Reliability Estimate using Degradation Data

Size: px
Start display at page:

Download "Reliability Estimate using Degradation Data"

Transcription

1 Reliabiliy Esimae using Degradaion Daa G. EGHBALI and E. A. ELSAYED Deparmen of Indusrial Engineering Rugers Universiy 96 Frelinghuysen Road Piscaaway, NJ USA Absrac:-The use of degradaion daa o esimae reliabiliy is an alernaive o he use of failure daa when no failures or few failures are epeced o occur in a life esing under normal or acceleraed condiions. Models for reliabiliy esimae using degradaion daa can be classified ino wo groups: physics-based (or eperimenallybased and saisics-based models. The applicaion of a physics-based model is limied o hose unis ha ehibi he same underlying degradaion phenomenon. The saisics-based models are more general han he physicsbased models; however, hey assume ha he degradaion pahs are linear and/or he sandard deviaion of he degradaion daa is consan. In his paper, we propose a saisics-based approach ha relaes hese assumpions and illusrae is applicabiliy using numerical eample. Key-ords:- Degradaion, reliabiliy models, saisics-based models INTRODUCTION Noaion S( S resisance drif a ime X random variable represening he degradaion measure, X ime f( ; probabiliy densiy funcion ( pdf of X a ime F( ; cumulaive disribuion funcion (CDF complemen of X r ( ; hazard funcion of f( ;, referred o as he degradaion hazard funcion g (, q ( posiive funcions T random variable represening he ime o degrade o a,b,, λ, θ consans R ( reliabiliy a ime given a hreshold degradaion level R ( T > H ( = ln R ( There are many producs ha ehibi performance degradaion over ime. They include appliances, auomobiles, and many elecronic componens. For eample, consider a resisor wih resisance S a = ha ehibis a change S( of is value wih ime resuling in a drif of S( S. This, in urn, will cause a gradual degradaion in he performance of he sysem in which he resisor is a componen unil he drif reaches a hreshold level ha causes he sysem s failure. Therefore, i is of ineres o observe he degradaion of he sysem s performance over ime and uilize such observaions in esimaing he reliabiliy of he sysem. Elsayed (996 classifies he acceleraed failure daa models as saisics-based models (parameric and nonparameric, physics-saisics based models, and physics-eperimenally based models. Similarly, we classify he degradaion models as physics-based and saisics-based models. The physics-based degradaion models are hose in which he degradaion phenomenon is described by a physicsbased relaionship like Arrhenius law or eperimenally-based resuls such as ho carrier degradaion model in Leblebici and Kang (993. The saisics-based degradaion models are hose in which he degradaion phenomenon is described by a saisical model such as regression.

2 . Model Developmen I is assumed ha he effec of he degradaion phenomenon on he produc performance can be epressed by a random variable called degradaion measure. Typical measures include he amoun of wear of mechanical pars such as shafs and bearings, he drif of a resisor, oupu power drop of ligh emiing diodes, and he propagaion delay of an elecronic chip. I is clear ha unis wih he same age would have differen degradaion measure levels; he degradaion measure is a sochasic process. For a specific ime, he degradaion measure, X, is a random variable ha is disribuion is ime dependen [Papoulis (965]. The degradaion measure disribuion, in general, migh change wih ime in he ype of he disribuion family and is parameers as shown in Figure. The solid curve represens he mean of he degradaion measure versus ime and he areas under he densiy funcions bu above he hreshold level line represen he failure probabiliy a he corresponding imes. In his paper, we assume ha he degradaion measure follows he same disribuion family bu is parameers may change wih ime. I is also assumed ha he degradaion pahs are monoonic funcions of ime: Monoonically Increasing Degradaion Pahs (MIDP or Monoonically Decreasing Degradaion Pahs (MDDP. P P( X < ;, for MIDP ( T > = P( X > ;, ( for MDDP P ( X < ; corresponds o producs ha fail when he degradaion measure reaches above a hreshold level (MIDP such as he case of he IFL devices described in Carey and Koenig (99. On he oher hand, P ( X > ; corresponds o producs ha fail when he degradaion measure reaches below a hreshold level (MDDP such as he case of he srengh of insulaion maerial [Nelson (98]. e prove Eq.( for MDDP as follows: PT ( > = PT ( > X= s; f( s; ds = P( T > X = s; f( s; ds + P( T > X = s; f ( s; ds = + f( s; ds X> ; or P( T > X > ;. I should be noed ha P( T > X = s; equals zero for s < since he uni fails as soon as he degradaion measure reaches a level less han. Likewise, P( T > X = s; equals for s >. Eq.( for MIDP can be easily proven using he same approach.. Degradaion hazard funcion. Relaionship beween he ime o degrade and degradaion measure disribuions The relaionships beween he ime o degrade and degradaion measure disribuion is epressed as e define he degradaion hazard funcion as f( ; r ( ; =. ( F( ; Unlike he radiional failure rae funcion, f ( R(, he degradaion hazard funcion considers boh ime and degradaion measure level. I is useful in developing a reliabiliy funcion based on degradaion daa wihou making assumpions abou he degradaion pahs and/or he sandard deviaion of he degradaion daa. I can also be used o invesigae he effec of a change in he hreshold

