Proceedings of the 5th WSEAS Int. Conf. on SIMULATION, MODELING AND OPTIMIZATION, Corfu, Greece, August 17-19, 2005 (pp55-60)

Size: px
Start display at page:

Download "Proceedings of the 5th WSEAS Int. Conf. on SIMULATION, MODELING AND OPTIMIZATION, Corfu, Greece, August 17-19, 2005 (pp55-60)"

Transcription

1 Proceedngs of the 5th WSEAS Int. Conf. on SIMULATIO, MODELIG AD OPTIMIZATIO, Corfu, Greece, August 7-9, 005 (pp55-60) A eural etwork Realzaton of Schedulng n Grd Computng Envronment MOHAMMAD KALATARI, KAZEM AKBARI Computer Engneerng Department Amrkabr Unversty of Technology (Tehran Polytechnc) TEHRA-IRA Abstract: - The Computatonal Grds provde a promsng platform for effcent executon of computatonal and data ntensve applcatons. Schedulng n such envronments s challengng because target resources are heterogeneous and ther load and avalablty vares dynamcally. In ths paper, we propose a mathematcal neural network based schedulng soluton for grd computng envronment. Usng mathematcal method guarantees rapd convergenc that s essental for such envronments wth prolferaton of resources. Key-Words: - Schedulng, Grd Computng, eural etworks. Introducton Grd schedulng s ntrnscally more complcated than local schedulng of resources, because t must manpulate large-scale resources across management boundares. In such a dynamc dstrbuted computng envronment, resource avalablty vares dramatcally, so schedulng becomes qute challengng. There have been extensve research actvtes on schedulng problems n dstrbuted systems that must be extended for the purpose of grd computng envronment [,,3]. Most problems n schedulng area are P- Complete. Ths fact mples that an optmal soluton for a large schedulng problem s qute tmeconsumng. Therefore, some researchers translated the job-schedulng problem nto a format of lnear programmng or K-out-of- rule and mapped t nto an approprate neural network structure to obtan a reasonable soluton [4,5,6]. eural networks for combnatoral optmzaton problems were frst ntroduced by Hopfeld and Tank n 985 [7]. They used the predefned energy functon E whch follows the quadratc form: E = = j = W VV j j + = V I () where W s the strength of a synaptc lnk between j the th and the jth neuron where the condton of W j = W j must be always satsfed. ote that I s constant bas of the th neuron. Hopfeld gves the moton equaton of the th neuron: du U E = () dt τ V where the output follows the contnuous, nondecreasng, and dfferentable functon called sgmod functon: V = f ( U ) = ( tanh( λ 0 U ) + ) (3) where λ 0 s constant and s called gan whch determnes the slope of the sgmod functon. Snce Wlson and Pawley strongly crtczed the neural network methods (specfcally Hopfeld model) for optmzaton problems [8], and n addton, after the publcaton of dscouragng report of Paell [9] regardng the drawbacks of Hopfeld nets (e.g., convergence to local mnma, lmted capacty of network, and dsablty for solvng hardlearnng problems), t has been wdely beleved that the neural network methods are not sutable for optmzaton problems. But Takefuj and others n ther contnuous and unfalng efforts have demonstrated the capablty of the artfcal neural networks (.e., Hopfeld-lke method) for solvng optmzaton problems, over the best known algorthms and methods. They found that the use of decay term ( U / τ ) n Eq.() ncreases the computatonal energy functon E under some condtons nstead of decreasng t [0]. In hs method, Takefuj explots the topology of Hopfeld net n conjuncton wth both mathematcal method of McCulloch-Ptts (wth or wthout

2 Proceedngs of the 5th WSEAS Int. Conf. on SIMULATIO, MODELIG AD OPTIMIZATIO, Corfu, Greece, August 7-9, 005 (pp55-60) hysteress) and Maxmum (wnner-take-all) functon to tackle and solve the problems [0]. Hs works cover a wde varety of professonal felds ncludng game theory, computer scence, graph theory, molecular bology, VLSI computer aded desgn, communcaton, and computer networks. In [] Yueh-Mn Huang et al. represented a Hopfeld neural network based soluton to schedulng multprocessor job wth resource and tmng constrans. In ther model, they assume that all resources are homogeneous and avalable for schedulng at tme 0, and durng schedulng, no resources are added to or deleted from system, whch s ratonal for such a system. However n Grd computng envronments, resources are heterogeneous and can be added or deleted dynamcally. Ths work ams to overcome these new constrants by usng mathematcal neural model rather than Hopfeld neural method. The rest of ths paper s organzed as follows. Secton contans an overvew of the mathematcal neural network model. In secton 3 our grd computng envronment s descrbed. In secton 4 the schedulng problem s descrbed n detal and mapped onto a neural network, followed by smulaton results n secton 5. Fnally, we wll summarze the outcomes and future work n secton 6. Mathematcal eural etwork Model The mathematcal model of the artfcal neural network conssts of two components; neurons and synaptc lnks. The output sgnal transmtted from a neuron propagates to other neurons through the synaptc lnks. The state of the nput sgnal of a neuron s determned by the lnear sum of weghted nput sgnals from the other neurons where the respectve weght s strength of the synaptc lnks. Every artfcal neuron has the nput U and the output V. The output of the th neuron s gven by V = f ( U ) where f s called the neuron s nput/output functon. The nterconnectons between the th neuron and other neurons are determned by the moton equaton. The change of the nput state of the th neuron s gven by the partal dervatons of the computatonal energy functon E wth respect to the output of the th neuron where E follows an n- varable functon: E ( V V,..., ) equaton of the th neuron s gven by:, V n. The moton du E( V, V,..., Vn ) de = = (4) dt V dv In general, the goal of neural computaton s to optmze the fabrcated computatonal energy functon. The energy functon not only determnes how many neurons should be used n the system but also t specfes the strength of synaptc lnks between neurons. Indeed, energy functon s constructed from nformaton n the gven problem, consderng the requred constrants and/or cost functon. Practcally, t s usually easer to calculate the moton equaton (partal dfferental of the energy functon) than the energy functon tself. The superorty of the moton equaton over energy functon can be artculated as follows: ts smplcty (step by step computatons and ease of formulaton), bnary behavor, ease of applcaton, and the flexblty n whch all constrants can be ncorporated. It also resolves the defcences of the Hopfeld net whch was dscussed earler. The energy functon, however, can be defned: du E = de = dv (5) dt In order to numercally solve the partal dfferental equaton or the dfferental equaton to determne the value of moton equaton, the frst order Euler method s wdely used where t s the smplest among the exstng numercal methods. Therefore, based upon the frst order Euler method the value of U ( t +) s determned as below: U ( t + ) = U ( t) + U ( t). t (6) where U (t) s gven by Eq. (4) and termnaton condton s gven by: U ( t) = 0 (7) The condton of the Eq. (7) mples that the constrants are all satsfed. 3 System Model The Grd computng envronment n ths work (shown n Fg.) conssts of n stes, S, S,... S ; n where a ste S ( n) conssts of a number of heterogeneous computatonal resources. Wthn each local ste, there s a forecastng system such as PACE (Performance Analyss and Characterzaton Envronment) toolkt [,] to predct the Job s executon tme on the canddate resources pror to run tme. Selecton of canddate resources s

