A Markov Decision Approach for the Computation of Testability of RTL Constructs

Size: px
Start display at page:

Download "A Markov Decision Approach for the Computation of Testability of RTL Constructs"

Transcription

1 A Makov Decision Appoach fo the Computation of Testability of RTL Constucts José Miguel Fenandes Abstact In the analysis of digital cicuits, to study testability estimation measues, dissipated powe and electomagnetic infeence,it is cucial to obtain with pecision the switching pobability of the cicuit intenal nodes. By solving the Chapman-Kolmogoov equations that descibe the steady state behaviou of the cicuit, we can calculate the pobability associated with each state of the MC that epesents the undelying FSM [6][7]. By supevising the behaviou of the MC, the allowed events, associated with a tansition pobability, will conduct the MC to the states whee we obtain highe levels of contollability/obsevability fo the intenal vaiables. If we model the poblem as a Makov decision pocess (Contolled Makov Chain), we can solve it using Dynamic Pogamming Methods (DP). This way, the tansition pobability between states will follow, not a fied distibution, but instead some contollable distibution using a set of contol actions.. Intoduction Validation of RTL desciptions emains one of the pincipal bottlenecks in the cicuit design pocess. The steady gowth in compleity of integated cicuits and the need to educe the time to maket of poducts has contibuted to incease the pecentage of time spent in cicuit veification. This veification is impotant both in the design phase (functional veification) and in the post- manufactuing test phase (defect testing). In both cases, the eistence of appopiate test vectos is citical to ensue defect fee cicuits and to avoid the need fo costly e-design cycles. Thee ae essentially two appoaches fo the veification of RTL desciptions: simulation based methods and fomal veification methods. Simulation based methods ty to eecise all pats of the cicuits by using a high numbe of vectos, obtained eithe by using knowledge of the design o by using some pseudo-andom test vecto geneato. Fomal based methods can be used to veify RTL desciptions against oiginal specifications of the cicuit, sometimes obtained fom behavioual desciptions. Simulation based method equie the eistence of appopiate test vectos. Regettably, automatic geneation of test vectos at highe abstaction levels [2] fo comple designs emains an open poblem, although significant advances have been made in this field [3][4]. The key poblem is that andom vectos don t eecise adequately the had to each conditions that lead to the eecution of the dak spots in the design, and efficient algoithms fo sequential test patten geneation ae unlikely to eist since the poblem is known to be PSPACE-complete.[5] Veification based appoaches, on the othe hand, equie the eistence of fomal highe level specifications that ae not always available. Futhemoe, algoithms fo fomal veification of sequential cicuits ae also inheently comple, although advances in heuistics have made them applicable in a wide ange of designs [8]. The pesent wok addesses this poblem by poposing an appoimate statistic modeling appoach that obtains accuate estimates of the contollability/obsevability of RTL constucts. These estimates can be used to impove the design and test pocesses in a numbe of ways. In the design phase, they can be used to infom the designe that a given constuct is not being adequately tested and that it may equie changes o some othe manual intevention. Ou appoach is specially appopiate fo this type of intevention, since thee is a vey close connection between the RTL constucts and the intenal model signals whose testability is being evaluated. At this level, it can also be used to bias the geneation of andomized tests, in ode to achieve adequate functional coveage of had to test constucts. Ou appoach is based on a statistical modeling and addesses the contollability/obsevability of stuctues diectly at the RTL level. In this way, the feedback given to the designe is easie to use, since testability esults ae given in tems of RTL constucts and not in tems of post-synthesis logic nodes. This wok solve the Chapman-Kolmogoov equations that descibe the steady state behaviou of the cicuit, which can be used to compute the pobability associated with each state of the MC. The events allowed by the supeviso ae associated with a tansition pobability. By contolling these pobabilities is possible to conduct the MC to the states whee we obtain

2 highe levels of contollability/obsevability fo the intenal vaiables[7]. Using DP methods we model the system as a Makov Decision Pocess. Fo that pupose, the tansition pobability between states will follow a contollable distibution, using a set of contol actions. 2. Poblem Fomulation Duing the design pocess seveal abstaction levels ae nomally used to achieve apid development of digital cicuits. Fom the algoithmic to the physical level, design testability assessment is an impotant issue. Accuate assessment of the testability of a given pat of a design is impotant not only because it avoids poblems in the poduction testing phase, but also because it makes sue that the design is being popely tested fom a functional point of view. In paticula, the eistence of dak spots in the design, i.e., blocks o constucts that ae not being popely eecised is to be avoided in an agile development pocess. In this wok, we model the behavio o the RTL desciption of a cicuit using a discete time Makov chain. Fo the most geneic case, that of sequential cicuits, we ae inteested in the cicuit behavio in the steady-state. This is impotant because, fo sequential cicuits (e.g., countes, shift-egistes, contol systems), many constucts only become active and eecisable when a given set of conditions is met. By computing the steady-state behavio of a cicuit, we make sue that the pobabilities of occuence of events ae calculated with pecision, even if the events ae ae o depend on vey specific input conditions. The method descibed hee solves the Chapman-Kolmogoov equations that descibe the steady state behavio of the cicuit, and calculates the pobability associated with each state of the Makov chain. To educe the computation effot and cope with lage designs we use symbolic epesentation methods that descibe the cicuit function using Binay Decision Diagams (BDD). Figue epesents the geneal scheme of a geneic synchonous sequential cicuit. Its behavio can be epesented by a tansition gaph, modeled by a tuple ( Σ,, χ,, δ, λ) whee Σ is a finite set of input symbols, is a finite set of output symbols, χ is a finite set of states, χ is the initial eset state, δ : χ Σ χ is the tansition function, and λ : χ Σ is the output function. Fig. : Scheme of a geneic synchonous sequential cicuit Unde athe geneal assumptions, the FSM associated with any synchonous sequential cicuit can be modeled by a Makov chain and the equations that descibe the steady state pobabilities of each state in the tansition gaph (the Chapman-Kolmogoov equations) have a unique solution. Moe pecisely, attaching to each out-going edge of each state in the taget FSM a tansition pobability that coesponds to a paticula tansition, one actually obtains a MC. As an eample on how to model the behaviou of an RTL desciption, lets considee the following FSM, that epesents an hadwae cicuit to validate a BCD wod with 4 bits: A B Fig. : FSM of the BCD validation cicuit The used alphabet Σ is the following: C Symbol Desciption Logic zeo Logic one Don t cae Reset signal F D G E Table : Alphabet fo the BCD validation cicuit Σ = χ = = {,,, } { A, B, C, D, E, F, G} A