3 degradaion level on he reliabiliy of he sysem during is design sage. Le us assume ha he degradaion hazard funcion r ( ; can be epressed as he produc of funcions: r ( ; = g( q(, q( >, g( >, (3 where g( and q( are posiive funcions of he degradaion measure and ime, respecively. This assumpion ensures ha he disribuion family of he degradaion measure does no change wih ime as shown below. From Eq.(3 he raio of he degradaion hazard funcions a wo differen imes, and, can be wrien as: r ( ; q ( = (4 r ( ; q ( which means he change in degradaion hazard funcion wih ime is independen of g ( and is proporional o he raio of q q(... Consrains on g ( ( e uilize he properies of he CDF complemen in order o deermine he consrain( on g (. e rewrie F( ; in erms of he degradaion hazard funcion as follows: F( ; X > ; = ep( r( s; d or (5 F ( ; = ep( q( g( d. (6 The following condiions mus be saisfied for Eq.(6. (i F( ; = ep( q( g( d = (ii F( ; = ep( q( g( d = which implies ha gsds ( =. Therefore, he only consrain on g ( is gsds ( =... Consrains on q ( Consrains on q ( are differen for MDDP and MIDP. e firs assume ha he degradaion pahs are monoonically decreasing, MDDP, and uilize Eqs.( and (6 o deermine he consrains on q ( as follows: R ( T > X > ; = ep( q( g( d (7 The necessary and sufficien condiions for R ( o be a valid reliabiliy funcion are: lim R ( = lim ep( q( g( d = ep( lim q ( gsds ( = which implies ha lim ( = q lim R ( = lim ep( q( g( d = ep( lim q ( gsds ( = which implies ha (8 (9 ( lim q ( = ( Therefore, Eqs.(9 and ( are consrains on q (. The consrain on q ( for he monoonically increasing degradaion pahs, MIDP, is differen when as follows: 3 lim R ( = lim { ep( q( g( d} = which implies ha

4 lim ( = q. In summary, q ( approaches infiniy as ime approaches infiniy for he monoonically decreasing degradaion pahs and q ( approaches zero as ime approaches infiniy for he monoonically increasing degradaion pahs. e now show ha he relaionship beween he degradaion pahs and degradaion hazard funcion is as q ( > implies monoonically decreasing degradaion pahs. q ( < implies monoonically increasing degradaion pahs. Proof- Eq.(6 can be wrien as F ( ; F ( ; = ep[ q( ep[ q( = ep[( q( where < <. g( ds] g( ds] q( g( ds] (..3 Inerpreaions of he degradaion hazard funcion The degradaion hazard funcion can have monoonically decreasing or increasing pah. e show he analysis for he increasing pah below...3. Monoonically increasing degradaion pahs Assuming ha he degradaion pahs are monoonically increasing, he condiional probabiliy of a small change in he degradaion measure given ha is value is less han a specified level a ime can be wrien as: PX [ (, ; ] P[ X (, X < ; ] = PX [ < ; ] f(; s ds f( ; = F( ; F( ; (3 Dividing boh sides of Eq.(5 by and aking limis as approaches zero yields: d f ( ; u ( ; = P[ X (, X < ; ] =. (4 d F( ; Assuming ha failure occurs when he degradaion measure reaches, hen u ( ; is he failure rae a ime in erms of degradaion measure. Assuming F( ;, u( ; can be wrien in erms of degradaion hazard funcion as f ( ; F ( ; F ( ; u( ; = = r( ;. (5 F( ; F ( ; F( ; Eq.(5 reveals ha in he monoonically increasing case he degradaion hazard funcion is no he failure rae in erms of he degradaion measure. This can be also undersood from he relaionship beween he cumulaive failure rae and cumulaive degradaion hazard funcion for he monoonically increasing degradaion pahs as shown in Eq.(6. The reliabiliy funcion for he monoonically increasing degradaion pahs is R ( = ep( r( s; d = ep( rs ( ; d(ep( rs ( ; d Taking he logarihm of boh sides yields: H ( = r( s; ds lnψ ( ; (6 o where ψ ( ; = ep( r( s; d. 4

5 In summary, he degradaion hazard funcion represens he failure rae in erms of he degradaion measure when he degradaion pahs are monoonically decreasing bu i only has a conribuion o he failure rae when he degradaion pahs are monoonically increasing. 3. APPLICATION e now uilize he proposed approach o predic he reliabiliy of an insulaion maerial. e use he degradaion daa presened in Table aken from Nelson (98. I is imporan o noe ha each observaion in Table comes from a differen specimen; herefore, he daa are assumed o be independen. The dielecric srengh of he insulaion maerial is considered as he degradaion measure. e consider he following degradaion hazard funcion: r ( ; = qg ( ( ee k where Diele cric sren gh (kv b >>. Table - Degradaion daa ee k Diele cric sren gh (kv eek Diel ecri c sren gh (kv ee k q ( =, g ( = bep( a Diel ecri c sren gh (kv , and The parameric form of q ( is deermined based on graphing he degradaion daa versus ime. Moreover, he disribuion of he degradaion daa in each week is sudied in order o deermine g (. I is realized ha g ( = is a good fi for all 5 weeks. The corresponding degradaion measure disribuion for his degradaion hazard funcion is a eibull disribuion wih a ime-dependen scale parameer as f ( ; = θ ( ep(, > θ ( where θ( = bep( a is he scale parameer. (7 e fi he eibull model given in Eq.(7 o he degradaion daa shown in Table. The Maimum Likelihood mehod was uilized o esimae he parameers of he model as follows: m L(, a, b; = ( bep( a ni i= i m n i ij ij i= j= b ai ep( ep( (8 where m is he number of weeks, n i is he oal number of degradaion observaions in week i and ij is he degradaion measure of uni j in week i. Taking he logarihm of Eq.(8 we obain: m m m ln L= n ln n ln b+ na i i i i i= i= i= m ni m n i ij ( ln ij i= j= i= j= b ai + ep( (9 Taking he parial derivaives of Eq.( wih respec o, a and b yields a =., b = 4993, = Subsiuing he values of q( and g( ino Eq.(7, he reliabiliy funcion can hen be deermined as R R ( X > ; = ep[ ] b ep( a 5.65 ( = ep[ ]. ( 4994ep(-. For =, R ( equals o and R ( equals o zero. Therefore, he necessary and sufficien condiions are saisfied for his model.

