sifing propery 0 x[ n] x[ k] [ n k] k x[ 2] [ n 2] x[ 1] [ n1] x[0] [

More information

Stochastic models and their distributions

Stochastic models and their distributions Sochasic models and heir disribuions Couning cusomers Suppose ha n cusomers arrive a a grocery a imes, say T 1,, T n, each of which akes any real number in he inerval (, ) equally likely The values T 1,,

More information

Internet Traffic Modeling for Efficient Network Research Management Prof. Zhili Sun, UniS Zhiyong Liu, CATR

Internet Traffic Modeling for Efficient Network Research Management Prof. Zhili Sun, UniS Zhiyong Liu, CATR Inerne Traffic Modeling for Efficien Nework Research Managemen Prof. Zhili Sun, UniS Zhiyong Liu, CATR UK-China Science Bridge Workshop 13-14 December 2011, London Ouline Inroducion Background Classical

More information

Module 3: The Damped Oscillator-II Lecture 3: The Damped Oscillator-II

Module 3: The Damped Oscillator-II Lecture 3: The Damped Oscillator-II Module 3: The Damped Oscillaor-II Lecure 3: The Damped Oscillaor-II 3. Over-damped Oscillaions. This refers o he siuaion where β > ω (3.) The wo roos are and α = β + α 2 = β β 2 ω 2 = (3.2) β 2 ω 2 = 2

More information

The Strong Law of Large Numbers

The Strong Law of Large Numbers Lecure 9 The Srong Law of Large Numbers Reading: Grimme-Sirzaker 7.2; David Williams Probabiliy wih Maringales 7.2 Furher reading: Grimme-Sirzaker 7.1, 7.3-7.5 Wih he Convergence Theorem (Theorem 54) and

More information

Hybrid Control and Switched Systems. Lecture #3 What can go wrong? Trajectories of hybrid systems

Hybrid Control and Switched Systems. Lecture #3 What can go wrong? Trajectories of hybrid systems Hybrid Conrol and Swiched Sysems Lecure #3 Wha can go wrong? Trajecories of hybrid sysems João P. Hespanha Universiy of California a Sana Barbara Summary 1. Trajecories of hybrid sysems: Soluion o a hybrid

More information

9/9/99 (T.F. Weiss) Signals and systems This subject deals with mathematical methods used to describe signals and to analyze and synthesize systems.

9/9/99 (T.F. Weiss) Signals and systems This subject deals with mathematical methods used to describe signals and to analyze and synthesize systems. 9/9/99 (T.F. Weiss) Lecure #: Inroducion o signals Moivaion: To describe signals, boh man-made and naurally occurring. Ouline: Classificaion ofsignals Building-block signals complex exponenials, impulses

More information

Stochastic Reservoir Systems with Different Assumptions for Storage Losses

Stochastic Reservoir Systems with Different Assumptions for Storage Losses American Journal of Operaions Research, 26, 6, 44-423 hp://www.scirp.org/journal/ajor ISSN Online: 26-8849 ISSN Prin: 26-883 Sochasic Reservoir Ssems wih Differen Assumpions for Sorage Losses Carer Browning,

More information

EE 435. Lecture 35. Absolute and Relative Accuracy DAC Design. The String DAC

EE 435. Lecture 35. Absolute and Relative Accuracy DAC Design. The String DAC EE 435 Lecure 35 Absolue and Relaive Accuracy DAC Design The Sring DAC Makekup Lecures Rm 6 Sweeney 5:00 Rm 06 Coover 6:00 o 8:00 . Review from las lecure. Summary of ime and ampliude quanizaion assessmen

More information

CHAPTER 2 Signals And Spectra

CHAPTER 2 Signals And Spectra CHAPER Signals And Specra Properies of Signals and Noise In communicaion sysems he received waveform is usually caegorized ino he desired par conaining he informaion, and he undesired par. he desired par

More information

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8.