3 As can be obseved in fig., the open loop ealization of the poposed hadwae cicuit will geneate a language L(G) with the following stings: uncontollable event is the (Reset) signal. All the othes ae contollable and obsevable. Evey fou input symbols, the system gives a validation signal fo the BDC wod. Sting Valid Y/N Y Y Y Y Y Y Y Y Y Y N N N N N N Table 2: L(G) fo the BCD validation cicuit As showed in table 2, thee ae some stings geneated by the open loop FSM that ae not allowed (not valid BDC wods). 3. Supeviso ealization To implement the supeviso, a PN has been chosen: The objective is to design a supeviso S fo the admissible language L a (G) given a set of uncontollable events E uc. In closed loop the system is epesented in Fig. 3: S s S G L( S / G) Fig.2: Closed loop epesentation of the cicuit Validation We ae using the concepts of supevisoy contol applied to an hadwae design cicuit, to implement a supeviso that foces the cicuit to comply with a set of specifications. The events ae followed by the supeviso that, knowing the system cuent state, decides on the symbols allowed to be visualized by the system (policy ). The only S s Fig. 3: PN ealization fo the supeviso With this supeviso ealization, the invalid stings and ae not allowed in the L( S / G) language. The symbol (don t cae) may epesent a o a. Rule: IF (bit 2= OR bit 3=) => bit Makov Chain As showed in fig. 2, the closed loop epesentation fo the system is composed by a single seve with an infinite queue fo the aival symbols. The seve can only pocess a symbol at a time. The symbol aival can be epesented by a Poisson distibution with aveage value λ. Symbols ae pocessed following an eponential distibution with aveage value µ. As stated befoe, the tansition pobability between states will follow a contollable distibution, using a set of contol actions. The goal is to each the maked state following an event sequence that minimize a given cost function ove a specified inteval. 4. CTMC

4 Makov pocesses have the memoyless popety. Knowing the cuent state fo the system, the futue state only depends on epessed as k k and not on the past histoy []. This can be P[ X ( t ) X ( t ) =, X ( t ) =,..., X t = ]= k+ = k+ k k k k ( [ X t ) X ( t ] P ( k+ = k+ k ) = k () fo any t t... t k tk +. The MC epessed this way is called a lag-one MC. The conditional pobabilities P [ X ( tk+ ) = k+ X ( tk ) = k ] ae called single-step tansition pobabilities and epesent the conditional pobabilities of making a tansition fom state X ( t k ) to state X ( t k+ ) at time step k. In homogeneous MC these pobabilities ae independent of k and consequently witten as P = P( X + = j X fo all k=,2, k k = To calculate the tansition pobabilities [], we must geneate a tansition ate mati Q. The ate associated with a state tansition is epesented in this mati. Then, a tansition pobability mati P can be deived. As eplained in [], a GSMP with a Poisson clock stuctue educes to a MC and inheits the memoyless popety of the Poisson pocess. The state holding time V ( at state i has an eponential distibution Λ( t [ ] P V ( t = e, t (2) with Λ( = λ (3) e Γ( Λ( is the sum of the Poisson ates of all active events at state i, e is a feasible event at state i, and Γ( is the set of all feasible events at state i. To obtain the tems fo the Q mati, afte futhe manipulation [] we obtain the esults: and q ii = Λ( q P (4) = λ (5) Consideing a cicuit with N egistes. The state space χ = {,,..., M } to eploe has, in the wost case, N M = 2 possible states. Assume that the system is in state i. Unde the Makov assumption, the tansition between state i and j occus with pobability P, unde some specific, time invaiant, input distibution. Then, in steady state, the pobability of state i is given by: P ( j ) = π P( i ) (7) i with P ( j ) =. j Let s associate ates to the tansitions of diagam epesented in Fig.. Tansitions with events, o, have the same ate of. Tansition associated with the eset signal have a ate of µ. 4.2 DTMC Thee ae applications wee discete time models ae moe convenient to model the systems unde study, because geneally ae easie to set up and simple to analyse. Having specified the tansition ate mati Q of the CTMC, we can obtain the equivalent DTMC using a unifomization pocess based on the choice of a unifom tansition ate defined by the following elation ma { } q ii i χ with tansition pobabilities U P q = qii +, i j, i = j Fo ou eample, we can choose a unifom ate of and obtain fo the U P = µ + 2 mati (8) (9) - q ii epesents the total event ate chaacteizing state i, q is the instantaneous ate at which a state tansition fom i to j takes place. Fo a GSMP with Poisson clock stuctue, being at state i the pobability of a tansition e to state j is P q =, j i (6) q ii

5 U P µ + µ µ µ = µ µ µ 5. Optimal Contol Policy Vk+ ( = min C( i, u) + P ( u) Vk ( j) u U i j (2) consideing a N step finite vesion of the poblem, with V ( = fo all i, k =,..., N. Fo the specific eample poposed, because the system has to validate a 4 bits BCD wod, we conside N=4. As defined befoe, ou goal is to to conduct the MC to the states whee we obtain highe levels of contollability/obsevability fo the intenal vaiables. In this eample we have only one maked state (E). Then we can define the following contol action: = at states D o G othewise The closed loop system eliminates fom L(S/G) the fobidden stings of the L(G) language. Addicionaly, by using dynamic pogamming techniques is possible, with the automaton epesentation of the system (o the equivalent state tansition diagam of the implicit FSM), to obtain the optimal sequence of actions that minimizes a given cost function ove a specified time inteval. Having the pobability tansition mati P and the set of possible contol actions fo each state, is possible to find the policy that minimizes the cost associated with the optimal opeation of the system. Consideing the poblem of finding an optimal policy π unde an infinite undiscounted hoizon, if at a time t the state is X (t) then a specific action t) is taken which depends on (t), and the esulting cost is C X ( t), t). Then we have fo the total epected undiscounted cost ove an infinite hoizon X [ ] Vπ ( ) = Eπ [ ] () C X ( t), t) dt whee is the initial state. Having a DTMC with unifom tansition ate, equation () is conveted to the equivalent one E π [ C X k, u k ] () K = Unde the assumption that the cost is bounded ( C( j, u) K ) fo all states j and all contol actions u U j, we can define () ecusively and fo the cost function: [ i ] 2 C( i, u) = C + ) C with C 2 > C. Many cicuits of inteest descibed at the egiste tansfe level ehibit stuctues that lead to vey deep state tansition gaphs. Fo instance, a 6 bit counte with a eset signal cannot be easonably tested by andom pattens, since the eset signal needs to be held inactive fo a long peiod in ode to let the count poceed. This is also the case of ou eample, as showed in the net chapte. Fo instance, in this case, the validate signal at state E, and any pats of the RTL code that depend on the activation of this signal, will be not be well tested unless the eset signal is actuated with vey low pobability. This means a low ate µ, and a bigge ate, which is in accodance with the U mati P. A possible algoithm that can solve this poblem is pesented:. Geneate CDFG of each FSM 2. Fo each CDFG { 3. Geneate espective MC (steady state) 4. Calculate the pobabilities to contol/obseve the vaiables 5. Identify citical vas v i to contol/obseve 6. Fo each v i { 7. Identify the states of the espective MC 8. Find the inputs vectos (event sequence) that will eecise these states 9. Establish the Optimal Contol Policy fo enteing these states with minimal cost. }. }