6 I is of ineres o deermine effec of changes in he hreshold degradaion level on he componen lifeime a he design sage where he componen specificaions such as he hreshold degradaion level are deermined based on he design requiremens and cos consideraions. 6. Conclusion e inroduce a degradaion hazard funcion which is used o esimae reliabiliy using degradaion daa wihou making assumpions abou he degradaion pahs and he sandard deviaion of he degradaion daa. The developed reliabiliy funcion includes he hreshold degradaion level a which failure occurs as a parameer. Therefore, sensiiviy of he reliabiliy o he hreshold degradaion level can be easily deermined. The proposed saisics-based approach is uilized in esimaing reliabiliy of an insulaion maerial. The reliabiliy esimae is hen compared wih a physics-based reliabiliy esimae of he insulaion maerial. REFERENCES [] I. F. Blake and. C. Lindsey, Level Crossing Problems for Random Processes, IEEE Transacions on Informaion Technology Vol. IT-9 No. 3 (973, [] M. B. Carey and R. H. Koenig, Reliabiliy Assessmen Based on Acceleraed Degradaion: A Case Sudy, IEEE Transacions on Reliabiliy Vol. 4 No. 5 (99, [3] S. E. Chick and M. B. Mendel, An Engineering Basis for Saisical Lifeime Models wih an Applicaion o Tribology, IEEE Transacions on Reliabiliy Vol. 45 No. (996, 8-4. [4] S. L. Chuang, A. Ishibashi, S. Kijima, N. Nakayama, M. Ukia, and S. Taniguchi, Kineic Model for Degradaion of Ligh Emiing Diodes, IEEE Journal of Quanum Elecronics Vol. 33 No. 6 (997, [5] K. A. Doksum and A. Hoyland, Models for Variable-Sress Acceleraed Life Tesing Eperimens Based on iener Processes and he Inverse Gaussian Disribuion, Technomerics Vol. 34 No. (99, [6] M. Domine, Momens of he firs passage ime of a iener process wih drif beween wo elasic barriers, J. Appl. Prob. Vol. 3 (995, 7-3. [7] M. Domine, Firs passage ime disribuion of a iener process wih drif concerning wo elasic barriers, J. Appl. Prob. Vol. 33 (996, [8] E. A. Elsayed, Reliabiliy Engineering, Addison- esley (996. [9] A. A. Feinberg and A. idom, Connecing Parameric Aging o Caasrophic Failure Through Thermodynamics, IEEE Transacions on Reliabiliy Vol. 45 No. (996, [] E. Ioannides, E. Beghini, G. Bergling, J. Goodall and B. Jacobson, Cleanliness and is imporance for bearing performance, Ball Bearing Journal 4 (993, 8-5. [] Y. Leblebici and S-M Kang, Ho carrier Reliabiliy of MOS VLSI Circuis, Boson, Kluwer (993. [] J. C. Lu and. Q. Meeker, Using Degradaion Measures o Esimae a Time-o-Failure Disribuion, Technomerics Vol. 35 No. (993, [3] J. Lu, J. Park and Q. Yang, Saisical Inference of a Time-o-Failure Disribuion Derived From Linear Degradaion Daa, Technomerics Vol. 39 No. 4 (997, 39-4 [4]. Q. Meeker and M. Hamada, Saisical Tools for he Rapid Developmen & Evaluaion of High-Reliabiliy Producs, IEEE Transacions on reliabiliy Vol. 44 No. (995, [5]. Q. Meeker, L. A. Escobar and C. J. Lu, Acceleraed Degradaion Tess: Modeling and Analysis, Technomerics Vol.4 No. (998, [6]. Nelson, Analysis of performancedegradaion Daa from Acceleraed Tess, IEEE Transacions on reliabiliy Vol. R-3 No. (98, [7] A. Papoulis, Probabiliy, Random Variables, and Sochasic Process, McGraw-Hill, (965. [8] V. Pieper, M. Domine, P. Kurh, Level Crossing Problem and Drif Reliabiliy, Mahemaical Mehods of Operaion Research Vol. 45 (997, [9] F. S. Qureshi and A. K. Sheikh, A Probabilisic Characerizaion of Adhesive wear in Meals, IEEE Transacions on Reliabiliy Vol. 46 No. (997,

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

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

Chapter 4. Location-Scale-Based Parametric Distributions. William Q. Meeker and Luis A. Escobar Iowa State University and Louisiana State University

Chapter 4. Location-Scale-Based Parametric Distributions. William Q. Meeker and Luis A. Escobar Iowa State University and Louisiana State University Chaper 4 Locaion-Scale-Based Parameric Disribuions 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 on he auhors

More information

On Multicomponent System Reliability with Microshocks - Microdamages Type of Components Interaction

On Multicomponent System Reliability with Microshocks - Microdamages Type of Components Interaction On Mulicomponen Sysem Reliabiliy wih Microshocks - Microdamages Type of Componens Ineracion Jerzy K. Filus, and Lidia Z. Filus Absrac Consider a wo componen parallel sysem. The defined new sochasic dependences

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

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

Exponential Weighted Moving Average (EWMA) Chart Under The Assumption of Moderateness And Its 3 Control Limits

Exponential Weighted Moving Average (EWMA) Chart Under The Assumption of Moderateness And Its 3 Control Limits DOI: 0.545/mjis.07.5009 Exponenial Weighed Moving Average (EWMA) Char Under The Assumpion of Moderaeness And Is 3 Conrol Limis KALPESH S TAILOR Assisan Professor, Deparmen of Saisics, M. K. Bhavnagar Universiy,

More information

Navneet Saini, Mayank Goyal, Vishal Bansal (2013); Term Project AML310; Indian Institute of Technology Delhi