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8. Kinemaics Vocabulary Kinemaics and One Dimensional Moion 8.1 WD1 Kinema means movemen Mahemaical descripion of moion Posiion Time Inerval Displacemen Velociy; absolue value: speed Acceleraion Averages

More information

Chapter 2. Models, Censoring, and Likelihood for Failure-Time Data

Chapter 2. Models, Censoring, and Likelihood for Failure-Time Data Chaper 2 Models, Censoring, and Likelihood for Failure-Time Daa William Q. Meeker and Luis A. Escobar Iowa Sae Universiy and Louisiana Sae Universiy Copyrigh 1998-2008 W. Q. Meeker and L. A. Escobar. Based

More information

The Arcsine Distribution

The Arcsine Distribution The Arcsine Disribuion Chris H. Rycrof Ocober 6, 006 A common heme of he class has been ha he saisics of single walker are ofen very differen from hose of an ensemble of walkers. On he firs homework, we

More information

Basic Circuit Elements Professor J R Lucas November 2001

Basic Circuit Elements Professor J R Lucas November 2001 Basic Circui Elemens - J ucas An elecrical circui is an inerconnecion of circui elemens. These circui elemens can be caegorised ino wo ypes, namely acive and passive elemens. Some Definiions/explanaions

More information

SOLUTIONS TO ECE 3084

SOLUTIONS TO ECE 3084 SOLUTIONS TO ECE 384 PROBLEM 2.. For each sysem below, specify wheher or no i is: (i) memoryless; (ii) causal; (iii) inverible; (iv) linear; (v) ime invarian; Explain your reasoning. If he propery is no

More information

Guest Lectures for Dr. MacFarlane s EE3350 Part Deux

Guest Lectures for Dr. MacFarlane s EE3350 Part Deux Gues Lecures for Dr. MacFarlane s EE3350 Par Deux Michael Plane Mon., 08-30-2010 Wrie name in corner. Poin ou his is a review, so I will go faser. Remind hem o go lisen o online lecure abou geing an A

More information

Stationary Distribution. Design and Analysis of Algorithms Andrei Bulatov

Stationary Distribution. Design and Analysis of Algorithms Andrei Bulatov Saionary Disribuion Design and Analysis of Algorihms Andrei Bulaov Algorihms Markov Chains 34-2 Classificaion of Saes k By P we denoe he (i,j)-enry of i, j Sae is accessible from sae if 0 for some k 0

More information

PHYSICS 149: Lecture 9

PHYSICS 149: Lecture 9 PHYSICS 149: Lecure 9 Chaper 3 3.2 Velociy and Acceleraion 3.3 Newon s Second Law of Moion 3.4 Applying Newon s Second Law 3.5 Relaive Velociy Lecure 9 Purdue Universiy, Physics 149 1 Velociy (m/s) The

More information

SPDE LIMITS OF MANY-SERVER QUEUES. By Haya Kaspi and Kavita Ramanan Technion, Israel and Brown University, USA

SPDE LIMITS OF MANY-SERVER QUEUES. By Haya Kaspi and Kavita Ramanan Technion, Israel and Brown University, USA Submied o he Annals of Applied Probabiliy SPDE LIMITS OF MANY-SERVER QUEUES By Haya Kaspi and Kavia Ramanan Technion, Israel and Brown Universiy, USA This papers sudies a queueing sysem in which cusomers

More information

Designing Information Devices and Systems I Spring 2019 Lecture Notes Note 17

Designing Information Devices and Systems I Spring 2019 Lecture Notes Note 17 EES 16A Designing Informaion Devices and Sysems I Spring 019 Lecure Noes Noe 17 17.1 apaciive ouchscreen In he las noe, we saw ha a capacior consiss of wo pieces on conducive maerial separaed by a nonconducive

More information

Laplace Transform and its Relation to Fourier Transform

Laplace Transform and its Relation to Fourier Transform Chaper 6 Laplace Transform and is Relaion o Fourier Transform (A Brief Summary) Gis of he Maer 2 Domains of Represenaion Represenaion of signals and sysems Time Domain Coninuous Discree Time Time () [n]

More information

Module 4: Time Response of discrete time systems Lecture Note 2

Module 4: Time Response of discrete time systems Lecture Note 2 Module 4: Time Response of discree ime sysems Lecure Noe 2 1 Prooype second order sysem The sudy of a second order sysem is imporan because many higher order sysem can be approimaed by a second order model

More information

15. Vector Valued Functions

15. Vector Valued Functions 1. Vecor Valued Funcions Up o his poin, we have presened vecors wih consan componens, for example, 1, and,,4. However, we can allow he componens of a vecor o be funcions of a common variable. For example,

More information

KEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow

KEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow 1 KEY Mah 4 Miderm I Fall 8 secions 1 and Insrucor: Sco Glasgow Please do NOT wrie on his eam. No credi will be given for such work. Raher wrie in a blue book, or on our own paper, preferabl engineering

More information

EXERCISES FOR SECTION 1.5

EXERCISES FOR SECTION 1.5 1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler

More information

Reading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4.