3 Proceedngs of the 5th WSEAS Int. Conf. on SIMULATIO, MODELIG AD OPTIMIZATIO, Corfu, Greece, August 7-9, 005 (pp55-60) accomplshed va a selector component n each ste. Canddate resources are those whch are avalable at the tme or wthn a predetermned tme. To avod the race condton we can reserve the canddate resources. The schedulng mechansm n our work s done n batch-mode, n whch arrvng jobs are collected at prescheduled tmes and are scheduled as a meta-task when a schedulng event s trggered. The followng two steps are accomplshed for schedulng; frst scheduler sends the characterstcs of jobs to each ste; and then n each ste, selector and predctor components return whatever requred for schedulng to the scheduler (.e. a lst of canddate resources and the executon tme of each job on each resource). Scheduler uses a neural network based schedulng mechansm (see secton 4) along wth the nformaton for the schedulng purposes. For the sake of smplcty, we gnore the communcaton overhead n ths work. Therefore, schedulng parameters comprse the lsted jobs, the requred machnes, and tme varables as depcted n Fg., where the x axs denotes the job varable wthn a range from to (the total number of jobs to be scheduled) and the y axs represents the machne varable wthn a range from to M (the total number of machnes) and the z axs s for the tme varable and k represents a specfc tme whch should be less than or equal to T, the amount of total schedulng tme. Thus, a state varable V s defned to ndcate whether or not the jk job s executed on machne j at a certan tme k. In case of V jk =, t denotes that the job s run on machne j at the tme k; otherwse, V jk = 0. It should be noted that, each V corresponds to a neuron of the jk neural network. Scheduler Selector & Predctor Component..... Ste Ste Fg. System Model Ste n 4 Problem Formulaton Wth eural etwork Method Our schedulng approach consders jobs to be run on some machnes (resources) and the followng assumptons are made regardng the problem doman. Frst, the executon tme of each job on each machne s predetermned (see secton 3). Second, a job can not be assgned to dfferent machnes, mplyng that no job mgraton s allowed between machnes. Thrd, resources are added to or deleted from envronment dynamcally and the tme of addton or deleton s estmated by predctor component. The constrants mposed to our model are a deadlne( d ) for each job and a processng tme along wth avalable resources on systems. Fg. Three-dmensonal modelng of problem Mappng constrants nto the moton equaton s as follows: du dt jk * = = A V V - st nhbtory factor jk M T * jk j= k= j j jk B V jk V - nd nhbtory factor T C * L * V jk P j -3 rd nhbtory or st k= exctatory factor. D * K * V jk -4 th nhbtory factor = E * H k d -5 th nhbtory factor ( ( ))

4 Proceedngs of the 5th WSEAS Int. Conf. on SIMULATIO, MODELIG AD OPTIMIZATIO, Corfu, Greece, August 7-9, 005 (pp55-60) ( ) F * H P j d -6 th nhbtory factor (8) Moreover, the effects of overall nhbtory and exctatory factors n the moton equaton can be summarzed as : The frst nhbtory factor states that a machne j can only execute one job at a certan tme k. The second nhbtory factor states that no mgraton s allowed, on the other word, job can only be executed on machne j or machne j at any tme. The thrd nhbtory factor or the frst exctatory factor states that the tme spent by job should be equal to P, where j P s the j estmated executon tme of job on machne j. The fourth nhbtory factor states that only one job can be executed on a specfed machne and at a certan tme. The ffth and sxth nhbtory factors state that no volaton of deadlne s allowed. The functons L, K and H s defned as follow: α > 0 L ( α) = 0 α = 0, α α 0 K ( α ) =, 0 α < 0 - α < 0 α > 0 H ( α ) = 0 α 0 we have used hysteress McCulloch-Ptts neuron model where the nput/output functon of the th hysteress neuron s gven by: f U > UTP V = f ( U ) = 0 f U < LTP (9) unchenged otherwse where UTP and LTP are upper trp pont and lower trp pont respectvely, as well as a modfed form of Maxmum euron Model. Maxmum neuron model s composed of M cluster where each cluster conssts of n neurons. In ths model wnner-take-all functon s embedded. Ths mples that one and only one neuron out of n neurons n every cluster wth a maxmum value s encouraged to be fred. The correspondng nput/output functon of the th neuron n the mth cluster s gven by: V m f Um = max m = Um Umj 0 otherwse { U,..., U } mn and for > j (0) In the maxmum neuron model t s always guaranteed to generate satsfactory solutons [0]. The advantages of the maxmum neural model can be summarzed [0]: Every local mnmum s one of the acceptable solutons, whle other exstng neural models cannot guarantee that. Tunng of coeffcent parameters for the actvaton functon s not requred. The termnaton condton of the equlbrum state s clearly defned by a smple mathematcal formula. It should be noted that there are some mportant ponts n our method, whch can be summarzed n the followng: Although t s possble to fnd the exact form of energy functon E, but we do not need t n the process because of the moton equaton du / dt = de / dv. When we use du / dt to fnd a new state of the system, the energy functon wll be employed mplctly. The termnaton condton and the maxmum neuron model together cause the convergence of system n the global mnmum. By usng the moton equaton method, n fact we are employng a sparsely connected network whenever we need that, as opposed to the Hopfeld s fully connected networks. Therefore, for the bg problems there s no need to employ a huge number of synaptc connectons whch would cause a spurous convergence. The correspondng algorthm s gven n Fg.3. 5 Smulaton Results The neural network based schedulng algorthm descrbed n the prevous sectons has been mplemented n C and executed on computer wth Pentum IV processor and 5 mega byte RAM. For the evaluaton of the system s performance, dfferent examples of all szes: small, medum and large were run for 0 tmes. Some of the experments and the overall results are lsted below.

5 Proceedngs of the 5th WSEAS Int. Conf. on SIMULATIO, MODELIG AD OPTIMIZATIO, Corfu, Greece, August 7-9, 005 (pp55-60) The nput data for the frst, the second, and the thrd experments and ther correspondng results have been shown n Fg.4, 5 and 6 respectvely. In the frst example, some machnes are not avalable at tme 0. We compute the maxmum executon tme of each job on each machne and use these values as nputs to the algorthm. Job 0 Job Job Job 3 deadlne Job 4 Job 5 Job 6 deadlne Job Job3 Job4 Algorthm: begn ntalze U jk s randomly. whle (a set of conflcts s not empty) do begn for := to do for j:= to M do for k:= to T do begn Ujk = Ujk + Ujk V jk = f ( Ujk ) end for := to do begn. fnd the maxmum U jk. determne a segment (j) n whch the maxmum U jk exsts. If there s te remove t randomly. 3. The output of the other segment s neurons s set to zero. end end end. Job0 Job Tme Fg.4 The frst experment However f the deadlnes of all jobs are set to 5 (The mnmum makespan), our algorthm can t be converged. In Fg.6 no constrants on avalablty mposed but the problem sze has been ncreased and the deadlnes of all jobs have been set to 8. m 0 m m Job Job Job Job Job Job6 Job5 m 0 m m tme of avalablty Job 0 Job Job Job 3 Job 4 deadlne Fg.3 The Schedulng Algorthm 3 Job Job3 Job4 m 0 m m Job Job 5 Job 0 0 Job 3 4 Job 4 7 Job Job maxmum fnshng tme of m each job 0 m m on each machne Job Job 8 4 Job Job Job Job Job Job0 Job Tme Fg.5 The second experment m 0 m m tme of avalablty 3 0