Navneet Saini, Mayank Goyal, Vishal Bansal (2013); Term Project AML310; Indian Institute of Technology Delhi Creep in Viscoelasic Subsances Numerical mehods o calculae he coefficiens of he Prony equaion using creep es daa and Herediary Inegrals Mehod Navnee Saini, Mayank Goyal, Vishal Bansal (23); Term Projec

More information

A new flexible Weibull distribution

A new flexible Weibull distribution Communicaions for Saisical Applicaions and Mehods 2016, Vol. 23, No. 5, 399 409 hp://dx.doi.org/10.5351/csam.2016.23.5.399 Prin ISSN 2287-7843 / Online ISSN 2383-4757 A new flexible Weibull disribuion

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

FAULT PROGNOSTICS AND RELIABILITY ESTIMATION OF DC MOTOR USING TIME SERIES ANALYSIS BASED ON DEGRADATION DATA

FAULT PROGNOSTICS AND RELIABILITY ESTIMATION OF DC MOTOR USING TIME SERIES ANALYSIS BASED ON DEGRADATION DATA FAULT PROGNOSTICS AND RELIABILITY ESTIMATION OF DC MOTOR USING TIME SERIES ANALYSIS BASED ON DEGRADATION DATA LI WANG, HUIYAN ZHANG, HONG XUE School of Compuer and Informaion Engineering, Beijing Technology

More information

Robust estimation based on the first- and third-moment restrictions of the power transformation model

Robust estimation based on the first- and third-moment restrictions of the power transformation model h Inernaional Congress on Modelling and Simulaion, Adelaide, Ausralia, 6 December 3 www.mssanz.org.au/modsim3 Robus esimaion based on he firs- and hird-momen resricions of he power ransformaion Nawaa,

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

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3 and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or

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

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

On a Discrete-In-Time Order Level Inventory Model for Items with Random Deterioration

On a Discrete-In-Time Order Level Inventory Model for Items with Random Deterioration Journal of Agriculure and Life Sciences Vol., No. ; June 4 On a Discree-In-Time Order Level Invenory Model for Iems wih Random Deerioraion Dr Biswaranjan Mandal Associae Professor of Mahemaics Acharya

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

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

Outline. lse-logo. Outline. Outline. 1 Wald Test. 2 The Likelihood Ratio Test. 3 Lagrange Multiplier Tests

Outline. lse-logo. Outline. Outline. 1 Wald Test. 2 The Likelihood Ratio Test. 3 Lagrange Multiplier Tests Ouline Ouline Hypohesis Tes wihin he Maximum Likelihood Framework There are hree main frequenis approaches o inference wihin he Maximum Likelihood framework: he Wald es, he Likelihood Raio es and he Lagrange

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

Electrical and current self-induction

Electrical and current self-induction Elecrical and curren self-inducion F. F. Mende hp://fmnauka.narod.ru/works.hml mende_fedor@mail.ru Absrac The aricle considers he self-inducance of reacive elemens. Elecrical self-inducion To he laws of

More information

ACE 562 Fall Lecture 4: Simple Linear Regression Model: Specification and Estimation. by Professor Scott H. Irwin

ACE 562 Fall Lecture 4: Simple Linear Regression Model: Specification and Estimation. by Professor Scott H. Irwin ACE 56 Fall 005 Lecure 4: Simple Linear Regression Model: Specificaion and Esimaion by Professor Sco H. Irwin Required Reading: Griffihs, Hill and Judge. "Simple Regression: Economic and Saisical Model

More information

1. Introduction. Rawid Banchuin

1. Introduction. Rawid Banchuin 011 Inernaional Conerence on Inormaion and Elecronics Engineering IPCSIT vol.6 (011 (011 IACSIT Press, Singapore Process Induced Random Variaion Models o Nanoscale MOS Perormance: Eicien ool or he nanoscale

More information

5.2. The Natural Logarithm. Solution

5.2. The Natural Logarithm. Solution 5.2 The Naural Logarihm The number e is an irraional number, similar in naure o π. Is non-erminaing, non-repeaing value is e 2.718 281 828 59. Like π, e also occurs frequenly in naural phenomena. In fac,

More information

EE650R: Reliability Physics of Nanoelectronic Devices Lecture 9:

EE650R: Reliability Physics of Nanoelectronic Devices Lecture 9: EE65R: Reliabiliy Physics of anoelecronic Devices Lecure 9: Feaures of Time-Dependen BTI Degradaion Dae: Sep. 9, 6 Classnoe Lufe Siddique Review Animesh Daa 9. Background/Review: BTI is observed when he

More information

Shiva Akhtarian MSc Student, Department of Computer Engineering and Information Technology, Payame Noor University, Iran

Shiva Akhtarian MSc Student, Department of Computer Engineering and Information Technology, Payame Noor University, Iran Curren Trends in Technology and Science ISSN : 79-055 8hSASTech 04 Symposium on Advances in Science & Technology-Commission-IV Mashhad, Iran A New for Sofware Reliabiliy Evaluaion Based on NHPP wih Imperfec

More information

Time series Decomposition method

Time series Decomposition method Time series Decomposiion mehod A ime series is described using a mulifacor model such as = f (rend, cyclical, seasonal, error) = f (T, C, S, e) Long- Iner-mediaed Seasonal Irregular erm erm effec, effec,

More information

Physics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution

Physics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution Physics 7b: Saisical Mechanics Fokker-Planck Equaion The Langevin equaion approach o he evoluion of he velociy disribuion for he Brownian paricle migh leave you uncomforable. A more formal reamen of his