6 6. Results Ou tool calculates the pobability of contolling/obseving intenal egiste signals, togethe with pimay inputs, fo diffeent eset pobability values.. These esults ae pesented in the net tables. Reset pobability input,5,5,5,5,5 state(),437,4366,4355,4325,4228 state(),3695,364,3527,3297,288 state(2),4396,454,4322,36,3252 validate,495,429,34,73,694 Table 3: Vaiable Contollability esults The contollability deceases fo the validate signal, when the eset pobability inceases. Reset pobability input,,,,, state(),2655,2537,239,89,22 state(),237,2247,24,6,966 state(2),889,24,224,2556,2988 validate,,,,, Table 4: Vaiable Obsevability esults Obseving the validate signal is also moe difficult fo a bigge eset pobability. Reset pobability A,33,3,323,75,252 B,255,253,256,267,27 C,242,234,26,78,84 D,63,6,578,53,434 E,54,466,372,92,867 F,242,234,26,78,84 G,84,84,733,59,3 In this wok we pesented a method to conduct the MC, that models the tansition pobabilities of a FSM associated with an hadwae cicuit, to the states whee we obtain highe levels of contollability/obsevability of intenal vaiables. Using Dynamic Pogamming methods we model the system as a Makov Decision Pocess. Fo that pupose, the tansition pobability between states will follow a contollable distibution, using a contol action. Refeences [] Chistos Cassandas, Stéphane Lafotune, Intoduction to Discete Event Systems, Kluwe Academic Publishes, Massachusetts, 999. [2] Cho C. H., Amstong J. R., B-Algoithm: A Behavioal Test Geneation Algoithm, Poc. IEEE Intenational Test Confeence (ITC), pp , 994. [3] Feandi F., Fummi F., Sciuto D., Implicit Test Geneation fo Behavioal VHDL Models. Poc. IEEE Intenational Test Confeence (ITC), pp , 998. [4] Feaa G., Feandi F., Fin A., Fummy F., Sciuto D., Functional Test Geneation fo Behavioally Sequential Models, Poc. of the Design Automation and Test in Euope Confeence (DATE), pp. 43-4, Mach 2. [5] Feitas A. T., Neto H. C. and Oliveia A. L.. On the compleity of powe estimation poblems. In Intenational Wokshop on Logic Synthesis (ILWS), pages , June 2. [6] J.M. Fenandes, M.B. Santos, A. Oliveia, J.P. Teieia, "A Pobabilistic Method fo the Computation of Testability of RTL Constucts", Poc. of the Design Automation and Test in Euope (DATE) Conf., pp. 76-8, 24. [7] Santos M.B., Fenandes J.M., Teieia I.C., Teieia J.P., RTL Test Patten Geneation fo High Quality Loosely Deteministic BIST, Poc. of the Design Automation and Test in Euope Confeence (DATE), pp , Mach 23. [8] Ken C., Geensteet M.R., Fomal Veification In Hadwae Design: A Suvey, ACM Tansactions on Design Automation of Electonic Systems, 4:2, pp , 999. Table 5: State pobability esults Also fo state E, the only maked state whee the validate signal is activated, its pobability deceases when eset pobability inceases. The same happens to states D and G, which ae the pedecessos of state E. 7. Conclusions

3.1 Random variables

3.1 Random variables 3 Chapte III Random Vaiables 3 Random vaiables A sample space S may be difficult to descibe if the elements of S ae not numbes discuss how we can use a ule by which an element s of S may be associated

More information

Stanford University CS259Q: Quantum Computing Handout 8 Luca Trevisan October 18, 2012

Stanford University CS259Q: Quantum Computing Handout 8 Luca Trevisan October 18, 2012 Stanfod Univesity CS59Q: Quantum Computing Handout 8 Luca Tevisan Octobe 8, 0 Lectue 8 In which we use the quantum Fouie tansfom to solve the peiod-finding poblem. The Peiod Finding Poblem Let f : {0,...,

More information

4/18/2005. Statistical Learning Theory

4/18/2005. Statistical Learning Theory Statistical Leaning Theoy Statistical Leaning Theoy A model of supevised leaning consists of: a Envionment - Supplying a vecto x with a fixed but unknown pdf F x (x b Teache. It povides a desied esponse

More information

Macro Theory B. The Permanent Income Hypothesis

Macro Theory B. The Permanent Income Hypothesis Maco Theoy B The Pemanent Income Hypothesis Ofe Setty The Eitan Beglas School of Economics - Tel Aviv Univesity May 15, 2015 1 1 Motivation 1.1 An econometic check We want to build an empiical model with

More information

The Substring Search Problem

The Substring Search Problem The Substing Seach Poblem One algoithm which is used in a vaiety of applications is the family of substing seach algoithms. These algoithms allow a use to detemine if, given two chaacte stings, one is

More information

HOW TO TEACH THE FUNDAMENTALS OF INFORMATION SCIENCE, CODING, DECODING AND NUMBER SYSTEMS?

HOW TO TEACH THE FUNDAMENTALS OF INFORMATION SCIENCE, CODING, DECODING AND NUMBER SYSTEMS? 6th INTERNATIONAL MULTIDISCIPLINARY CONFERENCE HOW TO TEACH THE FUNDAMENTALS OF INFORMATION SCIENCE, CODING, DECODING AND NUMBER SYSTEMS? Cecília Sitkuné Göömbei College of Nyíegyháza Hungay Abstact: The

More information

Central Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution

Central Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution Statistics Reseach Lettes Vol. Iss., Novembe Cental Coveage Bayes Pediction Intevals fo the Genealized Paeto Distibution Gyan Pakash Depatment of Community Medicine S. N. Medical College, Aga, U. P., India

More information

Explosive Contagion in Networks (Supplementary Information)

Explosive Contagion in Networks (Supplementary Information) Eplosive Contagion in Netwoks (Supplementay Infomation) Jesús Gómez-Gadeñes,, Laua Loteo, Segei N. Taaskin, and Fancisco J. Péez-Reche Institute fo Biocomputation and Physics of Comple Systems (BIFI),

More information

10/04/18. P [P(x)] 1 negl(n).