6 Proceedngs of the 5th WSEAS Int. Conf. on SIMULATIO, MODELIG AD OPTIMIZATIO, Corfu, Greece, August 7-9, 005 (pp55-60) m 0 m m m 3 m 4 m 5 Job Job Job Job Job Job Job Job Job Job Job Job0 Job3 Job4 Job5 Job9 Job8 Job6 Job Job Tme Job0 Fg.6 The thrd experment Table shows the average number of teratons and executon tme of algorthm for dfferent examples of dfferent szes. The number of teraton and the executon tme of program decrease or ncrease smoothly when the problem sze ncreases, as shown n Table. Job7 o. # of Job # of machnes Avg # of Iteraton Avg Conv. Tme(sec.) < < < Table : The overall results 6 Concluson and Future Work We have presented a neuro-based schedulng soluton for grd computng envronment. As mentoned before, f all machnes are avalable at tme 0, our algorthm always gves the schedulng soluton wth respect to the gven deadlnes. Anyway, rapd convergence s an mportant characterstc of the proposed soluton. In the future, a neuro-based schedulng algorthm whch ncludes communcaton overhead wll be presented. References: [] Y. M. Huang and R. M. Chen, Schedulng multprocessor job wth resources and tmng constrants usng neural networks. IEEE Transacton on system, man, and cybernetcs, Vol. 9, o. 4, August 999. [] T. D. Braun, Howard Jay Segel, oah Beck, A comparson of eleven statc heurstcs for mappng a class of ndependent tasks onto heterogeneous dstrbuted computng systems, Journal of Parallel and Dstrbuted Computng, 00. [3]. Fujmoto and K. Haghara, A comparson among grd schedulng algorthms for ndependent coarse-graned tasks. IEEE Int. Symp. on Applcatons and the Internet Workshops (SAITW 04), 004. [4] Y. P. S. Foo and Y. Takefuj, Integer lnear programmng neural networks for job-shop schedulng, IEEE Int. Conf. eural etworks, 99, pp [5] C. Y. Chang and M. D. Jeng, Expermental study of a neural model for schedulng job shop, IEEE Int. Conf. System, Man, Cybernetcs, 995, Vol., pp [6] J. M. Gallone, F. Charpllet, and F. Alexandre, Anytme schedulng wth neural networks, Proc. RIA/IEEE Symp [7] J. J. Hopfeld and D. W. Tank, eural computaton of decson n optmzaton, Journal of Bologcal Cybernetcs, Vol. 5, 985, pp [8] G. V. Wlson and G. S. Pawley, On stablty of the travelng salesman problem algorthm of Hopfeld and Tank, Bologcal Cybernetcs, Vol 58, 988, pp [9] R. A. Paell, Smulaton tests of the optmzaton method of Hopfeld and Tank usng neural networks, ASA Techncal Memorandom 0047, 988. [0] Yoshyasu Takefuj, eural etwork Parallel Computng, Kluwer Academc Publshers, 99. [] G. R. udd, D. J. Kerbyson, E. Papaefastathou, J. S. C. Perry and D. V. Wlcox, PACE: A toolset for the performance predcton of parallel and dstrbuted systems, In Internatonal journal of Hgh Performance Computng, 999. [] L. He, S. A. Jarvs, D. P. Spooner, X. Chen and G. R. udd, Dynamc schedulng of parallel jobs wth Qos demands n multclusters and Grds, In Proc. of 5 th IEEE/ACM Int. Workshop on Grd Computng, 004.

CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE

CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE Analytcal soluton s usually not possble when exctaton vares arbtrarly wth tme or f the system s nonlnear. Such problems can be solved by numercal tmesteppng

More information

Resource Allocation with a Budget Constraint for Computing Independent Tasks in the Cloud

Resource Allocation with a Budget Constraint for Computing Independent Tasks in the Cloud Resource Allocaton wth a Budget Constrant for Computng Independent Tasks n the Cloud Wemng Sh and Bo Hong School of Electrcal and Computer Engneerng Georga Insttute of Technology, USA 2nd IEEE Internatonal

More information

Module 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur

Module 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur Module 3 LOSSY IMAGE COMPRESSION SYSTEMS Verson ECE IIT, Kharagpur Lesson 6 Theory of Quantzaton Verson ECE IIT, Kharagpur Instructonal Objectves At the end of ths lesson, the students should be able to:

More information

Note 10. Modeling and Simulation of Dynamic Systems

Note 10. Modeling and Simulation of Dynamic Systems Lecture Notes of ME 475: Introducton to Mechatroncs Note 0 Modelng and Smulaton of Dynamc Systems Department of Mechancal Engneerng, Unversty Of Saskatchewan, 57 Campus Drve, Saskatoon, SK S7N 5A9, Canada

More information

Some modelling aspects for the Matlab implementation of MMA

Some modelling aspects for the Matlab implementation of MMA Some modellng aspects for the Matlab mplementaton of MMA Krster Svanberg krlle@math.kth.se Optmzaton and Systems Theory Department of Mathematcs KTH, SE 10044 Stockholm September 2004 1. Consdered optmzaton

More information

Single-Facility Scheduling over Long Time Horizons by Logic-based Benders Decomposition

Single-Facility Scheduling over Long Time Horizons by Logic-based Benders Decomposition Sngle-Faclty Schedulng over Long Tme Horzons by Logc-based Benders Decomposton Elvn Coban and J. N. Hooker Tepper School of Busness, Carnege Mellon Unversty ecoban@andrew.cmu.edu, john@hooker.tepper.cmu.edu

More information

The Minimum Universal Cost Flow in an Infeasible Flow Network

The Minimum Universal Cost Flow in an Infeasible Flow Network Journal of Scences, Islamc Republc of Iran 17(2): 175-180 (2006) Unversty of Tehran, ISSN 1016-1104 http://jscencesutacr The Mnmum Unversal Cost Flow n an Infeasble Flow Network H Saleh Fathabad * M Bagheran

More information

Winter 2008 CS567 Stochastic Linear/Integer Programming Guest Lecturer: Xu, Huan

Winter 2008 CS567 Stochastic Linear/Integer Programming Guest Lecturer: Xu, Huan Wnter 2008 CS567 Stochastc Lnear/Integer Programmng Guest Lecturer: Xu, Huan Class 2: More Modelng Examples 1 Capacty Expanson Capacty expanson models optmal choces of the tmng and levels of nvestments