More information

Stochastic Model for Cancer Cell Growth through Single Forward Mutation

Stochastic Model for Cancer Cell Growth through Single Forward Mutation Journal of Modern Applied Saisical Mehods Volume 16 Issue 1 Aricle 31 5-1-2017 Sochasic Model for Cancer Cell Growh hrough Single Forward Muaion Jayabharahiraj Jayabalan Pondicherry Universiy, jayabharahi8@gmail.com

More information

Sensors, Signals and Noise

Sensors, Signals and Noise Sensors, Signals and Noise COURSE OUTLINE Inroducion Signals and Noise: 1) Descripion Filering Sensors and associaed elecronics rv 2017/02/08 1 Noise Descripion Noise Waveforms and Samples Saisics of Noise

More information

Empirical Process Theory

Empirical Process Theory Empirical Process heory 4.384 ime Series Analysis, Fall 27 Reciaion by Paul Schrimpf Supplemenary o lecures given by Anna Mikusheva Ocober 7, 28 Reciaion 7 Empirical Process heory Le x be a real-valued

More information

Part III: Chap. 2.5,2.6 & 12

Part III: Chap. 2.5,2.6 & 12 Survival Analysis Mah 434 Fall 2011 Par III: Chap. 2.5,2.6 & 12 Jimin Ding Mah Dep. www.mah.wusl.edu/ jmding/mah434/index.hml Jimin Ding, Ocober 4, 2011 Survival Analysis, Fall 2011 - p. 1/14 Jimin Ding,

More information

Two Coupled Oscillators / Normal Modes

Two Coupled Oscillators / Normal Modes Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own

More information

International Journal of Scientific & Engineering Research, Volume 4, Issue 10, October ISSN

International Journal of Scientific & Engineering Research, Volume 4, Issue 10, October ISSN Inernaional Journal of Scienific & Engineering Research, Volume 4, Issue 10, Ocober-2013 900 FUZZY MEAN RESIDUAL LIFE ORDERING OF FUZZY RANDOM VARIABLES J. EARNEST LAZARUS PIRIYAKUMAR 1, A. YAMUNA 2 1.

More information

Solutions to Odd Number Exercises in Chapter 6

Solutions to Odd Number Exercises in Chapter 6 1 Soluions o Odd Number Exercises in 6.1 R y eˆ 1.7151 y 6.3 From eˆ ( T K) ˆ R 1 1 SST SST SST (1 R ) 55.36(1.7911) we have, ˆ 6.414 T K ( ) 6.5 y ye ye y e 1 1 Consider he erms e and xe b b x e y e b

More information

STRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN

STRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN Inernaional Journal of Applied Economerics and Quaniaive Sudies. Vol.1-3(004) STRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN 001-004 OBARA, Takashi * Absrac The

More information

Maintenance Models. Prof. Robert C. Leachman IEOR 130, Methods of Manufacturing Improvement Spring, 2011

Maintenance Models. Prof. Robert C. Leachman IEOR 130, Methods of Manufacturing Improvement Spring, 2011 Mainenance Models Prof Rober C Leachman IEOR 3, Mehods of Manufacuring Improvemen Spring, Inroducion The mainenance of complex equipmen ofen accouns for a large porion of he coss associaed wih ha equipmen

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

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

Exponentially Weighted Moving Average (EWMA) Chart Based on Six Delta Initiatives

Exponentially Weighted Moving Average (EWMA) Chart Based on Six Delta Initiatives hps://doi.org/0.545/mjis.08.600 Exponenially Weighed Moving Average (EWMA) Char Based on Six Dela Iniiaives KALPESH S. TAILOR Deparmen of Saisics, M. K. Bhavnagar Universiy, Bhavnagar-36400 E-mail: kalpesh_lr@yahoo.co.in

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

Cash Flow Valuation Mode Lin Discrete Time

Cash Flow Valuation Mode Lin Discrete Time IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728,p-ISSN: 2319-765X, 6, Issue 6 (May. - Jun. 2013), PP 35-41 Cash Flow Valuaion Mode Lin Discree Time Olayiwola. M. A. and Oni, N. O. Deparmen of Mahemaics

More information

Chapter 2. First Order Scalar Equations

Chapter 2. First Order Scalar Equations Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.

More information

Circuit Variables. AP 1.1 Use a product of ratios to convert two-thirds the speed of light from meters per second to miles per second: 1 ft 12 in

Circuit Variables. AP 1.1 Use a product of ratios to convert two-thirds the speed of light from meters per second to miles per second: 1 ft 12 in Circui Variables 1 Assessmen Problems AP 1.1 Use a produc of raios o conver wo-hirds he speed of ligh from meers per second o miles per second: ( ) 2 3 1 8 m 3 1 s 1 cm 1 m 1 in 2.54 cm 1 f 12 in 1 mile

More information

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits EEE25 ircui Analysis I Se 4: apaciors, Inducors, and Firs-Order inear ircuis Shahriar Mirabbasi Deparmen of Elecrical and ompuer Engineering Universiy of Briish olumbia shahriar@ece.ubc.ca Overview Passive

More information

Final Spring 2007

Final Spring 2007 .615 Final Spring 7 Overview The purpose of he final exam is o calculae he MHD β limi in a high-bea oroidal okamak agains he dangerous n = 1 exernal ballooning-kink mode. Effecively, his corresponds o

More information

20. Applications of the Genetic-Drift Model

20. Applications of the Genetic-Drift Model 0. Applicaions of he Geneic-Drif Model 1) Deermining he probabiliy of forming any paricular combinaion of genoypes in he nex generaion: Example: If he parenal allele frequencies are p 0 = 0.35 and q 0

More information

WATER ABSTRACTUION AND RESERVOIR VOLUME DESIGN

WATER ABSTRACTUION AND RESERVOIR VOLUME DESIGN WATER ABSTRACTUION AND RESERVOIR VOLUME DESIGN SURFACE WATER Wihou river regulaion Wih river regulaion Coninuous Lakes (regulaed) Selecive Reservoirs CONTINUOUS DERIVATION FROM A RIVER HYDROGRAPH Q FLOW