Reading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4. PHY1 Elecriciy Topic 7 (Lecures 1 & 11) Elecric Circuis n his opic, we will cover: 1) Elecromoive Force (EMF) ) Series and parallel resisor combinaions 3) Kirchhoff s rules for circuis 4) Time dependence

More information

Continuous Time. Time-Domain System Analysis. Impulse Response. Impulse Response. Impulse Response. Impulse Response. ( t) + b 0.

Continuous Time. Time-Domain System Analysis. Impulse Response. Impulse Response. Impulse Response. Impulse Response. ( t) + b 0. Time-Domain Sysem Analysis Coninuous Time. J. Robers - All Righs Reserved. Edied by Dr. Rober Akl 1. J. Robers - All Righs Reserved. Edied by Dr. Rober Akl 2 Le a sysem be described by a 2 y ( ) + a 1

More information

This document was generated at 7:34 PM, 07/27/09 Copyright 2009 Richard T. Woodward

This document was generated at 7:34 PM, 07/27/09 Copyright 2009 Richard T. Woodward his documen was generaed a 7:34 PM, 07/27/09 Copyrigh 2009 Richard. Woodward 15. Bang-bang and mos rapid approach problems AGEC 637 - Summer 2009 here are some problems for which he opimal pah does no

More information

Written Exercise Sheet 5

Written Exercise Sheet 5 jian-jia.chen [ ] u-dormund.de lea.schoenberger [ ] u-dormund.de Exercise for he lecure Embedded Sysems Winersemeser 17/18 Wrien Exercise Shee 5 Hins: These assignmens will be discussed a E23 OH14, from

More information

2. Nonlinear Conservation Law Equations

2. Nonlinear Conservation Law Equations . Nonlinear Conservaion Law Equaions One of he clear lessons learned over recen years in sudying nonlinear parial differenial equaions is ha i is generally no wise o ry o aack a general class of nonlinear

More information

The Contradiction within Equations of Motion with Constant Acceleration

The Contradiction within Equations of Motion with Constant Acceleration The Conradicion wihin Equaions of Moion wih Consan Acceleraion Louai Hassan Elzein Basheir (Daed: July 7, 0 This paper is prepared o demonsrae he violaion of rules of mahemaics in he algebraic derivaion

More information

Question 1: Question 2: Topology Exercise Sheet 3

Question 1: Question 2: Topology Exercise Sheet 3 Topology Exercise Shee 3 Prof. Dr. Alessandro Siso Due o 14 March Quesions 1 and 6 are more concepual and should have prioriy. Quesions 4 and 5 admi a relaively shor soluion. Quesion 7 is harder, and you

More information

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes Some common engineering funcions 2.7 Inroducion This secion provides a caalogue of some common funcions ofen used in Science and Engineering. These include polynomials, raional funcions, he modulus funcion

More information

= ( ) ) or a system of differential equations with continuous parametrization (T = R

= ( ) ) or a system of differential equations with continuous parametrization (T = R XIII. DIFFERENCE AND DIFFERENTIAL EQUATIONS Ofen funcions, or a sysem of funcion, are paramerized in erms of some variable, usually denoed as and inerpreed as ime. The variable is wrien as a funcion of

More information

The Quantum Theory of Atoms and Molecules: The Schrodinger equation. Hilary Term 2008 Dr Grant Ritchie

The Quantum Theory of Atoms and Molecules: The Schrodinger equation. Hilary Term 2008 Dr Grant Ritchie e Quanum eory of Aoms and Molecules: e Scrodinger equaion Hilary erm 008 Dr Gran Ricie An equaion for maer waves? De Broglie posulaed a every paricles as an associaed wave of waveleng: / p Wave naure of

More information

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon 3..3 INRODUCION O DYNAMIC OPIMIZAION: DISCREE IME PROBLEMS A. he Hamilonian and Firs-Order Condiions in a Finie ime Horizon Define a new funcion, he Hamilonian funcion, H. H he change in he oal value of