More information

Solving Nonlinear Differential Equations by a Neural Network Method

Solving Nonlinear Differential Equations by a Neural Network Method Solvng Nonlnear Dfferental Equatons by a Neural Network Method Luce P. Aarts and Peter Van der Veer Delft Unversty of Technology, Faculty of Cvlengneerng and Geoscences, Secton of Cvlengneerng Informatcs,

More information

Chapter Newton s Method

Chapter Newton s Method Chapter 9. Newton s Method After readng ths chapter, you should be able to:. Understand how Newton s method s dfferent from the Golden Secton Search method. Understand how Newton s method works 3. Solve

More information

The Study of Teaching-learning-based Optimization Algorithm

The Study of Teaching-learning-based Optimization Algorithm Advanced Scence and Technology Letters Vol. (AST 06), pp.05- http://dx.do.org/0.57/astl.06. The Study of Teachng-learnng-based Optmzaton Algorthm u Sun, Yan fu, Lele Kong, Haolang Q,, Helongang Insttute

More information

Numerical Heat and Mass Transfer

Numerical Heat and Mass Transfer Master degree n Mechancal Engneerng Numercal Heat and Mass Transfer 06-Fnte-Dfference Method (One-dmensonal, steady state heat conducton) Fausto Arpno f.arpno@uncas.t Introducton Why we use models and

More information

Wavelet chaotic neural networks and their application to continuous function optimization

Wavelet chaotic neural networks and their application to continuous function optimization Vol., No.3, 04-09 (009) do:0.436/ns.009.307 Natural Scence Wavelet chaotc neural networks and ther applcaton to contnuous functon optmzaton Ja-Ha Zhang, Yao-Qun Xu College of Electrcal and Automatc Engneerng,

More information

Design and Optimization of Fuzzy Controller for Inverse Pendulum System Using Genetic Algorithm

Design and Optimization of Fuzzy Controller for Inverse Pendulum System Using Genetic Algorithm Desgn and Optmzaton of Fuzzy Controller for Inverse Pendulum System Usng Genetc Algorthm H. Mehraban A. Ashoor Unversty of Tehran Unversty of Tehran h.mehraban@ece.ut.ac.r a.ashoor@ece.ut.ac.r Abstract:

More information

Simultaneous Optimization of Berth Allocation, Quay Crane Assignment and Quay Crane Scheduling Problems in Container Terminals

Simultaneous Optimization of Berth Allocation, Quay Crane Assignment and Quay Crane Scheduling Problems in Container Terminals Smultaneous Optmzaton of Berth Allocaton, Quay Crane Assgnment and Quay Crane Schedulng Problems n Contaner Termnals Necat Aras, Yavuz Türkoğulları, Z. Caner Taşkın, Kuban Altınel Abstract In ths work,

More information

Lecture Notes on Linear Regression

Lecture Notes on Linear Regression Lecture Notes on Lnear Regresson Feng L fl@sdueducn Shandong Unversty, Chna Lnear Regresson Problem In regresson problem, we am at predct a contnuous target value gven an nput feature vector We assume

More information

An Interactive Optimisation Tool for Allocation Problems

An Interactive Optimisation Tool for Allocation Problems An Interactve Optmsaton ool for Allocaton Problems Fredr Bonäs, Joam Westerlund and apo Westerlund Process Desgn Laboratory, Faculty of echnology, Åbo Aadem Unversty, uru 20500, Fnland hs paper presents

More information

Chapter - 2. Distribution System Power Flow Analysis

Chapter - 2. Distribution System Power Flow Analysis Chapter - 2 Dstrbuton System Power Flow Analyss CHAPTER - 2 Radal Dstrbuton System Load Flow 2.1 Introducton Load flow s an mportant tool [66] for analyzng electrcal power system network performance. Load

More information

MMA and GCMMA two methods for nonlinear optimization

MMA and GCMMA two methods for nonlinear optimization MMA and GCMMA two methods for nonlnear optmzaton Krster Svanberg Optmzaton and Systems Theory, KTH, Stockholm, Sweden. krlle@math.kth.se Ths note descrbes the algorthms used n the author s 2007 mplementatons

More information

EEL 6266 Power System Operation and Control. Chapter 3 Economic Dispatch Using Dynamic Programming

EEL 6266 Power System Operation and Control. Chapter 3 Economic Dispatch Using Dynamic Programming EEL 6266 Power System Operaton and Control Chapter 3 Economc Dspatch Usng Dynamc Programmng Pecewse Lnear Cost Functons Common practce many utltes prefer to represent ther generator cost functons as sngle-

More information

ECE559VV Project Report

ECE559VV Project Report ECE559VV Project Report (Supplementary Notes Loc Xuan Bu I. MAX SUM-RATE SCHEDULING: THE UPLINK CASE We have seen (n the presentaton that, for downlnk (broadcast channels, the strategy maxmzng the sum-rate

More information

Kernel Methods and SVMs Extension

Kernel Methods and SVMs Extension Kernel Methods and SVMs Extenson The purpose of ths document s to revew materal covered n Machne Learnng 1 Supervsed Learnng regardng support vector machnes (SVMs). Ths document also provdes a general

More information

Supporting Information

Supporting Information Supportng Informaton The neural network f n Eq. 1 s gven by: f x l = ReLU W atom x l + b atom, 2 where ReLU s the element-wse rectfed lnear unt, 21.e., ReLUx = max0, x, W atom R d d s the weght matrx to

More information

COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS

COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS Avalable onlne at http://sck.org J. Math. Comput. Sc. 3 (3), No., 6-3 ISSN: 97-537 COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS

More information

Chapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems

Chapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems Numercal Analyss by Dr. Anta Pal Assstant Professor Department of Mathematcs Natonal Insttute of Technology Durgapur Durgapur-713209 emal: anta.bue@gmal.com 1 . Chapter 5 Soluton of System of Lnear Equatons

More information

Integrated approach in solving parallel machine scheduling and location (ScheLoc) problem

Integrated approach in solving parallel machine scheduling and location (ScheLoc) problem Internatonal Journal of Industral Engneerng Computatons 7 (2016) 573 584 Contents lsts avalable at GrowngScence Internatonal Journal of Industral Engneerng Computatons homepage: www.growngscence.com/ec

More information

NUMERICAL DIFFERENTIATION

NUMERICAL DIFFERENTIATION NUMERICAL DIFFERENTIATION 1 Introducton Dfferentaton s a method to compute the rate at whch a dependent output y changes wth respect to the change n the ndependent nput x. Ths rate of change s called the

More information

4DVAR, according to the name, is a four-dimensional variational method.

4DVAR, according to the name, is a four-dimensional variational method. 4D-Varatonal Data Assmlaton (4D-Var) 4DVAR, accordng to the name, s a four-dmensonal varatonal method. 4D-Var s actually a drect generalzaton of 3D-Var to handle observatons that are dstrbuted n tme. The

More information

Real-Time Systems. Multiprocessor scheduling. Multiprocessor scheduling. Multiprocessor scheduling

Real-Time Systems. Multiprocessor scheduling. Multiprocessor scheduling. Multiprocessor scheduling Real-Tme Systems Multprocessor schedulng Specfcaton Implementaton Verfcaton Multprocessor schedulng -- -- Global schedulng How are tasks assgned to processors? Statc assgnment The processor(s) used for

More information

Module 9. Lecture 6. Duality in Assignment Problems

Module 9. Lecture 6. Duality in Assignment Problems Module 9 1 Lecture 6 Dualty n Assgnment Problems In ths lecture we attempt to answer few other mportant questons posed n earler lecture for (AP) and see how some of them can be explaned through the concept

More information

Report on Image warping

Report on Image warping Report on Image warpng Xuan Ne, Dec. 20, 2004 Ths document summarzed the algorthms of our mage warpng soluton for further study, and there s a detaled descrpton about the mplementaton of these algorthms.