More information

Basic notions of probability theory (Part 2)

Basic notions of probability theory (Part 2) Basic noions of probabiliy heory (Par 2) Conens o Basic Definiions o Boolean Logic o Definiions of probabiliy o Probabiliy laws o Random variables o Probabiliy Disribuions Random variables Random variables

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

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

A Generalized Poisson-Akash Distribution: Properties and Applications

A Generalized Poisson-Akash Distribution: Properties and Applications Inernaional Journal of Saisics and Applicaions 08, 8(5): 49-58 DOI: 059/jsaisics0808050 A Generalized Poisson-Akash Disribuion: Properies and Applicaions Rama Shanker,*, Kamlesh Kumar Shukla, Tekie Asehun

More information

Theory of! Partial Differential Equations!

Theory of! Partial Differential Equations! hp://www.nd.edu/~gryggva/cfd-course/! Ouline! Theory o! Parial Dierenial Equaions! Gréar Tryggvason! Spring 011! Basic Properies o PDE!! Quasi-linear Firs Order Equaions! - Characerisics! - Linear and

More information

Bias in Conditional and Unconditional Fixed Effects Logit Estimation: a Correction * Tom Coupé

Bias in Conditional and Unconditional Fixed Effects Logit Estimation: a Correction * Tom Coupé Bias in Condiional and Uncondiional Fixed Effecs Logi Esimaion: a Correcion * Tom Coupé Economics Educaion and Research Consorium, Naional Universiy of Kyiv Mohyla Academy Address: Vul Voloska 10, 04070

More information

ACE 562 Fall Lecture 8: The Simple Linear Regression Model: R 2, Reporting the Results and Prediction. by Professor Scott H.

ACE 562 Fall Lecture 8: The Simple Linear Regression Model: R 2, Reporting the Results and Prediction. by Professor Scott H. ACE 56 Fall 5 Lecure 8: The Simple Linear Regression Model: R, Reporing he Resuls and Predicion by Professor Sco H. Irwin Required Readings: Griffihs, Hill and Judge. "Explaining Variaion in he Dependen

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

Mathematical Theory and Modeling ISSN (Paper) ISSN (Online) Vol 3, No.3, 2013

Mathematical Theory and Modeling ISSN (Paper) ISSN (Online) Vol 3, No.3, 2013 Mahemaical Theory and Modeling ISSN -580 (Paper) ISSN 5-05 (Online) Vol, No., 0 www.iise.org The ffec of Inverse Transformaion on he Uni Mean and Consan Variance Assumpions of a Muliplicaive rror Model

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

Kriging Models Predicting Atrazine Concentrations in Surface Water Draining Agricultural Watersheds

Kriging Models Predicting Atrazine Concentrations in Surface Water Draining Agricultural Watersheds 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 Kriging Models Predicing Arazine Concenraions in Surface Waer Draining Agriculural Waersheds Paul L. Mosquin, Jeremy Aldworh, Wenlin Chen Supplemenal Maerial Number

More information

Chapter 5. Heterocedastic Models. Introduction to time series (2008) 1

Chapter 5. Heterocedastic Models. Introduction to time series (2008) 1 Chaper 5 Heerocedasic Models Inroducion o ime series (2008) 1 Chaper 5. Conens. 5.1. The ARCH model. 5.2. The GARCH model. 5.3. The exponenial GARCH model. 5.4. The CHARMA model. 5.5. Random coefficien

More information

04. Kinetics of a second order reaction

04. Kinetics of a second order reaction 4. Kineics of a second order reacion Imporan conceps Reacion rae, reacion exen, reacion rae equaion, order of a reacion, firs-order reacions, second-order reacions, differenial and inegraed rae laws, Arrhenius

More information

The Optimal Stopping Time for Selling an Asset When It Is Uncertain Whether the Price Process Is Increasing or Decreasing When the Horizon Is Infinite

The Optimal Stopping Time for Selling an Asset When It Is Uncertain Whether the Price Process Is Increasing or Decreasing When the Horizon Is Infinite American Journal of Operaions Research, 08, 8, 8-9 hp://wwwscirporg/journal/ajor ISSN Online: 60-8849 ISSN Prin: 60-8830 The Opimal Sopping Time for Selling an Asse When I Is Uncerain Wheher he Price Process

More information

Comparing Means: t-tests for One Sample & Two Related Samples

Comparing Means: t-tests for One Sample & Two Related Samples Comparing Means: -Tess for One Sample & Two Relaed Samples Using he z-tes: Assumpions -Tess for One Sample & Two Relaed Samples The z-es (of a sample mean agains a populaion mean) is based on he assumpion

More information

CHERNOFF DISTANCE AND AFFINITY FOR TRUNCATED DISTRIBUTIONS *

CHERNOFF DISTANCE AND AFFINITY FOR TRUNCATED DISTRIBUTIONS * haper 5 HERNOFF DISTANE AND AFFINITY FOR TRUNATED DISTRIBUTIONS * 5. Inroducion In he case of disribuions ha saisfy he regulariy condiions, he ramer- Rao inequaliy holds and he maximum likelihood esimaor

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

Semi-Competing Risks on A Trivariate Weibull Survival Model

Semi-Competing Risks on A Trivariate Weibull Survival Model Semi-Compeing Risks on A Trivariae Weibull Survival Model Jenq-Daw Lee Graduae Insiue of Poliical Economy Naional Cheng Kung Universiy Tainan Taiwan 70101 ROC Cheng K. Lee Loss Forecasing Home Loans &

More information

14 Autoregressive Moving Average Models

14 Autoregressive Moving Average Models 14 Auoregressive Moving Average Models In his chaper an imporan parameric family of saionary ime series is inroduced, he family of he auoregressive moving average, or ARMA, processes. For a large class

More information

Nature Neuroscience: doi: /nn Supplementary Figure 1. Spike-count autocorrelations in time.