More information

Optima and Equilibria for Traffic Flow on a Network

Optima and Equilibria for Traffic Flow on a Network Opima and Equilibria for Traffic Flow on a Nework Albero Bressan Deparmen of Mahemaics, Penn Sae Universiy bressan@mah.psu.edu Albero Bressan (Penn Sae) Opima and equilibria for raffic flow 1 / 1 A Traffic

More information

Math 111 Midterm I, Lecture A, version 1 -- Solutions January 30 th, 2007

Math 111 Midterm I, Lecture A, version 1 -- Solutions January 30 th, 2007 NAME: Suden ID #: QUIZ SECTION: Mah 111 Miderm I, Lecure A, version 1 -- Soluions January 30 h, 2007 Problem 1 4 Problem 2 6 Problem 3 20 Problem 4 20 Toal: 50 You are allowed o use a calculaor, a ruler,

More information

Traveling Waves. Chapter Introduction

Traveling Waves. Chapter Introduction Chaper 4 Traveling Waves 4.1 Inroducion To dae, we have considered oscillaions, i.e., periodic, ofen harmonic, variaions of a physical characerisic of a sysem. The sysem a one ime is indisinguishable from

More information

Comparison between the Discrete and Continuous Time Models

Comparison between the Discrete and Continuous Time Models Comparison beween e Discree and Coninuous Time Models D. Sulsky June 21, 2012 1 Discree o Coninuous Recall e discree ime model Î = AIS Ŝ = S Î. Tese equaions ell us ow e populaion canges from one day o

More information

Summary of shear rate kinematics (part 1)

Summary of shear rate kinematics (part 1) InroToMaFuncions.pdf 4 CM465 To proceed o beer-designed consiuive equaions, we need o know more abou maerial behavior, i.e. we need more maerial funcions o predic, and we need measuremens of hese maerial

More information

Representation of Stochastic Process by Means of Stochastic Integrals

Representation of Stochastic Process by Means of Stochastic Integrals Inernaional Journal of Mahemaics Research. ISSN 0976-5840 Volume 5, Number 4 (2013), pp. 385-397 Inernaional Research Publicaion House hp://www.irphouse.com Represenaion of Sochasic Process by Means of

More information

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems.

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems. Mah 2250-004 Week 4 April 6-20 secions 7.-7.3 firs order sysems of linear differenial equaions; 7.4 mass-spring sysems. Mon Apr 6 7.-7.2 Sysems of differenial equaions (7.), and he vecor Calculus we need

More information

On Measuring Pro-Poor Growth. 1. On Various Ways of Measuring Pro-Poor Growth: A Short Review of the Literature

On Measuring Pro-Poor Growth. 1. On Various Ways of Measuring Pro-Poor Growth: A Short Review of the Literature On Measuring Pro-Poor Growh 1. On Various Ways of Measuring Pro-Poor Growh: A Shor eview of he Lieraure During he pas en years or so here have been various suggesions concerning he way one should check

More information

h[n] is the impulse response of the discrete-time system:

h[n] is the impulse response of the discrete-time system: Definiion Examples Properies Memory Inveribiliy Causaliy Sabiliy Time Invariance Lineariy Sysems Fundamenals Overview Definiion of a Sysem x() h() y() x[n] h[n] Sysem: a process in which inpu signals are

More information

( ) a system of differential equations with continuous parametrization ( T = R + These look like, respectively:

( ) a system of differential equations with continuous parametrization ( T = R + These look like, respectively: XIII. DIFFERENCE AND DIFFERENTIAL EQUATIONS Ofen funcions, or a sysem of funcion, are paramerized in erms of some variable, usually denoed as and inerpreed as ime. The variable is wrien as a funcion of

More information

Laplace Transforms. Examples. Is this equation differential? y 2 2y + 1 = 0, y 2 2y + 1 = 0, (y ) 2 2y + 1 = cos x,

Laplace Transforms. Examples. Is this equation differential? y 2 2y + 1 = 0, y 2 2y + 1 = 0, (y ) 2 2y + 1 = cos x, Laplace Transforms Definiion. An ordinary differenial equaion is an equaion ha conains one or several derivaives of an unknown funcion which we call y and which we wan o deermine from he equaion. The equaion

More information

Lecture Outline. Introduction Transmission Line Equations Transmission Line Wave Equations 8/10/2018. EE 4347 Applied Electromagnetics.