10/04/18. P [P(x)] 1 negl(n). Mastemath, Sping 208 Into to Lattice lgs & Cypto Lectue 0 0/04/8 Lectues: D. Dadush, L. Ducas Scibe: K. de Boe Intoduction In this lectue, we will teat two main pats. Duing the fist pat we continue the

More information

6 PROBABILITY GENERATING FUNCTIONS

6 PROBABILITY GENERATING FUNCTIONS 6 PROBABILITY GENERATING FUNCTIONS Cetain deivations pesented in this couse have been somewhat heavy on algeba. Fo example, detemining the expectation of the Binomial distibution (page 5.1 tuned out to

More information

New problems in universal algebraic geometry illustrated by boolean equations

New problems in universal algebraic geometry illustrated by boolean equations New poblems in univesal algebaic geomety illustated by boolean equations axiv:1611.00152v2 [math.ra] 25 Nov 2016 Atem N. Shevlyakov Novembe 28, 2016 Abstact We discuss new poblems in univesal algebaic

More information

Probablistically Checkable Proofs

Probablistically Checkable Proofs Lectue 12 Pobablistically Checkable Poofs May 13, 2004 Lectue: Paul Beame Notes: Chis Re 12.1 Pobablisitically Checkable Poofs Oveview We know that IP = PSPACE. This means thee is an inteactive potocol

More information

Pearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms

Pearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms Peason s Chi-Squae Test Modifications fo Compaison of Unweighted and Weighted Histogams and Two Weighted Histogams Univesity of Akueyi, Bogi, v/noduslód, IS-6 Akueyi, Iceland E-mail: nikolai@unak.is Two

More information

( ) [ ] [ ] [ ] δf φ = F φ+δφ F. xdx.

( ) [ ] [ ] [ ] δf φ = F φ+δφ F. xdx. 9. LAGRANGIAN OF THE ELECTROMAGNETIC FIELD In the pevious section the Lagangian and Hamiltonian of an ensemble of point paticles was developed. This appoach is based on a qt. This discete fomulation can

More information

A Bijective Approach to the Permutational Power of a Priority Queue

A Bijective Approach to the Permutational Power of a Priority Queue A Bijective Appoach to the Pemutational Powe of a Pioity Queue Ia M. Gessel Kuang-Yeh Wang Depatment of Mathematics Bandeis Univesity Waltham, MA 02254-9110 Abstact A pioity queue tansfoms an input pemutation

More information

F-IF Logistic Growth Model, Abstract Version

F-IF Logistic Growth Model, Abstract Version F-IF Logistic Gowth Model, Abstact Vesion Alignments to Content Standads: F-IFB4 Task An impotant example of a model often used in biology o ecology to model population gowth is called the logistic gowth

More information

Quantum Fourier Transform

Quantum Fourier Transform Chapte 5 Quantum Fouie Tansfom Many poblems in physics and mathematics ae solved by tansfoming a poblem into some othe poblem with a known solution. Some notable examples ae Laplace tansfom, Legende tansfom,

More information

On Polynomials Construction

On Polynomials Construction Intenational Jounal of Mathematical Analysis Vol., 08, no. 6, 5-57 HIKARI Ltd, www.m-hikai.com https://doi.og/0.988/ima.08.843 On Polynomials Constuction E. O. Adeyefa Depatment of Mathematics, Fedeal

More information

FUSE Fusion Utility Sequence Estimator

FUSE Fusion Utility Sequence Estimator FUSE Fusion Utility Sequence Estimato Belu V. Dasaathy Dynetics, Inc. P. O. Box 5500 Huntsville, AL 3584-5500 belu.d@dynetics.com Sean D. Townsend Dynetics, Inc. P. O. Box 5500 Huntsville, AL 3584-5500

More information

ME 210 Applied Mathematics for Mechanical Engineers

ME 210 Applied Mathematics for Mechanical Engineers Tangent and Ac Length of a Cuve The tangent to a cuve C at a point A on it is defined as the limiting position of the staight line L though A and B, as B appoaches A along the cuve as illustated in the

More information

ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0},

ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0}, ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION E. J. IONASCU and A. A. STANCU Abstact. We ae inteested in constucting concete independent events in puely atomic pobability

More information

CHAPTER 3. Section 1. Modeling Population Growth

CHAPTER 3. Section 1. Modeling Population Growth CHAPTER 3 Section 1. Modeling Population Gowth 1.1. The equation of the Malthusian model is Pt) = Ce t. Apply the initial condition P) = 1. Then 1 = Ce,oC = 1. Next apply the condition P1) = 3. Then 3

More information

A scaling-up methodology for co-rotating twin-screw extruders

A scaling-up methodology for co-rotating twin-screw extruders A scaling-up methodology fo co-otating twin-scew extudes A. Gaspa-Cunha, J. A. Covas Institute fo Polymes and Composites/I3N, Univesity of Minho, Guimaães 4800-058, Potugal Abstact. Scaling-up of co-otating

More information

Relating Branching Program Size and. Formula Size over the Full Binary Basis. FB Informatik, LS II, Univ. Dortmund, Dortmund, Germany

Relating Branching Program Size and. Formula Size over the Full Binary Basis. FB Informatik, LS II, Univ. Dortmund, Dortmund, Germany Relating Banching Pogam Size and omula Size ove the ull Binay Basis Matin Saueho y Ingo Wegene y Ralph Wechne z y B Infomatik, LS II, Univ. Dotmund, 44 Dotmund, Gemany z ankfut, Gemany sauehof/wegene@ls.cs.uni-dotmund.de

More information

Lecture 28: Convergence of Random Variables and Related Theorems

Lecture 28: Convergence of Random Variables and Related Theorems EE50: Pobability Foundations fo Electical Enginees July-Novembe 205 Lectue 28: Convegence of Random Vaiables and Related Theoems Lectue:. Kishna Jagannathan Scibe: Gopal, Sudhasan, Ajay, Swamy, Kolla An

More information

EM Boundary Value Problems

EM Boundary Value Problems EM Bounday Value Poblems 10/ 9 11/ By Ilekta chistidi & Lee, Seung-Hyun A. Geneal Desciption : Maxwell Equations & Loentz Foce We want to find the equations of motion of chaged paticles. The way to do

More information

Multiple Criteria Secretary Problem: A New Approach

Multiple Criteria Secretary Problem: A New Approach J. Stat. Appl. Po. 3, o., 9-38 (04 9 Jounal of Statistics Applications & Pobability An Intenational Jounal http://dx.doi.og/0.785/jsap/0303 Multiple Citeia Secetay Poblem: A ew Appoach Alaka Padhye, and

More information

Rigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018

Rigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018 Rigid Body Dynamics 2 CSE169: Compute Animation nstucto: Steve Rotenbeg UCSD, Winte 2018 Coss Poduct & Hat Opeato Deivative of a Rotating Vecto Let s say that vecto is otating aound the oigin, maintaining