Nature Neuroscience: doi: /nn Supplementary Figure 1. Spike-count autocorrelations in time. Supplemenary Figure 1 Spike-coun auocorrelaions in ime. Normalized auocorrelaion marices are shown for each area in a daase. The marix shows he mean correlaion of he spike coun in each ime bin wih he spike

More information

GMM - Generalized Method of Moments

GMM - Generalized Method of Moments GMM - Generalized Mehod of Momens Conens GMM esimaion, shor inroducion 2 GMM inuiion: Maching momens 2 3 General overview of GMM esimaion. 3 3. Weighing marix...........................................

More information

R t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t

R t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t Exercise 7 C P = α + β R P + u C = αp + βr + v (a) (b) C R = α P R + β + w (c) Assumpions abou he disurbances u, v, w : Classical assumions on he disurbance of one of he equaions, eg. on (b): E(v v s P,

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

Random variables. A random variable X is a function that assigns a real number, X(ζ), to each outcome ζ in the sample space of a random experiment.

Random variables. A random variable X is a function that assigns a real number, X(ζ), to each outcome ζ in the sample space of a random experiment. Random variables Some random eperimens may yield a sample space whose elemens evens are numbers, bu some do no or mahemaical purposes, i is desirable o have numbers associaed wih he oucomes A random variable

More information

CHAPTER 2: Mathematics for Microeconomics

CHAPTER 2: Mathematics for Microeconomics CHAPTER : Mahemaics for Microeconomics The problems in his chaper are primarily mahemaical. They are inended o give sudens some pracice wih he conceps inroduced in Chaper, bu he problems in hemselves offer

More information

A Group Acceptance Sampling Plans Based on Truncated Life Tests for Type-II Generalized Log-Logistic Distribution

A Group Acceptance Sampling Plans Based on Truncated Life Tests for Type-II Generalized Log-Logistic Distribution ProbSa Forum, Volume 09, July 2016, Pages 88 94 ISSN 0974-3235 ProbSa Forum is an e-journal. For deails please visi www.probsa.org.in A Group Accepance Sampling Plans Based on Truncaed Life Tess for Type-II

More information

Západočeská Univerzita v Plzni, Czech Republic and Groupe ESIEE Paris, France

Západočeská Univerzita v Plzni, Czech Republic and Groupe ESIEE Paris, France ADAPTIVE SIGNAL PROCESSING USING MAXIMUM ENTROPY ON THE MEAN METHOD AND MONTE CARLO ANALYSIS Pavla Holejšovsá, Ing. *), Z. Peroua, Ing. **), J.-F. Bercher, Prof. Assis. ***) Západočesá Univerzia v Plzni,

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

Linear Circuit Elements

Linear Circuit Elements 1/25/2011 inear ircui Elemens.doc 1/6 inear ircui Elemens Mos microwave devices can be described or modeled in erms of he hree sandard circui elemens: 1. ESISTANE () 2. INDUTANE () 3. APAITANE () For he

More information

Testing the Random Walk Model. i.i.d. ( ) r

Testing the Random Walk Model. i.i.d. ( ) r he random walk heory saes: esing he Random Walk Model µ ε () np = + np + Momen Condiions where where ε ~ i.i.d he idea here is o es direcly he resricions imposed by momen condiions. lnp lnp µ ( lnp lnp

More information

Theory of! Partial Differential Equations-I!

Theory of! Partial Differential Equations-I! hp://users.wpi.edu/~grear/me61.hml! Ouline! Theory o! Parial Dierenial Equaions-I! Gréar Tryggvason! Spring 010! Basic Properies o PDE!! Quasi-linear Firs Order Equaions! - Characerisics! - Linear and

More information

Chapter 14 Wiener Processes and Itô s Lemma. Options, Futures, and Other Derivatives, 9th Edition, Copyright John C. Hull

Chapter 14 Wiener Processes and Itô s Lemma. Options, Futures, and Other Derivatives, 9th Edition, Copyright John C. Hull Chaper 14 Wiener Processes and Iô s Lemma Copyrigh John C. Hull 014 1 Sochasic Processes! Describes he way in which a variable such as a sock price, exchange rae or ineres rae changes hrough ime! Incorporaes

More information

Evaluation of Mean Time to System Failure of a Repairable 3-out-of-4 System with Online Preventive Maintenance

Evaluation of Mean Time to System Failure of a Repairable 3-out-of-4 System with Online Preventive Maintenance American Journal of Applied Mahemaics and Saisics, 0, Vol., No., 9- Available online a hp://pubs.sciepub.com/ajams/// Science and Educaion Publishing DOI:0.69/ajams--- Evaluaion of Mean Time o Sysem Failure

More information

- If one knows that a magnetic field has a symmetry, one may calculate the magnitude of B by use of Ampere s law: The integral of scalar product

- If one knows that a magnetic field has a symmetry, one may calculate the magnitude of B by use of Ampere s law: The integral of scalar product 11.1 APPCATON OF AMPEE S AW N SYMMETC MAGNETC FEDS - f one knows ha a magneic field has a symmery, one may calculae he magniude of by use of Ampere s law: The inegral of scalar produc Closed _ pah * d

More information

ACE 562 Fall Lecture 5: The Simple Linear Regression Model: Sampling Properties of the Least Squares Estimators. by Professor Scott H.