More information

High resolution entropy stable scheme for shallow water equations

High resolution entropy stable scheme for shallow water equations Internatonal Symposum on Computers & Informatcs (ISCI 05) Hgh resoluton entropy stable scheme for shallow water equatons Xaohan Cheng,a, Yufeng Ne,b, Department of Appled Mathematcs, Northwestern Polytechncal

More information

LOW BIAS INTEGRATED PATH ESTIMATORS. James M. Calvin

LOW BIAS INTEGRATED PATH ESTIMATORS. James M. Calvin Proceedngs of the 007 Wnter Smulaton Conference S G Henderson, B Bller, M-H Hseh, J Shortle, J D Tew, and R R Barton, eds LOW BIAS INTEGRATED PATH ESTIMATORS James M Calvn Department of Computer Scence

More information

Problem Set 9 Solutions

Problem Set 9 Solutions Desgn and Analyss of Algorthms May 4, 2015 Massachusetts Insttute of Technology 6.046J/18.410J Profs. Erk Demane, Srn Devadas, and Nancy Lynch Problem Set 9 Solutons Problem Set 9 Solutons Ths problem

More information

Suppose that there s a measured wndow of data fff k () ; :::; ff k g of a sze w, measured dscretely wth varable dscretzaton step. It s convenent to pl

Suppose that there s a measured wndow of data fff k () ; :::; ff k g of a sze w, measured dscretely wth varable dscretzaton step. It s convenent to pl RECURSIVE SPLINE INTERPOLATION METHOD FOR REAL TIME ENGINE CONTROL APPLICATIONS A. Stotsky Volvo Car Corporaton Engne Desgn and Development Dept. 97542, HA1N, SE- 405 31 Gothenburg Sweden. Emal: astotsky@volvocars.com

More information

Outline. Communication. Bellman Ford Algorithm. Bellman Ford Example. Bellman Ford Shortest Path [1]

Outline. Communication. Bellman Ford Algorithm. Bellman Ford Example. Bellman Ford Shortest Path [1] DYNAMIC SHORTEST PATH SEARCH AND SYNCHRONIZED TASK SWITCHING Jay Wagenpfel, Adran Trachte 2 Outlne Shortest Communcaton Path Searchng Bellmann Ford algorthm Algorthm for dynamc case Modfcatons to our algorthm

More information

An Admission Control Algorithm in Cloud Computing Systems

An Admission Control Algorithm in Cloud Computing Systems An Admsson Control Algorthm n Cloud Computng Systems Authors: Frank Yeong-Sung Ln Department of Informaton Management Natonal Tawan Unversty Tape, Tawan, R.O.C. ysln@m.ntu.edu.tw Yngje Lan Management Scence

More information

Lecture 10 Support Vector Machines II

Lecture 10 Support Vector Machines II Lecture 10 Support Vector Machnes II 22 February 2016 Taylor B. Arnold Yale Statstcs STAT 365/665 1/28 Notes: Problem 3 s posted and due ths upcomng Frday There was an early bug n the fake-test data; fxed

More information

DETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM

DETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM Ganj, Z. Z., et al.: Determnaton of Temperature Dstrbuton for S111 DETERMINATION OF TEMPERATURE DISTRIBUTION FOR ANNULAR FINS WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY BY HPM by Davood Domr GANJI

More information

Errors for Linear Systems

Errors for Linear Systems Errors for Lnear Systems When we solve a lnear system Ax b we often do not know A and b exactly, but have only approxmatons  and ˆb avalable. Then the best thng we can do s to solve ˆx ˆb exactly whch

More information

FUZZY GOAL PROGRAMMING VS ORDINARY FUZZY PROGRAMMING APPROACH FOR MULTI OBJECTIVE PROGRAMMING PROBLEM

FUZZY GOAL PROGRAMMING VS ORDINARY FUZZY PROGRAMMING APPROACH FOR MULTI OBJECTIVE PROGRAMMING PROBLEM Internatonal Conference on Ceramcs, Bkaner, Inda Internatonal Journal of Modern Physcs: Conference Seres Vol. 22 (2013) 757 761 World Scentfc Publshng Company DOI: 10.1142/S2010194513010982 FUZZY GOAL

More information

EEE 241: Linear Systems

EEE 241: Linear Systems EEE : Lnear Systems Summary #: Backpropagaton BACKPROPAGATION The perceptron rule as well as the Wdrow Hoff learnng were desgned to tran sngle layer networks. They suffer from the same dsadvantage: they

More information

Econ107 Applied Econometrics Topic 3: Classical Model (Studenmund, Chapter 4)

Econ107 Applied Econometrics Topic 3: Classical Model (Studenmund, Chapter 4) I. Classcal Assumptons Econ7 Appled Econometrcs Topc 3: Classcal Model (Studenmund, Chapter 4) We have defned OLS and studed some algebrac propertes of OLS. In ths topc we wll study statstcal propertes

More information

Calculation of time complexity (3%)

Calculation of time complexity (3%) Problem 1. (30%) Calculaton of tme complexty (3%) Gven n ctes, usng exhaust search to see every result takes O(n!). Calculaton of tme needed to solve the problem (2%) 40 ctes:40! dfferent tours 40 add

More information

Hongyi Miao, College of Science, Nanjing Forestry University, Nanjing ,China. (Received 20 June 2013, accepted 11 March 2014) I)ϕ (k)

Hongyi Miao, College of Science, Nanjing Forestry University, Nanjing ,China. (Received 20 June 2013, accepted 11 March 2014) I)ϕ (k) ISSN 1749-3889 (prnt), 1749-3897 (onlne) Internatonal Journal of Nonlnear Scence Vol.17(2014) No.2,pp.188-192 Modfed Block Jacob-Davdson Method for Solvng Large Sparse Egenproblems Hongy Mao, College of

More information

Fuzzy Boundaries of Sample Selection Model

Fuzzy Boundaries of Sample Selection Model Proceedngs of the 9th WSES Internatonal Conference on ppled Mathematcs, Istanbul, Turkey, May 7-9, 006 (pp309-34) Fuzzy Boundares of Sample Selecton Model L. MUHMD SFIIH, NTON BDULBSH KMIL, M. T. BU OSMN

More information

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD Ákos Jósef Lengyel, István Ecsed Assstant Lecturer, Professor of Mechancs, Insttute of Appled Mechancs, Unversty of Mskolc, Mskolc-Egyetemváros,

More information

For now, let us focus on a specific model of neurons. These are simplified from reality but can achieve remarkable results.