More information

Surveillance Points in High Dimensional Spaces

Surveillance Points in High Dimensional Spaces Société de Calcul Mathématique SA Tools fo decision help since 995 Suveillance Points in High Dimensional Spaces by Benad Beauzamy Januay 06 Abstact Let us conside any compute softwae, elying upon a lage

More information

Bifurcation Analysis for the Delay Logistic Equation with Two Delays

Bifurcation Analysis for the Delay Logistic Equation with Two Delays IOSR Jounal of Mathematics (IOSR-JM) e-issn: 78-578, p-issn: 39-765X. Volume, Issue 5 Ve. IV (Sep. - Oct. 05), PP 53-58 www.iosjounals.og Bifucation Analysis fo the Delay Logistic Equation with Two Delays

More information

Control Chart Analysis of E k /M/1 Queueing Model

Control Chart Analysis of E k /M/1 Queueing Model Intenational OPEN ACCESS Jounal Of Moden Engineeing Reseach (IJMER Contol Chat Analysis of E /M/1 Queueing Model T.Poongodi 1, D. (Ms. S. Muthulashmi 1, (Assistant Pofesso, Faculty of Engineeing, Pofesso,

More information

A Deep Convolutional Neural Network Based on Nested Residue Number System

A Deep Convolutional Neural Network Based on Nested Residue Number System A Deep Convolutional Neual Netwok Based on Nested Residue Numbe System Hioki Nakahaa Ehime Univesity, Japan Tsutomu Sasao Meiji Univesity, Japan Abstact A pe-tained deep convolutional neual netwok (DCNN)

More information

Lifting Private Information Retrieval from Two to any Number of Messages

Lifting Private Information Retrieval from Two to any Number of Messages Lifting Pivate Infomation Retieval fom Two to any umbe of Messages Rafael G.L. D Oliveia, Salim El Rouayheb ECE, Rutges Univesity, Piscataway, J Emails: d746@scaletmail.utges.edu, salim.elouayheb@utges.edu

More information

arxiv: v1 [quant-ph] 15 Nov 2018

arxiv: v1 [quant-ph] 15 Nov 2018 Bayesian estimation of switching ates fo blinking emittes axiv:8.6627v [quant-ph] 5 Nov 28 Jemy Geody,, 2 Lachlan J Roges,, 2, Cameon M Roges, 3 Thomas Volz,, 2 and Alexei Gilchist, 2 Depatment of Physics

More information

Duality between Statical and Kinematical Engineering Systems

Duality between Statical and Kinematical Engineering Systems Pape 00, Civil-Comp Ltd., Stiling, Scotland Poceedings of the Sixth Intenational Confeence on Computational Stuctues Technology, B.H.V. Topping and Z. Bittna (Editos), Civil-Comp Pess, Stiling, Scotland.

More information

Linear Program for Partially Observable Markov Decision Processes. MS&E 339B June 9th, 2004 Erick Delage

Linear Program for Partially Observable Markov Decision Processes. MS&E 339B June 9th, 2004 Erick Delage Linea Pogam fo Patiall Obsevable Makov Decision Pocesses MS&E 339B June 9th 2004 Eick Delage Intoduction Patiall Obsevable Makov Decision Pocesses Etension of the Makov Decision Pocess to a wold with uncetaint

More information

International Journal of Mathematical Archive-3(12), 2012, Available online through ISSN

International Journal of Mathematical Archive-3(12), 2012, Available online through  ISSN Intenational Jounal of Mathematical Achive-3(), 0, 480-4805 Available online though www.ijma.info ISSN 9 504 STATISTICAL QUALITY CONTROL OF MULTI-ITEM EOQ MOEL WITH VARYING LEAING TIME VIA LAGRANGE METHO

More information

1 Explicit Explore or Exploit (E 3 ) Algorithm

1 Explicit Explore or Exploit (E 3 ) Algorithm 2.997 Decision-Making in Lage-Scale Systems Mach 3 MIT, Sping 2004 Handout #2 Lectue Note 9 Explicit Exploe o Exploit (E 3 ) Algoithm Last lectue, we studied the Q-leaning algoithm: [ ] Q t+ (x t, a t

More information

7.2. Coulomb s Law. The Electric Force

7.2. Coulomb s Law. The Electric Force Coulomb s aw Recall that chaged objects attact some objects and epel othes at a distance, without making any contact with those objects Electic foce,, o the foce acting between two chaged objects, is somewhat

More information

Centripetal Force OBJECTIVE INTRODUCTION APPARATUS THEORY

Centripetal Force OBJECTIVE INTRODUCTION APPARATUS THEORY Centipetal Foce OBJECTIVE To veify that a mass moving in cicula motion expeiences a foce diected towad the cente of its cicula path. To detemine how the mass, velocity, and adius affect a paticle's centipetal

More information

Markscheme May 2017 Calculus Higher level Paper 3

Markscheme May 2017 Calculus Higher level Paper 3 M7/5/MATHL/HP3/ENG/TZ0/SE/M Makscheme May 07 Calculus Highe level Pape 3 pages M7/5/MATHL/HP3/ENG/TZ0/SE/M This makscheme is the popety of the Intenational Baccalaueate and must not be epoduced o distibuted

More information

Chem 453/544 Fall /08/03. Exam #1 Solutions

Chem 453/544 Fall /08/03. Exam #1 Solutions Chem 453/544 Fall 3 /8/3 Exam # Solutions. ( points) Use the genealized compessibility diagam povided on the last page to estimate ove what ange of pessues A at oom tempeatue confoms to the ideal gas law

More information

Introduction to Nuclear Forces

Introduction to Nuclear Forces Intoduction to Nuclea Foces One of the main poblems of nuclea physics is to find out the natue of nuclea foces. Nuclea foces diffe fom all othe known types of foces. They cannot be of electical oigin since

More information

Truncated Squarers with Constant and Variable Correction

Truncated Squarers with Constant and Variable Correction Please veify that ) all pages ae pesent, 2) all figues ae acceptable, 3) all fonts and special chaactes ae coect, and ) all text and figues fit within the Tuncated Squaes with Constant and Vaiable Coection

More information

Physics 2B Chapter 22 Notes - Magnetic Field Spring 2018

Physics 2B Chapter 22 Notes - Magnetic Field Spring 2018 Physics B Chapte Notes - Magnetic Field Sping 018 Magnetic Field fom a Long Staight Cuent-Caying Wie In Chapte 11 we looked at Isaac Newton s Law of Gavitation, which established that a gavitational field

More information

Goodness-of-fit for composite hypotheses.