ACE 562 Fall Lecture 5: The Simple Linear Regression Model: Sampling Properties of the Least Squares Estimators. by Professor Scott H. ACE 56 Fall 005 Lecure 5: he Simple Linear Regression Model: Sampling Properies of he Leas Squares Esimaors by Professor Sco H. Irwin Required Reading: Griffihs, Hill and Judge. "Inference in he Simple

More information

PENALIZED LEAST SQUARES AND PENALIZED LIKELIHOOD

PENALIZED LEAST SQUARES AND PENALIZED LIKELIHOOD PENALIZED LEAST SQUARES AND PENALIZED LIKELIHOOD HAN XIAO 1. Penalized Leas Squares Lasso solves he following opimizaion problem, ˆβ lasso = arg max β R p+1 1 N y i β 0 N x ij β j β j (1.1) for some 0.

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

4.5 Constant Acceleration

4.5 Constant Acceleration 4.5 Consan Acceleraion v() v() = v 0 + a a() a a() = a v 0 Area = a (a) (b) Figure 4.8 Consan acceleraion: (a) velociy, (b) acceleraion When he x -componen of he velociy is a linear funcion (Figure 4.8(a)),

More information

6.003 Homework 1. Problems. Due at the beginning of recitation on Wednesday, February 10, 2010.

6.003 Homework 1. Problems. Due at the beginning of recitation on Wednesday, February 10, 2010. 6.003 Homework Due a he beginning of reciaion on Wednesday, February 0, 200. Problems. Independen and Dependen Variables Assume ha he heigh of a waer wave is given by g(x v) where x is disance, v is velociy,

More information

Reliability Assessment and Residual Life Prediction Method based on Wiener Process and Current Degradation Quantity

Reliability Assessment and Residual Life Prediction Method based on Wiener Process and Current Degradation Quantity Engineering Leers, 4:, EL_4 08 Reliabiliy Assessmen Residual Life Predicion Mehod based on Wiener Process Curren Degradaion Quaniy Huibing Hao, Chunping Li Absrac In his aricle, he populaion reliabiliy

More information

Excel-Based Solution Method For The Optimal Policy Of The Hadley And Whittin s Exact Model With Arma Demand

Excel-Based Solution Method For The Optimal Policy Of The Hadley And Whittin s Exact Model With Arma Demand Excel-Based Soluion Mehod For The Opimal Policy Of The Hadley And Whiin s Exac Model Wih Arma Demand Kal Nami School of Business and Economics Winson Salem Sae Universiy Winson Salem, NC 27110 Phone: (336)750-2338

More information

CHAPTER 12 DIRECT CURRENT CIRCUITS

CHAPTER 12 DIRECT CURRENT CIRCUITS CHAPTER 12 DIRECT CURRENT CIUITS DIRECT CURRENT CIUITS 257 12.1 RESISTORS IN SERIES AND IN PARALLEL When wo resisors are conneced ogeher as shown in Figure 12.1 we said ha hey are conneced in series. As

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

Foundations of Statistical Inference. Sufficient statistics. Definition (Sufficiency) Definition (Sufficiency)

Foundations of Statistical Inference. Sufficient statistics. Definition (Sufficiency) Definition (Sufficiency) Foundaions of Saisical Inference Julien Beresycki Lecure 2 - Sufficiency, Facorizaion, Minimal sufficiency Deparmen of Saisics Universiy of Oxford MT 2016 Julien Beresycki (Universiy of Oxford BS2a MT

More information

Georey E. Hinton. University oftoronto. Technical Report CRG-TR February 22, Abstract

Georey E. Hinton. University oftoronto.   Technical Report CRG-TR February 22, Abstract Parameer Esimaion for Linear Dynamical Sysems Zoubin Ghahramani Georey E. Hinon Deparmen of Compuer Science Universiy oftorono 6 King's College Road Torono, Canada M5S A4 Email: zoubin@cs.orono.edu Technical

More information

Explaining Total Factor Productivity. Ulrich Kohli University of Geneva December 2015

Explaining Total Factor Productivity. Ulrich Kohli University of Geneva December 2015 Explaining Toal Facor Produciviy Ulrich Kohli Universiy of Geneva December 2015 Needed: A Theory of Toal Facor Produciviy Edward C. Presco (1998) 2 1. Inroducion Toal Facor Produciviy (TFP) has become

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

not to be republished NCERT MATHEMATICAL MODELLING Appendix 2 A.2.1 Introduction A.2.2 Why Mathematical Modelling?

not to be republished NCERT MATHEMATICAL MODELLING Appendix 2 A.2.1 Introduction A.2.2 Why Mathematical Modelling? 256 MATHEMATICS A.2.1 Inroducion In class XI, we have learn abou mahemaical modelling as an aemp o sudy some par (or form) of some real-life problems in mahemaical erms, i.e., he conversion of a physical

More information

CHAPTER 10 VALIDATION OF TEST WITH ARTIFICAL NEURAL NETWORK

CHAPTER 10 VALIDATION OF TEST WITH ARTIFICAL NEURAL NETWORK 175 CHAPTER 10 VALIDATION OF TEST WITH ARTIFICAL NEURAL NETWORK 10.1 INTRODUCTION Amongs he research work performed, he bes resuls of experimenal work are validaed wih Arificial Neural Nework. From he

More information

5.1 - Logarithms and Their Properties

5.1 - Logarithms and Their Properties Chaper 5 Logarihmic Funcions 5.1 - Logarihms and Their Properies Suppose ha a populaion grows according o he formula P 10, where P is he colony size a ime, in hours. When will he populaion be 2500? We

More information

STATE-SPACE MODELLING. A mass balance across the tank gives:

STATE-SPACE MODELLING. A mass balance across the tank gives: B. Lennox and N.F. Thornhill, 9, Sae Space Modelling, IChemE Process Managemen and Conrol Subjec Group Newsleer STE-SPACE MODELLING Inroducion: Over he pas decade or so here has been an ever increasing

More information