For now, let us focus on a specific model of neurons. These are simplified from reality but can achieve remarkable results. Neural Networks : Dervaton compled by Alvn Wan from Professor Jtendra Malk s lecture Ths type of computaton s called deep learnng and s the most popular method for many problems, such as computer vson

More information

A PROBABILITY-DRIVEN SEARCH ALGORITHM FOR SOLVING MULTI-OBJECTIVE OPTIMIZATION PROBLEMS

A PROBABILITY-DRIVEN SEARCH ALGORITHM FOR SOLVING MULTI-OBJECTIVE OPTIMIZATION PROBLEMS HCMC Unversty of Pedagogy Thong Nguyen Huu et al. A PROBABILITY-DRIVEN SEARCH ALGORITHM FOR SOLVING MULTI-OBJECTIVE OPTIMIZATION PROBLEMS Thong Nguyen Huu and Hao Tran Van Department of mathematcs-nformaton,

More information

Speeding up Computation of Scalar Multiplication in Elliptic Curve Cryptosystem

Speeding up Computation of Scalar Multiplication in Elliptic Curve Cryptosystem H.K. Pathak et. al. / (IJCSE) Internatonal Journal on Computer Scence and Engneerng Speedng up Computaton of Scalar Multplcaton n Ellptc Curve Cryptosystem H. K. Pathak Manju Sangh S.o.S n Computer scence

More information

A new Approach for Solving Linear Ordinary Differential Equations

A new Approach for Solving Linear Ordinary Differential Equations , ISSN 974-57X (Onlne), ISSN 974-5718 (Prnt), Vol. ; Issue No. 1; Year 14, Copyrght 13-14 by CESER PUBLICATIONS A new Approach for Solvng Lnear Ordnary Dfferental Equatons Fawz Abdelwahd Department of

More information

Introduction to Vapor/Liquid Equilibrium, part 2. Raoult s Law:

Introduction to Vapor/Liquid Equilibrium, part 2. Raoult s Law: CE304, Sprng 2004 Lecture 4 Introducton to Vapor/Lqud Equlbrum, part 2 Raoult s Law: The smplest model that allows us do VLE calculatons s obtaned when we assume that the vapor phase s an deal gas, and

More information

VQ widely used in coding speech, image, and video

VQ widely used in coding speech, image, and video at Scalar quantzers are specal cases of vector quantzers (VQ): they are constraned to look at one sample at a tme (memoryless) VQ does not have such constrant better RD perfomance expected Source codng

More information

Polynomial Regression Models

Polynomial Regression Models LINEAR REGRESSION ANALYSIS MODULE XII Lecture - 6 Polynomal Regresson Models Dr. Shalabh Department of Mathematcs and Statstcs Indan Insttute of Technology Kanpur Test of sgnfcance To test the sgnfcance

More information

Internet Engineering. Jacek Mazurkiewicz, PhD Softcomputing. Part 3: Recurrent Artificial Neural Networks Self-Organising Artificial Neural Networks

Internet Engineering. Jacek Mazurkiewicz, PhD Softcomputing. Part 3: Recurrent Artificial Neural Networks Self-Organising Artificial Neural Networks Internet Engneerng Jacek Mazurkewcz, PhD Softcomputng Part 3: Recurrent Artfcal Neural Networks Self-Organsng Artfcal Neural Networks Recurrent Artfcal Neural Networks Feedback sgnals between neurons Dynamc

More information

NON-CENTRAL 7-POINT FORMULA IN THE METHOD OF LINES FOR PARABOLIC AND BURGERS' EQUATIONS

NON-CENTRAL 7-POINT FORMULA IN THE METHOD OF LINES FOR PARABOLIC AND BURGERS' EQUATIONS IJRRAS 8 (3 September 011 www.arpapress.com/volumes/vol8issue3/ijrras_8_3_08.pdf NON-CENTRAL 7-POINT FORMULA IN THE METHOD OF LINES FOR PARABOLIC AND BURGERS' EQUATIONS H.O. Bakodah Dept. of Mathematc

More information

Physics 5153 Classical Mechanics. D Alembert s Principle and The Lagrangian-1

Physics 5153 Classical Mechanics. D Alembert s Principle and The Lagrangian-1 P. Guterrez Physcs 5153 Classcal Mechancs D Alembert s Prncple and The Lagrangan 1 Introducton The prncple of vrtual work provdes a method of solvng problems of statc equlbrum wthout havng to consder the

More information

A Hybrid Variational Iteration Method for Blasius Equation

A Hybrid Variational Iteration Method for Blasius Equation Avalable at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 1932-9466 Vol. 10, Issue 1 (June 2015), pp. 223-229 Applcatons and Appled Mathematcs: An Internatonal Journal (AAM) A Hybrd Varatonal Iteraton Method

More information

Week 5: Neural Networks

Week 5: Neural Networks Week 5: Neural Networks Instructor: Sergey Levne Neural Networks Summary In the prevous lecture, we saw how we can construct neural networks by extendng logstc regresson. Neural networks consst of multple

More information

2E Pattern Recognition Solutions to Introduction to Pattern Recognition, Chapter 2: Bayesian pattern classification

2E Pattern Recognition Solutions to Introduction to Pattern Recognition, Chapter 2: Bayesian pattern classification E395 - Pattern Recognton Solutons to Introducton to Pattern Recognton, Chapter : Bayesan pattern classfcaton Preface Ths document s a soluton manual for selected exercses from Introducton to Pattern Recognton

More information

1 Convex Optimization

1 Convex Optimization Convex Optmzaton We wll consder convex optmzaton problems. Namely, mnmzaton problems where the objectve s convex (we assume no constrants for now). Such problems often arse n machne learnng. For example,

More information

Neural Networks & Learning

Neural Networks & Learning Neural Netorks & Learnng. Introducton The basc prelmnares nvolved n the Artfcal Neural Netorks (ANN) are descrbed n secton. An Artfcal Neural Netorks (ANN) s an nformaton-processng paradgm that nspred

More information

Annexes. EC.1. Cycle-base move illustration. EC.2. Problem Instances

Annexes. EC.1. Cycle-base move illustration. EC.2. Problem Instances ec Annexes Ths Annex frst llustrates a cycle-based move n the dynamc-block generaton tabu search. It then dsplays the characterstcs of the nstance sets, followed by detaled results of the parametercalbraton

More information

VARIATION OF CONSTANT SUM CONSTRAINT FOR INTEGER MODEL WITH NON UNIFORM VARIABLES

VARIATION OF CONSTANT SUM CONSTRAINT FOR INTEGER MODEL WITH NON UNIFORM VARIABLES VARIATION OF CONSTANT SUM CONSTRAINT FOR INTEGER MODEL WITH NON UNIFORM VARIABLES BÂRZĂ, Slvu Faculty of Mathematcs-Informatcs Spru Haret Unversty barza_slvu@yahoo.com Abstract Ths paper wants to contnue