Goodness-of-fit for composite hypotheses. Section 11 Goodness-of-fit fo composite hypotheses. Example. Let us conside a Matlab example. Let us geneate 50 obsevations fom N(1, 2): X=nomnd(1,2,50,1); Then, unning a chi-squaed goodness-of-fit test

More information

Information Retrieval Advanced IR models. Luca Bondi

Information Retrieval Advanced IR models. Luca Bondi Advanced IR models Luca Bondi Advanced IR models 2 (LSI) Pobabilistic Latent Semantic Analysis (plsa) Vecto Space Model 3 Stating point: Vecto Space Model Documents and queies epesented as vectos in the

More information

16 Modeling a Language by a Markov Process

16 Modeling a Language by a Markov Process K. Pommeening, Language Statistics 80 16 Modeling a Language by a Makov Pocess Fo deiving theoetical esults a common model of language is the intepetation of texts as esults of Makov pocesses. This model

More information

The Implementation of the Conditions for the Existence of the Most Specific Generalizations w.r.t. General EL-TBoxes

The Implementation of the Conditions for the Existence of the Most Specific Generalizations w.r.t. General EL-TBoxes The Implementation of the Conditions fo the Existence of the Most Specific Genealizations w..t. Geneal EL-TBoxes Adian Nuadiansyah Technische Univesität Desden Supevised by: Anni-Yasmin Tuhan Febuay 12,

More information

ASTR415: Problem Set #6

ASTR415: Problem Set #6 ASTR45: Poblem Set #6 Cuan D. Muhlbege Univesity of Mayland (Dated: May 7, 27) Using existing implementations of the leapfog and Runge-Kutta methods fo solving coupled odinay diffeential equations, seveal

More information

Nuclear Medicine Physics 02 Oct. 2007

Nuclear Medicine Physics 02 Oct. 2007 Nuclea Medicine Physics Oct. 7 Counting Statistics and Eo Popagation Nuclea Medicine Physics Lectues Imaging Reseach Laboatoy, Radiology Dept. Lay MacDonald 1//7 Statistics (Summaized in One Slide) Type

More information

An extended target tracking method with random finite set observations

An extended target tracking method with random finite set observations 4th Intenational Confeence on Infomation Fusion Chicago Illinois USA July 5-8 0 An extended taget tacing method with andom finite set obsevations Hongyan Zhu Chongzhao Han Chen Li Dept. of Electonic &

More information

A Multivariate Normal Law for Turing s Formulae

A Multivariate Normal Law for Turing s Formulae A Multivaiate Nomal Law fo Tuing s Fomulae Zhiyi Zhang Depatment of Mathematics and Statistics Univesity of Noth Caolina at Chalotte Chalotte, NC 28223 Abstact This pape establishes a sufficient condition

More information

State tracking control for Takagi-Sugeno models

State tracking control for Takagi-Sugeno models State tacing contol fo Taagi-Sugeno models Souad Bezzaoucha, Benoît Max,3,DidieMaquin,3 and José Ragot,3 Abstact This wo addesses the model efeence tacing contol poblem It aims to highlight the encouteed

More information

COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS

COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS Pogess In Electomagnetics Reseach, PIER 73, 93 105, 2007 COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS T.-X. Song, Y.-H. Liu, and J.-M. Xiong School of Mechanical Engineeing

More information

Utility Estimation and Preference Aggregation under Uncertainty by Maximum Entropy Inference

Utility Estimation and Preference Aggregation under Uncertainty by Maximum Entropy Inference Utility Estimation and Pefeence Aggegation unde Uncetainty by Maximum Entopy Infeence Andé Ahua FenUnivesität in Hagen D-5884 Hagen ande.ahua@fenuni-hagen.de ABSTRACT. This pape deals with the poblem how

More information

Classical Worm algorithms (WA)

Classical Worm algorithms (WA) Classical Wom algoithms (WA) WA was oiginally intoduced fo quantum statistical models by Pokof ev, Svistunov and Tupitsyn (997), and late genealized to classical models by Pokof ev and Svistunov (200).

More information

CASCADE OPTIMIZATION AND CONTROL OF BATCH REACTORS

CASCADE OPTIMIZATION AND CONTROL OF BATCH REACTORS CASCADE OPIMIZAION AND CONROL OF BACH REACORS Xiangming Hua, Sohab Rohani and Athu Jutan* Depatment of Chemical and Biochemical Engineeing Univesity of Westen Ontaio, London, Canada N6A B9 * ajutan@uwo.ca

More information

Temporal-Difference Learning

Temporal-Difference Learning .997 Decision-Making in Lage-Scale Systems Mach 17 MIT, Sping 004 Handout #17 Lectue Note 13 1 Tempoal-Diffeence Leaning We now conside the poblem of computing an appopiate paamete, so that, given an appoximation

More information

HYBRID FDI ON CHEMICAL PLANTS. Ferreiro García, Ramón; Pardo Martínez, Xoán C. & Vidal Paz, José

HYBRID FDI ON CHEMICAL PLANTS. Ferreiro García, Ramón; Pardo Martínez, Xoán C. & Vidal Paz, José HYBRID FDI ON CHEMICL PLNTS Feeio Gacía, Ramón; Pado Matínez, Xoán C. & Vidal Paz, José Gupo de Enxeñeia de Sistemas e Contol utomático. Depatamento de Electónica e Sistemas. Univesidade da Couña. E.S.

More information

A NEW VARIABLE STIFFNESS SPRING USING A PRESTRESSED MECHANISM

A NEW VARIABLE STIFFNESS SPRING USING A PRESTRESSED MECHANISM Poceedings of the ASME 2010 Intenational Design Engineeing Technical Confeences & Computes and Infomation in Engineeing Confeence IDETC/CIE 2010 August 15-18, 2010, Monteal, Quebec, Canada DETC2010-28496

More information

On the Meaning of Message Sequence Charts

On the Meaning of Message Sequence Charts On the Meaning of Message Sequence Chats Manfed Boy Institut fü Infomatik Technische Univesität München Topics: We discuss Message Sequence Chats (MSCs) as a technique to descibe pattens of the inteaction

More information

Hammerstein Model Identification Based On Instrumental Variable and Least Square Methods

Hammerstein Model Identification Based On Instrumental Variable and Least Square Methods Intenational Jounal of Emeging Tends & Technology in Compute Science (IJETTCS) Volume 2, Issue, Januay Febuay 23 ISSN 2278-6856 Hammestein Model Identification Based On Instumental Vaiable and Least Squae

More information

Encapsulation theory: the transformation equations of absolute information hiding.

Encapsulation theory: the transformation equations of absolute information hiding. 1 Encapsulation theoy: the tansfomation equations of absolute infomation hiding. Edmund Kiwan * www.edmundkiwan.com Abstact This pape descibes how the potential coupling of a set vaies as the set is tansfomed,

More information

Reading Assignment. Problem Description for Homework #9. Read Chapters 29 and 30.