Lecture Outline. Introduction Transmission Line Equations Transmission Line Wave Equations 8/10/2018. EE 4347 Applied Electromagnetics. 8/10/018 Course Insrucor Dr. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: rcrumpf@uep.edu EE 4347 Applied Elecromagneics Topic 4a Transmission Line Equaions Transmission These Line noes

More information

Laplace transfom: t-translation rule , Haynes Miller and Jeremy Orloff

Laplace transfom: t-translation rule , Haynes Miller and Jeremy Orloff Laplace ransfom: -ranslaion rule 8.03, Haynes Miller and Jeremy Orloff Inroducory example Consider he sysem ẋ + 3x = f(, where f is he inpu and x he response. We know is uni impulse response is 0 for

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLEMENTARY INFORMATION DOI: 0.038/NCLIMATE893 Temporal resoluion and DICE * Supplemenal Informaion Alex L. Maren and Sephen C. Newbold Naional Cener for Environmenal Economics, US Environmenal Proecion

More information

2 Modern Stochastic Process Methods for Multi-state System Reliability Assessment

2 Modern Stochastic Process Methods for Multi-state System Reliability Assessment 2 Modern Sochasic Process Mehods for Muli-sae Sysem Reliabiliy Assessmen The purpose of his chaper is o describe basic conceps of applying a random process heory o MSS reliabiliy assessmen. Here, we do

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

Let us start with a two dimensional case. We consider a vector ( x,

Let us start with a two dimensional case. We consider a vector ( x, Roaion marices We consider now roaion marices in wo and hree dimensions. We sar wih wo dimensions since wo dimensions are easier han hree o undersand, and one dimension is a lile oo simple. However, our

More information

Lecture Notes 2. The Hilbert Space Approach to Time Series

Lecture Notes 2. The Hilbert Space Approach to Time Series Time Series Seven N. Durlauf Universiy of Wisconsin. Basic ideas Lecure Noes. The Hilber Space Approach o Time Series The Hilber space framework provides a very powerful language for discussing he relaionship

More information

Econ107 Applied Econometrics Topic 7: Multicollinearity (Studenmund, Chapter 8)

Econ107 Applied Econometrics Topic 7: Multicollinearity (Studenmund, Chapter 8) I. Definiions and Problems A. Perfec Mulicollineariy Econ7 Applied Economerics Topic 7: Mulicollineariy (Sudenmund, Chaper 8) Definiion: Perfec mulicollineariy exiss in a following K-variable regression

More information

MANAGEMENT SCIENCE doi /mnsc ec pp. ec1 ec20

MANAGEMENT SCIENCE doi /mnsc ec pp. ec1 ec20 MANAGEMENT SCIENCE doi.287/mnsc.7.82ec pp. ec ec2 e-companion ONLY AVAILABLE IN ELECTRONIC FORM informs 28 INFORMS Elecronic Companion Saffing of Time-Varying Queues o Achieve Time-Sable Performance by

More information

Applied Probability. Nathanaël Berestycki, University of Cambridge. Part II, Lent 2014

Applied Probability. Nathanaël Berestycki, University of Cambridge. Part II, Lent 2014 Applied Probabiliy Nahanaël Beresycki, Universiy of Cambridge Par II, Len 214 c Nahanaël Beresycki 214. The copyrigh remains wih he auhor of hese noes. 1 Conens 1 Queueing Theory 3 1.1 Inroducion.....................................

More information

Course Notes for EE227C (Spring 2018): Convex Optimization and Approximation

Course Notes for EE227C (Spring 2018): Convex Optimization and Approximation Course Noes for EE7C Spring 018: Convex Opimizaion and Approximaion Insrucor: Moriz Hard Email: hard+ee7c@berkeley.edu Graduae Insrucor: Max Simchowiz Email: msimchow+ee7c@berkeley.edu Ocober 15, 018 3

More information

Reliability of Technical Systems

Reliability of Technical Systems eliabiliy of Technical Sysems Main Topics Inroducion, Key erms, framing he problem eliabiliy parameers: Failure ae, Failure Probabiliy, Availabiliy, ec. Some imporan reliabiliy disribuions Componen reliabiliy

More information