More information

A FAST HEURISTIC FOR TASKS ASSIGNMENT IN MANYCORE SYSTEMS WITH VOLTAGE-FREQUENCY ISLANDS

A FAST HEURISTIC FOR TASKS ASSIGNMENT IN MANYCORE SYSTEMS WITH VOLTAGE-FREQUENCY ISLANDS Shervn Haamn A FAST HEURISTIC FOR TASKS ASSIGNMENT IN MANYCORE SYSTEMS WITH VOLTAGE-FREQUENCY ISLANDS INTRODUCTION Increasng computatons n applcatons has led to faster processng. o Use more cores n a chp

More information

CHAPTER III Neural Networks as Associative Memory

CHAPTER III Neural Networks as Associative Memory CHAPTER III Neural Networs as Assocatve Memory Introducton One of the prmary functons of the bran s assocatve memory. We assocate the faces wth names, letters wth sounds, or we can recognze the people

More information

One-sided finite-difference approximations suitable for use with Richardson extrapolation

One-sided finite-difference approximations suitable for use with Richardson extrapolation Journal of Computatonal Physcs 219 (2006) 13 20 Short note One-sded fnte-dfference approxmatons sutable for use wth Rchardson extrapolaton Kumar Rahul, S.N. Bhattacharyya * Department of Mechancal Engneerng,

More information

Hidden Markov Models

Hidden Markov Models Hdden Markov Models Namrata Vaswan, Iowa State Unversty Aprl 24, 204 Hdden Markov Model Defntons and Examples Defntons:. A hdden Markov model (HMM) refers to a set of hdden states X 0, X,..., X t,...,

More information

Additional Codes using Finite Difference Method. 1 HJB Equation for Consumption-Saving Problem Without Uncertainty

Additional Codes using Finite Difference Method. 1 HJB Equation for Consumption-Saving Problem Without Uncertainty Addtonal Codes usng Fnte Dfference Method Benamn Moll 1 HJB Equaton for Consumpton-Savng Problem Wthout Uncertanty Before consderng the case wth stochastc ncome n http://www.prnceton.edu/~moll/ HACTproect/HACT_Numercal_Appendx.pdf,

More information

Support Vector Machines. Vibhav Gogate The University of Texas at dallas

Support Vector Machines. Vibhav Gogate The University of Texas at dallas Support Vector Machnes Vbhav Gogate he Unversty of exas at dallas What We have Learned So Far? 1. Decson rees. Naïve Bayes 3. Lnear Regresson 4. Logstc Regresson 5. Perceptron 6. Neural networks 7. K-Nearest

More information

The Geometry of Logit and Probit

The Geometry of Logit and Probit The Geometry of Logt and Probt Ths short note s meant as a supplement to Chapters and 3 of Spatal Models of Parlamentary Votng and the notaton and reference to fgures n the text below s to those two chapters.

More information

On the Multicriteria Integer Network Flow Problem

On the Multicriteria Integer Network Flow Problem BULGARIAN ACADEMY OF SCIENCES CYBERNETICS AND INFORMATION TECHNOLOGIES Volume 5, No 2 Sofa 2005 On the Multcrtera Integer Network Flow Problem Vassl Vasslev, Marana Nkolova, Maryana Vassleva Insttute of

More information

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look

More information

4 Analysis of Variance (ANOVA) 5 ANOVA. 5.1 Introduction. 5.2 Fixed Effects ANOVA

4 Analysis of Variance (ANOVA) 5 ANOVA. 5.1 Introduction. 5.2 Fixed Effects ANOVA 4 Analyss of Varance (ANOVA) 5 ANOVA 51 Introducton ANOVA ANOVA s a way to estmate and test the means of multple populatons We wll start wth one-way ANOVA If the populatons ncluded n the study are selected

More information

The Order Relation and Trace Inequalities for. Hermitian Operators

The Order Relation and Trace Inequalities for. Hermitian Operators Internatonal Mathematcal Forum, Vol 3, 08, no, 507-57 HIKARI Ltd, wwwm-hkarcom https://doorg/0988/mf088055 The Order Relaton and Trace Inequaltes for Hermtan Operators Y Huang School of Informaton Scence

More information

On a direct solver for linear least squares problems

On a direct solver for linear least squares problems ISSN 2066-6594 Ann. Acad. Rom. Sc. Ser. Math. Appl. Vol. 8, No. 2/2016 On a drect solver for lnear least squares problems Constantn Popa Abstract The Null Space (NS) algorthm s a drect solver for lnear

More information

Neuro-Adaptive Design - I:

Neuro-Adaptive Design - I: Lecture 36 Neuro-Adaptve Desgn - I: A Robustfyng ool for Dynamc Inverson Desgn Dr. Radhakant Padh Asst. Professor Dept. of Aerospace Engneerng Indan Insttute of Scence - Bangalore Motvaton Perfect system

More information

Feature Selection: Part 1

Feature Selection: Part 1 CSE 546: Machne Learnng Lecture 5 Feature Selecton: Part 1 Instructor: Sham Kakade 1 Regresson n the hgh dmensonal settng How do we learn when the number of features d s greater than the sample sze n?

More information

Appendix B: Resampling Algorithms

Appendix B: Resampling Algorithms 407 Appendx B: Resamplng Algorthms A common problem of all partcle flters s the degeneracy of weghts, whch conssts of the unbounded ncrease of the varance of the mportance weghts ω [ ] of the partcles

More information

(Online First)A Lattice Boltzmann Scheme for Diffusion Equation in Spherical Coordinate

(Online First)A Lattice Boltzmann Scheme for Diffusion Equation in Spherical Coordinate Internatonal Journal of Mathematcs and Systems Scence (018) Volume 1 do:10.494/jmss.v1.815 (Onlne Frst)A Lattce Boltzmann Scheme for Dffuson Equaton n Sphercal Coordnate Debabrata Datta 1 *, T K Pal 1

More information

A New Algorithm Using Hopfield Neural Network with CHN for N-Queens Problem

A New Algorithm Using Hopfield Neural Network with CHN for N-Queens Problem 36 IJCSS Internatonal Journal of Computer Scence and etwork Securt, VOL9 o4, Aprl 009 A ew Algorthm Usng Hopfeld eural etwork wth CH for -Queens Problem We Zhang and Zheng Tang, Facult of Engneerng, Toama

More information

The Multiple Classical Linear Regression Model (CLRM): Specification and Assumptions. 1. Introduction

The Multiple Classical Linear Regression Model (CLRM): Specification and Assumptions. 1. Introduction ECONOMICS 5* -- NOTE (Summary) ECON 5* -- NOTE The Multple Classcal Lnear Regresson Model (CLRM): Specfcaton and Assumptons. Introducton CLRM stands for the Classcal Lnear Regresson Model. The CLRM s also

More information

A New Evolutionary Computation Based Approach for Learning Bayesian Network

A New Evolutionary Computation Based Approach for Learning Bayesian Network Avalable onlne at www.scencedrect.com Proceda Engneerng 15 (2011) 4026 4030 Advanced n Control Engneerng and Informaton Scence A New Evolutonary Computaton Based Approach for Learnng Bayesan Network Yungang

More information

Turbulence classification of load data by the frequency and severity of wind gusts. Oscar Moñux, DEWI GmbH Kevin Bleibler, DEWI GmbH