Reading Assignment. Problem Description for Homework #9. Read Chapters 29 and 30. Reading Assignment Read Chaptes 29 and 30. Poblem Desciption fo Homewok #9 In this homewok, you will solve the inhomogeneous Laplace s equation to calculate the electic scala potential that exists between

More information

STABILITY AND PARAMETER SENSITIVITY ANALYSES OF AN INDUCTION MOTOR

STABILITY AND PARAMETER SENSITIVITY ANALYSES OF AN INDUCTION MOTOR HUNGARIAN JOURNAL OF INDUSTRY AND CHEMISTRY VESZPRÉM Vol. 42(2) pp. 109 113 (2014) STABILITY AND PARAMETER SENSITIVITY ANALYSES OF AN INDUCTION MOTOR ATTILA FODOR 1, ROLAND BÁLINT 1, ATTILA MAGYAR 1, AND

More information

A Converse to Low-Rank Matrix Completion

A Converse to Low-Rank Matrix Completion A Convese to Low-Rank Matix Completion Daniel L. Pimentel-Alacón, Robet D. Nowak Univesity of Wisconsin-Madison Abstact In many pactical applications, one is given a subset Ω of the enties in a d N data

More information

Analytical Solutions for Confined Aquifers with non constant Pumping using Computer Algebra

Analytical Solutions for Confined Aquifers with non constant Pumping using Computer Algebra Poceedings of the 006 IASME/SEAS Int. Conf. on ate Resouces, Hydaulics & Hydology, Chalkida, Geece, May -3, 006 (pp7-) Analytical Solutions fo Confined Aquifes with non constant Pumping using Compute Algeba

More information

arxiv: v1 [math.co] 1 Apr 2011

arxiv: v1 [math.co] 1 Apr 2011 Weight enumeation of codes fom finite spaces Relinde Juius Octobe 23, 2018 axiv:1104.0172v1 [math.co] 1 Ap 2011 Abstact We study the genealized and extended weight enumeato of the - ay Simplex code and

More information

Notes on McCall s Model of Job Search. Timothy J. Kehoe March if job offer has been accepted. b if searching

Notes on McCall s Model of Job Search. Timothy J. Kehoe March if job offer has been accepted. b if searching Notes on McCall s Model of Job Seach Timothy J Kehoe Mach Fv ( ) pob( v), [, ] Choice: accept age offe o eceive b and seach again next peiod An unemployed oke solves hee max E t t y t y t if job offe has

More information

Lecture 8 - Gauss s Law

Lecture 8 - Gauss s Law Lectue 8 - Gauss s Law A Puzzle... Example Calculate the potential enegy, pe ion, fo an infinite 1D ionic cystal with sepaation a; that is, a ow of equally spaced chages of magnitude e and altenating sign.

More information

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in Supplementay Figue 1. Cicula paallel lamellae gain size as a function of annealing time at 50 C. Eo bas epesent the σ uncetainty in the measued adii based on image pixilation and analysis uncetainty contibutions

More information

Analytical time-optimal trajectories for an omni-directional vehicle

Analytical time-optimal trajectories for an omni-directional vehicle Analytical time-optimal tajectoies fo an omni-diectional vehicle Weifu Wang and Devin J. Balkcom Abstact We pesent the fist analytical solution method fo finding a time-optimal tajectoy between any given

More information

To Feel a Force Chapter 7 Static equilibrium - torque and friction

To Feel a Force Chapter 7 Static equilibrium - torque and friction To eel a oce Chapte 7 Chapte 7: Static fiction, toque and static equilibium A. Review of foce vectos Between the eath and a small mass, gavitational foces of equal magnitude and opposite diection act on

More information

Power efficiency and optimum load formulas on RF rectifiers featuring flow-angle equations

Power efficiency and optimum load formulas on RF rectifiers featuring flow-angle equations LETTE IEICE Electonics Expess, Vol.10, No.11, 1 9 Powe efficiency and optimum load fomulas on F ectifies featuing flow-angle equations Takashi Ohia a) Toyohashi Univesity of Technology, 1 1 Hibaigaoka,

More information

Circular Orbits. and g =

Circular Orbits. and g = using analyse planetay and satellite motion modelled as unifom cicula motion in a univesal gavitation field, a = v = 4π and g = T GM1 GM and F = 1M SATELLITES IN OBIT A satellite is any object that is

More information

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS The 8 th Intenational Confeence of the Slovenian Society fo Non-Destuctive Testing»pplication of Contempoay Non-Destuctive Testing in Engineeing«Septembe 1-3, 5, Potoož, Slovenia, pp. 17-1 MGNETIC FIELD

More information

Suggested Solutions to Homework #4 Econ 511b (Part I), Spring 2004

Suggested Solutions to Homework #4 Econ 511b (Part I), Spring 2004 Suggested Solutions to Homewok #4 Econ 5b (Pat I), Sping 2004. Conside a neoclassical gowth model with valued leisue. The (epesentative) consume values steams of consumption and leisue accoding to P t=0

More information

Review: Electrostatics and Magnetostatics

Review: Electrostatics and Magnetostatics Review: Electostatics and Magnetostatics In the static egime, electomagnetic quantities do not vay as a function of time. We have two main cases: ELECTROSTATICS The electic chages do not change postion

More information

, the tangent line is an approximation of the curve (and easier to deal with than the curve).

, the tangent line is an approximation of the curve (and easier to deal with than the curve). 114 Tangent Planes and Linea Appoimations Back in-dimensions, what was the equation of the tangent line of f ( ) at point (, ) f ( )? (, ) ( )( ) = f Linea Appoimation (Tangent Line Appoimation) of f at

More information

Recent Advances in Chemical Engineering, Biochemistry and Computational Chemistry

Recent Advances in Chemical Engineering, Biochemistry and Computational Chemistry Themal Conductivity of Oganic Liquids: a New Equation DI NICOLA GIOVANNI*, CIARROCCHI ELEONORA, PIERANTOZZI ARIANO, STRYJEK ROAN 1 DIIS, Univesità Politecnica delle ache, 60131 Ancona, ITALY *coesponding

More information

A matrix method based on the Fibonacci polynomials to the generalized pantograph equations with functional arguments

A matrix method based on the Fibonacci polynomials to the generalized pantograph equations with functional arguments A mati method based on the Fibonacci polynomials to the genealized pantogaph equations with functional aguments Ayşe Betül Koç*,a, Musa Çama b, Aydın Kunaz a * Coespondence: aysebetuloc @ selcu.edu.t a

More information

Solution to HW 3, Ma 1a Fall 2016

Solution to HW 3, Ma 1a Fall 2016 Solution to HW 3, Ma a Fall 206 Section 2. Execise 2: Let C be a subset of the eal numbes consisting of those eal numbes x having the popety that evey digit in the decimal expansion of x is, 3, 5, o 7.

More information

Chapter 3 Optical Systems with Annular Pupils

Chapter 3 Optical Systems with Annular Pupils Chapte 3 Optical Systems with Annula Pupils 3 INTRODUCTION In this chapte, we discuss the imaging popeties of a system with an annula pupil in a manne simila to those fo a system with a cicula pupil The

More information

biologically-inspired computing lecture 9 Informatics luis rocha 2015 INDIANA UNIVERSITY biologically Inspired computing

biologically-inspired computing lecture 9 Informatics luis rocha 2015 INDIANA UNIVERSITY biologically Inspired computing luis ocha 25 lectue 9 -inspied luis ocha 25 Sections I485/H4 couse outlook Assignments: 35% Students will complete 4/5 assignments based on algoithms pesented in class Lab meets in I (West) 9 on Lab Wednesdays

More information

Evolutionary approach to Quantum and Reversible Circuits synthesis

Evolutionary approach to Quantum and Reversible Circuits synthesis Evolutionay appoach to Quantum and Revesible Cicuits synthesis Matin Lukac, Maek Pekowski, Hilton Goi, Mikhail Pivtoaiko +, Chung Hyo Yu, Kyusik Chung, Hyunkoo Jee, Byung-guk Kim, Yong-Duk Kim Depatment

More information

Fresnel Diffraction. monchromatic light source

Fresnel Diffraction. monchromatic light source Fesnel Diffaction Equipment Helium-Neon lase (632.8 nm) on 2 axis tanslation stage, Concave lens (focal length 3.80 cm) mounted on slide holde, iis mounted on slide holde, m optical bench, micoscope slide

More information

Heat transfer has direction as well as magnitude. The rate of heat conduction

Heat transfer has direction as well as magnitude. The rate of heat conduction cen58933_ch2.qd 9/1/22 8:46 AM Page 61 HEAT CONDUCTION EQUATION CHAPTER 2 Heat tansfe has diection as well as magnitude. The ate of heat conduction in a specified diection is popotional to the tempeatue

More information

Hypothesis Test and Confidence Interval for the Negative Binomial Distribution via Coincidence: A Case for Rare Events

Hypothesis Test and Confidence Interval for the Negative Binomial Distribution via Coincidence: A Case for Rare Events Intenational Jounal of Contempoay Mathematical Sciences Vol. 12, 2017, no. 5, 243-253 HIKARI Ltd, www.m-hikai.com https://doi.og/10.12988/ijcms.2017.7728 Hypothesis Test and Confidence Inteval fo the Negative

More information

In many engineering and other applications, the. variable) will often depend on several other quantities (independent variables).

In many engineering and other applications, the. variable) will often depend on several other quantities (independent variables). II PARTIAL DIFFERENTIATION FUNCTIONS OF SEVERAL VARIABLES In man engineeing and othe applications, the behaviou o a cetain quantit dependent vaiable will oten depend on seveal othe quantities independent

More information

Rate Splitting is Approximately Optimal for Fading Gaussian Interference Channels

Rate Splitting is Approximately Optimal for Fading Gaussian Interference Channels Rate Splitting is Appoximately Optimal fo Fading Gaussian Intefeence Channels Joyson Sebastian, Can Kaakus, Suhas Diggavi, I-Hsiang Wang Abstact In this pape, we study the -use Gaussian intefeence-channel

More information

Exploration of the three-person duel

Exploration of the three-person duel Exploation of the thee-peson duel Andy Paish 15 August 2006 1 The duel Pictue a duel: two shootes facing one anothe, taking tuns fiing at one anothe, each with a fixed pobability of hitting his opponent.

More information

Conservative Averaging Method and its Application for One Heat Conduction Problem

Conservative Averaging Method and its Application for One Heat Conduction Problem Poceedings of the 4th WSEAS Int. Conf. on HEAT TRANSFER THERMAL ENGINEERING and ENVIRONMENT Elounda Geece August - 6 (pp6-) Consevative Aveaging Method and its Application fo One Heat Conduction Poblem

More information

Coupled Electromagnetic and Heat Transfer Simulations for RF Applicator Design for Efficient Heating of Materials

Coupled Electromagnetic and Heat Transfer Simulations for RF Applicator Design for Efficient Heating of Materials Coupled Electomagnetic and Heat Tansfe Simulations fo RF Applicato Design fo Efficient Heating of Mateials Jeni Anto 1 and Raj C Thiagaajan 2 * 1 Reseache, Anna Univesity, Chennai, 2 ATOA Scientific Technologies

More information

MATH 415, WEEK 3: Parameter-Dependence and Bifurcations

MATH 415, WEEK 3: Parameter-Dependence and Bifurcations MATH 415, WEEK 3: Paamete-Dependence and Bifucations 1 A Note on Paamete Dependence We should pause to make a bief note about the ole played in the study of dynamical systems by the system s paametes.

More information

LINEAR AND NONLINEAR ANALYSES OF A WIND-TUNNEL BALANCE

LINEAR AND NONLINEAR ANALYSES OF A WIND-TUNNEL BALANCE LINEAR AND NONLINEAR ANALYSES O A WIND-TUNNEL INTRODUCTION BALANCE R. Kakehabadi and R. D. Rhew NASA LaRC, Hampton, VA The NASA Langley Reseach Cente (LaRC) has been designing stain-gauge balances fo utilization

More information

Steady State and Transient Performance Analysis of Three Phase Induction Machine using MATLAB Simulations

Steady State and Transient Performance Analysis of Three Phase Induction Machine using MATLAB Simulations Intenational Jounal of Recent Tends in Engineeing, Vol, No., May 9 Steady State and Tansient Pefomance Analysis of Thee Phase Induction Machine using MATAB Simulations Pof. Himanshu K. Patel Assistant

More information

Lab #4: Newton s Second Law

Lab #4: Newton s Second Law Lab #4: Newton s Second Law Si Isaac Newton Reading Assignment: bon: Januay 4, 1643 Chapte 5 died: Mach 31, 1727 Chapte 9, Section 9-7 Intoduction: Potait of Isaac Newton by Si Godfey Knelle http://www.newton.cam.ac.uk/at/potait.html

More information

Gauss Law. Physics 231 Lecture 2-1

Gauss Law. Physics 231 Lecture 2-1 Gauss Law Physics 31 Lectue -1 lectic Field Lines The numbe of field lines, also known as lines of foce, ae elated to stength of the electic field Moe appopiately it is the numbe of field lines cossing

More information

Basic Gray Level Transformations (2) Negative

Basic Gray Level Transformations (2) Negative Gonzalez & Woods, 22 Basic Gay Level Tansfomations (2) Negative 23 Basic Gay Level Tansfomations (3) Log Tansfomation (Example fo Fouie Tansfom) Fouie spectum values ~1 6 bightest pixels dominant display

More information