Turbulence classification of load data by the frequency and severity of wind gusts. Oscar Moñux, DEWI GmbH Kevin Bleibler, DEWI GmbH Turbulence classfcaton of load data by the frequency and severty of wnd gusts Introducton Oscar Moñux, DEWI GmbH Kevn Blebler, DEWI GmbH Durng the wnd turbne developng process, one of the most mportant

More information

Computing Correlated Equilibria in Multi-Player Games

Computing Correlated Equilibria in Multi-Player Games Computng Correlated Equlbra n Mult-Player Games Chrstos H. Papadmtrou Presented by Zhanxang Huang December 7th, 2005 1 The Author Dr. Chrstos H. Papadmtrou CS professor at UC Berkley (taught at Harvard,

More information

Embedded Systems. 4. Aperiodic and Periodic Tasks

Embedded Systems. 4. Aperiodic and Periodic Tasks Embedded Systems 4. Aperodc and Perodc Tasks Lothar Thele 4-1 Contents of Course 1. Embedded Systems Introducton 2. Software Introducton 7. System Components 10. Models 3. Real-Tme Models 4. Perodc/Aperodc

More information

A PROCEDURE FOR SIMULATING THE NONLINEAR CONDUCTION HEAT TRANSFER IN A BODY WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY.

A PROCEDURE FOR SIMULATING THE NONLINEAR CONDUCTION HEAT TRANSFER IN A BODY WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY. Proceedngs of the th Brazlan Congress of Thermal Scences and Engneerng -- ENCIT 006 Braz. Soc. of Mechancal Scences and Engneerng -- ABCM, Curtba, Brazl,- Dec. 5-8, 006 A PROCEDURE FOR SIMULATING THE NONLINEAR

More information

9 Derivation of Rate Equations from Single-Cell Conductance (Hodgkin-Huxley-like) Equations

9 Derivation of Rate Equations from Single-Cell Conductance (Hodgkin-Huxley-like) Equations Physcs 171/271 - Chapter 9R -Davd Klenfeld - Fall 2005 9 Dervaton of Rate Equatons from Sngle-Cell Conductance (Hodgkn-Huxley-lke) Equatons We consder a network of many neurons, each of whch obeys a set

More information

Scroll Generation with Inductorless Chua s Circuit and Wien Bridge Oscillator

Scroll Generation with Inductorless Chua s Circuit and Wien Bridge Oscillator Latest Trends on Crcuts, Systems and Sgnals Scroll Generaton wth Inductorless Chua s Crcut and Wen Brdge Oscllator Watcharn Jantanate, Peter A. Chayasena, and Sarawut Sutorn * Abstract An nductorless Chua

More information

Linear Approximation with Regularization and Moving Least Squares

Linear Approximation with Regularization and Moving Least Squares Lnear Approxmaton wth Regularzaton and Movng Least Squares Igor Grešovn May 007 Revson 4.6 (Revson : March 004). 5 4 3 0.5 3 3.5 4 Contents: Lnear Fttng...4. Weghted Least Squares n Functon Approxmaton...

More information

Multilayer Perceptrons and Backpropagation. Perceptrons. Recap: Perceptrons. Informatics 1 CG: Lecture 6. Mirella Lapata

Multilayer Perceptrons and Backpropagation. Perceptrons. Recap: Perceptrons. Informatics 1 CG: Lecture 6. Mirella Lapata Multlayer Perceptrons and Informatcs CG: Lecture 6 Mrella Lapata School of Informatcs Unversty of Ednburgh mlap@nf.ed.ac.uk Readng: Kevn Gurney s Introducton to Neural Networks, Chapters 5 6.5 January,

More information

A Bayes Algorithm for the Multitask Pattern Recognition Problem Direct Approach

A Bayes Algorithm for the Multitask Pattern Recognition Problem Direct Approach A Bayes Algorthm for the Multtask Pattern Recognton Problem Drect Approach Edward Puchala Wroclaw Unversty of Technology, Char of Systems and Computer etworks, Wybrzeze Wyspanskego 7, 50-370 Wroclaw, Poland

More information

Finding Dense Subgraphs in G(n, 1/2)

Finding Dense Subgraphs in G(n, 1/2) Fndng Dense Subgraphs n Gn, 1/ Atsh Das Sarma 1, Amt Deshpande, and Rav Kannan 1 Georga Insttute of Technology,atsh@cc.gatech.edu Mcrosoft Research-Bangalore,amtdesh,annan@mcrosoft.com Abstract. Fndng

More information

NP-Completeness : Proofs

NP-Completeness : Proofs NP-Completeness : Proofs Proof Methods A method to show a decson problem Π NP-complete s as follows. (1) Show Π NP. (2) Choose an NP-complete problem Π. (3) Show Π Π. A method to show an optmzaton problem

More information

Tracking with Kalman Filter

Tracking with Kalman Filter Trackng wth Kalman Flter Scott T. Acton Vrgna Image and Vdeo Analyss (VIVA), Charles L. Brown Department of Electrcal and Computer Engneerng Department of Bomedcal Engneerng Unversty of Vrgna, Charlottesvlle,

More information

6.3.4 Modified Euler s method of integration

6.3.4 Modified Euler s method of integration 6.3.4 Modfed Euler s method of ntegraton Before dscussng the applcaton of Euler s method for solvng the swng equatons, let us frst revew the basc Euler s method of numercal ntegraton. Let the general from

More information

On the Interval Zoro Symmetric Single-step Procedure for Simultaneous Finding of Polynomial Zeros

On the Interval Zoro Symmetric Single-step Procedure for Simultaneous Finding of Polynomial Zeros Appled Mathematcal Scences, Vol. 5, 2011, no. 75, 3693-3706 On the Interval Zoro Symmetrc Sngle-step Procedure for Smultaneous Fndng of Polynomal Zeros S. F. M. Rusl, M. Mons, M. A. Hassan and W. J. Leong

More information

Newton s Method for One - Dimensional Optimization - Theory

Newton s Method for One - Dimensional Optimization - Theory Numercal Methods Newton s Method for One - Dmensonal Optmzaton - Theory For more detals on ths topc Go to Clck on Keyword Clck on Newton s Method for One- Dmensonal Optmzaton You are free to Share to copy,

More information

Application of B-Spline to Numerical Solution of a System of Singularly Perturbed Problems

Application of B-Spline to Numerical Solution of a System of Singularly Perturbed Problems Mathematca Aeterna, Vol. 1, 011, no. 06, 405 415 Applcaton of B-Splne to Numercal Soluton of a System of Sngularly Perturbed Problems Yogesh Gupta Department of Mathematcs Unted College of Engneerng &

More information

Department of Electrical & Electronic Engineeing Imperial College London. E4.20 Digital IC Design. Median Filter Project Specification

Department of Electrical & Electronic Engineeing Imperial College London. E4.20 Digital IC Design. Median Filter Project Specification Desgn Project Specfcaton Medan Flter Department of Electrcal & Electronc Engneeng Imperal College London E4.20 Dgtal IC Desgn Medan Flter Project Specfcaton A medan flter s used to remove nose from a sampled

More information